The Fine-Tuning of the Universe for Intelligent Life
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Fiziksel yasalar, sabitler ve başlangıç koşullarındaki ince ayar literatürünü değerlendirir.
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Claims the paper makes
22 of 167 cited sources checked · 6 supported · 2 flagged · accuracy not yet measured
- Premisecitation
The universe re-collapses before life can form for rho_L greater than about -10^-121.
“The universe re-collapses before life can form for r L t À10 À121 (Peacock 2007).”
Quote in the paperNot a substantial claim1 of 1 sources checked- cites Peacock 2007 source
Section 3 says that highly negative vacuum densities can make the universe turn around before it cools enough for observer formation. That is the opposite direction from the claimed threshold of greater than −10^-121. Our copy also does not state that numerical threshold. (LLM, conf=0.86)
Checked by a reasoning model — may be wrong.
Experimental — accuracy not yet measured
- Interpretationcitation
The evidence that inflation actually happened is quite strong, though not indubitable.
“The evidence is quite strong, though not indubitable (Turok 2002;Brandenberger 2011).”
Quote in the paperNot a substantial claim1 of 2 sources checked- cites Turok 2002 source
Section 4, “Inflationary perturbations” (page unavailable), says observations had tested the HPZ hypothesis rather than inflation itself, and that the observed pattern is not specific to inflation. Section 6 also describes a paucity of observational tests. Turok thus cautions against treating the evidence as strong evidence that inflation actually happened. (LLM, conf=0.84)
Checked by a reasoning model — may be wrong.
Experimental — accuracy not yet measured - cites Brandenberger 2011
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisecitation
Life-permitting inflation potentials are highly unnatural.
“Tegmark (2005, partic-ularly figure 11) argues that on very general grounds we can conclude that life-permitting inflation potentials are highly unnatural.”
Quote in the paperNot a substantial claim1 of 1 sources checked- cites Tegmark (2005) source
Figure 11 describes the physically natural expectation for the potential’s energy scales and says the hoped-for model matching the observed fluctuation amplitude does not work in the models examined. The paper also says some models require tuning, but it does not conclude on very general grounds that all life-permitting inflation potentials are highly unnatural; it notes a potentially more compatible natural expectation in supersymmetric models. Our copy provides no page number for these passages. (LLM, conf=0.85)
Experimental — accuracy not yet measured
- Findingcitation
For the model of Tegmark (2005), the mean value of Q ranges from 10 to almost 10,000.
“The upper blue region of Figure 4 shows the distribution of Q for the model of Tegmark (2005), using the 'physically natural expectation' m v ¼ m h .The mean value of Q ranges from 10 to almost 10 000.”
Quote in the paperSubstantial claim1 of 1 sources checked- cites Tegmark (2005) source
Section 5.1 describes Tegmark’s model and says its energy scales may naturally satisfy m_h ∼ m_v, supporting the identification of the model used in the citing paper. Our copy does not report a mean Q ranging from 10 to nearly 10,000; instead, its discussion of the Q distribution says quantum diffusion cuts it off around Q ∼ 1. The numerical range appears to be the citing paper’s result, not a value established by this source. (LLM, conf=0.85)
Experimental — accuracy not yet measured
- Premisecitation
The life-permitting range for Q is given by the inequality (3) derived by Tegmark & Rees (1998).
“Tegmark & Rees (1998) were the first to calculate the range of Q which permits life, deriving the following limits for the case where r L ¼ 0:”
Quote in the paperSubstantial claim1 of 1 sources checked- cites Tegmark & Rees (1998) source
Section 3 derives an approximate upper limit of Q ≲ 10⁻⁴, and Section 6 identifies cooling difficulties below Q ≈ 10⁻⁶; the paper says its main analysis assumes a flat universe with zero cosmological constant. But Section 6 explicitly allows that life might arise at more extreme Q values, so these are not strict life-permitting bounds. Our copy also does not establish the claim that Tegmark and Rees were the first to calculate them. (LLM, conf=0.85)
Experimental — accuracy not yet measured
- Interpretationcitation
A given inflationary model will only predict a life-permitting value for Q if the parameters of the inflaton potential are suitably fine-tuned.
“A given inflationary model will predict Q, and it will only predict a lifepermitting value for Q if the parameters of the inflaton potential are suitably fine-tuned.”
Quote in the paperSubstantial claim1 of 1 sources checked- cites Turok (2002) source
Section 3, “Inflationary quantum fluctuations” (page not available), says that in the power-law inflaton-potential model discussed, obtaining the observed density-perturbation amplitude requires adjusting the coupling to a very small value, which it calls a fine-tuning problem. It does not establish a life-permitting range for Q or show that every given inflationary model requires such tuning. (LLM, conf=0.86)
Experimental — accuracy not yet measured
- Premisecitation
To obtain density perturbations of the level required by observations, the coupling m for a power law potential mf^n must be very small, ~10^-13 in Planck units.
“to obtain density perturbations of the level required by observations ywe need to adjust the coupling m [for a power law potential mf n ] to be very small, ,10 À13 in Planck units.This is the famous fine-tuning problem of inflation”
Quote in the paperSubstantial claim1 of 1 sources checked- cites Turok (2002) source
- Interpretationcitation
Quintessence models must be fine-tuned in exactly the same way as the cosmological constant.
“Quintessence models must be fine-tuned in exactly the same way as the cosmological constant (see also Durrer & Maartens 2007).”
Quote in the paperSubstantial claim1 of 2 sources checked- cites Peacock (2007) source
The Introduction says a simple quintessence model appears to require introducing an energy scale by hand, and that quintessence models do not solve the scale problem. It does not say that all quintessence models must be fine-tuned in exactly the same way as the cosmological constant. Page numbers are unavailable in our copy. (LLM, conf=0.86)
Experimental — accuracy not yet measured - cites Durrer & Maartens 2007
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationcitation
An appeal to the multiverse is motivated by and dependent on the fine-tuning of the cosmological constant.
“Here we note what Stenger doesn't: an appeal to the multiverse is motivated by and dependent on the fine-tuning of the cosmological constant.”
Quote in the paperSubstantial claim1 of 3 sources checked- cites Arkani-Hamed, Dimopoulos & Kachru 2005 source
Section 1 (p. 2) presents the cosmological constant’s extreme smallness as an unsolved naturalness problem, and Section 2.1 (p. 9) says the paper’s landscape has the many vacua needed to address it. This supports fine-tuning as a motivation for the landscape approach, but not the broader assertion that an appeal to the multiverse depends on cosmological-constant fine-tuning; the Outlook (p. 44) also describes addressing hierarchy problems. (LLM, conf=0.83)
Experimental — accuracy not yet measured - cites Susskind 2005
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- cites Bousso 2008
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisecitation
Many mechanisms aimed at selecting a small value for r_L can only explain why the cosmological constant vanishes in an empty universe.
“Polchinski (2006) notes that many of the mechanisms aimed at selecting a small value for r L -the Hawking-Hartle wavefunction, the de Sitter entropy and the Coleman-de Luccia amplitude for tunneling -can only explain why the cosmological constant vanishes in an empty universe.”
Quote in the paperSubstantial claim1 of 1 sources checked- cites Polchinski (2006) source
In §1.2 (pp. 10–11), Polchinski names the Hartle–Hawking wavefunction, de Sitter entropy, and Coleman–de Luccia tunneling, then argues that these gravitational mechanisms can act on the cosmological constant only when matter is essentially absent. But he says they favor the smallest positive value, not that they explain why the cosmological constant vanishes exactly; he also states that zero cannot be a special value (p. 10). (LLM, conf=0.87)
Experimental — accuracy not yet measured
- Interpretationcitation
Stenger's assertion that there is no fine-tuning problem for quintessence is false.
“Stenger's assertion that there is no fine-tuning problem for quintessence is false, as a number of authors have pointed out.”
Quote in the paperSubstantial claim1 of 2 sources checked- cites Peacock (2007) source
- cites Durrer & Maartens 2007
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisecitation
Only ~1% of the oxygen in our universe comes from accretion supernovae.
“Only ,1% of the oxygen in our universe comes from accretion supernovae.”
Quote in the paperSubstantial claim1 of 1 sources checked- cites Clavelli & White 2006 source
- Premisecitation
The absence of core-collapse supernovae will seriously affect the oxygen available for planet formation and life.
“Stars will still be able to undergo accretion supernovae (Type 1a), but the absence of core-collapse supernovae will seriously affect the oxygen available for planet formation and life (Clavelli & White 2006).”
Quote in the paperSubstantial claim1 of 1 sources checked- cites Clavelli & White 2006 source
- Findingreasoning
For every observer in a universe as old as ours, there are 10^10^38 observers who live in a universe that is one second younger.
“For every observer in a universe as old as ours, there are 10 10 38 observers who live in a universe that is one second younger.”
Quote in the paperSubstantial claim1 of 1 sources checked- cites Tegmark (2005) source
In the discussion of time ordering (JCAP04(2005)001; page unavailable), the paper gives a probability of about 10^-10^38 for a universe as cool as ours relative to one that is one second younger, supporting the quoted ratio. But it presents this as a consequence of a particular time-ordering measure, which it concludes is wrong—not as an unconditional count of observers. (LLM, conf=0.88)
Experimental — accuracy not yet measured
- Findingreasoning
The probability of observing a universe with a CMB temperature of 2.75 K or less is approximately 1 in 10^10^56.
“The probability of observing a universe with a CMB temperature of 2.75 K or less is approximately 1 in 10 10 56 .”
Quote in the paperSubstantial claim1 of 1 sources checked- cites Tegmark (2005) source
In §7.3, equation (91) gives approximately 10^−10^56 for a CMB temperature below 3 K, under an eternal-inflation model with time ordering. The paper says the probability at the observed temperature of 2.728 ± 0.004 K is even smaller; it does not give that probability for 2.75 K or less. (LLM, conf=0.88)
Experimental — accuracy not yet measured
- Interpretationcitation
It is not clear whether the cold big bang island connects to the hot big bang island (10^6 < Z_g < 10^11) investigated by Tegmark & Rees (1998).
“Aguirre (2001) only considers the case Z g , 1 in detail, so it is not clear whether the CBB island connects to the HBB island (10 6 t Z g t 10 11 ) investigated by Tegmark & Rees (1998).”
Quote in the paperSubstantial claim1 of 2 sources checked- cites Aguirre (2001)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- cites Tegmark & Rees (1998) source
Section 6 (Discussion; page unavailable) says Tegmark and Rees explored cosmological scenarios with different values of Q. Section 2.1 (Notation; page unavailable) gives a baryon-to-photon ratio, but our copy does not identify a hot-big-bang island with 10^6 < Z_g < 10^11. Searches for Z_g, that interval, and hot- or cold-big-bang islands found no passage establishing the cited identification; the uncertainty about whether the islands connect is the citing authors’ own statement. (LLM, conf=0.72)
Experimental — accuracy not yet measured
- Findingreasoning
The probability calculated by varying only one parameter is actually an overestimate of the probability calculated using the full wedge.
“The probability calculated by varying only one parameter is actually an overestimate of the probability calculated using the full wedge.”
Quote in the paperSubstantial claim- The authors state this as an assumption: The probability distribution over the parameters x and y is uniform.
- The authors state this as an assumption: The possible range of y can be conservatively estimated by y0.
- The authors state this as an assumption: The full life-permitting criterion that defines the wedge is given by the equation 1 - y/x = (y0/x0)(1 + epsilon).
- Findingcitation
When parameter space is explored in the scientific literature, it rarely if ever looks like the wedge; instead many intersecting wedges are seen.
“When parameter space is explored in the scientific literature, it rarely (if ever) looks like the wedge.We instead see many intersecting wedges.”
Quote in the paperSubstantial claim - Findingnone given
A power-law prior has no significant effect on the wedge.
“One can show that a power-law prior has no significant effect on the wedge.”
Quote in the paperNot a substantial claim - Findingnone given
13.7 billion years of concordance model expansion will blow up a Planck volume until it is roughly the size of a grain of sand.
“13.7 billion years of (concordance model) expansion will blow up this Planck volume until it is roughly the size of a grain of sand.”
Quote in the paperNot a substantial claim - Findingreasoning
The observed value of Q (~10^-5) isn't close to either edge of the anthropic range.
“The observed value (,10 À5 ) isn't close to either edge of the anthropic range.”
Quote in the paperSubstantial claim - Premisecitation
General relativity is not the only covariant theory of spacetime.
“General relativity is not the only covariant theory of spacetime (Norton 1995).”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Norton 1995 source
- Interpretationreasoning
The anthropic principle cannot explain why life and its necessary conditions exist at all.
“Similarly, AP cannot explain why life and its necessary conditions exist at all.”
Quote in the paperSubstantial claim - Premisecitation
Very small changes in the laws, parameters and initial conditions of physics would result in a universe unable to evolve and support intelligent life.
“Beginning with the classic papers of Carter (1974) and Carr & Rees (1979), and the extensive discussion of Barrow & Tipler (1986), a number of authors have noticed that very small changes in the laws, parameters and initial conditions of physics would result in a universe unable to evolve and support intelligent life.”
Quote in the paperSubstantial claim0 of 3 sources checked - Interpretationreasoning
Physicists do not have to put gravity into any model of the universe that contains separate masses.
“Physicists clearly don't have to put gravity into any model of the universe that contains separate masses.”
Quote in the paperNot a substantial claim - Interpretationreasoning
A selection bias alone cannot explain anything.
“A selection bias alone cannot explain anything.”
Quote in the paperNot a substantial claim - Interpretationreasoning
The density needed for life, the critical density, and the actual density of our universe are all aligned.
“There is in fact a three-fold coincidence -A: the density needed for life, B: the critical density, and C: the actual density of our universe are all aligned.”
Quote in the paperSubstantial claim- Rests on an assumption: The range of densities that permit the existence of cosmic structure in a long-lived universe is very narrow.
- Rests on an assumption: The range of densities that permit cosmic structure neatly straddles the critical density.
- Interpretationreasoning
The conservation principles of this universe are not merely principles governing our formulation of the laws of nature.
“The conservation principles of this universe are not merely principles governing our formulation of the laws of nature.”
Quote in the paperSubstantial claim - Premisecitation
The gauge group of the standard model, SU(3) × SU(2) × U(1), is far from unique.
“The gauge group of the standard model, SU(3) Â SU(2) Â U(1), is far from unique.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Schellekens 2008
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationreasoning
Given general covariance (or PoVI), the additional assumptions constitute the entire empirical content of the theory.
“Given general covariance (or PoVI), the additional assumptions constitute the entire empirical content of the theory.”
Quote in the paperNot a substantial claim - Interpretationreasoning
For a universe to be life-permitting, it must satisfy a number of constraints simultaneously.
“For a universe to be life-permitting, it must satisfy a number of constraints simultaneously.”
Quote in the paperSubstantial claim - Premisecitation
Special relativity is perfectly able to preserve invariance between reference frames accelerating with respect to one another.
“Special relativity is perfectly able to preserve invariance between reference frames accelerating with respect to one another.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Hartle (2003) source
- Interpretationreasoning
A universe with G=0 is a counterexample to Stenger's assertion that no gravity means no universe.
“This G ¼ 0 universe is a counterexample to Stenger's assertion that no gravity means no universe.”
Quote in the paperSubstantial claim - Interpretationreasoning
Stenger's argument that the laws of nature could not have been different because they can be derived from PoVI commits the fallacy of equivocation, because the term 'invariant' changes meaning between LN1 and LN2.
“This argument commits the fallacy of equivocation -the term 'invariant' has changed its meaning between LN1 and LN2.”
Quote in the paperSubstantial claim - Premisenone given
The violation of Lorentz invariance is currently just a theoretical possibility.
“At the moment, the violation of Lorentz invariance is just a theoretical possibility.”
Quote in the paperNot a substantial claim - Premisecitation
The principle of general covariance is useless as a sieve for separating viable theories from nonviable theories.
“Hence, as a sieve for separating viable theories from nonviable theories, the principle of general covariance is useless.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Misner, Thorne & Wheeler (1973)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationnone given
We cannot deduce gauge invariance from PoVI.
“We cannot deduce gauge invariance from PoVI.”
Quote in the paperNot a substantial claim - Interpretationnone given
None of the invariant/covariant properties of general relativity depend on the value of Newton's constant G.
“None of the invariant/ covariant properties of general relativity depend on the value of Newton's constant G.”
Quote in the paperNot a substantial claim - Interpretationreasoning
One cannot refute FT by considering life-permitting criteria one-at-a-time and noting that each can be satisfied in a wide region of parameter space.
“One cannot refute FT by considering life-permitting criteria one-at-a-time and noting that each can be satisfied in a wide region of parameter space.”
Quote in the paperNot a substantial claim - Premisecitation
Supersymmetry must be a broken symmetry in any life-permitting universe, since the selectron would make chemistry impossible.
“Supersymmetry, too, must be a broken symmetry in any lifepermitting universe, since the bosonic partner of the electron (the selectron) would make chemistry impossible (see the discussion in Susskind 2005, p. 250).”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Susskind 2005
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationnone given
The perfect homogeneity and isotropy of the Robertson-Walker spacetime precludes the possibility of any form of complexity, including life.
“For example, the perfect homogeneity and isotropy of the Robertson-Walker spacetime precludes the possibility of any form of complexity, including life.”
Quote in the paperNot a substantial claim - Interpretationreasoning
PoVI does not imply symmetry.
“This is Stenger's confusion: PoVI does not imply symmetry.”
Quote in the paperNot a substantial claim - Premisecitation
A universe governed by Maxwell's Laws all the way down, with no quantum regime at small scales, would not have stable atoms and hence no chemistry.
“A universe governed by Maxwell's Laws 'all the way down' (i.e. with no quantum regime at small scales) would not have stable atoms -electrons radiate their kinetic energy and spiral rapidly into the nucleus -and hence no chemistry (Barrow & Tipler 1986, p. 303).”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Barrow & Tipler 1986
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisecitation
MacDonald & Mullan (2009) and Bradford (2009) have shown that binding of the diproton is not sufficient to burn all the hydrogen to helium in big bang nucleosynthesis.
“MacDonald & Mullan (2009) and Bradford (2009) have shown that the binding of the diproton is not sufficient to burn all the hydrogen to helium in big bang nucleosynthesis.”
Quote in the paperSubstantial claim0 of 2 sources checked- cites MacDonald & Mullan (2009)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- cites Bradford (2009)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisecitation
Collins (2003) noted that decay of the diproton will happen too slowly for the resulting deuteron to be converted into helium, leaving at least some deuterium to power stars and take the place of hydrogen in organic compounds.
“Also, Collins (2003) has noted that the decay of the diproton will happen too slowly for the resulting deuteron to be converted into helium, leaving at least some deuterium to power stars and take the place of hydrogen in organic compounds.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Collins (2003)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationnone given
Under fairly reasonable assumptions such as uniform probability, varying only one variable provides a useful estimate of the relevant probability.
“Under fairly reasonable assumptions (uniform probability etc.), varying only one variable provides a useful estimate of the relevant probability.”
Quote in the paperSubstantial claim- The authors state this as an assumption: The probability distribution over the parameters x and y is uniform.
- Premisecitation
Below the orange curve, isolated protons are unstable, leaving no hydrogen left over from the early universe.
“Below the orange curve, isolated protons are unstable, leaving no hydrogen left over from the early universe”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Barr & Khan (2007)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationcitation
We know what a high-entropy big bang spacetime looks like, and it looks nothing like the state of our universe in its earliest stages.
“We conclude that we know what a high-entropy big bang spacetime looks like, and it looks nothing like the state of our universe in its earliest stages.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Penrose (1979)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisecitation
In Q versus x space, similar constraints relate to the ability of galaxies to form stars by fragmentation due to gas cooling and for the universe to form anything other than black holes.
“The right panel shows similar constraints in the Q vs. x space.We see similar constraints relating to the ability of galaxies to successfully form stars by fragmentation due to gas cooling and for the universe to form anything other than black holes.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Tegmark et al. (2006)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationreasoning
The wedge, even as a distortion, would still be able to support a fine-tuning claim.
“The wedge, distortion that it is, would still be able to support a fine-tuning claim.”
Quote in the paperSubstantial claim - Interpretationreasoning
These two examples show that the wedge, by only considering a single life-permitting criterion, seriously distorts typical cases of fine-tuning by committing the sequential juggler fallacy.
“These two examples show that the wedge, by only considering a single life-permitting criterion, seriously distorts typical cases of fine-tuning by committing the sequential juggler fallacy (Section 2).”
Quote in the paperSubstantial claim - Premisenone given
If gravity were repulsive rather than attractive, matter would not clump into complex structures.
“If gravity were repulsive rather than attractive, then matter wouldn't clump into complex structures.”
Quote in the paperNot a substantial claim - Premisecitation
Below the green curve, protons in nuclei decay, so any atoms that formed would disintegrate into a cloud of neutrons.
“Below this green curve, protons in nuclei decay, so that any atoms that formed would disintegrate into a cloud of neutrons.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Barr & Khan (2007)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisenone given
If in electromagnetism like charges attracted and opposites repelled, there would be no atoms and only undifferentiated lumps of matter.
“If, in electromagnetism, like charges attracted and opposites repelled, then there would be no atoms.As above, we would just have undifferentiated lumps of matter.”
Quote in the paperSubstantial claim - Interpretationreasoning
If the probability that a random universe with given laws supports intelligent life is robustly small, then that region of possible-physics-space contributes negligibly to the total life-permitting subset.
“If that probability is robustly small, then we conclude that that region of possible-physics-space contributes negligibly to the total life-permitting subset.”
Quote in the paperNot a substantial claim - Premisecitation
Inflationary models create new fine-tuning issues with regard to the properties of the scalar field.
“although inflationary models may alleviate the 'fine tuning' in the choice of initial conditions, the models themselves create new 'fine tuning' issues with regard to the properties of the scalar field”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Hollands & Wald 2002b
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationcitation
The observed value of Q is very likely to be close to one of the boundaries of the life-permitting range.
“Thus, we expect that the observed value of Q is very likely to be close to one of the boundaries of the life-permitting range.”
Quote in the paperSubstantial claim - Interpretationown data
Stenger's claim that large values of Q are unlikely to result from inflation is false.
“Stenger seems to see this problem, and so argues that large values of Q are unlikely to result from inflation.This claim is false 19 .”
Quote in the paperSubstantial claim - Interpretationreasoning
Not all fine-tuning cases could be solved by inflation.
“We contend not, because inflation has a target.”
Quote in the paperSubstantial claim- Rests on an assumption: The range of densities that permit the existence of cosmic structure in a long-lived universe is very narrow.
- Rests on an assumption: The range of densities that permit cosmic structure neatly straddles the critical density.
- Interpretationcitation
Inflation by itself cannot solve the horizon problem, in the sense of making the smooth early universe a natural outcome of a wide variety of initial conditions.
“Carroll & Tam (2010) conclude that while inflation is not without its attractions (e.g. it may give a theory of initial conditions a slightly easier target to hit at the Planck scale), 'inflation by itself cannot solve the horizon problem, in the sense of making the smooth early universe a natural outcome of a wide variety of initial conditions'.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Carroll & Tam (2010)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisecitation
The freedom to increase Q and r_L together is limited by the life-permitting range of galaxy densities.
“In particular, the freedom to increase Q and r L together is limited by the life-permitting range of galaxy densities.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Tegmark et al. (2006)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisecitation
The probability distribution for Q across a multiverse typically increases or decreases sharply through the anthropic window.
“Garriga & Vilenkin (2006) discuss what they call the 'Q catastrophe': the probability distribution for Q across a multiverse typically increases or decreases sharply through the anthropic window.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Garriga & Vilenkin (2006)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationreasoning
A given inflationary model will predict Q.
“A given inflationary model will predict Q, and it will only predict a lifepermitting value for Q if the parameters of the inflaton potential are suitably fine-tuned.”
Quote in the paperSubstantial claim - Interpretationreasoning
The fine-tuning of Q stands up well under examination.
“The fine-tuning of Q stands up well under examination.”
Quote in the paperSubstantial claim - Interpretationcitation
Inflation, in and of itself, cannot solve the entropy problem.
“Note that this argument also shows that inflation, in and of itself, cannot solve the entropy problemfoot_8 .”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Carroll & Tam (2010)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisecitation
If Q were smaller than 10^-6, gas would never condense into gravitationally bound structures at all, and such a universe would remain forever dark and featureless.
“'If Q were smaller than 10 À6 , gas would never condense into gravitationally bound structures at all, and such a universe would remain forever dark and featureless, even if its initial 'mix' of atoms, dark energy and radiation were the same as our own.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Rees 1999
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Rests on an assumption: In our universe, the amplitude of primordial fluctuations Q is approximately 2 × 10^-5.
- Interpretationnone given
The allowed change in Q relative to its value in our universe is necessarily an underestimate of the degree of fine-tuning.
“The allowed change in Q relative to its value in our universe ('an order of magnitude') is necessarily an underestimate of the degree of finetuning.”
Quote in the paperSubstantial claim - Premisenone given
To set up a life-permitting universe, inflation must start: there must come a time when the energy density of the inflaton field dominates the total energy density of the universe.
“I2.Inflation must start.There must come a time in the history of the universe when the energy density of the inflaton field dominates the total energy density of the universe, dictating its dynamics.”
Quote in the paperNot a substantial claim - Interpretationreasoning
Rees' life-permitting range for Q implies a fine-tuning of the inflaton potential of ~10^-11 with respect to the Planck scale.
“Rees' life-permitting range for Q implies a fine-tuning of the inflaton potential of ,10 À11 with respect to the Planck scale.”
Quote in the paperSubstantial claim - Premisecitation
Requirement I3 comes rather naturally to inflation: Peacock (1999) shows that requiring inflation to produce a large number of e-folds is essentially the same as requiring inflation to happen, namely f_start much greater than m_Pl.
“Requirement I3 comes rather naturally to inflation: Peacock (1999, p. 337) shows that the requirement that inflation produce a large number of e-folds is essentially the same as the requirement that inflation happen in the first place (i.e.SRA), namely f start c m Pl .”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Peacock (1999) source
- Premisecitation
The life-permitting region for the parameters considered by Tegmark et al. (2006) is boxed-in on all sides.
“Figure 2 (bottom row) shows that the lifepermitting region is boxed-in on all sides.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Tegmark et al. (2006)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisenone given
The second law of thermodynamics tells us that the most probable world is one in which the entropy is always high.
“The second law of thermodynamics tells us that the most probable world is one in which the entropy is always high.”
Quote in the paperNot a substantial claim - Premisereasoning
To set up a life-permitting universe, inflation requires an inflaton field capable of satisfying the slow roll approximation, with potential energy much greater than kinetic energy and negative pressure.
“I1.There must be an inflaton field.To make the expansion of the universe accelerate, there must exist a form of energy (a field) capable of satisfying the so-called Slow Roll Approximation (SRA), which is equivalent to requiring that the potential energy of the field is much greater than its kinetic energy, giving the field negative pressure.”
Quote in the paperSubstantial claim - Interpretationcitation
A variety of physical phenomena, atomic, gravitational and cosmological, must combine in the right way in order to produce a life-permitting universe.
“This inequality demonstrates the variety of physical phenomena, atomic, gravitational and cosmological, that must combine in the right way in order to produce a life-permitting universe.”
Quote in the paperSubstantial claim - Interpretationreasoning
There can be no inflation-like dynamical solution to the fine-tuning problems of quark masses, fundamental force strengths, or dimensionality of spacetime because dynamical processes are blind to the requirements of intelligent life.
“There can be no inflation-like dynamical solution to these fine-tuning problems because dynamical processes are blind to the requirements of intelligent life.”
Quote in the paperNot a substantial claim - Premisenone given
There is no known physical scale waiting in the life-permitting range of the quark masses, fundamental force strengths or the dimensionality of spacetime.
“There is no known physical scale waiting in the lifepermitting range of the quark masses, fundamental force strengths or the dimensionality of spacetime.”
Quote in the paperNot a substantial claim - Interpretationreasoning
Inflation represents a very special case among fine-tuning cases.
“Inflation thus represents a very special case.”
Quote in the paperSubstantial claim - Interpretationreasoning
Even if Stenger could show that L_bare = 0, this would do nothing to address why L_eff is observed to be so much smaller than the predicted contributions to L_vacuum.
“Even if Stenger could show that L bare ¼ 0, this would do nothing to address why L eff is observed to be so much smaller than the predicted contributions to L vacuum .”
Quote in the paperSubstantial claim - Interpretationreasoning
The cosmological constant has observable consequences that no amount of redefinition can disguise.
“The cosmological constant has observable consequences that no amount of redefinition can disguise.”
Quote in the paperSubstantial claim - Interpretationreasoning
There are certain contexts where we know that the calculation of vacuum energy is correct.
“There are certain contexts where we know that the calculation is correct.”
Quote in the paperSubstantial claim - Premisecitation
Adams (2008) showed there is another criterion that must be fulfilled for stars to have a stable burning configuration: hG m_e / a^2 C >~ 3.1 × 10^-6.
“Adams (2008) showed there is another criterion that must be fulfilled for stars have a stable burning configuration, hG m e a 2 C t 3:1 Â 10 À6 ;ð5Þ”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Adams (2008)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationcitation
Those who defend the multiverse solution to the cosmological constant problem do so because they have judged other solutions to have failed.
“Those who defend the multiverse solution to the cosmological constant problem are quite clear that they do so because they have judged other solutions to have failed.”
Quote in the paperNot a substantial claim - Interpretationcitation
Whatever is causing the accelerated expansion of the universe quacks like vacuum energy.
“Whatever is causing the accelerated expansion of the universe quacks like vacuum energy.”
Quote in the paperSubstantial claim - Interpretationreasoning
It is unlikely that quantum gravity will solve the cosmological constant problem.
“It is thus unlikely that quantum gravity will solve the problem.”
Quote in the paperNot a substantial claim - Premisenone given
Only gravity can measure r_L.
“Secondly, a dynamical selection mechanism for the cosmological constant is made difficult by the fact that only gravity can measure r L , and r L only becomes dynamically important quite recently in the history of the universe.”
Quote in the paperSubstantial claim - Interpretationreasoning
Stenger's argument fails because he has given no reason to believe the antecedent of his conditional.
“Stenger's argument fails because of this premise: if (T mn ¼ 0 .G mn ¼ 0) then L ¼ 0. This is true as a conditional, but Stenger has given no reason to believe the antecedent.”
Quote in the paperSubstantial claim - Interpretationreasoning
Amidst the possible universes, life-permitting ones are exceedingly rare.
“Amidst the possible universes, life-permitting ones are exceedingly rare.This is fine-tuning par excellence.”
Quote in the paperSubstantial claim - Premisecitation
It is unlikely that there is a technically natural resolution to the cosmological constant's fine-tuning problem.
“For example, Donoghue (2007) says 'It is unlikely that there is technically natural resolution to the cosmological constant's fine-tuning problem -this would require new physics at 10 À3 eV.[Such attempts are] highly contrived to have new dynamics at this extremely low scale which modifies only gravity and not the other interactions.'”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Donoghue (2007) source
- Interpretationreasoning
The cosmological constant problem is not that physicists have made an incorrect prediction.
“The problem is not that physicists have made an incorrect prediction.”
Quote in the paperNot a substantial claim - Interpretationreasoning
In general relativity there is no freedom to redefine L.
“In general relativity there is no freedom to redefine L.”
Quote in the paperSubstantial claim - Interpretationnone given
Particle physics is blind to the absolute value of the vacuum energy.
“Particle physics is blind to the absolute value of the vacuum energy.”
Quote in the paperNot a substantial claim - Interpretationreasoning
The fine-tuning problem is that different independent contributions to vacuum energy manage to cancel each other to a life-permitting degree.
“The finetuning problem is that these different independent contributions, including perhaps some that we don't know about, manage to cancel each other to such an alarming, life-permitting degree.”
Quote in the paperSubstantial claim - Interpretationcitation
If one allows G to increase until gravity is as strong as the strong force and uses linear rather than logarithmic axes, the stable-star-permitting region occupies ~10^-38 of parameter space.
“If one allows G to increase until gravity is as strong as the strong force (a G E a s E 1), and uses linear rather than logarithmic axes, the stablestar-permitting region occupies , 10 À38 of parameter space.”
Quote in the paperSubstantial claim - Premisecitation
Barrow & Tipler (1986) showed that the window for stable stars is open when kT_nuc / m_e c^2 >~ a^2 m_p/m_e ~ 10^2.
“Barrow & Tipler (1986, p. 332) showed that this window is open when, kT nuc m e c 2 t 2 ) a 2 m p m e t10 2 ;ð4Þ”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Barrow & Tipler (1986)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisenone given
Each QFT contribution to the total dark energy from matter fields is 10^120 times larger than the total.
“Each of these contributions turns out to be 10 120 times larger than the total.”
Quote in the paperSubstantial claim- Rests on an assumption: QFT predicts contributions to the vacuum energy of the universe that are ~10^120 times greater than the observed total value.
- Premisecitation
Within the parameter space shown by Adams, which spans 10 orders of magnitude in both a and G, about one-fourth of the space supports the existence of stars.
“Adams remarks that 'within the parameter space shown, which spans 10 orders of magnitude in both a and G, about one-fourth of the space supports the existence of stars'.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Adams (2008)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationreasoning
There is no direct theory-vs-observation contradiction because one is calculating and measuring different things.
“There is no direct theory-vs.-observationcontradiction as one is calculating and measuring different things.”
Quote in the paperNot a substantial claim - Interpretationnone given
The cosmological constant problem is not a problem that appears only at the Planck scale.
“Further, this is not a problem that appears only at the Planck scale.”
Quote in the paperSubstantial claim - Interpretationreasoning
The existence of stable stars is a fine-tuned property of our universe.
“We conclude that the existence of stable stars is indeed a fine-tuned property of our universe.”
Quote in the paperSubstantial claim - Interpretationnone given
The most plausible small-vacuum-selecting mechanisms don't work in a universe that contains matter.
“The most plausible small-vacuum-selecting mechanisms don't work in a universe that contains matter.”
Quote in the paperNot a substantial claim - Interpretationreasoning
Observations measure an effective cosmological constant L_eff = L_bare + L_vacuum.
“L eff ¼ L bare þ L vacuum .”
Quote in the paperSubstantial claim - Interpretationreasoning
In the absence of a physical theory of quintessence, the natural guess for the dark energy scale is the Planck scale.
“In the absence of a physical theory of quintessence, and with the hint (as discussed above) that gravitational physics must be involved, the natural guess for the dark energy scale is the Planck scale.”
Quote in the paperSubstantial claim - Interpretationreasoning
We do not know the possible range of r_Q because we have no well-tested, well-understood theory of quintessence.
“We don't know, because we have no well-tested, wellunderstood theory of quintessence.”
Quote in the paperSubstantial claim - Interpretationnone given
A particle physics solution to the cosmological constant problem would be just as significant a coincidence as the cosmological constant problem itself.
“A particle physics solution to the cosmological constant problem would be just as significant a coincidence as the cosmological constant problem itself.”
Quote in the paperNot a substantial claim - Interpretationnone given
The cosmological constant problem cannot be defined away.
“The problem cannot be defined away.”
Quote in the paperNot a substantial claim - Interpretationreasoning
The 120 order-of-magnitude fine-tuning remains.
“The 120 order-of-magnitude fine-tuning remains.”
Quote in the paperSubstantial claim - Interpretationnone given
If gravity depends on the absolute value of mass/energy, then we cannot set the zero-level to our convenience.
“If gravity depends on the absolute value of mass/energy, then we cannot set the zero-level to our convenience.”
Quote in the paperSubstantial claim - Premisereasoning
The electron vacuum energy does gravitate in some situations.
“The first is that we know that the electron vacuum energy does gravitate in some situations.”
Quote in the paperSubstantial claim - Premisenone given
r_L only becomes dynamically important quite recently in the history of the universe.
“Secondly, a dynamical selection mechanism for the cosmological constant is made difficult by the fact that only gravity can measure r L , and r L only becomes dynamically important quite recently in the history of the universe.”
Quote in the paperSubstantial claim - Premisecitation
r_L = 0 is not a special value from the particle physics point of view.
“This implies that r L ¼ 0 [i.e.zero cosmological constant] is not a special value from the particle physics point of view.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Bousso (2008)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationnone given
However many ways there are of producing a life-permitting universe, there are vastly many more ways of making a life-prohibiting one.
“The point is this: however many ways there are of producing a lifepermitting universe, there are vastly many more ways of making a life-prohibiting one.”
Quote in the paperNot a substantial claim - Interpretationreasoning
The present energy density of quintessence must fall in the same life-permitting range that was required of the cosmological constant.
“The present energy density of quintessence must fall in the same life-permitting range that was required of the cosmological constant.”
Quote in the paperSubstantial claim - Interpretationreasoning
If the universe underwent a period of inflation in its earliest stages, then the laws of nature are more than capable of producing life-prohibiting accelerated expansion.
“If the universe underwent a period of inflation in its earliest stages, then the laws of nature are more than capable of producing lifeprohibiting accelerated expansion.”
Quote in the paperSubstantial claim - Interpretationreasoning
The solution to the cosmological constant problem must be selective, allowing acceleration in the early universe but severely limiting it later on.
“The solution must therefore be rather selective, allowing acceleration in the early universe but severely limiting it later on.”
Quote in the paperSubstantial claim - Premisecitation
The dashed line shows a striking coincidence discussed by Carter (1974), namely alpha^{12} beta^4 ~ alpha_G.
“The dashed line in the left plot shows a striking coincidence discussed by Carter (1974), namely a 12 b 4 , a G .”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Carter (1974) source
- Premisecitation
Unless alpha << 1, the electrons in atoms and molecules are unstable to pair creation.
“Unless a { 1, the electrons in atoms and molecules are unstable to pair creation (Barrow & Tipler 1986, p. 297).”
Quote in the paperSubstantial claim0 of 2 sources checked- cites Barrow & Tipler 1986
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- cites Lieb & Yau 1988
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisecitation
Unless m_d - m_u + m_e < 3.4 MeV, the pp reaction is energetically unfavourable.
“A similar effect would be achieved 27 unless m d À m u þ m e , 3.4 MeV which makes the pp reaction energetically unfavourable (Hogan 2000).”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Hogan 2000
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationcitation
Hoyle's prediction is not an 'anthropic prediction'.
“Hoyle's prediction is not an 'anthropic prediction'.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Smolin (2007) source
- Interpretationnone given
The limits placed on alpha and beta from chemistry are weaker than the constraints listed above.
“The limits placed on a and b from chemistry are weaker than the constraints listed above.”
Quote in the paperNot a substantial claim - Premisecitation
The permitted shift represents a 0.7% change in the energy of the level itself.
“The permitted shift represents a 0.7% change in the energy of the level itself.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Livio et al. (1989) source
- Premisecitation
Near this line, the universe will contain both radiative and convective stars.
“Near this line, the universe will contain both radiative and convective stars.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Carter (1974) source
- Premisecitation
King et al. (2010) considered the bond angle and length in water, and the reaction energy of a number of organic reactions.
“This has been investigated by King et al. (2010) who considered the bond angle and length in water, and the reaction energy of a number of organic reactions.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites King et al. (2010)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationreasoning
The life-permitting region is likely to be a 2D strip in both the (alpha, beta) and (alpha, alpha_s) plane.
“This only considers the change in a i.e. horizontally, and the life-permitting region is likely to be a 2D strip in both the (a, b) and (a, a s ) plane.”
Quote in the paperNot a substantial claim - Premisecitation
Livio et al. (1989) found one could increase the energy of the 0+ level by 60 keV without affecting the level of carbon production.
“They found one could increase the energy of the level by 60 keV without effecting the level of carbon production.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Livio et al. (1989) source
- Premisecitation
If the Hoyle resonance level did not exist at just the right place, then stars would be unable to produce the carbon required by life.
“Hoyle reasoned that if such a resonance level did not exist at just the right place, then stars would be unable to produce the carbon required by life 24 .”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Hoyle
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisecitation
Unless beta^{1/4} << 1, stable ordered molecular structures (like chromosomes) are not stable; atoms will too easily stray and the substance will spontaneously melt.
“Unless b 1/4 { 1, stable ordered molecular structures (like chromosomes) are not stable.The atoms will too easily stray from their place in the lattice and the substance will spontaneously melt (Barrow & Tipler 1986, p. 305).”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Barrow & Tipler 1986
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisecitation
The amount of hydrogen left over from big bang nucleosynthesis is significantly diminished when alpha_s > 0.27.
“The upper limit shown in the right plot of Figure 6 is the result of MacDonald & Mullan (2009) that the amount of hydrogen left over from big bang nucleosynthesis is significantly diminished when a s .0.27.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites MacDonald & Mullan (2009)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationcitation
The main process by which carbon and oxygen are synthesised in our universe is drastically curtailed by a tiny change in the fundamental constants.
“Nevertheless, these calculations are highly suggestive -the main process by which carbon and oxygen are synthesised in our universe is drastically curtailed by a tiny change in the fundamental constants.”
Quote in the paperSubstantial claim - Premisecitation
For stable atoms, the radius of the electron orbit must be significantly larger than the nuclear radius, which requires alpha beta / alpha_s << 1.
“For stable atoms, we need the radius of the electron orbit to be significantly larger than the nuclear radius, which requires ab/a s { 1 (Barrow & Tipler 1986, p. 320).”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Barrow & Tipler 1986
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisecitation
Unless alpha_s > 0.3 alpha^{1/2}, carbon and all larger elements are unstable.
“Unless a s t 0.3a 1/2 , carbon and all larger elements are unstable (Barrow & Tipler 1986, p. 326).”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Barrow & Tipler 1986
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisecitation
The constraint on carbon production from Ekstrom et al. (2010) is -3.5e-5 < Delta alpha/alpha < +1.8e-5.
“The constraint on carbon production from Ekstr€ om et al. ( 2010) is À3.5 Â 10 À5 t Da/a t þ1.8 Â 10 À5 , as discussed in Section 4.7.2.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Ekstr€ om et al. (2010)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisecitation
Agrawal et al. find that only for values in a narrow window is life likely to be possible.
“After exploring the range [Àm Pl , m Pl ], they find that 'only for values in a narrow window is life likely to be possible'.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Agrawal et al. (1998a, b)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisecitation
The stability of the proton requires alpha_t (m_d - m_u)/141 MeV, so that the extra electromagnetic mass-energy of a proton relative to a neutron is more than counter-balanced by the bare quark masses.
“The stability of the proton requires a t (m d À m u )/ 141 MeV, so that the extra electromagnetic massenergy of a proton relative to a neutron is more than counter-balanced by the bare quark masses (Hogan 2000;Hall & Nomura 2008).”
Quote in the paperSubstantial claim0 of 2 sources checked- cites Hogan 2000
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- cites Hall & Nomura 2008
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisecitation
For v > 4e-17, the deuteron is strongly unstable.
“for v .4 Â 10 À17 , the deuteron is strongly unstable (see point 10 above);”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Agrawal et al. (1998a, b)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationreasoning
The conclusion of Hoyle's prediction does not depend in any way on the first, 'anthropic' premise.
“The conclusion does not depend in any way on the first, 'anthropic' premise.”
Quote in the paperNot a substantial claim - Premisecitation
The same coincidence can be shown to ensure that the surface temperature of stars is close to 'biological temperature'.
“The same coincidence can be shown to ensure that the surface temperature of stars is close to 'biological temperature' (Barrow & Tipler 1986, p. 338).”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Barrow & Tipler 1986
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisecitation
Agrawal et al. (1998a,b) considered the life-permitting range of the Higgs mass parameter m^2, and the corresponding limits on v = (-m^2/lambda)^{1/2}, which takes the value 246 GeV = 2e-17 m_Pl in our universe.
“Agrawal et al. (1998a, b) considered the lifepermitting range of the Higgs mass parameter m 2 , and the corresponding limits on the vacuum expectation value, v ¼ (Àm 2 /l) 1/2 , which takes the value 246 GeV ¼ 2 Â 10 À17 m Pl in our universe.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Agrawal et al. (1998a, b)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationreasoning
Stenger has failed to turn back the force of the fine-tuning case concerning carbon and oxygen production.
“We conclude that Stenger has failed to turn back the force of this fine-tuning case.”
Quote in the paperSubstantial claim - Premisecitation
If the nucleus is considered fixed in space, the time-independent, non-relativistic Schrödinger equation scales with alpha^2 m_e, so the relative energy and properties of the energy levels of electrons are unchanged.
“If we consider the nucleus as fixed in space, then the time-independent, non-relativistic Schr€ odinger equation scales with a 2 m e i.e. the relative energy and properties of the energy levels of electrons (which determine chemical bonding) are unchanged (Barrow & Tipler 1986, p. 533).”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Barrow & Tipler 1986
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationreasoning
The argument for the Hoyle resonance would work just as well if the element in question were the inert gas neon, for which the first premise is (probably) false.
“The argument would work just as well if the element in question were the inert gas neon, for which the first premise is (probably) false.”
Quote in the paperNot a substantial claim - Premisecitation
A fractional change in the fine-structure constant alpha of one part in 10^5 would change the energy of the Hoyle resonance enough that stars would contain carbon or oxygen at the end of helium burning but not both.
“A fractional change in a of one part in 10 5 would change the energy of the Hoyle resonance enough that stars would contain carbon or oxygen at the end of helium burning but not both.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Ekstr€ om et al. (2010)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisecitation
The limit of Adams (2008) on stellar stability is alpha > 7.3e-5.
“The limit shown is a .7.3 Â 10 À5 , as read off figure 5 of Adams (2008).”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Adams (2008)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationreasoning
The ability of stars in our universe to produce both carbon and oxygen seems to be a rare talent.
“The ability of stars in our universe to produce both carbon and oxygen seems to be a rare talent.”
Quote in the paperSubstantial claim - Premisecitation
The Higgs mass squared m_H^2 receives quantum corrections from the virtual effects of every particle that couples to the Higgs field.
“The problem (as ably explained by Martin 1998) is that the Higgs mass (squared) m H 2 receives quantum corrections from the virtual effects of every particle that couples, directly or indirectly, to the Higgs field.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Martin 1998
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisenone given
The majority of the other 95% comes from the strong force binding energy of the valence quarks.
“The majority of the other 95% comes from the strong force binding energy of the valence quarks.”
Quote in the paperSubstantial claim - Interpretationnone given
If the Planck mass is the natural mass scale in physics, then it sets the scale for all mass terms, corrections or otherwise.
“If the Planck mass is the 'natural' (FOFT 175) mass scale in physics, then it sets the scale for all mass terms, corrections or otherwise.”
Quote in the paperNot a substantial claim - Premisenone given
The bare quark masses only account for a small fraction of the mass of the proton and neutron.
“The bare quark masses, discussed above, only account for a small fraction of the mass of the proton and neutron.”
Quote in the paperSubstantial claim - Premisereasoning
Supersymmetry ties v to Lambda_SM.
“This ties v to L SM .”
Quote in the paperNot a substantial claim - Premisecitation
To prevent big bang nucleosynthesis burning all hydrogen to helium in the early universe, they set the baryon to photon ratio eta_b = 4e-12.
“To prevent big bang nucleosynthesis burning all hydrogen to helium in the early universe, they must use a 'judicious parameter adjustment' and set the baryon to photon radio Z b ¼ 4 Â 10 À12 .”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Harnik, Kribs & Perez (2006)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationreasoning
Galaxy formation in the weakless universe will be considerably less efficient, relying on rare statistical fluctuations and cooling via molecular viscosity.
“Galaxy formation in the weakless universe will thus be considerably less efficient, relying on rare statistical fluctuations and cooling via molecular viscosity.”
Quote in the paperSubstantial claim - Interpretationreasoning
It is precisely the smallness of the quantum corrections wherein the fine-tuning lies.
“It is precisely the smallness of the quantum corrections wherein the fine-tuning lies.”
Quote in the paperSubstantial claim - Premisecitation
The result is a substantially increased abundance of deuterium, ~10% by mass.
“The result is a substantially increased abundance of deuterium, ,10% by mass.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Harnik, Kribs & Perez (2006)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationreasoning
'Congenial' is almost certainly a weaker constraint than 'life-permitting', since only nuclear stability is investigated.
“Finally, 'congenial' is almost certainly a weaker constraint than 'life-permitting', since only nuclear stability is investigated.”
Quote in the paperSubstantial claim - Interpretationreasoning
The need for a life-permitting universe to be fine-tuned is not significantly affected.
“The need for a lifepermitting universe to be fine-tuned is not significantly affected.”
Quote in the paperSubstantial claim - Premisereasoning
Moving from the centre (m_T = m_T,0) to the right (m_T = 2m_T,0) triangle of Figure 8, the congenial fraction drops from 14% to 7%.
“Moving from the centre (m T ¼ m T,0 ) to the right (m T ¼ 2m T,0 ) triangle of Figure 8, the congenial fraction drops from 14% to 7%.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Jaffe et al. (2009)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationreasoning
Unlike the bare masses of the quarks and leptons, we can answer this question from within the standard model.
“Unlike the bare masses of the quarks and leptons, we can answer this question from within the standard model.”
Quote in the paperNot a substantial claim - Interpretationcitation
Smallness is not sufficient for life.
“Secondly, smallness is not sufficient for life.”
Quote in the paperSubstantial claim - Interpretationreasoning
The question why gravity is feeble is at least partly answered if we can explain why Lambda_QCD << m_Pl.
“The question 'why is gravity so feeble?' (i.e. a G { 1) is at least partly answered if we can explain why L QCD { m Pl .”
Quote in the paperSubstantial claim - Premisereasoning
This does not completely explain the smallness of the proton mass, since m_p is the sum of a number of contributions: QCD, electromagnetism, the masses of the valence quarks, and the mass of the virtual quarks, including the strange quark.
“Note that this does not completely explain the smallness of the proton mass, since m p is the sum of a number of contributions: QCD (L QCD ), electromagnetism, the masses of the valence quarks (m u and m d ), and the mass of the virtual quarks, including the strange quark, which makes a surprisingly large contribution to the mass of ordinary matter.”
Quote in the paperNot a substantial claim - Premisereasoning
Baryogenesis is crucial to life because a universe which contained equal numbers of protons and antiprotons at annihilation would only contain radiation, which cannot form complex structures.
“Baryogenesis is clearly crucial to life -a universe which contained equal numbers of protons and antiprotons at annihilation would only contain radiation, which cannot form complex structures.”
Quote in the paperSubstantial claim - Interpretationnone given
Even if Equation 6 holds, the weakless universe at best opens up a life-permitting region of parameter space of similar size to the region in which our universe resides.
“Note that, even if Equation 6 holds, the weakless universe at best opens up a lifepermitting region of parameter space of similar size to the region in which our universe resides.”
Quote in the paperNot a substantial claim - Premisecitation
The weakless universe requires Omega_baryon/Omega_dark matter ~ 10^-3, 100 times less than in our universe.
“The weakless universe requires O baryon /O dark matter , 10 À3 , 100 times less than in our universe.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Harnik, Kribs & Perez (2006)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationreasoning
Potential problems arise when we need the proton mass to fall within a specific range, rather than just be small, since the proton mass depends very sensitively (exponentially) on alpha_U.
“Potential problems arise when we need the proton mass to fall within a specific range, rather than just be small, since the proton mass depends very sensitively (exponentially) on a U .”
Quote in the paperSubstantial claim - Premisecitation
Jeltema & Sher (1999) concluded that a 1% change in v from its value in our universe would significantly affect the ability of stars to synthesise both oxygen and carbon.
“They conclude that a 1% change in v from its value in our universe would significantly affect the ability of stars to synthesise both oxygen and carbon.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Jeltema & Sher (1999)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisecitation
These corrections must be fine-tuned to mutually cancel to one part in m_Pl^2/m_H^2 ~ 10^32.
“These corrections are enormous -their natural scale is the Planck scale, so that these contributions must be fine-tuned to mutually cancel to one part in m Pl 2 /m H 2 E 10 32 .”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Martin 1998
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisereasoning
There is an exponential relationship between Lambda_QCD and the scale of grand unification m_U: Lambda_QCD/m_U ~ exp(-b/alpha_s(m_U)).
“Given that the strength of the strong force runs very slowly (logarithmically) with energy, there is a exponential relationship between L QCD and the scale of grand unification m U : L QCD m U $ exp À b a s ðm U Þ ;ð7Þ”
Quote in the paperSubstantial claim - Premisecitation
Unless 0.78e-17 < v/m_Pl < 3.3e-17, the elements are unstable.
“Recall that Damour & Donoghue (2008) showed that unless 0.78 Â 10 À17 , v/m Pl , 3.3 Â 10 À17 , the elements are unstable.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Damour & Donoghue (2008)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisereasoning
Stars in the weakless universe burn via proton-deuterium reactions, using deuterium left over from the big bang.
“The proton-proton reaction which powers stars in our universe relies on the weak interaction, so stars in the weakless universe burn via proton-deuterium reactions, using deuterium left over from the big bang.”
Quote in the paperSubstantial claim - Interpretationreasoning
We need all of the contributions to be small in order for m_p to be small.
“We need all of the contributions to be small in order for m p to be small.”
Quote in the paperSubstantial claim - Premisecitation
The bare masses of the quarks are not related to the strong force.
“Note that, contra Stenger, the bare masses of the quarks are not related to the strong force 30 .”
Quote in the paperNot a substantial claim - Interpretationreasoning
From a fine-tuning perspective, this replaces the major miracle Lambda_QCD/m_Pl ~ 10^-20 with a more minor one, alpha_s(m_U) ~ 10^-1.
“From a fine-tuning perspective, however, this seems to be good progress, replacing the major miracle L QCD /m Pl , 10 À20 with a more minor one, a s (m U ) , 10 À1 .”
Quote in the paperSubstantial claim - Premisecitation
Since string theory unifies the four fundamental forces at the Planck scale, it doesn't really need grand unification.
“Since string theory unifies the four fundamental forces at the Planck scale, it doesn't really need grand unification.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Schellekens (2008)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisenone given
General relativity will not allow a unique way to specify 'now'.
“But general relativity will not allow it -there is no unique way to specify 'now'.”
Quote in the paperNot a substantial claim - Interpretationreasoning
A random observer is overwhelmingly likely to observe that they are in the smallest fluctuation able to support an observer.
“This means that a random observer is overwhelmingly likely to observe that they are in the smallest fluctuation able to support an observer.”
Quote in the paperSubstantial claim - Interpretationreasoning
We must be able to compare the properties of our universe with some subset of the multiverse - otherwise the multiverse proposal cannot make predictions.
“But we must be able to compare the properties of our universe with some subset of the multiverse -otherwise the multiverse proposal cannot make predictions.”
Quote in the paperNot a substantial claim - Premisenone given
It is a mathematical fact that in a universe with four spatial dimensions you could, with a judicious choice of axis, make a left-footed shoe into a right-footed one by rotating it.
“It is a mathematical fact that in a universe with four spatial dimensions you could, with a judicious choice of axis, make a left-footed shoe into a right-footed one by rotating it.”
Quote in the paperNot a substantial claim - Interpretationnone given
To show (or conjecture) that a parameter is derived rather than fundamental does not mean that it is not fine-tuned.
“At the risk of repetition: to show (or conjecture) that a parameter is derived rather than fundamental does not mean that it is not fine-tuned.”
Quote in the paperSubstantial claim - Interpretationreasoning
Region 7 will be entered if alpha_U is increased by ~0.008.
“Similarly, Region 7 will be entered if a U is increased 31 by ,0.008.”
Quote in the paperNot a substantial claim - Interpretationreasoning
The calculation of α1, α2, α3 from α_U and M_U also requires that the masses, charges and quantum numbers of all fundamental particles be given to allow terms like sum Q_i^2 to be computed.
“The calculation also requires that the masses, charges and quantum numbers of all fundamental particles be given to allow terms like P Q i 2 to be computed.”
Quote in the paperNot a substantial claim - Interpretationreasoning
The difficulty in ruling out multiverses speaks to their unfalsifiability, rather than their steadfastness in the face of cosmological data.
“Firstly, the difficulty in ruling out multiverses speaks to their unfalsifiability, rather than their steadfastness in the face of cosmological data.”
Quote in the paperNot a substantial claim - Premisecitation
Every LQCD calculation takes care to explain that they are inferring the quark masses from the masses of observed hadrons.
“Every LQCD calculation takes great care to explain that they are inferring the quark masses from the masses of observed hadrons (see, for example, Davies et al. 2004;Du ¨rr et al. 2008;Laiho 2011).”
Quote in the paperNot a substantial claim0 of 3 sources checked- cites Davies et al. 2004
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- cites Du ¨rr et al. 2008
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- cites Laiho 2011
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationreasoning
The hypothesis that a multiverse actually exists will always be untestable.
“The hypothesis that a multiverse actually exists will always be untestable.”
Quote in the paperNot a substantial claim - Premisenone given
String theorists must compactify all but 3+1 of the extra dimensions for the theory to have a chance of describing our universe.
“They must compactify all but 3þ1 of the extra dimensions for the theory to have a chance of describing our universe.”
Quote in the paperNot a substantial claim - Interpretationreasoning
There is no particular reason why three of the forces should unify first, three orders of magnitude below the Planck scale.
“That is, there is no particular reason why three of the forces should unify first, three orders of magnitude below the Planck scale.”
Quote in the paperNot a substantial claim - Interpretationreasoning
The running of the coupling constants does not fix the integration constants.
“As can be seen from Equation 9, the running of the coupling does not fix the integration constants.”
Quote in the paperNot a substantial claim - Interpretationreasoning
The Boltzmann multiverse is definitively ruled out.
“The Boltzmann multiverse is thus definitively ruled out.”
Quote in the paperSubstantial claim - Interpretationreasoning
An extremely small fraction of life-permitting universes are as old and cold as ours.
“The results of this survey would be rather surprising: an extremely small fraction of life-permitting universes are as old and cold as ours.”
Quote in the paperSubstantial claim - Interpretationreasoning
We cannot observe any of the properties of a multiverse {M; f(m); p}, as they have no causal effect on our universe.
“In contrast, we cannot observe any of the properties of a multiverse {M; f ðmÞ; p}, as they have no causal effect on our universe.”
Quote in the paperNot a substantial claim - Interpretationreasoning
The running of the coupling constants does not change the status of the α_i as free parameters of the theory.
“The running of the coupling constants does not change the status of the a i as free parameters of the theory.”
Quote in the paperNot a substantial claim - Interpretationreasoning
This fine-tuning case refers to the number of macroscopic or 'large' space dimensions, which both string theory and classical physics agree to be three.
“This fine-tuning case refers to the number of macroscopic or 'large' space dimensions, which both string theory and classical physics agree to be three.”
Quote in the paperSubstantial claim - Interpretationreasoning
The analogy between undetectable universes and undetectable quarks is not a good one.
“FOFT 228 notes the similarity between undetectable universes and undetectable quarks, but the analogy is not a good one.”
Quote in the paperNot a substantial claim - Premisecitation
Barrow & Tipler found that GUTs provided the tightest anthropic bounds on the fine structure constant, associated with the decay of the proton into a positron and the requirement of grand unification below the Planck scale.
“They found that GUTs provided the tightest anthropic bounds on the fine structure constant, associated with the decay of the proton into a positron and the requirement of grand unification below the Planck scale.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Barrow & Tipler (1986, p. 354)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationreasoning
There is no unambiguous evidence in favour of the meta-law holding in this universe for any multiverse.
“There is no unambiguous evidence in favour of a.) for any multiverse, and b.) will surely forever hold the title of the most extreme extrapolation in all of science, if indeed it can be counted as part of science.”
Quote in the paperNot a substantial claim - Premisecitation
The strength of the fundamental forces, quantified by coupling constants α1, α2, α3, are a function of energy due to screening (or antiscreening) by virtual particles.
“In fact, these parameters are a function of energy due to screening (or antiscreening) by virtual particles.”
Quote in the paperSubstantial claim0 of 2 sources checked- cites De Boer 1994
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- cites Hogan 2000
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationreasoning
The fine-tuning of the mass of the proton can be translated into anthropic limits on GUT parameters.
“For the moment, we note that the fine-tuning of the mass of the proton can be translated into anthropic limits on GUT parameters.”
Quote in the paperSubstantial claim - Interpretationcitation
Stenger's statement that m_n - m_p results from m_d - m_u is false, because there is also a contribution from the electromagnetic force.
“Stenger states that m n À m p results from m d À m u .This is false, as there is also a contribution from the electromagnetic force (Gasser & Leutwyler 1982;Hall & Nomura 2008).”
Quote in the paperSubstantial claim0 of 2 sources checked- cites Gasser & Leutwyler 1982
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- cites Hall & Nomura 2008
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationown data
The pattern α3 > α2 > α1 is a good start but hardly guarantees a life-permitting universe.
“As can be seen from Figure 6, this is a good start but hardly guarantees a life-permitting universe.”
Quote in the paperNot a substantial claim - Interpretationreasoning
Whatever the fundamental properties of spacetime are, it is an objective fact about physical reality - by Stenger's own criterion - that in the appropriate limit space is accurately modelled by R^3.
“Whatever the fundamental properties of spacetime are, it is an objective fact about physical reality -by Stenger's own criterion -that in the appropriate limit space is accurately modelled by R 3 .”
Quote in the paperSubstantial claim - Interpretationreasoning
Stenger's assertion that the Higgs mechanism (with mass scale 246 GeV) accounts for the smallness of the electron mass (0.000511 GeV) is false.
“Stenger's assertion that the Higgs mechanism (with mass scale 246 GeV) accounts for the smallness of the electron mass (0.000511 GeV) is false.”
Quote in the paperSubstantial claim - Interpretationcitation
Penrose's argument is based on the place of our universe in phase space, and is thus generic enough to apply to any multiverse proposal that creates more small universe domains than large ones.
“Penrose's argument is based on the place of our universe in phase space, and is thus generic enough to apply to any multiverse proposal that creates more small universe domains than large ones.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Penrose (2004, p. 763ff)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisenone given
Fixing other cosmological parameters, the anthropically allowed range for Q is 10^-6 < Q < 10^-4.
“Fixing other cosmological parameters, the anthropically allowed range is 10 À6 t Q t 10 À4 .”
Quote in the paperSubstantial claim - Interpretationreasoning
This particular multiverse dies the same death as the Boltzmann multiverse.
“This particular multiverse dies the same death as the Boltzmann multiverse.”
Quote in the paperSubstantial claim - Interpretationcitation
It is almost certainly not true that string theory is a unique physical theory whose unique solution describes the universe as we know it, because string theory has 'anthropic principle written all over it'.
“It is almost certainly not true of our best hope for a theory of quantum gravity, string theory, which has 'anthropic principle written all over it' (Schellekens 2008).”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Schellekens 2008
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisereasoning
Physical laws are material and efficient causes, not final causes.
“Physical laws are material and efficient causes, not final causes.”
Quote in the paperNot a substantial claim - Interpretationreasoning
Physics at the Planck scale will not rewrite the standard model of particle physics.
“Physics at the Planck scale will not rewrite the standard model of particle physics.”
Quote in the paperNot a substantial claim - Interpretationreasoning
The category of 'physically possible' is not much help, because the laws of nature tell us what is physically possible, but not which laws are possible.
“The category of 'physically possible' isn't much help either, as the laws of nature tell us what is physically possible, but not which laws are possible.”
Quote in the paperNot a substantial claim - Interpretationreasoning
There is no reason to think that future progress in physics will render a life-permitting universe inevitable.
“There is, then, no reason to think that future progress in physics will render a life-permitting universe inevitable.”
Quote in the paperNot a substantial claim - Interpretationreasoning
The beauty of string theory's principles has not saved us from the complexity and contingency of the solutions to its equations.
“The beauty of its principles has not saved us from the complexity and contingency of the solutions to its equations.”
Quote in the paperSubstantial claim - Interpretationreasoning
When physics is finished, fine-tuning may remain, basic and irreducible.
“When physics is finished, when the equation is written on the blackboard and fundamental physics has gone as deep as it can go, fine-tuning may remain, basic and irreducible.”
Quote in the paperNot a substantial claim - Interpretationreasoning
Either way, life does not have free run of parameter space.
“Either way, life does not have free run of parameter space.”
Quote in the paperSubstantial claim - Interpretationreasoning
The universe is fine-tuned for the existence of life.
“We conclude that the universe is fine-tuned for the existence of life.”
Quote in the paperSubstantial claim - Interpretationreasoning
For a multiverse proposal to make predictions, it must be able to calculate and justify a measure over the set of universes it creates.
“For a multiverse proposal to make predictions, it must be able to calculate and justify a measure over the set of universes it creates.”
Quote in the paperSubstantial claim - Interpretationreasoning
A universe with one chemical reaction (2H -> H2) would not be able to create and sustain the complexity necessary for life.
“We do not need a rigorous definition of life to reasonably conclude that a universe with one chemical reaction (2H -H 2 ) would not be able to create and sustain the complexity necessary for life.”
Quote in the paperSubstantial claim - Interpretationnone given
There is not the slightest bit of evidence that a simple, beautiful physical principle from which we can derive a unique physical theory describing the universe is true.
“While this has been the dream of physicists for centuries, there is not the slightest bit of evidence that this idea is true.”
Quote in the paperNot a substantial claim - Interpretationcitation
The conclusion of Aguirre (2001) that the cold big bang should be discouraging for proponents of the anthropic program seems sound.
“Nevertheless, the conclusion of Aguirre (2001) seems sound: '[the CBB] should be discouraging for proponents of the anthropic program: it implies that it is quite important to know the [prior] probabilities P, which depend on poorly constrained models of the early universe'.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Aguirre (2001)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Rests on an assumption: There is no successful theory of baryogenesis and leptogenesis.
- Premisecitation
The 'principle of living dangerously' states that if the prior probability for a parameter is a rapidly increasing (or decreasing) function, then we expect the observed value of the parameter to lie near the edge of the anthropically allowed range.
“It is called the 'principle of living dangerously': if the prior probability for a parameter is a rapidly increasing (or decreasing) function, then we expect the observed value of the parameter to lie near the edge of the anthropically allowed range.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Aguirre (2007) source
- Interpretationnone given
Even if inflation is not eternal and the universe is finite, the measure problem can still paralyse our analysis.
“In fact, even if inflation is not eternal and the universe is finite, the measure problem can still paralyse our analysis.”
Quote in the paperSubstantial claim - Interpretationreasoning
The anthropic coincidences are not like the coincidence between inertial mass and gravitational mass in Newtonian gravity, which is a coincidence between two seemingly independent physical quantities.
“In particular, the anthropic coincidences are not like, say, the coincidence between inertial mass and gravitational mass in Newtonian gravity, which is a coincidence between two seemingly independent physical quantities.”
Quote in the paperSubstantial claim - Interpretationnone given
Unlike biologically evolved life like ourselves, Boltzmann brains do not require a fine-tuned universe.
“The most serious problem is that, unlike biologically evolved life like ourselves, Boltzmann brains do not require a fine-tuned universe.”
Quote in the paperSubstantial claim- Rests on an assumption: Boltzmann brains can fluctuate into existence with memories of being observers like us.
- Interpretationcitation
If we live in a multiverse generated by a process like chaotic inflation, then for every observer who observes a universe of our size, there are 10^10^123 who observe a universe that is just 10 times smaller.
“In other words, if we live in a multiverse generated by a process like chaotic inflation, then for every observer who observes a universe of our size, there are 10 10 123 who observe a universe that is just 10 times smaller.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Penrose (2004, p. 763ff)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationcitation
At best, Aguirre's inequality would show that there is a continuous life-permitting region stretching along the Z_g axis.
“At best, this would show that there is a continuous life-permitting region, stretching along the Z g axis.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Aguirre (2001)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationreasoning
The discovery of another life-permitting island in parameter space potentially creates a problem for the multiverse.
“The discovery of another life-permitting island in parameter space potentially creates a problem for the multiverse.”
Quote in the paperNot a substantial claim- Rests on an assumption: A multiverse measure exists that allows comparison of the sizes of life-permitting islands.
- Interpretationreasoning
Of all the ways that the laws of nature, constants of physics and initial conditions of the universe could have been, only a very small subset permits the existence of intelligent life.
“Of all the ways that the laws of nature, constants of physics and initial conditions of the universe could have been, only a very small subset permits the existence of intelligent life.”
Quote in the paperNot a substantial claim - Interpretationreasoning
Fine-tuning is not a gap.
“It is not a gap.”
Quote in the paperNot a substantial claim - Interpretationnone given
If another life-permitting island is significantly larger than ours for a given multiverse measure, observers should expect to be on that other island.
“If the other island is significantly larger than ours (for a given multiverse measure), then observers should expect to be on the other island.”
Quote in the paperNot a substantial claim- Rests on an assumption: A multiverse measure exists that allows comparison of the sizes of life-permitting islands.
- Interpretationreasoning
If we condition on observers rather than biologically evolved life, then the multiverse may fail to predict a universe like ours.
“If we condition on observers, rather than biological evolved life, then the multiverse may fail to predict a universe like ours.”
Quote in the paperSubstantial claim - Interpretationreasoning
It is not true that fine-tuning must eventually yield to the relentless march of science.
“It is not true that fine-tuning must eventually yield to the relentless march of science.”
Quote in the paperNot a substantial claim - Premisenone given
If the strong force were weaker, the periodic table would consist of only hydrogen.
“If the strong force were weaker, the periodic table would consist of only hydrogen.”
Quote in the paperNot a substantial claim - Interpretationcitation
The multiverse would not explain why our universe is fine-tuned for biological life.
“The multiverse would not explain why our universe is finetuned for biological life (R.Collins, forthcoming).”
Quote in the paperSubstantial claim0 of 1 sources checked- cites R.Collins, forthcoming
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationreasoning
Stenger's statement that the cold big-bang model shows that we don't necessarily need the Hoyle resonance, or even significant stellar nucleosynthesis, for life is wrong.
“Stenger states that '[t]he cold big-bang model shows that we don't necessarily need the Hoyle resonance, or even significant stellar nucleosynthesis, for life'.It shows nothing of the sort.”
Quote in the paperSubstantial claim - Interpretationreasoning
The cold big bang does not negate the need for long-lived, nuclear-fueled stars as an energy source for planetary life.
“Further, CBB does not negate the need for long-lived, nuclear-fueled stars as an energy source for planetary life.”
Quote in the paperSubstantial claim
- May combine two claims. 111
- Classified as probably not a substantial claim. 92
May combine two claims.
PremisecitationInflation predicts a nearly scale-invariant spectrum of fluctuations, but such a spectrum was proposed for independent reasons by Harrison (1970) and Zel'dovich (1972) a decade before inflation was proposed.
“Inflation predicts a nearly scale-invariant spectrum of fluctuations, but such a spectrum was proposed for independent reasons by Harrison (1970) and Zel'dovich (1972) a decade before inflation was proposed.”
Quote in the paperNot a substantial claim1 of 2 sources checked- cites Harrison (1970)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- cites Zel'dovich (1972) source
May combine two claims.
FindingcitationTegmark (2005) found that the success rate of inflation peaks at about 0.1 percent and drops rapidly as m_h increases or decreases away from m_Pl; even with a scalar field, inflation is far from guaranteed.
“The success rate peaks at ,0.1 percent, and drops rapidly as m h increases or decreases away from m Pl .Even with a scalar field, inflation is far from guaranteed.”
Quote in the paperSubstantial claim1 of 1 sources checked- cites Tegmark (2005) source
Split into 2 atoms — 1 confirmed, 1 partially supported, 0 disputed, 0 misattributed, 0 unverifiable. Expand the claim to see per-atom verdicts.
Experimental — accuracy not yet measured
Probably not a substantial claim: may not pass S3 (load-bearing). May combine two claims.
PremisecitationAs Ellis et al. (2004) point out, any multiverse proposal will have to deal with the problems of what determines {M; f(m); p}, actualized infinities, non-renormalisability, parameter dependence and non-uniqueness of p, and how one could possibly observationally confirm any of these quantities.
“As Ellis et al. (2004) point out, any such proposal will have to deal with the problems of what determines {M; f ðmÞ; p}, actualized infinities (in M, f(m) and the spatial extent of universes) and non-renormalisability, the parameter dependence and non-uniqueness of p, and how one could possibly observationally confirm any of these quantities.”
Quote in the paperNot a substantial claim1 of 1 sources checked- cites Ellis et al. (2004) source
Split into 2 atoms — 1 confirmed, 1 partially supported, 0 disputed, 0 misattributed, 0 unverifiable. Expand the claim to see per-atom verdicts.
Experimental — accuracy not yet measured
Classified as probably not a substantial claim.
PremisecitationAs Linde & Noorbala (2010) explains, one of the main problems is that 'in an eternally inflating universe the total volume occupied by all, even absolutely rare types of the 'universes', is indefinitely large'.
“As Linde & Noorbala (2010) explains, one of the main problems is that 'in an eternally inflating universe the total volume occupied by all, even absolutely rare types of the 'universes', is indefinitely large'.”
Quote in the paperSubstantial claim1 of 1 sources checked- cites Linde & Noorbala (2010) source
May combine two claims.
PremisecitationIn the cold big bang, nucleosynthesis generally proceeds further than in our universe, creating an approximately solar metallicity intergalactic medium and a 25% helium mass fraction.
“Nucleosynthesis generally proceeds further than in our universe, creating an approximately solar metalicity intergalactic medium along with a 25% helium mass fraction 35 .”
Quote in the paperSubstantial claim1 of 1 sources checked- cites [35] 35. Cs ot o, A., Oberhummer, H. & Schlattl, H., 2001, NuPhA, 688, 560 source
The Abstract describes a QCD calculation of light-hadron masses and mentions the early universe only in connection with a transition from quarks and gluons to hadrons. Searches for cold-big-bang nucleosynthesis, solar metallicity, and a 25% helium mass fraction found no passage addressing those claims in our copy. (LLM, conf=0.77)
Experimental — accuracy not yet measured
May combine two claims.
InterpretationcitationThe cold big bang does not alter nuclear physics and thus still relies on the triple-alpha process to create carbon in the early universe.
“The CBB does not alter nuclear physics and thus still relies on the triple-a process to create carbon in the early universe; see the more detailed discussion of CBB nucleosynthesis inAguirre (1999, p. 22).”
Quote in the paperSubstantial claim1 of 1 sources checked- cites Aguirre (1999, p. 22) source
Section 2 assumes the standard model of particle physics, and Section 4 identifies triple-alpha fusion as the most obvious reaction forming carbon. But Section 4 also says that this reaction becomes ineffective before carbon reaches appreciable abundance in some cold big bang models. The paper therefore does not support an unqualified claim that the process creates primordial carbon. (LLM, conf=0.83)
Experimental — accuracy not yet measured
May combine two claims.
FindingcitationTo make our universe, we would need around 10^90 Planck volumes, all arranged to transition to a classical expanding phase within a temporal window 100,000 times shorter than the Planck time.
“To make our universe, we would need around 10 90 such Planck volumes, all arranged to transition to a classical expanding phase within a temporal window 100 000 times shorter than the Planck time 11 .”
Quote in the paperSubstantial claimMay combine two claims.
FindingcitationThe result that non-flat FLRW universes are infinitely unlikely is independent of x_max and y_max and holds in the limit x_max, y_max -> infinity.
“Note that this is independent of x max and y max , and in particular holds in the limit x max , y max -N.”
Quote in the paperSubstantial claimMay combine two claims.
FindingreasoningThe neutron-proton mass difference is 1.29 MeV, well within the range of m_d - m_u from 1 to ... MeV.
“The neutron-proton mass difference is 1.29 MeV, well within that range.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S4 (based).
Interpretationnone givenNoether's theorems do not allow us to pull physically significant conclusions out of a mathematical hat.
“Neother's theorems do not allow us to pull physically significant conclusions out of a mathematical hat.”
Quote in the paperNot a substantial claimMay combine two claims.
PremisecitationPhysicists are free to postulate theories which are not Lorentz invariant, and a great deal of experimental and theoretical effort has been expended to this end.
“Physicists are perfectly free to postulate theories which are not Lorentz invariant, and a great deal of experimental and theoretical effort has been expended to this end.”
Quote in the paperSubstantial claim0 of 2 sources checked- cites Kostelecky ´& Russell (2011)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- cites Pospelov & Romalis (2004)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Probably not a substantial claim: may not pass S2 (checkable), S4 (based). May combine two claims.
Interpretationnone givenIf ours were the only universe, and the causes that established the physics of our universe were indifferent to whether it would evolve life, then the chances of hitting upon a life-permitting universe are very small.
“The intuition here is that, if ours were the only universe, and if the causes that established the physics of our universe were indifferent to whether it would evolve life, then the chances of hitting upon a life-permitting universe are very small.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S2 (checkable), S4 (based).
Interpretationnone givenMany of Stenger's claims will be found to be highly problematic.
“Many of Stenger's claims will be found to be highly problematic.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing), S4 (based).
Interpretationnone givenThe existence of gravity is not implied by the existence of the universe, separate masses or accelerating frames.
“The existence of gravity is not implied by the existence of the universe, separate masses or accelerating frames.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S2 (checkable), S4 (based).
Interpretationnone givenTo know whether a certain symmetry holds in nature, one needs a laboratory or a telescope, not a blackboard.
“If you want to know whether a certain symmetry holds in nature, you need a laboratory or a telescope, not a blackboard.”
Quote in the paperNot a substantial claimMay combine two claims.
InterpretationreasoningAny solution of the GR equation is covariant, or PoVI, but it does not follow that a particular solution will exhibit any symmetries.
“Thus, any solution of the GR equation is covariant, or PoVI.But it does not follow that a particular solution will exhibit any symmetries.”
Quote in the paperSubstantial claimMay combine two claims.
PremisecitationFor the universe to contain sufficient amounts of ordinary baryonic matter, interactions in the early universe must violate baryon number conservation, charge-symmetry and charge-parity-symmetry, and must spend some time out of thermal equilibrium.
“Sakharov (1967) showed that for the universe to contain sufficient amounts of ordinary baryonic matter, interactions in the early universe must violate baryon number conservation, charge-symmetry and charge-parity-symmetry, and must spend some time out of thermal equilibrium.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Sakharov (1967)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
PremisecitationAbove the blue line, there is only one stable element, a single particle D++, with the chemistry of helium, an inert monatomic gas above 4 K with no known stable chemical compounds.
“Above the blue line, there is only one stable element, which consists of a single particle D þþ .This element has the chemistry of helium -an inert, monatomic gas (above 4 K) with no known stable chemical compounds.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Barr & Khan (2007)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
InterpretationreasoningStenger has failed to solve the entropy problem; he has presented the problem itself as its solution, and homogeneous isotropic expansion cannot solve the entropy problem because it is the entropy problem.
“We conclude that Stenger has failed to solve the entropy problem.He has presented the problem itself as its solution.Homogeneous, isotropic expansion cannot solve the entropy problem -it is the entropy problem.”
Quote in the paperSubstantial claimMay combine two claims.
Premisenone givenIf electrons were bosons rather than fermions, they would not obey the Pauli exclusion principle and there would be no chemistry.
“If electrons were bosons, rather than fermions, then they would not obey the Pauli exclusion principle.There would be no chemistry.”
Quote in the paperNot a substantial claimMay combine two claims.
InterpretationreasoningStenger's statement that in the fine-tuning view there is no wedge and the point has infinitesimal area, so the probability of finding life is zero, is not true of the scientific literature; the wedge is a straw man.
“Stenger further distorts the case for fine-tuning by saying: 'In the fine-tuning view, there is no wedge and the point has infinitesimal area, so the probability of finding life is zero.' (FOFT 70) No reference is given, and this statement is not true of the scientific literature.The wedge is a straw man.”
Quote in the paperNot a substantial claimClassified as probably not a substantial claim.
PremisecitationTegmark et al. (2006) Table 4 summarizes 8 anthropic constraints on the 7 dimensional parameter space (a, b, m_p, rho_L, Q, x, x_baryon).
“See Table 4 of Tegmark et al. (2006) for a summary of 8 anthropic constraints on the 7 dimensional parameter space (a, b, m p , r L , Q, x, x baryon ).”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Tegmark et al. (2006)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
Premisenone givenIf the strong force were long-range rather than short-range, there would be no atoms, and any structures would be uniform, spherical, undifferentiated lumps of arbitrary size incapable of complexity.
“If the strong force were a long rather than short-range force, then there would be no atoms.Any structures that formed would be uniform, spherical, undifferentiated lumps, of arbitrary size and incapable of complexity.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S3 (load-bearing), S4 (based). May combine two claims.
Interpretationnone givenStars in a universe with a bound diproton would be significantly different from our own, and detailed predictions for their formation and evolution have not been investigated.
“However, stars in such a universe would be significantly different to our own, and detailed predictions for their formation and evolution have not been investigated.”
Quote in the paperNot a substantial claimMay combine two claims.
PremisecitationAbove the green curve, neutrons in nuclei decay, so hydrogen is the only stable element.
“Above the green curve, neutrons in nuclei decay, so that hydrogen is the only stable element.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Barr & Khan (2007)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Classified as probably not a substantial claim.
PremisecitationFigure 2 top right shows boundaries of 9 independent life-permitting criteria in the quark-mass parameter space.
“Figure 2 (top right) zooms in on a region of parameter space, showing boundaries of 9 independent lifepermitting criteria:”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Barr & Khan (2007)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Probably not a substantial claim: may not pass S3 (load-bearing).
InterpretationreasoningEven if the symmetries of the laws of nature were logically necessary, it would still be an open question as to precisely which symmetries were broken in our universe and which were unbroken.
“Even if the symmetries of the laws of nature were logically necessary, it would still be an open question as to precisely which symmetries were broken in our universe and which were unbroken.”
Quote in the paperNot a substantial claimMay combine two claims.
PremisereasoningThe entropy of the universe is not at its theoretical maximum, and since entropy cannot decrease, the universe must have started in a very special, low entropy state.
“The fact that the entropy of the universe is not at its theoretical maximum, coupled with the fact that entropy cannot decrease, means that the universe must have started in a very special, low entropy state.”
Quote in the paperSubstantial claimMay combine two claims.
PremisecitationBarr & Khan (2007) explored the parameter space of a model in which up-type and down-type fermions acquire mass from different Higgs doublets, varying the masses of the up and down quarks; the natural scale for these masses ranges over 60 orders of magnitude.
“Barr & Khan (2007) explored the parameter space of a model in which up-type and down-type fermions acquire mass from different Higgs doublets.As a first step, they vary the masses of the up and down quarks.The natural scale for these masses ranges over 60 orders of magnitude and is illustrated in Figure 2 (top left).”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Barr & Khan (2007)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
Premisenone givenThe electromagnetic force allows matter to cool into galaxies, stars, and planets; without such interactions, all matter would be like dark matter, forming only large diffuse roughly spherical haloes and subhaloes.
“The electromagnetic force allows matter to cool into galaxies, stars, and planets.Without such interactions, all matter would be like dark matter, which can only form into large, diffuse, roughly spherical haloes of matter whose only internal structure consists of smaller, diffuse, roughly spherical subhaloes.”
Quote in the paperSubstantial claimClassified as probably not a substantial claim. May combine two claims.
InterpretationreasoningStenger simply assumes that the universe is homogeneous and isotropic; once homogeneity and isotropy are assumed, the entropy problem does not seem so hard.
“Stenger simply assumes that the universe is homogeneous and isotropic.We can see this also in his use of the Friedmann equation, which assumes that spacetime is homogeneous and isotropic.Not surprisingly, once homogeneity and isotropy have been assumed, the entropy problem doesn't seem so hard.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S2 (checkable). May combine two claims.
Interpretationnone givenFine-tuning is not about what the parameters and laws are in a particular universe; rather, given some other set of laws, we ask what is the probability that a universe chosen at random from the set of universes with those laws would support intelligent life.
“In reply, fine-tuning isn't about what the parameters and laws are in a particular universe.Given some other set of laws, we ask: if a universe were chosen at random from the set of universes with those laws, what is the probability that it would support intelligent life?”
Quote in the paperNot a substantial claimMay combine two claims.
PremisecitationMacDonald & Mullan (2009) show that while a 13% increase in the strength of the strong force will bind the diproton, a less than 50% increase is needed to significantly affect the amount of hydrogen left over for stars.
“For example, MacDonald & Mullan (2009) show that while an increase in the strength of the strong force by 13% will bind the diproton, a ,50% increase is needed to significantly affect the amount of hydrogen left over for stars.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites MacDonald & Mullan (2009)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
InterpretationreasoningStenger's assertion that the universe starts out with maximum entropy or complete disorder is false; a homogeneous, isotropic spacetime is an incredibly low entropy state.
“Stenger's assertion that 'the universe starts out with maximum entropy or complete disorder' is false.A homogeneous, isotropic spacetime is an incredibly low entropy state.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
PremisecitationSpontaneous symmetry breaking allows the laws of nature to retain their symmetry and yet have asymmetric solutions.
“SSB allows the laws of nature to retain their symmetry and yet have asymmetric solutions.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Strocchi 2007 source
May combine two claims.
Premisenone givenFine-tuning relies on a number of independent life-permitting criteria; failing any of these criteria makes life dramatically less likely, if not impossible.
“In response, fine-tuning relies on a number of independent life-permitting criteria.Fail any of these criteria, and life becomes dramatically less likely, if not impossible.”
Quote in the paperSubstantial claimMay combine two claims.
InterpretationreasoningTo significantly change the probability of a life-permitting universe, we would need a prior that centres close to the observed value and has a narrow peak; this exchanges one fine-tuning for two, the centre and peak of the distribution.
“In short, to significantly change the probability of a lifepermitting universe, we would need a prior that centres close to the observed value, and has a narrow peak.But this simply exchanges one fine-tuning for two -the centre and peak of the distribution.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S2 (checkable), S3 (load-bearing).
InterpretationreasoningThe wedge commits the flippant funambulist fallacy.
“The wedge thus commits the flippant funambulist fallacy (Section 2).”
Quote in the paperNot a substantial claimMay combine two claims.
PremisecitationBelow the red line, a proton in a nucleus can capture an orbiting electron and become a neutron, so atoms are unstable.
“Below this red line, a proton in a nucleus can capture an orbiting electron and become a neutron.Thus, atoms are unstable.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Barr & Khan (2007)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
PremisecitationAbove the red line, the deuteron is strongly unstable, decaying via the strong force, so the first step in stellar nucleosynthesis in hydrogen burning stars would fail.
“Above this red line, the deuteron is strongly unstable, decaying via the strong force.The first step in stellar nucleosynthesis in hydrogen burning stars would fail.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Barr & Khan (2007)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
PremisecitationBelow the red curve, the diproton is stable; two protons can fuse to helium-2 via a very fast electromagnetic reaction rather than the much slower weak nuclear pp-chain.
“Below this red curve, the diproton is stable 9 .Two protons can fuse to helium-2 via a very fast electromagnetic reaction, rather than the much slower, weak nuclear pp-chain.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Barr & Khan (2007)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
Interpretationnone givenIf we vary x only and calculate P_x, and then vary y only and calculate P_y, we must not simply multiply P_w = P_x P_y; doing so will certainly underestimate the probability inside the wedge, assuming a single wedge.
“If we vary x only and calculate P x , and then vary y only and calculate P y , we must not simply multiply P w ¼ P x P y .This will certainly underestimate the probability inside the wedge, assuming that there is only a single wedge.”
Quote in the paperNot a substantial claim- The authors state this as an assumption: There is only a single wedge.
May combine two claims.
PremisecitationAbove the red line, production of deuterium in stars absorbs energy rather than releasing it, and the deuterium is unstable to weak decay.
“Above this red line, the production of deuterium in stars absorbs energy rather than releasing it.Also, the deuterium is unstable to weak decay.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Barr & Khan (2007)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
InterpretationreasoningThere are a number of problems with Stenger's argument, the most severe of which arises even if we assume his calculation is correct.
“There are a number of problems with Stenger's argument, the most severe of which arises even if we assume that his calculation is correct.”
Quote in the paperNot a substantial claimMay combine two claims.
InterpretationreasoningIf epsilon is small enough, the wedge is a tightrope; we have opened up more parameter space in which life can form, but also more parameter space in which life cannot form.
“If is small enough, then the wedge is a tightrope.We have opened up more parameter space in which life can form, but we have also opened up more parameter space in which life cannot form.”
Quote in the paperSubstantial claimMay combine two claims.
PremisecitationBelow the blue line, the only stable element is a single particle D-, which can combine with a positron to produce an element with the chemistry of hydrogen; a handful of chemical reactions are possible, with the most complex product being an analogue of H2.
“Below this blue line, the only stable element consists of a single particle D À , which can combine with a positron to produce an element with the chemistry of hydrogen.A handful of chemical reactions are possible, with their most complex product being (an analogue of) H 2 .”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Barr & Khan (2007)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Classified as probably not a substantial claim.
PremisecitationPenrose's reasoning is that if the universe started at t1 with an extremely homogeneous spacetime and ended at t2 with an extremely inhomogeneous spacetime full of black holes, then the t2 spacetime represents a significantly higher entropy state than the t1 spacetime.
“Penrose's reasoning is very simple.If we started at t 1 with an extremely homogeneous spacetime, and then allowed a few billion years of entropy increasing processes to take their toll, and ended at t 2 with an extremely inhomogeneous spacetime, full of black holes, then we must conclude that the t 2 spacetime represents a significantly higher entropy state than the t 1 spacetime.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Penrose (1979)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Probably not a substantial claim: may not pass S2 (checkable), S4 (based). May combine two claims.
Interpretationnone givenWith no physical model of the inflaton, the necessary coupling between the inflaton and ordinary matter or radiation is another postulate, but not an implausible one.
“With no physical model of the inflaton, the necessary coupling between the inflaton and ordinary matter/radiation is another postulate, but not an implausible one.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing). May combine two claims.
Premisenone givenInflation is not a specific model but a family of models sharing an early epoch of accelerating expansion; it is an effect rather than a cause.
“Firstly, inflation isn't a specific model as such; it is a family of models which share the desirable trait of having an early epoch of accelerating expansion.Inflation is an effect, rather than a cause.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S4 (based). May combine two claims.
PremisereasoningIf inflation ends, its energy must be converted into ordinary matter; inflation must not result in a universe filled with pure radiation or dark matter, which cannot form complex structures.
“If inflation ends, we need its energy to be converted into ordinary matter (Condition I5).Inflation must not result in a universe filled with pure radiation or dark matter, which cannot form complex structures.”
Quote in the paperNot a substantial claimMay combine two claims.
PremisecitationInflation predicts a Gaussian random field of density fluctuations, but this is not unique to inflation because of the central limit theorem.
“Inflation predicts a Gaussian random field of density fluctuations, but thanks to the central limit theorem this isn't particularly unique (Peacock 1999, p. 342, 503).”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Peacock 1999 source
May combine two claims.
Premisenone givenThere is no physical theory that predicts the form of the inflaton potential; different potentials and initial conditions produce different predictions.
“There is no physical theory that predicts the form of the inflaton potential.Different potentials, and different initial conditions for the same potential, will produce different predictions.”
Quote in the paperNot a substantial claimMay combine two claims.
Premisenone givenInflation solves the flatness, horizon, and monopole problems and gives concrete, testable, seemingly correct predictions for the origin of cosmic structure.
“The achievements of inflation are truly impressive -in one fell swoop, the universe is sent on its expanding way, the flatness, horizon, and monopole problem are solved and we have concrete, testable and seemingly correct predictions for the origin of cosmic structure.”
Quote in the paperSubstantial claimMay combine two claims.
PremisereasoningTo set up a life-permitting universe, inflation must end in the right way: the universe must be reheated with ordinary matter, and the post-inflation field must not possess a large negative potential energy that would cause quick recollapse.
“I5.Inflation must end in the right way.Inflation will have exponentially diluted the mass-energy density of the universe -it is this feature that allows inflation to solve the monopole problem.Once we are done inflating the universe, we must reheat the universe, i.e. refill it with ordinary matter.We must also ensure that the post-inflation field doesn't possess a large, negative potential energy,”
Quote in the paperSubstantial claimMay combine two claims.
PremisecitationSince life requires an almost-flat universe, inflation is potentially a solution to a particularly impressive fine-tuning problem; without inflation, the density of a life-permitting universe at the Planck time must be tuned to 60 decimal places.
“Since life requires an almost-flat universe (Barrow & Tipler 1986, p. 408ff.),inflation is potentially a solution to a particularly impressive fine-tuning problem -sans inflation, the density of a life-permitting universe at the Planck time must be tuned to 60 decimal places.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Barrow & Tipler 1986
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Probably not a substantial claim: may not pass S2 (checkable).
InterpretationreasoningThe question is not why the low entropy state was at the beginning of the universe, but why the universe was ever in a low entropy state.
“The question is not why the low entropy state was at the beginning of the universe, but why the universe was ever in a low entropy state.”
Quote in the paperNot a substantial claimMay combine two claims.
InterpretationcitationI1 is a bare hypothesis: we know of no deeper reason why there should be an inflaton field at all, and there is no direct evidence for its existence.
“I1 is a bare hypothesiswe know of no deeper reason why there should be an inflaton field at all.It was hoped that the inflaton field could be the Higgs field (Guth 1981).Alas, it wasn't to be, and it appears that the inflaton's sole raison d'e ˆtre is to cause the universe's expansion to briefly accelerate.There is no direct evidence for the existence of the inflaton field.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Guth 1981
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
PremisecitationI4 is non-trivial: the inflaton potential must have a region where the slow-roll approximation does not hold; if the inflaton rolls into a local minimum while the SRA still holds, inflation never ends.
“I4 is non-trivial.The inflaton potential (or, more specifically, the region of the inflaton potential which actually determines the evolution of the field) must have a region in which the slow-roll approximation does not hold.If the inflaton rolls into a local minimum (at f 0 ) while the SRA still holds (which requires V(f 0 ) c m Pl 2 / 8p d 2 V/df 2 9 f 0 Peacock 1999, p. 332), then inflation”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Peacock 1999 source
May combine two claims.
InterpretationreasoningInflation is a clever solution of the flatness and horizon problem, but could be rendered unnecessary by a quantum-gravity theory of initial conditions; the evidence for inflation is impressive but circumstantial.
“Inflation is a clever solution of the flatness and horizon problem, but could be rendered unnecessary by a quantum-gravity theory of initial conditions.The evidence for inflation is impressive but circumstantial.”
Quote in the paperNot a substantial claimMay combine two claims.
PremisereasoningTo set up a life-permitting universe, inflation must last: the inflaton must obey slow roll conditions for sufficiently long, with the number of e-folds greater than about 60 to solve the horizon and flatness problems.
“I3.Inflation must last.While the inflaton field controls the dynamics of the expansion of the universe, we need it to obey the slow roll conditions for a sufficiently long period of time.The 'amount of inflation' is usually quantified by N e , the number of e-folds of the size of the universe.To solve the horizon and flatness problems, this number must be greater than ,60.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S1 (asserted). May combine two claims.
InterpretationcitationHollands & Wald (2002b) contend that inflation does need special initial conditions: a collapsing universe would require an astonishing sequence of correlations and coincidences to convert all matter into a scalar field with enough kinetic energy to roll to the top of its potential and remain balanced long enough for deflation; the region of final-condition-space resulting from deflation is much较小
“Hollands & Wald (2002b) 15 contend not, for the following reason.Consider a collapsing universe.It would require an astonishing sequence of correlations and coincidences for the universe, in its final stages, to suddenly and coherently convert all its matter into a scalar field with just enough kinetic energy to roll to the top of its potential and remain perfectly balanced there for long enough”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Hollands & Wald (2002b)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
PremisereasoningRequirement I6 brought about the downfall of old inflation: when it ended, it did so in expanding bubbles too small to account for the homogeneity of the observed universe, and reheating only occurs when bubbles collide; as the space between bubbles is still inflating, homogeneity cannot be achieved.
“Requirement I6 brought about the downfall of 'old' inflation.When this version of inflation ended, it did so in expanding bubbles.Each bubble is too small to account for the homogeneity of the observed universe, and reheating only occurs when bubbles collide.As the space between the bubbles is still inflating, homogeneity cannot be achieved.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
PremisecitationThe cosmological constant problem is arguably the most severe theoretical problem in high-energy physics today.
“The cosmological constant problem is described in the textbook of Burgess & Moore (2006) as 'arguably the most severe theoretical problem in high-energy physics today, as measured by both the difference between observations and theoretical predictions, and by the lack of convincing theoretical ideas which address it'.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Burgess & Moore (2006)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Probably not a substantial claim: may not pass S3 (load-bearing), S4 (based).
Premisenone givenMore generally, the value of Q that results from inflation depends on the potential and initial conditions.
“More generally, the value of Q that results from inflation depends on the potential and initial conditions.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Premisenone givenInflation proposes that the universe underwent a period of accelerated expansion in its earliest stages.
“We turn now to cosmic inflation, which proposes that the universe underwent a period of accelerated expansion in its earliest stages.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S2 (checkable), S4 (based).
Premisenone givenIf the solution is just as fine-tuned as the problem, then no progress has been made.
“if the solution is just as fine-tuned as the problem, then no progress has been made.”
Quote in the paperNot a substantial claimMay combine two claims.
InterpretationreasoningPost inflation, our universe settles into the minimum at f = f0, and the V0 term contributes to the effective cosmological constant.
“Post inflation, our universe settles into the minimum at f 5 f 0 , and the V 0 term contributes to the effective cosmological constant.”
Quote in the paperSubstantial claimMay combine two claims.
InterpretationreasoningThe puzzle is not just to understand why the zero point energy does not gravitate, but why it gravitates in some environments but not in vacuum.
“The puzzle is not just to understand why the zero point energy does not gravitate, but why it gravitates in some environments but not in vacuum.”
Quote in the paperSubstantial claimMay combine two claims.
InterpretationreasoningThe cosmological constant problem is not a problem only at the Planck scale and thus quantum gravity is unlikely to provide a solution.
“The cosmological constant problem is not a problem only at the Planck scale and thus quantum gravity is unlikely to provide a solution.”
Quote in the paperNot a substantial claimMay combine two claims.
PremisereasoningThe vacuum polarisation contribution to the Lamb shift gives a nonzero contribution to the energy of the atom, and thus by the equivalence principle must couple to gravity.
“The vacuum polarisation contribution to the Lamb shift is known to give a nonzero contribution to the energy of the atom, and thus by the equivalence principle must couple to gravity.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Premisenone givenSupersymmetry, if it holds in our universe, would reduce the required fine-tuning of the cosmological constant to one part in ~10^50.
“Supersymmetry, if it holds in our universe, would cancel out some of the contributions to the vacuum energy, reducing the required fine-tuning to one part in ,10 50 .”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S4 (based).
Interpretationnone givenSupersymmetry won't help solve the cosmological constant problem.
“Supersymmetry won't help.”
Quote in the paperNot a substantial claimMay combine two claims.
InterpretationreasoningIf the dark energy scale is the Planck scale, then r_Q is 120 orders of magnitude larger than the life-permitting scale, exchanging the fine-tuning of the cosmological constant for the fine-tuning of dark energy.
“In that case, r Q is once again 120 orders of magnitude larger than the life-permitting scale, and we have simply exchanged the fine-tuning of the cosmological constant for the fine-tuning of dark energy.”
Quote in the paperSubstantial claimMay combine two claims.
PremisecitationThere is a window of opportunity for stars: too small and they won't ignite and sustain nuclear fusion, too large and radiation pressure will dominate over thermal pressure, allowing unstable pulsations.
“There is a window of opportunity for stars -too small and they won't be able to ignite and sustain nuclear fusion at their cores, being supported against gravity by degeneracy rather than thermal pressure; too large and radiation pressure will dominate over thermal pressure, allowing unstable pulsations.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Barrow & Tipler (1986)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
InterpretationreasoningThe inflaton field is yet another contributor to the vacuum energy of the universe, and one with universe-accelerating pedigree.
“Further, the inflaton field is yet another contributor to the vacuum energy of the universe, and one with universeaccelerating pedigree.”
Quote in the paperSubstantial claimMay combine two claims.
Interpretationnone givenQuintessence and the inflaton field are just more fields whose vacuum state must be sternly commanded not to gravitate, or else mutually balanced to an alarming degree.
“Quintessence and the inflaton field are just more fields whose vacuum state must be sternly commanded not to gravitate, or else mutually balanced to an alarming degree.”
Quote in the paperSubstantial claimMay combine two claims.
Interpretationnone givenThere is no known symmetry that would set V0 = 0, because we do not know what the inflaton is.
“There is no known symmetry that would set V 0 ¼ 0, because we do not know what the inflaton is.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S4 (based).
Interpretationnone givenThere is some physical reason why the large contributions to the vacuum energy of the universe don't make it life-prohibiting.
“There is some reason -some physical reasonwhy the large contributions to the vacuum energy of the universe don't make it life-prohibiting.”
Quote in the paperNot a substantial claimMay combine two claims.
InterpretationreasoningEven with logarithmic axes, fine-tuning cannot be avoided because zero is a possible value of G and thus is part of parameter space.
“Even with logarithmic axes, fine-tuning cannot be avoided -zero is a possible value of G, and thus is part of parameter space.”
Quote in the paperSubstantial claimClassified as probably not a substantial claim.
Premisenone givenQuintessence has an equation of state w = p/rho that causes the expansion of the universe to accelerate if w < -1/3.
“One could appeal to an as-yet-unknown form of energy called quintessence, which has an equation of state w 5 p/r that causes the expansion of the universe to accelerate 21 (w , À1/3).”
Quote in the paperSubstantial claimMay combine two claims.
PremisecitationNongravitational physics depends only on energy differences, so the standard model cannot respond to the actual value of the cosmological constant it sources.
“ynongravitational physics depends only on energy differences, so the standard model cannot respond to the actual value of the cosmological constant it sources.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Bousso (2008)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Probably not a substantial claim: may not pass S2 (checkable).
InterpretationcitationQuintessence is a unicorn in a duck outfit (i.e., pure speculation).
“Quintessence is a unicorn in a duck outfit.We are discounting a form of energy with a plausible, independent theoretical underpinning in favour of one that is pure speculation.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S4 (based).
Interpretationnone givenMost proposed inflation mechanisms operate near the Planck scale, so this defines the possible range of V0.
“Most proposed inflation mechanisms operate near the Planck scale, so this defines the possible range of V 0 .”
Quote in the paperNot a substantial claimMay combine two claims.
InterpretationreasoningA logarithmic axis, by placing G = 0 at negative infinity, puts an infinitely large region of parameter space outside of the life-permitting region, so stable stars would require infinite fine-tuning.
“A logarithmic axis, by placing G ¼ 0 at negative infinity, puts an infinitely large region of parameter space outside of the life-permitting region.Stable stars would then require infinite fine-tuning.”
Quote in the paperSubstantial claimMay combine two claims.
PremisecitationFor hydrogen to exist, m_e, m_n - m_p must hold; otherwise the electron will be captured by the proton to form a neutron.
“For hydrogen to exist -to power stars and form water and organic compounds -we must have m e , m n À m p .Otherwise, the electron will be captured by the proton to form a neutron (Hogan 2006;Damour & Donoghue 2008).”
Quote in the paperSubstantial claim0 of 2 sources checked- cites Hogan 2006
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- cites Damour & Donoghue 2008
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Probably not a substantial claim: may not pass S3 (load-bearing).
Premisenone givenThe Hoyle resonance in carbon is one of the most famous examples of fine-tuning.
“One of the most famous examples of fine-tuning is the Hoyle resonance in carbon.”
Quote in the paperNot a substantial claimMay combine two claims.
PremisecitationThe typical energy of chemical reactions must be much smaller than the typical energy of nuclear reactions to ensure atomic constituents maintain identity in chemical reactions; this requires alpha^2 beta / alpha_s^2 << 1.
“We require that the typical energy of chemical reactions is much smaller than the typical energy of nuclear reactions.This ensures that the atomic constituents of chemical species maintain their identity in chemical reactions.This requires a 2 b/a s 2 { 1 (Barrow & Tipler 1986, p. 320).”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Barrow & Tipler 1986
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Probably not a substantial claim: may not pass S3 (load-bearing).
PremisecitationThe right solid line shows the boundary of the condition that protons be stable on stellar timescales (beta^2 > alpha (alpha_G exp alpha^{-1})^{-1}).
“The right solid line shows the boundary of the condition that protons be stable on stellar timescales (b 2 .a (a G exp a À1 ) À1 , Barrow & Tipler 1986, p. 358).”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Barrow & Tipler 1986
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
PremisecitationFor v > 1e-16, the neutron is heavier than the proton by more than the nucleon's binding energy, so that even bound neutrons decay into protons and no nuclei larger than hydrogen are stable.
“for v .10 À16 , the neutron is heavier than the proton by more than the nucleon's binding energy, so that even bound neutrons decay into protons and no nuclei larger than hydrogen are stable;”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Agrawal et al. (1998a, b)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Probably not a substantial claim: may not pass S3 (load-bearing).
Premisenone givenThe left solid line shows the lower limit alpha > 1/180 for a grand-unified theory to unify no higher than the Planck scale.
“The left solid line shows the lower limit a .1/180 for a grand-unified theory to unify no higher than the Planck scale.”
Quote in the paperNot a substantial claimMay combine two claims.
PremisecitationModelling the later, post-hydrogen-burning stages of stellar evolution is difficult even for modern codes, and the inclusion of He-shell flashes seems to lessen the degree of fine-tuning of the Hoyle resonance.
“Modelling the later, post-hydrogen-burning stages of stellar evolution is difficult even for modern codes, and the inclusion of He-shell flashes seems to lessen the degree of fine-tuning of the Hoyle resonance.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Schlattl et al. (2004)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
InterpretationreasoningThis ensures that the photons emitted by stars have the right energy to break chemical bonds, permitting photosynthesis.
“In other words, it ensures that the photons emitted by stars have the right energy to break chemical bonds.This permits photosynthesis, allowing electromagnetic energy to be converted into and stored as chemical energy in plants.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S3 (load-bearing). May combine two claims.
PremisecitationThe 0+ state is known as a breathing mode, and all nuclei have such a state.
“As Cohen (2008) notes, the 0 þ state is known as a breathing mode; all nuclei have such a state.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Cohen (2008)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
PremisecitationUnless alpha_s/alpha_s,0 > 1.003 + 0.031 alpha/alpha_0, the diproton has a bound state, which affects stellar burning and big bang nucleosynthesis.
“Unless a s /a s,0 t 1.003 þ 0.031a/a 0 (Davies 1972), the diproton has a bound state, which affects stellar burning and big bang nucleosynthesis.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Davies 1972
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Classified as probably not a substantial claim.
Interpretationnone givenThe fact that our universe isn't particularly close to the life-permitting boundary is irrelevant to fine-tuning as defined.
“Note further that the fact that our universe (the triangle in Figure 5) isn't particularly close to the life-permitting boundary is irrelevant to fine-tuning as we have defined it.”
Quote in the paperSubstantial claimMay combine two claims.
PremisecitationA change of 0.4% in the strength of the nucleon-nucleon force would make carbon-based life impossible, because stars would produce either almost solely carbon or oxygen, but not both.
“Even with a change of 0.4% in the strength of [nucleon-nucleon] force, carbon-based life appears to be impossible, since all the stars then would produce either almost solely carbon or oxygen, but could not produce both elements.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Oberhummer, Cs ot o & Schlattl (2000a)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
PremisecitationDamour & Donoghue (2008) concluded that unless 0.78e-17 < v < 3.3e-17 hydrogen is unstable to the reaction p+e->n+nu (if v is too small) or else there is no nuclear binding at all (if v is too large).
“Damour & Donoghue (2008) refined the limits of Agrawal et al. by considering nuclear binding, concluding that unless 0.78 Â 10 À17 , v , 3.3 Â 10 À17 hydrogen is unstable to the reaction p”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Damour & Donoghue (2008)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Probably not a substantial claim: may not pass S3 (load-bearing).
PremisecitationJaffe et al. (2009) examined a different slice through parameter space, varying the masses of the quarks while holding as much as possible of the rest of the Standard Model phenomenology constant.
“Jaffe et al. (2009) examined a different slice through parameter space, varying the masses of the quarks while 'holding as much as possible of the rest of the Standard Model phenomenology constant' [emphasis original].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Jaffe et al. (2009)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
InterpretationcitationThe masses must be sufficiently small but not too small.
“The masses must be sufficiently small but not too small.”
Quote in the paperSubstantial claimClassified as probably not a substantial claim. May combine two claims.
PremisecitationGould (2010) argued that three or more generations of quarks and leptons are required for CP violation, which is one of the necessary conditions for baryogenesis.
“Gould (2010) has argued that three or more generations of quarks and leptons are required for CP violation, which is one of the necessary conditions for baryogenesis (Sakharov 1967;Cahn 1996;Schellekens 2008).”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Gould (2010)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Probably not a substantial claim: may not pass S4 (based).
Premisenone givenThe strength of the strong force alpha_s is a function of the energy of the interaction.
“The strength of the strong force a s is a function of the energy of the interaction.”
Quote in the paperNot a substantial claimMay combine two claims.
PremisecitationFor v > 2e-14, only the D++ particle is stable and the only stable nucleus has the chemistry of helium.
“for v . 2 Â 10 À14 , only the D þþ particle is stable and the only stable nucleus has the chemistry of helium;”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Agrawal et al. (1998a, b)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
PremisecitationIf all neutrinos are heavy, then neutrons would be stable and big bang nucleosynthesis would leave no hydrogen for stars and organic compounds.
“If all neutrinos are heavy, then neutrons would be stable and big bang nucleosynthesis would leave no hydrogen for stars and organic compounds.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Tegmark, Vilenkin & Pogosian (2005)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
PremisecitationFor v < 2e-19, stars will form very slowly (<10^17 yr) and burn out very quickly (<1 yr), and the large number of stable nucleon species may make nuclear reactions so easy that the universe contains no light nuclei.
“for v t 2 Â 10 À19 , stars will form very slowly (,10 17 yr) and burn out very quickly (,1 yr), and the large number of stable nucleon species may make nuclear reactions so easy that the universe contains no light nuclei.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Agrawal et al. (1998a, b)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Probably not a substantial claim: may not pass S3 (load-bearing).
PremisecitationHall & Nomura (2008) state that v/L_QCD ~ 1 is required so that the baryon asymmetry of the early universe is not washed out by sphaleron effects.
“Hall & Nomura (2008) state that v/L QCD , 1 is required 'so that the baryon asymmetry of the early universe is not washed out by sphaleron effects' (see also Arkani-Hamed et al. 2005).”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Hall & Nomura (2008)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Probably not a substantial claim: may not pass S3 (load-bearing).
Premisenone givenLambda_QCD is the mass-energy scale at which alpha_s diverges.
“L QCD is the mass-energy scale 30 The most charitable reading of Stenger's claim is that he is referring to the constituent quark model, wherein the mass-energy of the cloud of virtual quarks and gluons that surround a valence quark in a composite particle is assigned to the quark itself.”
Quote in the paperNot a substantial claimClassified as probably not a substantial claim.
PremisecitationHogan (2006) concluded that increases in v/L_QCD of more than a few percent lead to major changes in the overall cosmic carbon creation and distribution.
“Hogan (2006) reached a similar conclusion: 'In the absence of an identified compensating factor, increases in [v/L QCD ] of more than a few percent lead to major changes in the overall cosmic carbon creation and distribution'.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Hogan (2006)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Classified as probably not a substantial claim. May combine two claims.
PremisecitationOnly nuclear stability is considered, so that a universe is deemed congenial if both carbon and hydrogen are stable.
“Only nuclear stability is considered, so that a universe is deemed congenial if both carbon and hydrogen are stable.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Jaffe et al. (2009)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
InterpretationreasoningIf the LHC discovers that supersymmetry is a (broken) symmetry of our universe, this would not be the discovery that the universe could not have been different; it would at most show that our universe has chosen a particularly elegant and beautiful way to be life-permitting.
“Finally, suppose that the LHC discovers that supersymmetry is a (broken) symmetry of our universe.This would not be the discovery that the universe could not have been different.It would not be the discovery that the masses of the fundamental particles must be small.It would at most show that our universe has chosen a particularly elegant and beautiful way to be life-permitting.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S4 (based).
Premisenone givenIn Planck units, Lambda_QCD ~ 10^-20 m_Pl.
“In Planck units, L QCD E 10 À20 m Pl .”
Quote in the paperNot a substantial claimMay combine two claims.
InterpretationreasoningStars in the weakless universe will burn at a lower temperature, and probably with shorter lifetimes.
“Stars will burn at a lower temperature, and probably with shorter lifetimes.”
Quote in the paperSubstantial claimMay combine two claims.
PremisecitationHarnik, Kribs & Perez (2006) attempted to find a region of parameter space which is life-permitting in the absence of the weak force, and plausibly discovered one.
“Harnik, Kribs & Perez (2006) attempted to find a region of parameter space which is life-permitting in the absence of the weak force.With some ingenuity, they plausibly discovered one, subject to the following conditions.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Harnik, Kribs & Perez (2006)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Probably not a substantial claim: may not pass S1 (asserted), S3 (load-bearing), S4 (based).
Premisenone givenThe question why Lambda_SM << m_Pl is known as the mu-problem.
“This is known in the literature as 'the m-problem', in reference to the parameter in the supersymmetric potential that sets the relevant mass scale.”
Quote in the paperNot a substantial claimClassified as probably not a substantial claim.
PremisecitationJaffe et al. fix the electron mass, and vary Lambda_QCD so that the average mass of the lightest baryon(s) is 940 MeV, as in our universe.
“In particular, they fix the electron mass, and vary L QCD so that the average mass of the lightest baryon(s) is 940 MeV, as in our universe.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Jaffe et al. (2009)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
PremisecitationTo make this work in our universe, we need alpha_s(m_U) ~ 1/25, and m_U ~ 10^16 GeV.
“To make this work in our universe, we need a s (m U ) E 1/25, and m U E 10 16 GeV (De Boer & Sander 2004).”
Quote in the paperSubstantial claim0 of 1 sources checked- cites De Boer & Sander 2004
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
PremisecitationLow-energy supersymmetry does not by itself explain the magnitude of the weak scale, though it protects it from radiative correction.
“Low-energy supersymmetry does not by itself explain the magnitude of the weak scale, though it protects it from radiative correction (Barr & Khan 2007).”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Barr & Khan 2007
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Probably not a substantial claim: may not pass S3 (load-bearing), S4 (based).
Premisenone givenThe value of mu in our universe is probably 10^2-10^3 GeV.
“The value of m in our universe is probably ,10 2 -10 3 GeV.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S4 (based).
Premisenone givenThe probability of a thermal fluctuation decreases exponentially with its volume.
“Because the probability of a thermal fluctuation decreases exponentially with its volume.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Interpretationnone givenWhen Stenger compares two different values for the quark masses (3.3 MeV and 1.5-3 MeV), he is comparing two measurements, not a theoretical calculation with an experimental measurement.
“When Stenger compares two different values for the quark masses (3.3 MeV and 1.5-3 MeV), he is not comparing a theoretical calculation with an experimental measurement.He is comparing two measurements.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S2 (checkable).
InterpretationreasoningWe can rephrase the claim 'if space were not three dimensional, then life would not exist' as 'if whatever exists were not such that it is accurately described on macroscopic scales by a model with three space dimensions, then life would not exist'.
“We just rephrase the claim: instead of 'if space were not three dimensional, then life would not exist', we instead claim 'if whatever exists were not such that it is accurately described on macroscopic scales by a model with three space dimensions, then life would not exist'.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S2 (checkable), S3 (load-bearing).
Interpretationnone givenIf some meta-law is proposed to physically generate a multiverse, then we need to postulate not just that the meta-law holds in this universe, but that it holds in some pre-existing metaspace beyond our universe.
“If some meta-law is proposed to physically generate a multiverse, then we need to postulate not just a.) that the meta-law holds in this universe, but b.) that it holds in some pre-existing metaspace beyond our universe.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S2 (checkable), S4 (based).
InterpretationreasoningEmergent does not imply subjective.
“But emergent does not imply subjective.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
PremisecitationCahn notes that if the couplings are fixed at high energy, then their value at low energy depends on the masses of particles only ever seen in particle accelerators.
“Cahn (1996) notes that if the couplings are fixed at high energy, then their value at low energy depends on the masses of particles only ever seen in particle accelerators.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Cahn (1996)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Probably not a substantial claim: may not pass S3 (load-bearing).
InterpretationreasoningAs Stenger has presented it, grand unification is a cane toad solution, as no attempt is made to assess whether the GUT parameters are fine-tuned.
“As Stenger has presented it, grand unification is a cane toad solution, as no attempt is made to assess whether the GUT parameters are fine-tuned.”
Quote in the paperNot a substantial claimMay combine two claims.
PremisecitationThe pattern α3 > α2 > α1 seems to be generic, since the antiscreening or asymptotic freedom effect is more pronounced for larger gauge groups, which have more types of virtual gluons.
“The pattern a 3 c a 2 .a 1 seems to be generic, since 'the antiscreening or asymptotic freedom effect is more pronounced for larger gauge groups, which have more types of virtual gluons' (Wilczek 1997).”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Wilczek 1997
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Probably not a substantial claim: may not pass S3 (load-bearing). May combine two claims.
PremisecitationThis is the 'measure problem' of cosmology, on which there is an extensive literature - Page (2011a) lists 70 scientific papers.
“This is the 'measure problem' of cosmology, on which there is an extensive literature -Page (2011a) lists 70 scientific papers.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Page (2011a)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Probably not a substantial claim: may not pass S3 (load-bearing).
InterpretationreasoningThe multiverse is an explanation for the occurrence of an unlikely event like a lottery win: perhaps there are more universes sufficiently numerous and varied that it is not too improbable that at least one would be in the life-permitting subset.
“The multiverse is just such an explanation.Perhaps there are more universes out there (in some sense), sufficiently numerous and varied that it is not too improbable that at least one of them would be in the lifepermitting subset of possible-physics-space.”
Quote in the paperNot a substantial claimClassified as probably not a substantial claim. May combine two claims.
InterpretationreasoningThis replaces the fine-tuning of the white area with the fine-tuning of the line-segment, plus the constraints placed on the other GUT parameters to ensure that the dotted line passes through the white region at all.
“This replaces the fine-tuning of the white area with the fine-tuning of the line-segment, plus the constraints placed on the other GUT parameters to ensure that the dotted line passes through the white region at all.”
Quote in the paperSubstantial claimMay combine two claims.
InterpretationreasoningLQCD does not address either the life-permitting range or the possible range of quark masses.
“LQCD doesn't address either.It demonstrates that (with no small amount of cleverness) one can measure the quark masses in our universe.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S3 (load-bearing). May combine two claims.
Premisenone givenThe principle of mediocrity is a self-consistency test for a multiverse proposal; it cannot pick out a unique multiverse as the 'real' multiverse, but can be quite powerful.
“This is a selfconsistency test -it cannot pick out a unique multiverse as the 'real' multiverse -but can be quite powerful.”
Quote in the paperNot a substantial claimClassified as probably not a substantial claim. May combine two claims.
InterpretationreasoningStenger fails to distinguish between the concordance model of cosmology, which has excellent empirical support but in no way predicts a multiverse, and speculative models of the early universe, only some of which predict a multiverse, all of which rely on hypothetical physics, and none of which have unambiguous empirical support, if any at all.
“Stenger fails to distinguish between the concordance model of cosmology, which has excellent empirical support but in no way predicts a multiverse, and speculative models of the early universe, only some of which predict a multiverse, all of which rely on hypothetical physics, and none of which have unambiguous empirical support, if any at all.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
InterpretationreasoningAll that we should conclude from Stenger's discussion is that the parameters (α1, α2, α3) can be calculated given α_U and M_U.
“All that we should conclude from Stenger's discussion is that the parameters (a 1 , a 2 , a 3 ) can be calculated given a U and M U .”
Quote in the paperNot a substantial claimMay combine two claims.
InterpretationreasoningWe not only need the right GUT symmetry, we need to make sure it breaks in the right way.
“In other words, we not only need the right GUT symmetry, we need to make sure it breaks in the right way.”
Quote in the paperNot a substantial claimMay combine two claims.
PremisecitationThere is more than one way to unify the forces of the standard model (SU(5), SO(10), E8 and more), and more than one way to break the GUT symmetry.
“Note also that, just as there are more than one way to unify the forces of the standard model -SU(5), SO(10), E 8 and more -there is also more than one way to break the GUT symmetry.”
Quote in the paperNot a substantial claimMay combine two claims.
InterpretationreasoningA multiverse is not part of nor a prediction of the concordance model of cosmology.
“A multiverse is not part of nor a prediction of the concordance model of cosmology.”
Quote in the paperSubstantial claimMay combine two claims.
InterpretationreasoningAnthropic reasoning seems to provide interesting limits on GUTs, though much work remains to be done in this area.
“We conclude that anthropic reasoning seems to provide interesting limits on GUTs, though much work remains to be done in this area.”
Quote in the paperNot a substantial claimMay combine two claims.
InterpretationreasoningThe constraint beta^{1/4} < 1/3 would require a 20-fold decrease in the proton mass to be violated, which translates to decreasing alpha_U by ~0.003.
“The constraint shown, b 1/4 , 1/3 would require a 20-fold decrease in the proton mass to be violated, which (using Equation 7) translates to decreasing a U by ,0.003.”
Quote in the paperSubstantial claimClassified as probably not a substantial claim.
InterpretationreasoningThe fallacy of explaining the point of impact by the initial velocity makes much of Chapters 7 to 10 of FOFT irrelevant.
“This fallacy alone makes much of Chapters 7 to 10 of FOFT irrelevant.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S3 (load-bearing), S4 (based).
Interpretationnone givenStenger has compared our universe with our universe and found no evidence of fine-tuning.
“Stenger has compared our universe with our universe and found no evidence of fine-tuning.”
Quote in the paperNot a substantial claimMay combine two claims.
InterpretationreasoningThe electromagnetic contribution would tend to make the charged proton heavier than the neutral neutron, so the mass difference of the light quarks must be large enough to overcome this contribution.
“This would tend to make the (charged) proton heavier than the (neutral) neutron, and hence we need the mass difference of the light quarks to be large enough to overcome this contribution.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S2 (checkable), S3 (load-bearing), S4 (based).
Interpretationnone givenIf 'whatever works' was four dimensional, then life would not exist, whether the number of dimensions is simply a human invention or an objective fact about the universe.
“If 'whatever works' was four dimensional, then life would not exist, whether the number of dimensions is simply a human invention or an objective fact about the universe.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
PremisecitationA number of authors have emphasised the life-permitting properties of the particular combination of one time- and three space-dimensions, going back to Ehrenfest (1917) and Whitrow (1955), summarised in Barrow & Tipler (1986) and Tegmark (1997).
“A number of authors have emphasised the life-permitting properties of the particular combination of one time-and three space-dimensions, going back to Ehrenfest (1917) and Whitrow (1955), summarised in Barrow & Tipler (1986) and Tegmark (1997) 32 .”
Quote in the paperNot a substantial claim0 of 3 sources checked- cites Ehrenfest (1917)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- cites Whitrow (1955) source
- cites Barrow & Tipler (1986)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Classified as probably not a substantial claim.
InterpretationreasoningStenger's discussion of the neutron-proton mass difference has no relevance to fine-tuning because it does not discuss the life-permitting range or the possible range of m_n - m_p (or its relation to the possible range of m_d - m_u).
“There is no discussion of the life-permitting range, no discussion of the possible range of m n À m p (or its relation to the possible range of m d À m u ), and thus no relevance to fine-tuning whatsoever.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
InterpretationreasoningIf we suppose that α and α_s are related linearly to α_U, then the GUT would constrain the point (α, α_s) to lie on the blue dot-dashed line in Figure 6.
“If we suppose that a and a s are related linearly to a U , then the GUT would constrain the point (a, a s ) to lie on the blue dot-dashed line in Figure 6.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S2 (checkable), S4 (based).
Interpretationnone givenThe parameters of the standard model remain some of the best understood and most impressive cases of fine-tuning.
“The parameters of the standard model remain some of the best understood and most impressive cases of fine-tuning.”
Quote in the paperNot a substantial claimMay combine two claims.
PremisecitationLQCD does not calculate the quark masses from the fundamental parameters of the standard model; the quark masses are fundamental parameters of the standard model.
“LQCD does not calculate the quark masses from the fundamental parameters of the standard model -they are fundamental parameters of the standard model.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Iwasaki 2000
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Probably not a substantial claim: may not pass S3 (load-bearing), S4 (based).
InterpretationreasoningFOFT has compared the electron mass in our universe with the electron mass in universes 'like ours', thus missing the point entirely.
“FOFT has compared the electron mass in our universe with the electron mass in universes 'like ours', thus missing the point entirely.”
Quote in the paperNot a substantial claimMay combine two claims.
PremisereasoningIn the cold big bang, structure formation is not suppressed by CMB radiation pressure, so stars and galaxies require a smaller value of Q.
“Structure formation is not suppressed by CMB radiation pressure, and thus stars and galaxies require a smaller value of Q.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Interpretationnone givenMost of the multiverse scenario is still hypothetical.
“Sadly, most of this scenario is still hypothetical.”
Quote in the paperNot a substantial claimClassified as probably not a substantial claim.
PremisecitationThe cold big bang is a model of the universe in which the primordial ratio of photons to baryons is Z_g approximately 1.
“The cold big bang (CBB) is a model of the universe in which the (primordial) ratio of photons to baryons is Z g , 1.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Aguirre (2001)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Probably not a substantial claim: may not pass S2 (checkable).
Interpretationnone givenAnthropic coincidences involve a happy consonance between a physical quantity and the requirements of complex, embodied intelligent life.
“Anthropic coincidences, on the other hand, involve a happy consonance between a physical quantity and the requirements of complex, embodied intelligent life.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S4 (based).
Interpretationnone givenThe multiverse would predict what we expect to observe by predicting what conditions hold in universes able to support observers.
“The multiverse would predict what we expect to observe by predicting what conditions hold in universes able to support observers.”
Quote in the paperNot a substantial claimMay combine two claims.
InterpretationcitationThis creates problems for inflationary multiverses, which are either fine-tuned to have the prior for Q to peak near the observed value, or else are steep functions of Q in the anthropic range.
“This creates problems for inflationary multiverses, which are either fine-tuned to have the prior for Q to peak near the observed value, or else are steep functions of Q in the anthropic range (Graesser et al. 2004;Feldstein, Hall & Watari 2005).”
Quote in the paperSubstantial claim0 of 2 sources checked- cites Graesser et al. 2004
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- cites Feldstein, Hall & Watari 2005
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Probably not a substantial claim: may not pass S3 (load-bearing), S4 (based).
Premisenone givenThis requirement is set by the homogeneity of our universe.
“This requirement is set by the homogeneity of our universe.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S2 (checkable).
InterpretationreasoningThe anthropic coincidences are so arresting because we are accustomed to thinking of physical laws and initial conditions as being unconcerned with how things turn out.
“The anthropic coincidences are so arresting because we are accustomed to thinking of physical laws and initial conditions as being unconcerned with how things turn out.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
InterpretationcitationWilczek argues that it strains credulity that parameters determined uniquely by abstract theoretical principles just happen to exhibit all the apparent fine-tunings required to produce a universe containing complex structures.
“Here is Wilczek (2006b): 'It is logically possible that parameters determined uniquely by abstract theoretical principles just happen to exhibit all the apparent fine-tunings required to produce, by a lucky coincidence, a universe containing complex structures.But that, I think, really strains credulity.'”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Wilczek (2006b)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Probably not a substantial claim: may not pass S3 (load-bearing).
PremisecitationLength contraction in special relativity is not just an optical illusion resulting from the finite speed of light.
“Length contraction in special relativity is not just an optical illusion resulting from the finite speed of light.See, for example,Penrose (1959).”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Penrose (1959)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
May combine two claims.
InterpretationreasoningThe lack of an adequate definition of 'an observer' and of knowledge of all possible forms of life is reason for caution but not a fatal flaw of fine-tuning.
“This is reason for caution, but not a fatal flaw of fine-tuning.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S2 (checkable).
InterpretationcitationIt would be the ultimate anthropic coincidence if beauty and complexity in the mathematical principles of the fundamental theory of physics produced all the necessary low-energy conditions for intelligent life.
“Finally, it would be the ultimate anthropic coincidence if beauty and complexity in the mathematical principles of the fundamental theory of physics produced all the necessary low-energy conditions for intelligent life.”
Quote in the paperNot a substantial claimMay combine two claims.
InterpretationreasoningThe predictions of the inflationary multiverse are very sensitive to the measure, and thus in the absence of a measure, we cannot conclude that it survives the test of the principle of mediocrity.
“The predictions of the inflationary multiverse are very sensitive to the measure, and thus in the absence of a measure, we cannot conclude that it survives the test of the principle of mediocrity.”
Quote in the paperSubstantial claimMay combine two claims.
InterpretationreasoningMolecular cooling requires higher densities and metallicities, but not too high, or planetary orbits will be disrupted by collisions.
“Various compensating factors are needed along the way -we need a smaller value of Q, which renders atomic cooling inefficient, so we must rely on molecular cooling, which requires higher densities and metalicities, but not too high or planetary orbits will be disrupted collisions (whose frequency increases as Z g À4 Q 7/2 ).”
Quote in the paperSubstantial claimMay combine two claims.
InterpretationreasoningIn the cold big bang life-permitting region, a smaller value of Q is needed, which renders atomic cooling inefficient, so molecular cooling must be relied on.
“Various compensating factors are needed along the way -we need a smaller value of Q, which renders atomic cooling inefficient, so we must rely on molecular cooling, which requires higher densities and metalicities, but not too high or planetary orbits will be disrupted collisions (whose frequency increases as Z g À4 Q 7/2 ).”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
PremisecitationCarroll & Tam (2010) argue that the Gibbons-Hawking-Stewart canonical measure renders an inflationary solution to the flatness problem superfluous.
“We should also note thatCarroll & Tam (2010) argue that the Gibbons-Hawking-Stewart canonical measure renders an inflationary solution to the flatness problem superfluous.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Carroll & Tam (2010)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Classified as probably not a substantial claim. May combine two claims.
InterpretationreasoningObservers like us will die out, and eventually Boltzmann brains, dreaming that they are us, will outnumber us.
“Observers like us will die out, and eventually Boltzmann brains, dreaming that they are us, will outnumber us.”
Quote in the paperSubstantial claim- Rests on an assumption: Boltzmann brains can fluctuate into existence with memories of being observers like us.
May combine two claims.
InterpretationreasoningIt is unlikely that the set of life-permitting universes is much larger than previously thought, because the physics relevant to life is low-energy physics and thus well-understood.
“This is unlikely, since the physics relevant to life is low-energy physics, and thus well-understood.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S2 (checkable).
InterpretationreasoningFine-tuning is not a typical scientific problem, that is, a phenomenon in our universe that cannot be explained by our current understanding of physical laws.
“Fine-tuning is not a typical scientific problem, that is, a phenomenon in our universe that cannot be explained by our current understanding of physical laws.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S4 (based).
Interpretationnone givenIf the current accelerating phase of the universe persists arbitrarily into the future, then our universe will become vacuum dominated.
“This could be a problem in our universe -if the current, accelerating phase of the universe persists arbitrarily into the future, then our universe will become vacuum dominated.”
Quote in the paperNot a substantial claim- Rests on an assumption: The current accelerating phase of the universe could persist arbitrarily into the future.
May combine two claims.
Premisenone givenParticles and antiparticles pair off and mutually annihilate to photons as the universe cools, so the excess of particles over antiparticles determines the value of Z_g.
“Particles and antiparticles pair off and mutually annihilate to photons as the universe cools, so the excess of particles over antiparticles determines the value of Z g .”
Quote in the paperNot a substantial claimMay combine two claims.
InterpretationcitationThe claim that the laws of nature are fixed by logical and mathematical necessity is demonstrably wrong, because theoretical physicists find it easy to describe alternative universes free from logical contradiction.
“If the claim is that the laws of nature are fixed by logical and mathematical necessity, then this is demonstrably wrong -theoretical physicists find it rather easy to describe alternative universes that are free from logical contradiction (Davies, in Davies 2003).”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Davies, in Davies 2003
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Probably not a substantial claim: may not pass S3 (load-bearing).
InterpretationreasoningThe counter-argument presented in Stenger's book does not address the possibility of a deity which intervenes to sustain life in this universe.
“The counter-argument presented in Stenger's book (page 252), borrowing from a paper by Ikeda and Jeffreys, does not address this possibility.Rather, it argues against a deity which intervenes to sustain life in this universe.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S4 (based).
Interpretationnone givenMost multiverse mechanisms seem to fall into the category of creating more small universe domains than large ones.
“Most multiverse mechanisms seem to fall into this category.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S2 (checkable), S3 (load-bearing), S4 (based).
InterpretationcitationAs with the Boltzmann multiverse, the problem is that this universe seems uncomfortably roomy.
“As with the Boltzmann multiverse, the problem is that this universe seems uncomfortably roomy.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
InterpretationcitationThis result would seem to show that non-flat FLRW universes are infinitely unlikely.
“This is a puzzling result -it would seem to show that non-flat FLRW universes are infinitely unlikely, so to speak.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing), S4 (based).
Interpretationnone givenFor the cold big bang to be a serious contender as a model of our universe, there would need to be an early population of luminous objects such as PopIII stars.
“To be a serious contender as a model of our universe (in which Z g , 10 9 ) there would need to be an early population of luminous objects e.g.PopIII stars.”
Quote in the paperNot a substantial claimClassified as probably not a substantial claim.
Interpretationnone givenFor every observer who really is a carbon-based life form evolved on a planet orbiting a star in a galaxy, there are vastly more observers in a Boltzmann-brain multiverse for whom this is a passing dream, the fleeting fancies of a phantom fluctuation.
“The worry is that, for every observer who really is a carbonbased life form who evolved on a planet orbiting a star in a galaxy, there are vastly more for whom this is all a passing dream, the few, fleeting fancies of a phantom fluctuation.”
Quote in the paperSubstantial claim- Rests on an assumption: Boltzmann brains can fluctuate into existence with memories of being observers like us.
May combine two claims.
InterpretationreasoningBeauty and simplicity are not necessity.
“Beauty and simplicity are not necessity.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S2 (checkable). May combine two claims.
InterpretationreasoningThe multiverse may yet solve the fine-tuning of the universe for intelligent life, but it will not be an easy solution.
“The multiverse may yet solve the fine-tuning of the universe for intelligent life, but it will not be an easy solution.”
Quote in the paperNot a substantial claimMay combine two claims.
Study design and conductreasoningThe estimate that a small change in a_U will not significantly change a appears to hold because the dependence seems to be flatter than linear.
“This estimate assumes that this small change in a U will not significantly change a.The dependence seems to be flatter than linear, so this assumption appears to hold.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S3 (load-bearing), S4 (based). May combine two claims.
Interpretationnone givenThere are several things wrong with the scenario, not least that such a scenario is unstable to gravitational collapse.
“Actually, there are several things wrong, not least that such a scenario is unstable to gravitational collapse.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing), S4 (based).
Premisenone givenIn the absence of weak decay, the weakless universe will conserve each individual quark number.
“In the absence of weak decay, the weakless universe will conserve each individual quark number.”
Quote in the paperNot a substantial claimMay combine two claims.
InterpretationreasoningRegion 1 depends on the proton-neutron mass difference, which doesn't change with L_QCD and thus does not place a constraint on a_U.
“For example, Region 1 depends on the proton-neutron mass difference, which doesn't change with L QCD and thus does not place a constraint on a U .”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing). May combine two claims.
Study design and conductreasoningThe limit on a holds for constant C; as C appears to depend on a, the corresponding limit on a may be a different plane to the one shown in Figure 6.
“Even this limit should be noted with caution, as it holds for constant C. As C appears to depend on a, the corresponding limit on a may be a different plane to the one shown in Figure6.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S2 (checkable), S3 (load-bearing).
InterpretationreasoningAguirre (2001) is justifiably eager to demonstrate that stars will plausibly form in a CBB universe.
“Aguirre (2001) is thus justifiably eager to demonstrate that stars will plausibly form in a CBB universe.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Aguirre (2001)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
The authors state this as an assumption.
The probability distribution over the parameters x and y is uniform.
“The probability of a life-permitting universe, assuming that the probability distribution is uniform in (x, y) -which, as Stenger notes, is 'the best we can do' (FOFT 72) -is the ratio of the area inside the wedge to the area inside the dashed box.”
The authors state this as an assumption.
The possible range of y can be conservatively estimated by y0.
“We conservatively estimate the possible range of y by y 0 .”
The authors state this as an assumption.
The full life-permitting criterion that defines the wedge is given by the equation 1 - y/x = (y0/x0)(1 + epsilon).
“Suppose the full life-permitting criterion that defines the wedge is, 1 À y=x y 0 =x 0 1 þ ;ð2Þ”
The authors state this as an assumption.
There is only a single wedge.
“This will certainly underestimate the probability inside the wedge, assuming that there is only a single wedge.”
The authors state this as an assumption.
The parameters x and y can vary from zero to x_max and y_max, and these maximum values may approach infinity.
“Here, x and y are two physical parameters that can vary from zero to x max and y max , where we can allow these values to approach infinity if so desired.”
The paper relies on this without support.
The range of densities that permit the existence of cosmic structure in a long-lived universe is very narrow.
“Now let's note the range of densities that permit the existence of cosmic structure in a long-lived universe.We find that this range is very narrow.”
The paper relies on this without support.
The range of densities that permit cosmic structure neatly straddles the critical density.
“Very conveniently, this range neatly straddles the critical density.”
The paper relies on this without support.
In our universe, the amplitude of primordial fluctuations Q is approximately 2 × 10^-5.
“In our universe, its value is Q E 2 Â 10 À5 , meaning that in the early universe the density at any point was typically within 1 part in 100 000 of the mean density.”
The paper relies on this without support.
QFT predicts contributions to the vacuum energy of the universe that are ~10^120 times greater than the observed total value.
“A wellunderstood and well-tested theory of fundamental physics (Quantum Field Theory -QFT) predicts contributions to the vacuum energy of the universe that are ,10 120 times greater than the observed total value.”
The paper relies on this without support.
The electron vacuum energy does gravitate in some situations.
“The first is that we know that the electron vacuum energy does gravitate in some situations.”
The paper relies on this without support.
Intelligent life requires stars to produce both carbon and oxygen.
“The ability of stars in our universe to produce both carbon and oxygen seems to be a rare talent.”
The paper relies on this without support.
The conditions listed (hydrogen existence, stable atoms, chemistry, stable stars) are necessary for life.
“For hydrogen to exist -to power stars and form water and organic compounds -we must have m e , m n À m p .”
The authors state this as an assumption.
The life-permitting region can be assessed by varying one or two constants while holding the others at their observed values.
“The life-permitting region (shown in white) in the (a, b) (left) and (a, a s ) (right) parameter space, with other constants held at their values in our universe.”
The paper relies on this without support.
There is no successful theory of baryogenesis and leptogenesis.
“We are thus again faced with the absence of a successful theory of baryogenesis and leptogenesis.”
The paper relies on this without support.
A multiverse measure exists that allows comparison of the sizes of life-permitting islands.
“If the other island is significantly larger than ours (for a given multiverse measure), then observers should expect to be on the other island.”
The paper relies on this without support.
Boltzmann brains can fluctuate into existence with memories of being observers like us.
“We should be wary of any multiverse which allows for single brains, imprinted with memories, to fluctuate into existence.”
The paper relies on this without support.
The current accelerating phase of the universe could persist arbitrarily into the future.
“if the current, accelerating phase of the universe persists arbitrarily into the future, then our universe will become vacuum dominated.”
Claims other papers make about this one
Each is checked against this paper’s own text: does it say what the citing paper says it does?
The amplitude of primordial fluctuations q=Q_obs≈2×10^-5 is the dimensionless value of interest.
“The amplitude of primordial fluctuations, q = Q obs ≈ 2 × 10 -5 , is here the dimensionless value of interest [25].”
From Is cosmological tuning fine or coarse? (2021) · cites this paper as [25]
Self-check
Percentages, sums and reported differences re-computed from the paper’s own numbers.
Each contradiction between two passages listed here was confirmed by an independent check.
Inflationary outcomes are assigned to the wrong figure
MinorThe text attributes the five- and six-pointed stars to Figure 4, but its description places those stars in Figure 3. Figure 4 is described as showing inflation success rates and cosmological parameters.
“We have seen this point previously: the five-and six-pointed stars in Figure 4 show universes in which the value of V 0 is respectively too negative and too positive for the post-inflationary universe to support life.”
“Figure 3 An example of a randomly-generated inflaton potential.Thick lines show where the Slow Roll Approximation holds (SRA); thin lines show where it fails.The stars show four characteristic initial conditions.”
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<i>Just Six Numbers: The Deep Forces that Shape the Universe</i>
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“These quantities are among themost discussed in the fine-tuning literature, beginning with Carter (1974), Carr & Rees (1979) and Barrow & Tipler (1986).”
InfluentialEssay: An Alternative to Inflation
Hollands, S., & Wald, R. M. (2002) · General Relativity and Gravitation · doi:10.1023/a:1021175216055 · Cited by 129 · cited 4× · see citing works
“The time asymmetry is a consequence of low entropy initial conditions, not the physics itself (Penrose 1989; Hollands & Wald 2002a).”
BackgroundInfluentialGod and Design : The Teleological Argument and Modern Science
Manson, N. A. (2003) · Cited by 115 · see citing works
A finely-predicted Higgs boson mass from a finely-tuned weak scale
Hall, L. J., & Yasunori Nomura, A. (2010) · Journal of High Energy Physics · doi:10.1007/jhep03(2010)076 · Cited by 114 · cited 1× · see citing works
“…model: technicolor, the supersymmetric standard model, large extra dimensions, warped compactifications, little Higgs theories and more — even anthropic solutions (Arkani-Hamed & Dimopoulos 2005; Arkani-Hamed et al. 2005; Feldstein et al. 2006; Hall & Nomura 2008, 2010; Donoghue et al. 2010).”
BackgroundThe Goldilocks Enigma: Why is the Universe Just Right for Life?
Davies, P. (2007) · doi:10.1007/978-90-481-9748-4_20 · Cited by 111
Ludwig, W., & Falter, C. (1996) · Springer series in solid-state sciences · doi:10.1007/978-3-642-79977-8 · Cited by 108 · see citing works
Inflationary Theory and Alternative Cosmology
Kofman, L., Linde, A., & Mukhanov, V. (2002) · Journal of High Energy Physics · doi:10.1088/1126-6708/2002/10/057 · Cited by 97 · see citing works
Scientific alternatives to the anthropic principle
Smolin, L. (2007) · Universe or Multiverse? · doi:10.1017/cbo9781107050990.022 · Cited by 83 · cited 2× · see citing works
“As Smolin (2007) explains, the prediction can be formulated as follows: a.) Carbon is necessary for life. b.) There are substantial amounts of carbon in our universe. c.) If stars are to produce substantial amounts of carbon, then there must be a specific resonance level in carbon. d.) Thus, the…”
BackgroundMultiverses and physical cosmologyPreprint
Ellis, G., Kirchner, U., & Stoeger, W. R. (2003) · Cited by 83 · see citing works
Tracking down gauge: an ode to the constrained Hamiltonian formalism
Earman, J. (2003) · Cambridge University Press eBooks · doi:10.1017/cbo9780511535369.009 · Cited by 82 · cited 1× · see citing works
“Without such interactions, all matter would be like dark matter, which can only form into large, diffuse, roughly spherical haloes of matter whose only internal structure consists of smal- ler, diffuse, roughly spherical subhaloes.8See also the excellent articles by Martin (2003) and Earman (2003).”
BackgroundStellar production rates of carbon and its abundance in the universe.
Oberhummer, H., Csótó, A., & Schlattl, H. (2000) · Science · doi:10.1126/science.289.5476.88 · Cited by 82 · cited 2× · see citing works
“Jeltema & Sher (1999) combined the conclusions of Agrawal et al. and Oberhummer et al. (2000a) to place a constraint on the Higgs vev from the fine-tuning of the Hoyle resonance (Section 4.7.2).”
BackgroundInfluentialMultiverses and physical cosmology
Ellis, G. F. R., Kirchner, U., & Stoeger, W. R. (2004) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2004.07261.x · Cited by 82 · cited 1× · see citing works
“As Ellis et al. (2004) point out, any such proposal will have to deal with the problems of what determines {M; f ðmÞ; p}, actualized infinities (in M, f(m) and the spatial extent of universes) and non-renormalisability, the parameter dependence and non-uniqueness of p, and how one could possibly…”
BackgroundWHY PHYSICAL SPACE HAS THREE DIMENSIONS
WHITROW, G. J. (1955) · The British Journal for the Philosophy of Science · doi:10.1093/bjps/vi.21.13 · Cited by 80 · cited 1× · see citing works
“A number of authors have emphasised the life-permitting properties of the particular combination of one time- and three space-dimensions, going back to Ehrenfest (1917) and Whitrow (1955), summarised in Barrow & Tipler (1986) and Tegmark (1997)32.”
BackgroundStrocchi, F. (2008) · Lecture Notes in Physics · doi:10.1007/978-3-540-73593-9 · Cited by 79 · see citing works
An Introduction to Elementary Particles
Wyllie, G. (1962) · Physics Bulletin · doi:10.1088/0031-9112/13/12/017 · Cited by 77 · see citing works
Strocchi, F. (2005) · Cited by 76 · see citing works
Fitness of the Cosmos for Life
Barrow, J. D., Morris, S. C., Freeland, S. J., & Harper, C. L. (2007) · Cambridge University Press eBooks · doi:10.1017/cbo9780511536557 · Cited by 71 · see citing works
Phillips, A. C. (1994) · Cited by 63 · see citing works
Stars In Other Universes: Stellar structure with different fundamental constantsPreprint
Adams, F. C. (2012) · Cited by 59 · see citing works
A critical review of inflation
Turok, N. (2002) · Classical and Quantum Gravity · doi:10.1088/0264-9381/19/13/305 · Cited by 58 · cited 2× · see citing works
“The evidence is quite strong, though not indubitable (Turok 2002; Brandenberger 2011).”
BackgroundFitness of the cosmos for life: biochemistry and fine-tuning
(2008) · Choice Reviews Online · doi:10.5860/choice.46-2052 · Cited by 58 · see citing works
The anthropic significance of the existence of an excited state of 12C
Livio, M., Hollowell, D., Weiss, A., & Truran, J. W. (1989) · Nature · doi:10.1038/340281a0 · Cited by 57 · cited 2× · see citing works
“Stenger quotes the work of Livio et al. (1989), who considered the effect on the carbon and oxygen production of stars when the 0þ level is shifted.”
BackgroundMeasure problem for eternal and non-eternal inflation
Linde, A., & Noorbala, M. (2010) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2010/09/008 · Cited by 48 · see citing works
Collins, R. (2010) · Taylor & Francis eBooks · doi:10.4324/9780203398265_chapter_9 · Cited by 45 · see citing works
Testing anthropic predictions for and the cosmic microwave background temperature
Peacock, J. A. (2007) · Monthly Notices of the Royal Astronomical Society · doi:10.1111/j.1365-2966.2007.11978.x · Cited by 44 · cited 3× · see citing works
“For example, Peacock (2007) notes that most models of quintessence in the literature specify its properties via a potential V(f), and comments that ‘Quintessenceymodels do not solve the [cosmological constant] problem: the potentials asymptote to zero, even though there is no known symmetry that…”
BackgroundPredictive Landscapes and New Physics at a TeV
Arkani-Hamed, N., Dimopoulos, S., & Kachru, S. (2005) · arXiv · doi:10.48550/arxiv.hep-th/0501082 · Cited by 40 · see citing works
Effects of the variation of fundamental constants on Population III stellar evolution
Ekström, S., Coc, A., Descouvemont, P., Meynet, G., Olive, K., Uzan, J., & Vangioni, E. (2010) · Astronomy and Astrophysics · doi:10.1051/0004-6361/200913684 · Cited by 39 · cited 3× · see citing works
“Ekstr€om et al. (2010) considered changes to the Hoyle resonance in the context of Population III stars.”
BackgroundInfluentialOn continuous symmetries and the foundations of modern physics
Martin, C. A. (2003) · Cambridge University Press eBooks · doi:10.1017/cbo9780511535369.004 · Cited by 38 · cited 1× · see citing works
“Without such interactions, all matter would be like dark matter, which can only form into large, diffuse, roughly spherical haloes of matter whose only internal structure consists of smal- ler, diffuse, roughly spherical subhaloes.8See also the excellent articles by Martin (2003) and Earman (2003).”
The Road to Reality: A Complete Guide to the Laws of the Universe
Penrose, R. (2021) · Cited by 35 · see citing works
Did Einstein Stumble? The debate over general covariance
Norton, J. D. (1995) · Erkenntnis · doi:10.1007/bf01128809 · Cited by 30 · see citing works
Time’s Arrows Today: Recent Physical and Philosophical Work on the Direction of Time
Savitt, S. F., & Layzer, D. (1998) · American Journal of Physics · doi:10.1119/1.18954 · Cited by 30 · see citing works
Mathematical People: Profiles and Interviews.
Koblitz, A. H., Albers, D. J., & Alexanderson, G. L. (1986) · American Mathematical Monthly · doi:10.2307/2322310 · Cited by 30 · see citing works
Nagashima, Y. (2010) · Wiley eBooks · doi:10.1002/9783527630097 · Cited by 29 · cited 1× · see citing works
“…Lagrangian: L ¼ bm cgmg5c 1 2 Hmn csmnc km mnabAnAb;a; ð1Þ where the fields bm, km and Hmn are external vector and antisymmetric tensor backgrounds that introduce a preferred frame and therefore break Lorentz invariance; all other symbols have their usual meanings (e.g. Nagashima 2010).”
BackgroundPeacock, A. (1999) · Physica B: Condensed Matter · doi:10.1016/s0921-4526(98)01260-5 · Cited by 28 · cited 3× · see citing works
“For initial 14 These requirements can be found in any good cosmology textbook, e.g. Peacock (1999); Mo, van den Bosch & White (2010). conditions, Tegmark ‘sprays starting points randomly across the potential surface’.”
BackgroundInfluentialMaking predictions in a multiverse: conundrums, dangers, coincidences
Aguirre, A. (2007) · Universe or Multiverse? · doi:10.1017/cbo9781107050990.023 · Cited by 27 · cited 2× · see citing works
“A closer look at our island in parameter space reveals a refinement of the mediocrity test, as discussed by Aguirre (2007); see also Bousso, Hall & Nomura (2009).”
BackgroundThe fine-tuning problems of particle physics and anthropic mechanisms
Donoghue, J. F. (2007) · Universe or Multiverse? · doi:10.1017/cbo9781107050990.017 · Cited by 27 · cited 1× · see citing works
“For example, Donoghue (2007) says ‘It is unlikely that there is technically natural resolution to the cosmological constant’s fine-tuning problem — this would require new physics at 10 3 eV.”
BackgroundGauge Theories in Particle Physics
Aitchison, I. J. R., & Hey, A. (2002) · Graduate student series in physics · doi:10.1201/9780849387753 · Cited by 26 · cited 1× · see citing works
“Aitchison & Hey (2002) says that this line of thought is ‘not compelling motivation’ for the step from global to local gauge invariance, and along with Pokorski (2000), who 7 That is, the spacetime of a non-rotating, uncharged black hole. describes the argument as aesthetic, ultimately appeals to…”
BackgroundTHE APPEARANCE OF DESIGN IN PHYSICS AND COSMOLOGY
Davies, P. (2010) · Taylor & Francis eBooks · doi:10.4324/9780203398265_chapter_7 · Cited by 26 · cited 1× · see citing works
“If the claim is that the laws of nature are fixed by logical and mathematical necessity, then this is demonstrably wrong — theoretical physicists find it rather easy to describe alternative universes that are free from logical contradiction (Davies, in Davies 2003).”
BackgroundAstronomy, Cosmology and Fundamental Physics
Lella, L. D., Shaver, P., & Giménez, À. (2003) · ESO astrophysics symposia · doi:10.1007/b82980 · Cited by 25 · see citing works
On cosmic natural selectionPreprint
Vilenkin, A. (2006) · arXiv (Cornell University) · doi:10.48550/arxiv.hep-th/0610051 · Cited by 24 · see citing works
Comment on Inflation and Alternative CosmologyPreprint
Hollands, S., & Wald, R. M. (2002) · arXiv (Cornell University) · doi:10.48550/arxiv.hep-th/0210001 · Cited by 23 · see citing works
THE THERMODYNAMIC ARROW: PUZZLES AND PSEUDO-PUZZLES
Price, H. (2006) · Time and Matter International Colloquium on the Science of Time · doi:10.1142/9789812774392_0015 · Cited by 21 · cited 1× · see citing works
“See Price (1997, 2006) for an excellent discussion of these issues.”
BackgroundThe Influence of Evolving Dark Energy on Cosmology
Barnes, L. A., Francis, M., Lewis, G. F., & Linder, E. V. (2005) · Publications of the Astronomical Society of Australia · doi:10.1071/as05031 · Cited by 18 · cited 1× · see citing works
“We can use the term dark energy for any form of energy that causes the expansion of the universe to accelerate, including a ‘bare’ cosmological constant (see Barnes et al. 2005, for an introduction to dark energy).”
MethodSelf-citationAguirre, A. (1999) · The Astrophysical Journal · doi:10.1086/307534 · Cited by 18 · see citing works
Quarks, electrons and atoms in closely related universes
Hogan, C. J. (2007) · Universe or Multiverse? · doi:10.1017/cbo9781107050990.016 · Cited by 16 · cited 1× · see citing works
“This last point has been emphasised by Hogan (2007).”
BackgroundMasks of the Universe: Changing Ideas on the Nature of the Cosmos
Harrison, E. (2009) · Cambridge University Press eBooks · doi:10.1017/cbo9780511536564 · Cited by 15 · see citing works
The Future of the Universe and the Future of Our Civilization
(2000) · doi:10.1142/4383 · Cited by 14 · cited 2× · see citing works
“Jeltema & Sher (1999) combined the conclusions of Agrawal et al. and Oberhummer et al. (2000a) to place a constraint on the Higgs vev from the fine-tuning of the Hoyle resonance (Section 4.7.2).”
BackgroundInfluentialOn making predictions in a multiverse: conundrums, dangers, and coincidencesPreprint
Aguirre, A. N. (2005) · arXiv (Cornell University) · doi:10.48550/arxiv.astro-ph/0506519 · Cited by 11 · see citing works
Problems in a weakless universe
Clavelli, L., & White, R. E. (2006) · arXiv · doi:10.48550/arxiv.hep-ph/0609050 · Cited by 11 · see citing works
Enlightenment, knowledge, ignorance, temptation
Wilczek, F. A. (2007) · Cambridge University Press eBooks · doi:10.1017/cbo9781107050990.005 · Cited by 10 · cited 1× · see citing works
“(Wilczek 2005) 29 In the absence of weak decay, the weakless universe will conserve each individual quark number.”
BackgroundFINE-TUNING CARBON-BASED LIFE IN THE UNIVERSE BY THE TRIPLE-ALPHA PROCESS IN RED GIANTS
Oberhummer, H., Attila Csótó, A., & Schlattl, H. (2000) · doi:10.1142/9789812793324_0020 · Cited by 10 · cited 2× · see citing works
“Jeltema & Sher (1999) combined the conclusions of Agrawal et al. and Oberhummer et al. (2000a) to place a constraint on the Higgs vev from the fine-tuning of the Hoyle resonance (Section 4.7.2).”
BackgroundInfluentialAgnesi weighting for the measure problem of cosmology
Page, D. (2010) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2011/03/031 · Cited by 10 · cited 2× · see citing works
“…(2006) for Deutsch’s view on fine-tuning, Ellis (1993), Greene (2011), Guth (2007), Harrison (2003), Hawking & Mlodinow (2010, p. 161), Linde (2008), Page (2011b), Penrose (2004, p. 758), Polkinghorne & Beale (2009), Rees (1999), Smolin (2007), Susskind (2005), Tegmark et al. (2006), Vilenkin…”
BackgroundTime's arrows today: Recent physical and philosophical work on the direction of time
Denbigh, K. G. (1996) · Studies in History and Philosophy of Science Part B Studies in History and Philosophy of Modern Physics · doi:10.1016/1355-2198(96)00006-8 · Cited by 8 · see citing works
(2006) · doi:10.1142/6007 · Cited by 7 · see citing works
The Physics of Stars, 2nd Edition
Phillips, A. C. (1999) · Cited by 7 · see citing works
Professor Boltzmann's Letter on the Kinetic Theory of Gases
Boltzmann, L. (1895) · Nature · doi:10.1038/051581b0 · Cited by 6 · cited 1× · see citing works
“Boltzmann (1895), having discussed the discovery that the second law of thermodynamics is statistical in nature, asks why the universe is currently so far from thermal equilibrium.”
BackgroundQuestions of Truth: Fifty-One Responses to Questions about God, Science, and Belief
Poon, W. C. K. (2010) · Studies in World Christianity · doi:10.3366/e1354990110000924 · Cited by 6 · cited 1× · see citing works
“…Ellis (1993), Greene (2011), Guth (2007), Harrison (2003), Hawking & Mlodinow (2010, p. 161), Linde (2008), Page (2011b), Penrose (2004, p. 758), Polkinghorne & Beale (2009), Rees (1999), Smolin (2007), Susskind (2005), Tegmark et al. (2006), Vilenkin (2006), Weinberg (1994) and Wheeler…”
Questions of Truth: Fifty-one Responses to Questions about God, Science, and Belief
Polkinghorne, J. C., & Beale, N. (2009) · Cited by 6 · see citing works
Galaxy formation and evolution
Silk, J. I., & Khochfar, S. (2015) · AccessScience · doi:10.1036/1097-8542.803030 · Cited by 5 · see citing works
Bertola, F., & Curi, U. (1989) · Cited by 5 · see citing works
(2007) · ATF Press eBooks · doi:10.2307/j.ctv16f6d2r.12 · Cited by 5 · cited 7× · see citing works
“Modelling the later, post-hydrogen-burning stages of stellar evolution is difficult even for modern codes, and the inclusion of He-shell flashes seems to lessen the degree of fine-tuning of the Hoyle resonance. Ekström et al. (2010) considered changes to the Hoyle resonance in the context of Population III stars. Thes…”
InfluentialCosmological Constant Problems and Their Solutions
Vilenkin, A. (2006) · Springer eBooks · doi:10.1007/10857580_7 · Cited by 3 · see citing works
Burgess, C. P., & Moore, G. (2006) · doi:10.2277/0521860369 · Cited by 2 · see citing works
Four Big Questions with Pretty Good AnswersPreprint
Wilczek, F. (2002) · arXiv (Cornell University) · doi:10.48550/arxiv.hep-ph/0201222 · Cited by 2 · see citing works
Page, D. (2011) · arXiv (Cornell University) · doi:10.48550/arxiv.1101.2444 · Cited by 1 · see citing works
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Cited by
Sorted by citations
Life at the interface of particle physics and string theory
Schellekens, A. N. (2013) · Reviews of Modern Physics · doi:10.1103/revmodphys.85.1491 · Cited by 97 · see citing works
“See [63] and chapter IV of [521] for fascinating plots of many other limits.”
BackgroundInfluentialWilson, A. (2020) · doi:10.1093/oso/9780198846215.001.0001 · Cited by 100 · see citing works
Multiscale memory and bioelectric error correction in the cytoplasm–cytoskeleton‐membrane system
Fields, C., & Levin, M. G. (2017) · WIREs Systems Biology and Medicine · doi:10.1002/wsbm.1410 · Cited by 76 · see citing works
Vidal, C. (2014) · The frontiers collection · doi:10.1007/978-3-319-05062-1 · Cited by 67 · see citing works
The beginning and the end: the meaning of life in a cosmological perspective
Vidal, C. (2015) · Choice Reviews Online · doi:10.5860/choice.186550 · Cited by 56 · see citing works
A Reasonable Little Question: A Formulation of the Fine-Tuning Argument
Barnes, L. A. (2019) · Ergo an Open Access Journal of Philosophy · doi:10.3998/ergo.12405314.0006.042 · Cited by 55 · see citing works
Self-citationThe degree of fine-tuning in our universe — and others
Adams, F. C. (2019) · Physics Reports · doi:10.1016/j.physrep.2019.02.001 · Cited by 62 · see citing works
“Although many previous treatments have concluded that the universe is fine-tuned for the development of life [49, 57, 61, 89, 122, 131, 132, 166, 179, 184, 280, 345, 446, 467, 528, 529], it should be emphasized that different authors make this claim with widely varying degrees of conviction (see also [94, 125, 165, 23…”
BackgroundA Fortunate Universe: Life in a Finely Tuned Cosmos
(2016) · Thammasat University Digital Collections · doi:10.1017/9781316661413 · Cited by 48 · see citing works
Self-citationScreams for explanation: finetuning and naturalness in the foundations of physics
Hossenfelder, S. (2019) · Synthese · doi:10.1007/s11229-019-02377-5 · Cited by 85 · see citing works
“The reader interested in learning more details about this particular type of finetuning is referred to Barnes (2012), Ellis et al. (2004).”
BackgroundOn the philosophy of cosmology
Ellis, G. (2013) · Studies in History and Philosophy of Science Part B Studies in History and Philosophy of Modern Physics · doi:10.1016/j.shpsb.2013.07.006 · Cited by 40 · see citing works
The Fine-Tuning Argument: Exploring the Improbability of Our Existence
Landsman, K. (2016) · The frontiers collection · doi:10.1007/978-3-319-26300-7_6 · Cited by 32 · see citing works
“On the other hand, the difference can’t be too large, 10See Barrow and Tipler (1986), Leslie (1989), Davies (2006), Ellis (2007), and Barnes (2012) for further examples and more detailed references.”
BackgroundFriederich, S. (2021) · Cambridge University Press eBooks · doi:10.1017/9781108765947 · Cited by 34 · see citing works
Fundamental constants: from measurement to the universe, a window on gravitation and cosmology
Uzan, J.-P. (2025) · Living Reviews in Relativity · doi:10.1007/s41114-025-00059-y · Cited by 36 · see citing works
Producing the deuteron in stars: anthropic limits on fundamental constants
Barnes, L., & Lewis, G. (2017) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2017/07/036 · Cited by 12 · see citing works
Self-citationThe Teleological and Kalam Cosmological Arguments Revisited
Loke, A. T. E. (2022) · Palgrave frontiers in philosophy of religion · doi:10.1007/978-3-030-94403-2 · Cited by 31 · see citing works
Planets in other universes: habitability constraints on density fluctuations and galactic structure
Adams, F. C., Coppess, K. R., & Bloch, A. M. (2015) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2015/09/030 · Cited by 53 · see citing works
“Note that in order to determine the probability of life arising in a universe, we must not only determine the parameters that allow for life but also the probability of realizing those parameter values [19]; thus far, we have little understanding of the underlying probability distributions.”
BackgroundĆirković, M. M., & Perović, S. (2017) · Studies in History and Philosophy of Science Part B Studies in History and Philosophy of Modern Physics · doi:10.1016/j.shpsb.2017.04.005 · Cited by 26 · see citing works
“It seems obvious that such motivation is deeply intertwined with the controversy over fine-tuning physical constants and cosmological parameters for habitability (e.g., Barrow & Tipler, 1986; Barnes, 2012).”
BackgroundLee, D., Meißner, U.-G., Olive, K. A., Shifman, M., & Vonk, T. (2020) · Physical Review Research · doi:10.1103/physrevresearch.2.033392 · Cited by 29 · see citing works
“[33–37].”
Constraints on alternate universes: stars and habitable planets with different fundamental constants
Adams, F. C. (2016) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2016/02/042 · Cited by 23 · see citing works
“However, the definition of what constitutes fine-tuning is not the same for all authors and remains unsettled (a detailed discussion is given in [14]).”
BackgroundBarnes, L. A., Elahi, P. J., Salcido, J., Bower, R. G., Lewis, G. F., Theuns, T., Schaller, M., Crain, R. A., & Schaye, J. (2018) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/sty846 · Cited by 23 · see citing works
“The scientific literature on the fine-tuning of the universe for life has been reviewed in Hogan (2000); Barnes (2012); Schellekens (2013); Meißner (2014); Lewis & Barnes (2016).”
BackgroundSelf-citationEvolvability Is an Evolved Ability: The Coding Concept as the Arch-Unit of Natural Selection
Janković, S., & Ćirković, M. M. (2015) · Origins of Life and Evolution of Biospheres · doi:10.1007/s11084-015-9464-z · Cited by 19 · see citing works
Fine-tuning in the context of Bayesian theory testing
Barnes, L. A. (2017) · European Journal for Philosophy of Science · doi:10.1007/s13194-017-0184-2 · Cited by 22 · see citing works
“Albert (2015) My central concern here is the claim that chances of initial conditions are set by the theory.”
BackgroundSelf-citationAnthropic arguments outside of cosmology and string theory
Ćirković, M. (2016) · Belgrade Philosophical Annual · doi:10.5937/bpa1629091c · Cited by 3 · see citing works
Planets in other universes: habitability constraints on density fluctuations and galactic structure
Adams, F. C., Coppess, K. R., & Bloch, A. M. (2015) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2015/9/030 · Cited by 18 · see citing works
On the Habitability of Universes without Stable Deuterium
Adams, F., & Grohs, E. (2016) · Astroparticle Physics · doi:10.1016/j.astropartphys.2017.03.009 · Cited by 17 · see citing works
“The laws of physics allow for the development of life in our universe, but many authors have noted that sufficiently large variations could render the universe uninhabitable [1, 2, 3, 4, 5, 6, 7, 8].”
BackgroundUsing statistical methods to model the fine-tuning of molecular machines and systems
Thorvaldsen, S., & Hössjer, O. (2020) · Journal of Theoretical Biology · doi:10.1016/j.jtbi.2020.110352 · Cited by 15 · see citing works
“Luke Barnes has published a good review paper on the fine-tuning of the universe (Barnes, 2012), and Lewis and Barnes wrote an up to date book (2016).”
BackgroundSymmetry breaking and functional incompleteness in biological systems.
Korenić, A., Perović, S., Ćirković, M., & Miquel, P. (2020) · Progress in Biophysics and Molecular Biology · doi:10.1016/j.pbiomolbio.2019.02.001 · Cited by 13 · see citing works
Relativistic models and the expanding universe
Realdi, M. (2019) · Oxford University Press eBooks · doi:10.1093/oxfordhb/9780198817666.013.3 · Cited by 15 · see citing works
The Oxford Handbook of the History of Modern Cosmology
Kragh, H., & Longair, M. (2019) · Oxford University Press eBooks · doi:10.1093/oxfordhb/9780198817666.001.0001 · Cited by 17 · see citing works
A New Fine-Tuning Argument for the Multiverse
Friederich, S. (2019) · Foundations of Physics · doi:10.1007/s10701-019-00246-2 · Cited by 14 · see citing works
Sensitivity of carbon and oxygen yields to the triple-alpha resonance in massive stars
Huang, L., Adams, F., & Grohs, E. (2018) · Astroparticle physics · doi:10.1016/j.astropartphys.2018.09.005 · Cited by 16 · see citing works
“Many authors have studied the effects of these possible variations in the laws of physics and find that only certain ranges for the parameters allow for universes to form cosmic structure and support working stars [12, 13, 14, 15, 16, 17, 18].”
BackgroundProbing the cosmology of f(Q,T) gravity with holographic background fluid
Chokyi, K. K., & Chattopadhyay, S. (2024) · International Journal of Modern Physics D · doi:10.1142/s0218271824500020 · Cited by 13 · see citing works
Ćirković, M. M., & Perović, S. (2017) · PhilSci-Archive (University of Pittsburgh) · Cited by 13 · see citing works
Is cosmological tuning fine or coarse?
Díaz-Pachón, D. A., Hössjer, O., & Marks II, R. J. (2021) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2021/07/020 · Cited by 10 · see citing works
“The amplitude of primordial fluctuations, q = Qobs ≈ 2 × 10−5, is here the dimensionless value of interest [25].”
BackgroundBinding the diproton in stars: anthropic limits on the strength of gravity
Barnes, L. A. (2015) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2015/12/050 · Cited by 16 · see citing works
“We have elsewhere reviewed the scientific literature on the fine-tuning of the universe for intelligent life [3]; here are some illustrative examples.”
BackgroundSelf-citationStellar helium burning in other universes: A solution to the triple alpha fine-tuning problem
Adams, F., & Grohs, E. (2016) · Astroparticle Physics · doi:10.1016/j.astropartphys.2016.12.002 · Cited by 10 · see citing works
“As a result of these complications, this paper represents only one step toward understanding carbon production in other universes (see also [1, 2, 3, 4, 5, 18] and references therein).”
BackgroundTesting the Multiverse: Bayes, Fine-Tuning and Typicality
Barnes, L. A. (2017) · Cambridge University Press eBooks · doi:10.1017/9781316535783.023 · Cited by 11 · see citing works
Self-citationAssessing, Testing and Estimating the Amount of Fine-Tuning by Means of Active Information
Pachón, D. A. D., & Hössjer, O. (2022) · Entropy · doi:10.3390/e24101323 · Cited by 11 · see citing works
Beyond Physics? On the Prospects of Finding a Meaningful Oracle
Edis, T., & Boudry, M. (2014) · Foundations of Science · doi:10.1007/s10699-014-9349-z · Cited by 8 · see citing works
The problem of nomological harmony
Cutter, B., & Saad, B. (2023) · Noûs · doi:10.1111/nous.12463 · Cited by 11 · see citing works
Is It Possible to Know Cosmological Fine-tuning?
Pachón, D. A. D., Hössjer, O., & Mathew, C. (2024) · The Astrophysical Journal Supplement Series · doi:10.3847/1538-4365/ad2c88 · Cited by 7 · see citing works
Constraints on vacuum energy from structure formation and Nucleosynthesis
Adams, F. C., Alexander, S., Grohs, E., & Mersini-Houghton, L. (2017) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2017/03/021 · Cited by 8 · see citing works
“A secondary goal of this paper is to consider the overarching issue of the possible fine-tuning of the universe [6, 10, 27, 28].”
BackgroundFine-tuning as Old Evidence, Double Counting, and the Multiverse
Friederich, S. (2017) · International Studies in the Philosophy of Science · doi:10.1080/02698595.2019.1565214 · Cited by 7 · see citing works
“2), Davies (1982), Rees (2000), and Lewis and Barnes (2016); for more technical ones see Hogan (2000, 2007) and Barnes (2012).”
BackgroundInfluentialSometimes Size Does Not Matter
Pachón, D. A. D., Hössjer, O., & Marks, R. J. (2022) · Foundations of Physics · doi:10.1007/s10701-022-00650-1 · Cited by 7 · see citing works
Life, Intelligence, and the Selection of Universes
Vaas, R. (2019) · Springer proceedings in complexity · doi:10.1007/978-3-030-00075-2_3 · Cited by 5 · see citing works
Defending The Fallacy of Fine-TuningPreprint
Stenger, V. J. (2012) · arXiv (Cornell University) · doi:10.48550/arxiv.1202.4359 · Cited by 5 · see citing works
“ed with slight changes in parameters. In Fallacy I showed (1) that plausible explanations, consistent with existing knowledge, can be made for the observed values of the five critical parameters and, (2) plausible ranges for the other parameters exist that are far from infinitesimal, contrary to what is claimed in the…”
ResultThe fine-tuning argument against the multiverse
Boyce, K., & Swenson, P. (2024) · The Philosophical Quarterly · doi:10.1093/pq/pqae068 · Cited by 4 · see citing works
Revisiting the Scientific Nature of Multiverse Theories
Chan, M. H. (2023) · Journal for General Philosophy of Science · doi:10.1007/s10838-023-09644-7 · Cited by 3 · see citing works
“This problem is now known as the Q-catastrophe.”
Life, the Multiverse, and Fine-Tuning
Helbig, P. (2023) · Foundations of Physics · doi:10.1007/s10701-023-00732-8 · Cited by 3 · see citing works
Saving Science from Quantum Mechanics
Adlam, E. (2025) · doi:10.1093/9780197808887.001.0001 · Cited by 3 · see citing works
The cosmic microwave background: from discovery to precision cosmology
Partridge, R. B. (2019) · Oxford University Press eBooks · doi:10.1093/oxfordhb/9780198817666.013.8 · Cited by 3 · see citing works
Ćirković, M. M., & Dimitrijević, J. (2017) · Foundations of Science · doi:10.1007/s10699-017-9532-0 · Cited by 3 · see citing works
“1 For some of the reviews of an already voluminous literature on this topic, see Carr and Rees (1979), Barrow and Tipler (1986), Hogan (2000), Davies (2006), Barnes (2012).”
BackgroundAlternative cosmological theories
Kragh, H. (2019) · Oxford University Press eBooks · doi:10.1093/oxfordhb/9780198817666.013.4 · Cited by 3 · see citing works
Doko, E. (2026) · Cambridge University Press eBooks · doi:10.1017/9781009608350 · Cited by 2 · see citing works
Islamic Theism and the Multiverse
Doko, E. (2024) · Religions · doi:10.3390/rel15070861 · Cited by 2 · see citing works
“This indicates that many potential universes could feasibly sustain complex structures and life forms (Barnes 2012).”
BackgroundDie oorsprong van alles: "Dit was aand en dit was oggend"
Dreyer, J. S., van der Walt, K., & Denton, R. A. (2023) · Tydskrif vir Geesteswetenskappe · doi:10.17159/2224-7912/2023/v63n2a2 · Cited by 2 · see citing works
The Fine-Tuning Of The Universe For Life
Barnes, L. (2021) · The Routledge Companion to Philosophy of Physics · doi:10.4324/9781315623818-67 · Cited by 3 · see citing works
“This fine-tuning of the universe for life was first investigated by Carter (1974), Silk (1977), Carr & Rees (1979), Davies (1983), and Barrow & Tipler (1986), and has been reviewed recently by Hogan (2000), Barnes (2012), Schellekens (2013) and Lewis & Barnes (2016). We will consider a few examples.”
BackgroundSelf-citationPhilosophical discussions around cosmology
Prits, V. (2020) · Filosofska dumka (Philosophical Thought) · doi:10.15407/fd2020.03.096 · Cited by 2 · see citing works
The Fine-Tuning ArgumentPreprint
Landsman, K. (2015) · PhilSci-Archive (University of Pittsburgh) · doi:10.48550/arxiv.1505.05359 · Cited by 3 · see citing works
“First, in slightly different ways Smith (1993) and Barnes (2012) both made the point that the fta does not claim, or support the conclusion, that the present Universe is optimal for intelligent life.”
Relativistic astrophysics and cosmology
Longair, M. S. (2019) · Oxford University Press eBooks · doi:10.1093/oxfordhb/9780198817666.013.7 · Cited by 2 · see citing works
Emergent Structures of Effective Field Theories
Uzan, J. (2017) · Cambridge University Press eBooks · doi:10.1017/9781316535783.007 · Cited by 1 · see citing works
God Does Not Pick Locks: Fine-Tuning is Inconsistent with Omnipotence
McLauchlin, G. (2025) · Philosophia · doi:10.1007/s11406-025-00913-x · Cited by 1 · see citing works
““A divine designer” (Craig, 1988), a “theistic God” (Koperski, 2005), a “transcendent personal creator of the universe” and “God” (Barnes, 2012, 2020, respectively).”
The Universe’s Fine-Tuning Does Call for Explanation
Fumagalli, R. (2025) · Journal for General Philosophy of Science · doi:10.1007/s10838-025-09734-8 · Cited by 1 · see citing works
“…designer who deliberately set all the fundamental parameter values within the very narrow range of values that permits intelligent life (e.g., Barnes 2012; Collins 1999; Craig 2003; Davies 1992, Ch. 7–8; Holder 2004; Swinburne 2004, Ch. 8; White et al. 2018); 5 and appeals to future physical…”
InfluentialThe universal theory of structure: a fundamental ontology for ontic structural realism
Hamlin, C. E. (2026) · Synthese · doi:10.1007/s11229-025-05425-5 · Cited by 1 · see citing works
“Conventional fine-tuning arguments such as those reviewed in Barnes (2012) center on the claim that the constants and initial conditions of our physical laws seem delicately balanced to allow for the emergence of life.”
The Adaptive Niche Bias: an Adaptive Dynamics Perspective on the Anthropic Principle
Dolgikh, S. (2026) · Foundations of Science · doi:10.1007/s10699-026-10029-4 · Cited by 1 · see citing works
The Planck Power – A Numerical Coincidence or a Fundamental Number in Cosmology?
Denur, J. (2015) · InTech eBooks · doi:10.5772/61642 · Cited by 1 · see citing works
Steady-State theory and the cosmological controversy
Kragh, H. (2019) · Oxford University Press eBooks · doi:10.1093/oxfordhb/9780198817666.013.5 · Cited by 1 · see citing works
Observational and astrophysical cosmology: 1940–1980
Longair, M. S. (2019) · Oxford University Press eBooks · doi:10.1093/oxfordhb/9780198817666.013.6 · Cited by 1 · see citing works
Patra, E. A. D. I. (2021) · Türk bilgisayar ve matematik eğitimi dergisi · doi:10.17762/turcomat.v12i2.1126 · Cited by 1 · see citing works
“Barrow and Tipler (1986), Leslie (1989), Davies (2006), Ellis (2007), and Barnes (2012) have pointed out this fine-tuning aspect of cosmos.”
BackgroundAn introduction to gravitational waves through electrodynamics: a quadrupole comparison
Dorsch, G. C., & Porto, L. E. A. (2021) · European Journal of Physics · doi:10.1088/1361-6404/ac4645 · Cited by 1 · see citing works
The river of the water of life: Water as a theological symbol in Christian eschatology
Kotzé, M. (2023) · Reformed theology in Africa series · doi:10.4102/aosis.2023.bk377.04 · Cited by 1 · see citing works
Living Water: An interdisciplinary exploration of water as a theological theme
Viljoen, G., Vivier, J., Services, A. C., Vorster, J. M., Marais, N., Rheeder, R. A. L., Pretorius, S. J., AGES-group: Africa Geo-environmental Engineering and Science, & Lemmer, T. (2023) · Reformed theology in Africa series · doi:10.4102/aosis.2023.bk377 · Cited by 1 · see citing works
The role of groundwater in the Bible
Pretorius, S. J., & AGES-group: Africa Geo-environmental Engineering and Science (2023) · Reformed theology in Africa series · doi:10.4102/aosis.2023.bk377.07 · Cited by 1 · see citing works
Inflation, dark matter, and dark energy
Longair, M. S., & Smeenk, C. (2019) · Oxford University Press eBooks · doi:10.1093/oxfordhb/9780198817666.013.11 · Cited by 1 · see citing works
Philosophical aspects of cosmology
Smeenk, C. (2019) · Oxford University Press eBooks · doi:10.1093/oxfordhb/9780198817666.013.13 · Cited by 3 · see citing works
Smith, R. W. (2019) · Oxford University Press eBooks · doi:10.1093/oxfordhb/9780198817666.013.2 · Cited by 1 · see citing works
Worlds in a Stochastic Universe: On the Emergence of World Histories in Minimal Bohmian Mechanics
Ehmann, A. (2020) · Digital Commons - Lingnan (Lingnan University) · Cited by 1 · see citing works
Intelligent design and natural theology
Thorvaldsen, S. (2020) · Theofilos · doi:10.48032/theo/12/1/7 · Cited by 1 · see citing works
Ideology in Biology: Theism Meets Atheism in the Case of Abiogenesis
Ruffinengo, M. A., & Walsh, A. A. (2021) · Cited by 1 · see citing works
Review of: "Femmes finales: natural selection, physiology, and the return of the repressed"
Karwasz, G. P. (2023) · doi:10.32388/ydjp0s · Cited by 1 · see citing works
Gil, F. S. (2015) · Naturaleza y libertad revista de estudios interdisciplinares · doi:10.24310/natylib.2015.v0i05.6321
On a Relation of Vacuum Energy to the Hierarchy of ForcesPreprint
Alexander, S., & Mersini–Houghton, L. (2017) · arXiv (Cornell University) · doi:10.48550/arxiv.1705.10773
Review of Geraint F. Lewis and Luke A. Barnes, A Fortunate Universe: Life in a Finely Tuned CosmosPreprint
Benétreau-Dupin, Y. (2017) · arXiv (Cornell University) · doi:10.48550/arxiv.1706.09509
“edu/news/a-fortunate-universe-life-in-a-finely-tuned-cosmos/ (1)See for instance books by Leonard Susskind (2005), Sean Carroll (2010), and Lee Smolin (2013).”
BackgroundInfluentialNuclear Physics as Precision Science
Meißner, U.-G. (2018) · Journal of Physics Conference Series · doi:10.1088/1742-6596/1136/1/012001
Selected Topics and Case Studies
Beech, M. (2019) · Undergraduate lecture notes in physics · doi:10.1007/978-3-030-11704-7_6
Observational and astrophysical cosmology: 1980–2018
Longair, M. S. (2019) · Oxford University Press eBooks · doi:10.1093/oxfordhb/9780198817666.013.10
Cosmological theories before and without einstein
Kragh, H. (2019) · Oxford University Press eBooks · doi:10.1093/oxfordhb/9780198817666.013.1
Stranger things: multiverse, string cosmology, physical eschatology
Ćirković, M. M. (2019) · Oxford University Press eBooks · doi:10.1093/oxfordhb/9780198817666.013.12
Bianchi, S. D. (2019) · Oxford University Press eBooks · doi:10.1093/oxfordhb/9780198817666.013.9
Diverging Everettian Quantum Mechanics
Wilson, A. (2020) · Oxford University Press eBooks · doi:10.1093/oso/9780198846215.003.0003
Introduction: Explaining Contingency
Wilson, A. (2020) · Oxford University Press eBooks · doi:10.1093/oso/9780198846215.003.0001
Wilson, A. (2020) · Oxford University Press eBooks · doi:10.1093/oso/9780198846215.003.0008
Wilson, A. (2020) · Oxford University Press eBooks · doi:10.1093/oso/9780198846215.003.0005
Soler Gil, Francis. El universo a debate. Una introducción a la filosofía de la cosmología
Vilarroig, J. (2020) · Ideas y Valores · doi:10.15446/ideasyvalores.v69n173.84899
A Natural Introduction to Fine-TuningPreprint
Vuyst, J. D. (2020) · arXiv (Cornell University) · doi:10.48550/arxiv.2012.05617
“Taken from “The Fine-Tuning of the Universe for Intelligent Life”[12].”
MethodHow to formulate the fine-tuning argument for the existence of God?
Søvik, A. O. (2020) · Theofilos · doi:10.48032/theo/12/1/6
From Teleological Arguments to Thought Experiments
Kojonen, R. (2021) · Palgrave frontiers in philosophy of religion · doi:10.1007/978-3-030-69683-2_3
A New Fine-Tuning Argument for the Multiverse
Friederich, S. (2021) · Cambridge University Press eBooks · doi:10.1017/9781108765947.007
Wilson, A. (2020) · Oxford University Press eBooks · doi:10.1093/oso/9780198846215.003.0006
- Authors
- Barnes, L. A.
- Affiliations
- The University of Sydney (AU)
- Corresponding author
- Barnes, L. A.
- ORCID
- Barnes, L. A.
- Venue
- Publications of the Astronomical Society of Australia
- Publisher
- Cambridge University Press (CUP)
- Published
- 2012
- Volume
- 29
- Issue
- 4
- Pages
- 529-564
- ISSN
- 1323-3580 (ISSN-L)
- 1448-6083
- OpenAlex
- W2138231363
- Cited by
- 150
- References
- 125
- Citations by year
- 2026: 10 · 2025: 25 · 2024: 8 · 2023: 13 · 2022: 5 · 2021: 8 · 2020: 21 · 2019: 24 · 2018: 4 · 2017: 13 · 2016: 5 · 2015: 8 · 2014: 2 · 2013: 2 · 2012: 1
- FWCI
- 2.92
- Type
- journal article
- Language
- en
- Open access
- bronze
- doi.org
- Locations
- Publications of the Astronomical Society of Australia (publishedVersion)
- arXiv (Cornell University) (publishedVersion)
- reroDoc Digital Library (submittedVersion)
- Repository for Publications and Research Data (ETH Zurich) (submittedVersion, other-oa)
- arXiv (Cornell University)
- ETH Zürich Research Collection
- Topics
- Physical Sciences › Physics and Astronomy › Astronomy and Astrophysics › Cosmology and Gravitation Theories
- Physical Sciences › Physics and Astronomy › Astronomy and Astrophysics › Space Science and Extraterrestrial Life
- Physical Sciences › Earth and Planetary Sciences › Atmospheric Science › Earth Systems and Cosmic Evolution
- Keywords
- fine-tuning, intelligent life, multiverse, laws of nature, initial conditions, cosmic inflation, entropy, galaxy formation
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