What does inflation really predict?
Open accessAbstract
If the inflaton potential has multiple minima, as may be expected in, e.g., the string theory 'landscape', inflation predicts a probability distribution for the cosmological parameters describing spatial curvature (Ω tot ), dark energy (ρ Λ , w etc), the primordial density fluctuations ( Q , n s , d n s /d ln k etc) and primordial gravitational waves ( r , n t etc). We compute this multivariate probability distribution for various classes of single-field slow-roll models, exploring its dependence on the characteristic inflationary energy scales, the shape of the potential V and the choice of measure underlying the calculation. We find that unless the characteristic scale Δϕ on which V varies happens to be near the Planck scale, the only aspect of V that matters observationally is the statistical distribution of its peaks and troughs. For all energy scales and plausible measures considered, we obtain the predictions , w = −1 and ρ Λ in the observed ballpark but uncomfortably high. The high energy limit predicts , , and , consistent with observational data and indistinguishable from eternal inflation. The low energy limit predicts five parameters but favours larger Q and redder n s than observed. We discuss the coolness problem , the smoothness problem and the pothole paradox , which severely limit the viable class of models and measures. Predictions insensitive to pre-inflationary conditions can arise either from eternal inflation attractor behaviour or from anthropic selection effects probing merely a tiny non-special part of the initial distribution. We argue that these two mechanisms are severely challenged by the coolness problem and the smoothness problem, respectively. Our findings bode well for detecting an inflationary gravitational wave signature with future CMB polarization experiments, with the arguably best-motivated single-field models favouring the detectable level .
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Tegmark (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.”
From The Fine-Tuning of the Universe for Intelligent Life (2012) · cites this paper as Tegmark (2005)
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Experimental — accuracy not yet measuredFor 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.”
From The Fine-Tuning of the Universe for Intelligent Life (2012) · cites this paper as Tegmark (2005)
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 measuredLife-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.”
From The Fine-Tuning of the Universe for Intelligent Life (2012) · cites this paper as Tegmark (2005)
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 measuredThe 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 .”
From The Fine-Tuning of the Universe for Intelligent Life (2012) · cites this paper as Tegmark (2005)
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 measuredFor 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.”
From The Fine-Tuning of the Universe for Intelligent Life (2012) · cites this paper as Tegmark (2005)
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)
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References 112 · Cited by 216
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- Authors
- Tegmark, M.
- Affiliations
- Massachusetts Institute of Technology (US)
- Corresponding author
- Tegmark, Max
- ORCID
- Tegmark, Max
- Venue
- Journal of Cosmology and Astroparticle Physics
- Publisher
- IOP Publishing
- Published
- 2005-04-05
- Volume
- 2005
- Issue
- 04
- Pages
- 001-001
- ISSN
- 1475-7508 (ISSN-L)
- 1475-7516
- OpenAlex
- W1968750729
- Cited by
- 216
- References
- 112
- Citations by year
- 2026: 3 · 2025: 2 · 2024: 2 · 2023: 3 · 2022: 2 · 2021: 7 · 2020: 5 · 2019: 26 · 2018: 8 · 2017: 5 · 2016: 6 · 2015: 7 · 2014: 6 · 2013: 10 · 2012: 17
- FWCI
- 12.60
- Type
- journal article
- Language
- en
- Open access
- bronze
- doi.org
- Locations
- Journal of Cosmology and Astroparticle Physics (publishedVersion)
- arXiv (Cornell University) (submittedVersion)
- CERN Document Server (European Organization for Nuclear Research) (submittedVersion)
- arXiv (Cornell University)
- Funders
- National Science Foundation (CAREER, 0134999)
- National Aeronautics and Space Administration (NAG511099)
- Topics
- Physical Sciences › Physics and Astronomy › Astronomy and Astrophysics › Cosmology and Gravitation Theories
- Physical Sciences › Physics and Astronomy › Statistical and Nonlinear Physics › Noncommutative and Quantum Gravity Theories
- Physical Sciences › Physics and Astronomy › Nuclear and High Energy Physics › Dark Matter and Cosmic Phenomena
- Keywords
- inflation (cosmology), multiverse, string landscape, inflaton potential, slow-roll inflation, dark energy equation of state, primordial density fluctuations, primordial gravitational waves, CMB polarization, eternal inflation, measure problem, single-field inflation
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