The DOI matches its Crossref record; 11 of the 11 references it cites were found in a registry or an index; none of the 2 sources its claims cite is checked for support yet.
Gravitational Collapse and Space-Time Singularities
Open accessAbstract
A similar increase in the low-energy proton in- tensity, in coincidence with the passage of a blast wave, was observed on 12 November 1960 t J. F.
Overview
AI snapshot
Written from the paper’s full text.
TL;DR
Penrose argues that once a trapped surface forms during gravitational collapse, spacetime singularities must develop, irrespective of any assumption of spherical or other symmetry. The paper outlines a proof that a set of five plausible physical assumptions is internally inconsistent.
Key findings
- The five assumptions — (i) M⁺ is a nonsingular manifold with two separate null half-cone systems, (ii) null completeness (every null geodesic extends to arbitrarily large affine parameter), (iii) the Cauchy hypersurface condition (every timelike or null geodesic in M⁺ can be extended into the past until it meets C), (iv) non-negativeness of local energy, and (v) the existence of a trapped surface T² in M⁺ — are together inconsistent.
- A trapped surface is defined as a closed spacelike 2-surface whose two orthogonal systems of null geodesics converge locally in future directions. In spherical collapse such a surface exists once matter contracts within r = 2m; the Kerr solutions with m > a (angular momentum) also possess trapped surfaces, whereas those with m < a do not.
- If physical singularities are not permitted, then inside such a collapsing object at least one of the following must hold: (a) negative local energy occurs, (b) Einstein's equations are violated, (c) the spacetime manifold is incomplete, or (d) the concept of spacetime loses its meaning at very high curvatures, possibly because of quantum phenomena.
- The convergence argument: with p ≤ 0 at T² (trapped), the cross-sectional area A becomes zero at a finite affine distance to the future on each null geodesic, so each geodesic encounters a caustic and B' is compact; approximating B' by a smooth closed spacelike hypersurface B'* and using a degree argument, d(Q) = 1 near both B'* and C, which is impossible because C is noncompact.
Methods
- Design: a theoretical general-relativity argument, presented as an outline of a proof, deliberately avoiding symmetry assumptions (spherical symmetry precludes discussion of gravitational radiation, which requires at least quadrupole structure).
- Setup: an initial Cauchy hypersurface C carrying a matter distribution, with Einstein's field equations and suitable equations of state; the only assumption made about the equations of state is the non-negative definiteness of the energy expression.
- Main analysis: null geodesic convergence and shear for the null geodesic segments generating the boundary B' of the future set of the trapped surface, combined with a topological degree argument on the map from B'* back to C.
Limitations
- Stated by the paper: the result is given "in outline," with full details of this and other related results to be given elsewhere.
- Evident from the text: the provided text is a heavily corrupted OCR rendering, and the abstract printed with it concerns an unrelated observation of low-energy proton intensity and a blast wave, so it does not describe this paper's content.
Model-written summary. Check it against the paper before relying on it.
Integrity signals
Registry
Cites
Statistics
Verification
Claims the paper makes
12 No basis given · 6 Own interpretation · 2 Sources not found
The paper states this without a source or data behind it here, so there is nothing to check it against. The quote shows it is in the paper.
In the paper
“Aft the matter has contracted within r =2m, er e =, = t a space e sp e lik here S' (f =const, 2m &r= cson) can be found in the empty region surrounding the matter.”
§ GRAVITATIONAL COLLAPSE AND SPACE-TIME SINGULARITIES > Abstract
plaindirect- Asserted: passes — The authors put it forward as true.
- Checkable: passes — It can be checked against evidence.
- Load-bearing: passes — The paper’s conclusions depend on it.
- Based: passes — The paper gives a reason why it holds.
The paper states this without a source or data behind it here, so there is nothing to check it against. The quote shows it is in the paper.
In the paper
“The impossibility of this follows from the noncompactness of C'.”
§ GRAVITATIONAL COLLAPSE AND SPACE-TIME SINGULARITIES > Abstract
plaindirect- Asserted: passes — The authors put it forward as true.
- Checkable: passes — It can be checked against evidence.
- Load-bearing: passes — The paper’s conclusions depend on it.
- Based: passes — The paper gives a reason why it holds.
- The authors state this as an assumption: The manifold M+ is the future time development of an initial Cauchy surface C (the past boundary of the M+ region).
- The authors state this as an assumption: M+ is a nonsingular C∞ manifold for which the null half-cones form two separate systems (past and future).
- The authors state this as an assumption: Every null geodesic in M+ can be extended into the future to arbitrarily large affine parameter values (null completeness).
- The authors state this as an assumption: Every timelike or null geodesic in M+ can be extended into the past until it meets C (Cauchy hypersurface condition).
- The authors state this as an assumption: At every point of M+, all timelike vectors t satisfy (-R_ab + ... ) t^a t^b ≥ 0 (non-negativeness of local energy).
- The authors state this as an assumption: There exists a trapped surface T' in M+.
The paper states this without a source or data behind it here, so there is nothing to check it against. The quote shows it is in the paper.
In the paper
“Local considerations show that B' is null where it is nonsingular, being generated by the null geodesic segments which meet T' orthogonally at a past endpoint and have a future endpoint if this is a singularity (on a caustic or crossing region) of B'.”
§ GRAVITATIONAL COLLAPSE AND SPACE-TIME SINGULARITIES > Abstract
plaindirect- Asserted: passes — The authors put it forward as true.
- Checkable: passes — It can be checked against evidence.
- Load-bearing: passes — The paper’s conclusions depend on it.
- Based: passes — The paper gives a reason why it holds.
- The authors state this as an assumption: The manifold M+ is the future time development of an initial Cauchy surface C (the past boundary of the M+ region).
- The authors state this as an assumption: M+ is a nonsingular C∞ manifold for which the null half-cones form two separate systems (past and future).
- The authors state this as an assumption: Every null geodesic in M+ can be extended into the future to arbitrarily large affine parameter values (null completeness).
- The authors state this as an assumption: Every timelike or null geodesic in M+ can be extended into the past until it meets C (Cauchy hypersurface condition).
- The authors state this as an assumption: At every point of M+, all timelike vectors t satisfy (-R_ab + ... ) t^a t^b ≥ 0 (non-negativeness of local energy).
- The authors state this as an assumption: There exists a trapped surface T' in M+.
The paper states this without a source or data behind it here, so there is nothing to check it against. The quote shows it is in the paper.
In the paper
“Hence B' is compact (closed), being generated by a compact system of finite segments.”
§ GRAVITATIONAL COLLAPSE AND SPACE-TIME SINGULARITIES > Abstract
plaindirect- Asserted: passes — The authors put it forward as true.
- Checkable: passes — It can be checked against evidence.
- Load-bearing: passes — The paper’s conclusions depend on it.
- Based: passes — The paper gives a reason why it holds.
- The authors state this as an assumption: The manifold M+ is the future time development of an initial Cauchy surface C (the past boundary of the M+ region).
- The authors state this as an assumption: M+ is a nonsingular C∞ manifold for which the null half-cones form two separate systems (past and future).
- The authors state this as an assumption: Every null geodesic in M+ can be extended into the future to arbitrarily large affine parameter values (null completeness).
- The authors state this as an assumption: Every timelike or null geodesic in M+ can be extended into the past until it meets C (Cauchy hypersurface condition).
- The authors state this as an assumption: At every point of M+, all timelike vectors t satisfy (-R_ab + ... ) t^a t^b ≥ 0 (non-negativeness of local energy).
- The authors state this as an assumption: There exists a trapped surface T' in M+.
The paper states this without a source or data behind it here, so there is nothing to check it against. The quote shows it is in the paper.
In the paper
“To an outside observer the contraction to ~= 2m appears to take an infinite time.”
§ GRAVITATIONAL COLLAPSE AND SPACE-TIME SINGULARITIES > Abstract
hedgeddirect- Asserted: passes — The authors put it forward as true.
- Checkable: passes — It can be checked against evidence.
- Load-bearing: unclear — It is unclear whether the paper’s conclusions depend on it.
- Based: unclear — It is unclear why the paper says it holds.
A conclusion the paper draws from its own results — it cites no other source for it, so there is none to check. The quote shows it is in the paper.
In the paper
“the existence o a trapped sur ace 1m”
- Also stated in: § Abstract · plain
“that singularities necessarily il develop.metry”
§ GRAVITATIONAL COLLAPSE AND SPACE-TIME SINGULARITIES > Abstract
plaindirect- Asserted: passes — The authors put it forward as true.
- Checkable: passes — It can be checked against evidence.
- Load-bearing: passes — The paper’s conclusions depend on it.
- Based: passes — The paper gives a reason why it holds.
- The authors state this as an assumption: The only assumption made about the equations of state is the non-negative definiteness of the energy expression T_ab (with or without cosmological terms).
- The authors state this as an assumption: The matter distribution undergoes gravitational collapse in a way which, at first, qualitatively resembles the spherical case.
- Also stated in: § Abstract · plain
A conclusion the paper draws from its own results — it cites no other source for it, so there is none to check. The quote shows it is in the paper.
In the paper
“It will be shown here, in outline, that (i), ~~~, (v) are together inconsistent.”
§ GRAVITATIONAL COLLAPSE AND SPACE-TIME SINGULARITIES > Abstract
boosted- Asserted: passes — The authors put it forward as true.
- Checkable: passes — It can be checked against evidence.
- Load-bearing: passes — The paper’s conclusions depend on it.
- Based: passes — The paper gives a reason why it holds.
- The authors state this as an assumption: The manifold M+ is the future time development of an initial Cauchy surface C (the past boundary of the M+ region).
- The authors state this as an assumption: M+ is a nonsingular C∞ manifold for which the null half-cones form two separate systems (past and future).
- The authors state this as an assumption: Every null geodesic in M+ can be extended into the future to arbitrarily large affine parameter values (null completeness).
- The authors state this as an assumption: Every timelike or null geodesic in M+ can be extended into the past until it meets C (Cauchy hypersurface condition).
- The authors state this as an assumption: At every point of M+, all timelike vectors t satisfy (-R_ab + ... ) t^a t^b ≥ 0 (non-negativeness of local energy).
- The authors state this as an assumption: There exists a trapped surface T' in M+.
The paper states this without a source or data behind it here, so there is nothing to check it against. The quote shows it is in the paper.
In the paper
“The empty region surrounding the matter will, in th1s case, Schwarzsc 1 h ld field”
§ GRAVITATIONAL COLLAPSE AND SPACE-TIME SINGULARITIES > Abstract
plaindirect- Asserted: passes — The authors put it forward as true.
- Checkable: passes — It can be checked against evidence.
- Load-bearing: passes — The paper’s conclusions depend on it.
- Based: unclear — It is unclear why the paper says it holds.
A conclusion the paper draws from its own results — it cites no other source for it, so there is none to check. The quote shows it is in the paper.
In the paper
“The existence of a singular1ty can tion such d however, without an assump io inferre, ow r con- as completeness for the manifold under c si eration.”
§ GRAVITATIONAL COLLAPSE AND SPACE-TIME SINGULARITIES > Abstract
plain- Asserted: passes — The authors put it forward as true.
- Checkable: passes — It can be checked against evidence.
- Load-bearing: passes — The paper’s conclusions depend on it.
- Based: passes — The paper gives a reason why it holds.
In the paper
“The recent rotating solution of Kerr' also possesses a physical singularity”
§ GRAVITATIONAL COLLAPSE AND SPACE-TIME SINGULARITIES > Abstract
What the sources say
- Not matchedcites Kerr'
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
plain- Asserted: passes — The authors put it forward as true.
- Checkable: passes — It can be checked against evidence.
- Load-bearing: passes — The paper’s conclusions depend on it.
- Based: passes — The paper gives a reason why it holds.
- Not matched
- It may state two separate claims as one. 6
- Probably not a substantial claim. 1
- The quote only partly states this claim. 2
The paper states this without a source or data behind it here, so there is nothing to check it against. The quote shows it is in the paper.
In the paper
“Since T' is trapped, p& 0 at T', whence A becomes zero at a finite affine distance to the future of T' on each null geodesic.”
§ GRAVITATIONAL COLLAPSE AND SPACE-TIME SINGULARITIES > Abstract
plaindirect- Asserted: passes — The authors put it forward as true.
- Checkable: passes — It can be checked against evidence.
- Load-bearing: passes — The paper’s conclusions depend on it.
- Based: passes — The paper gives a reason why it holds.
It may state two separate claims as one.
- The authors state this as an assumption: The manifold M+ is the future time development of an initial Cauchy surface C (the past boundary of the M+ region).
- The authors state this as an assumption: M+ is a nonsingular C∞ manifold for which the null half-cones form two separate systems (past and future).
- The authors state this as an assumption: Every null geodesic in M+ can be extended into the future to arbitrarily large affine parameter values (null completeness).
- The authors state this as an assumption: Every timelike or null geodesic in M+ can be extended into the past until it meets C (Cauchy hypersurface condition).
- The authors state this as an assumption: At every point of M+, all timelike vectors t satisfy (-R_ab + ... ) t^a t^b ≥ 0 (non-negativeness of local energy).
- The authors state this as an assumption: There exists a trapped surface T' in M+.
The paper states this without a source or data behind it here, so there is nothing to check it against. The quote shows it is in the paper.
In the paper
“This sphere is an example of what will be called here a trapped surfacedefined T' with the property that the two systems of null eodesics which meet T' orthogonally con- verge locally in future directions at T'.”
§ GRAVITATIONAL COLLAPSE AND SPACE-TIME SINGULARITIES > Abstract
plain- Asserted: passes — The authors put it forward as true.
- Checkable: passes — It can be checked against evidence.
- Load-bearing: passes — The paper’s conclusions depend on it.
- Based: passes — The paper gives a reason why it holds.
Probably not a substantial claim.
The paper states this without a source or data behind it here, so there is nothing to check it against. The quote shows it is in the paper.
In the paper
“Each geodesic thus encounters a caustic.”
§ GRAVITATIONAL COLLAPSE AND SPACE-TIME SINGULARITIES > Abstract
plaindirect- Asserted: passes — The authors put it forward as true.
- Checkable: passes — It can be checked against evidence.
- Load-bearing: passes — The paper’s conclusions depend on it.
- Based: passes — The paper gives a reason why it holds.
The quote only partly states this claim.
- The authors state this as an assumption: The manifold M+ is the future time development of an initial Cauchy surface C (the past boundary of the M+ region).
- The authors state this as an assumption: M+ is a nonsingular C∞ manifold for which the null half-cones form two separate systems (past and future).
- The authors state this as an assumption: Every null geodesic in M+ can be extended into the future to arbitrarily large affine parameter values (null completeness).
- The authors state this as an assumption: Every timelike or null geodesic in M+ can be extended into the past until it meets C (Cauchy hypersurface condition).
- The authors state this as an assumption: At every point of M+, all timelike vectors t satisfy (-R_ab + ... ) t^a t^b ≥ 0 (non-negativeness of local energy).
- The authors state this as an assumption: There exists a trapped surface T' in M+.
The paper states this without a source or data behind it here, so there is nothing to check it against. The quote shows it is in the paper.
In the paper
“For a sufficiently great mass, there is no final equilibrium state.%'hen sufficient thermal energy has been radiated away, the body contracts and continues to contract until a physi- cal singularity is encountered at r = 0.”
§ GRAVITATIONAL COLLAPSE AND SPACE-TIME SINGULARITIES > Abstract
boosteddirect- Asserted: passes — The authors put it forward as true.
- Checkable: passes — It can be checked against evidence.
- Load-bearing: passes — The paper’s conclusions depend on it.
- Based: unclear — It is unclear why the paper says it holds.
It may state two separate claims as one.
The paper states this without a source or data behind it here, so there is nothing to check it against. The quote shows it is in the paper.
In the paper
“As measured by local comoving observers”
- Also stated in: § Abstract · plain
“the body passes within its Schwarzschild radius r = 2m.”
§ GRAVITATIONAL COLLAPSE AND SPACE-TIME SINGULARITIES > Abstract
plain- Asserted: passes — The authors put it forward as true.
- Checkable: passes — It can be checked against evidence.
- Load-bearing: passes — The paper’s conclusions depend on it.
- Based: passes — The paper gives a reason why it holds.
The quote only partly states this claim.
- Also stated in: § Abstract · plain
A conclusion the paper draws from its own results — it cites no other source for it, so there is none to check. The quote shows it is in the paper.
In the paper
“inside such a collapsing ob'ect at least one of the following holds: o ]ec a (a) Negative local energy occurs.stein's equations are v1olated.,c, The s ace- time manifold is incomplete.' (d} The concept”
§ GRAVITATIONAL COLLAPSE AND SPACE-TIME SINGULARITIES > Abstract
plainconditional- Asserted: passes — The authors put it forward as true.
- Checkable: passes — It can be checked against evidence.
- Load-bearing: passes — The paper’s conclusions depend on it.
- Based: passes — The paper gives a reason why it holds.
It may state two separate claims as one.
- The authors state this as an assumption: The only assumption made about the equations of state is the non-negative definiteness of the energy expression T_ab (with or without cosmological terms).
- The authors state this as an assumption: The matter distribution undergoes gravitational collapse in a way which, at first, qualitatively resembles the spherical case.
The paper states this without a source or data behind it here, so there is nothing to check it against. The quote shows it is in the paper.
In the paper
“Note that an exterior ob- server will always see matter outside r =2m, the collapse through r =2m to the singularity at r =0 being invisible to him.”
§ GRAVITATIONAL COLLAPSE AND SPACE-TIME SINGULARITIES > Abstract
plain- Asserted: passes — The authors put it forward as true.
- Checkable: passes — It can be checked against evidence.
- Load-bearing: passes — The paper’s conclusions depend on it.
- Based: passes — The paper gives a reason why it holds.
It may state two separate claims as one.
A conclusion the paper draws from its own results — it cites no other source for it, so there is none to check. The quote shows it is in the paper.
In the paper
“ly trapped surfaces will still exist if the matter region has no sharp boundary or if spherica tions from the above situation are not too great.”
§ GRAVITATIONAL COLLAPSE AND SPACE-TIME SINGULARITIES > Abstract
plainconditional- Asserted: passes — The authors put it forward as true.
- Checkable: passes — It can be checked against evidence.
- Load-bearing: passes — The paper’s conclusions depend on it.
- Based: passes — The paper gives a reason why it holds.
It may state two separate claims as one.
In the paper
“Indee, e d th Kerr solutions with m &a angular ) all possess trapped surfac momentum ma .' The whereas os th se for which m ~a do not.”
§ GRAVITATIONAL COLLAPSE AND SPACE-TIME SINGULARITIES > Abstract
What the sources say
- Not matchedcites Kerr'
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
plaincorrelational- Asserted: passes — The authors put it forward as true.
- Checkable: passes — It can be checked against evidence.
- Load-bearing: passes — The paper’s conclusions depend on it.
- Based: passes — The paper gives a reason why it holds.
It may state two separate claims as one.
- Not matched
The authors state this as an assumption.
The only assumption made about the equations of state is the non-negative definiteness of the energy expression T_ab (with or without cosmological terms).
“In fact the only assump- made here about these equations of sta e will be the non-negative definiteness o energy express1on w' (with or without cosmologi- c.”
The authors state this as an assumption.
The matter distribution undergoes gravitational collapse in a way which, at first, qualitatively resembles the spherical case.
“undergoes gravitational collapse in a way w ic, e s herical- at first, qualitatively resembles the p t ' al case.”
The authors state this as an assumption.
The manifold M+ is the future time development of an initial Cauchy surface C (the past boundary of the M+ region).
“It will be necessary, here, to sup- 4, 'ch is the future th t the manifold M+, which is development of an initial Cauchy yp time deve opm 4 re ion), sur ace f C~( past boundary of the M+ r g' re.”
The authors state this as an assumption.
M+ is a nonsingular C∞ manifold for which the null half-cones form two separate systems (past and future).
“(i) M+~i s a nonsingular (+--ifold for which the null half-cones form two separate systems (”
The authors state this as an assumption.
Every null geodesic in M+ can be extended into the future to arbitrarily large affine parameter values (null completeness).
“(ii) Every nu ge e ' the future to arbitrarily large affine param- into e u ster values (null completeness .”
The authors state this as an assumption.
Every timelike or null geodesic in M+ can be extended into the past until it meets C (Cauchy hypersurface condition).
“timelike or null geodesic in M+ can e FIG. 1. Spherically symmetrical collapse (one s ace dimension surpressed).The diagram essentially also serves for the discussion o e ym f the as metrical case.into the past until it meets C, (Cauchy hyper- surface condition).”
The authors state this as an assumption.
At every point of M+, all timelike vectors t satisfy (-R_ab + ... ) t^a t^b ≥ 0 (non-negativeness of local energy).
“(iv) At every point of M+~, all timelike vectors t& satisfy ( -R”
“non-negativeness of local ener- jLL V gy).”
The authors state this as an assumption.
There exists a trapped surface T' in M+.
“(v) There exists a trapped surface F' in M+4.”
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 source backs part of the claim, not all of it — or backs it for a different population, condition or comparison.
In the citing paper
“From the classical singularity theorems [3-6], one would expect such high curvatures to occur in collapsing stars and, in the past, at the beginning of the present espe se e oone o on oet e ne o e e osones of high curvature to be hidden from us by an event horizon [7].”
From Particle creation by black holes (1975) · cites this paper as [3]
Experimental — accuracy not yet measured
Citations
Cites
Gravitational Field of a Spinning Mass as an Example of Algebraically Special Metrics
Kerr, R. P. (1963) · Physical Review Letters · doi:10.1103/physrevlett.11.237 · Cited by 3,563
An Approach to Gravitational Radiation by a Method of Spin Coefficients
Newman, E., & Penrose, R. (1962) · Journal of Mathematical Physics · doi:10.1063/1.1724257 · Cited by 2,702
Self-citationOn Continued Gravitational Contraction
Oppenheimer, J. R., & Snyder, H. S. (1939) · Physical Review · doi:10.1103/physrev.56.455 · Cited by 2,054
Relativity, groups and topology
L.R. (1965) · Nuclear Physics · doi:10.1016/0029-5582(65)90020-9 · Cited by 1,104
Investigations in relativistic cosmology
LIFSHITZ, E. M., & Khalatnikov, I. M. (1963) · Advances In Physics · doi:10.1080/00018736300101283 · Cited by 915
Past-Future Asymmetry of the Gravitational Field of a Point Particle
Finkelstein, D. (1958) · Physical Review · doi:10.1103/physrev.110.965 · Cited by 542
On the Nature of Strong Radio Sources
Hoyle, F., & Fowler, W. A. (1962) · Monthly Notices of the Royal Astronomical Society · doi:10.1093/mnras/125.2.169 · Cited by 228
HOYLE, F., Fowler, W. A., Burbidge, G. R., & Burbidge, E. M. (1964) · The Astrophysical Journal · doi:10.1086/147825 · Cited by 185
Massive Stars, Relativistic Polytropes, and Gravitational Radiation
Fowler, W. A. (1964) · Reviews of Modern Physics · doi:10.1103/revmodphys.36.545 · Cited by 92
On the avoidance of singularities in C -field cosmology
HOYLE, F., & Narlikar, J. V. (1964) · Proceedings of the Royal Society of London A Mathematical and Physical Sciences · doi:10.1098/rspa.1964.0076 · Cited by 80
Research works printed but not linked: 4
- Ya. B. Zel'dovich, 1964, Dokl. Akad. Nauk SSSR, 155, 1033
- I. S. Shklovskiǐ, 1964, Dokl. Akad. Nauk SSSR, 155, 1039
- Ya. B. Zel'dovich, 1964, Dokl. Akad. Nauk SSSR, 156, 57
- Ya. B. Zel'dovich, 1964, Proceedings of the 1963 Dallas Conference on Gravitational Collapse
Cited by
Sorted by citations
Items 1,501–1,600 of 2,958
Measurement-Induced Nonlocality for Observers Near a Black Hole
Kaczmarek, A. Z., Szczęśniak, D., & Kais, S. (2023) · Universe · doi:10.3390/universe9040199 · Cited by 5
Can a variation of fine structure constant influence the fate of gravitational collapse?
Chakrabarti, S. (2023) · The European Physical Journal C · doi:10.1140/epjc/s10052-023-11877-1 · Cited by 6
Trajectory of a Spacecraft When It Passes by a Gravitational Body During Interstellar Travel
Silverberg, L. M., & Eischen, J. W. (2023) · Journal of Spacecraft and Rockets · doi:10.2514/1.a35684 · Cited by 5
Zhang, S.-J. (2023) · The European Physical Journal C · doi:10.1140/epjc/s10052-023-12144-z · Cited by 5
Tidal disruption of white dwarfs in a modified gravity theory with SPH
Garain, D., Banerjee, P., Chowdhury, S., & Sarkar, T. (2023) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2023/11/062 · Cited by 5
Ellis, G. (2023) · Foundations of Physics · doi:10.1007/s10701-023-00738-2 · Cited by 5
Comparing f(R) and scale-dependent gravities
Calzada, P. V., Rincón, Á., & Bargueño, P. (2023) · The European Physical Journal C · doi:10.1140/epjc/s10052-023-12269-1 · Cited by 5
NASHED, G. G. L. (2024) · The European Physical Journal C · doi:10.1140/epjc/s10052-023-12349-2 · Cited by 5
Triantafyllopoulos, A., Kapsabelis, E., & Stavrinos, P. C. (2024) · Universe · doi:10.3390/universe10010026 · Cited by 5
Adler, S. L. (2024) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.109.024020 · Cited by 5
Extension of Hayward black hole in f(R) gravity coupled with a scalar field
NASHED, G. G. L. (2024) · Physics of the Dark Universe · doi:10.1016/j.dark.2024.101462 · Cited by 5
Healthy Horndeski cosmologies with torsion
Mironov, S., & Valencia-Villegas, M. (2024) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2024/07/030 · Cited by 6
Violation of weak cosmic censorship in de Sitter space
Lin, F.-L., & Ning, B. (2024) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.110.044057 · Cited by 5
Black hole tunneling in loop quantum gravity*
Tan, H., Guo, R.-Z., & Zhang, J. (2025) · Chinese Physics C · doi:10.1088/1674-1137/adabd0 · Cited by 5
On the structure of black bounces sourced by anisotropic fluids
Lessa, L. A., & Olmo, G. J. (2025) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2025/03/019 · Cited by 5
Retrograde precession of relativistic orbits and the quest for charged black holes
Bambhaniya, P., Vyas, M. J., Joshi, P. S., & Pino, E. M. D. G. D. (2025) · Physics of the Dark Universe · doi:10.1016/j.dark.2025.101949 · Cited by 5
Jafarzade, K., Ghasemi-Nodehi, M., Sadeghi, F., & Mirza, B. (2025) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2025/03/063 · Cited by 5
Einstein equation at singularities
Stoica, O. C. (2014) · Open Physics · doi:10.2478/s11534-014-0427-1 · Cited by 5
Study of multi-black-hole and ring-singularity apparent horizons
Jaramillo, G., & Loustó, C. O. (2011) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.84.104011 · Cited by 5
On black hole singularities in quantum gravity
Russo, J. G. (1994) · Physics Letters B · doi:10.1016/0370-2693(94)91129-0 · Cited by 5
Nonlinear resonance in Hořava–Lifshitz bouncing cosmologies
Maier, R. (2013) · Classical and Quantum Gravity · doi:10.1088/0264-9381/30/11/115011 · Cited by 5
No open or flat bouncing cosmologies in Einstein gravity
Parikh, M. (2015) · Journal of High Energy Physics · doi:10.1007/jhep10(2015)089 · Cited by 8
MARGINALLY TRAPPED MERIDIAN SURFACES OF PARABOLIC TYPE IN THE FOUR-DIMENSIONAL MINKOWSKI SPACE
Ganchev, G., & Milousheva, V. (2013) · International Journal of Geometric Methods in Modern Physics · doi:10.1142/s0219887813500606 · Cited by 5
The mass formula for an exotic BTZ black hole
Zhang, B. (2016) · Annals of Physics · doi:10.1016/j.aop.2016.01.021 · Cited by 5
“All that Matter … in One Big Bang …”, &Other Cosmological Singularities
Elizalde, E. (2018) · Galaxies · doi:10.3390/galaxies6010025 · Cited by 5
Manifold-topology from K -causal order
Sorkin, R. D., Yazdi, Y. K., & Zwane, N. (2019) · Classical and Quantum Gravity · doi:10.1088/1361-6382/ab1166 · Cited by 5
A novel notion of null infinity for c-boundaries and generalized black holes
Silva, I. P. C. E., Flores, J. L., & Herrera, J. (2018) · Journal of High Energy Physics · doi:10.1007/jhep09(2018)123 · Cited by 5
Alternative route towards the change of metric signature
Zhang, F. (2019) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.100.064043 · Cited by 6
Aspects of marginally trapped and antitrapped surfaces in a D -dimensional evolving dust model
Raviteja, K., & Gutti, S. (2020) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.102.024072 · Cited by 5
Trapped region in Kerr–Vaidya space–time
Dahal, P. K. (2021) · Journal of Astrophysics and Astronomy · doi:10.1007/s12036-021-09741-3 · Cited by 5
Collisional Penrose process of 4D rotational Einstein-Gauss-Bonnet black holes *
Liu, Y., & Zhang, X. (2021) · Chinese Physics C · doi:10.1088/1674-1137/abe36a · Cited by 5
Exploring the cosmic censorship conjecture with a Gauss-Bonnet sector
Tavakoli, Y., Ardabili, A. K., & Moniz, P. V. (2021) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.103.084039 · Cited by 5
Vacuum Semiclassical Gravity Does Not Leave Space for Safe Singularities
Arrechea, J., Barceló, C., Boyanov, V., & Garay, L. J. (2021) · Universe · doi:10.3390/universe7080281 · Cited by 5
Emergent universe revisited through the CSL theory
Bengochea, G. R., Piccirilli, M. P., & León, G. (2021) · The European Physical Journal C · doi:10.1140/epjc/s10052-021-09842-x · Cited by 6
Crossing the Big Bang singularity
WETTERICH, C. (2021) · Physics of the Dark Universe · doi:10.1016/j.dark.2021.100866 · Cited by 5
Thermodynamics of a modified Schwarzschild white hole in the presence of a cosmological constant
Kubeka, A. S., & Amani, A. (2022) · International Journal of Modern Physics A · doi:10.1142/s0217751x22500397 · Cited by 5
Spacetime singularities and curvature blow-ups
Rácz, I. (2022) · General Relativity and Gravitation · doi:10.1007/s10714-022-03053-9 · Cited by 5
Applications of Thermodynamic Geometries to Conformal Regular Black Holes: A Comparative Study
Jawad, A., Hussain, M., & Rani, S. (2023) · Universe · doi:10.3390/universe9020087 · Cited by 5
Two-dimensional regular string black hole via complete $$\alpha ^{\prime }$$ corrections
Ying, S. (2023) · The European Physical Journal C · doi:10.1140/epjc/s10052-023-11756-9 · Cited by 10
Faizal, M. (2023) · International Journal of Modern Physics A · doi:10.1142/s0217751x23501889 · Cited by 6
de Oliveira, J., Fontana, R. D. B., & Pavan, A. B. (2024) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.109.024027 · Cited by 5
Testing the first law of black hole mechanics with gravitational waves
Wang, C.-W.-Z., Zhu, J.-B., Huang, G., & Shu, F.-W. (2024) · Science China Physics Mechanics and Astronomy · doi:10.1007/s11433-024-2442-3 · Cited by 5
Frozen stars: Black hole mimickers sourced by a string fluid
Brustein, R., & Medved, A. J. M. (2024) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.110.104004 · Cited by 5
Black Holes and Trapped Surfaces
Senovilla, J. M. M., Macı́as, A., & Maceda, M. (2010) · AIP conference proceedings · doi:10.1063/1.3531621 · Cited by 5
Focusing of world-lines in Weyl gravity
Mohseni, M., & Fathi, M. (2016) · The European Physical Journal Plus · doi:10.1140/epjp/i2016-16021-y · Cited by 5
Báez, C. (2021) · Cambridge University Press eBooks · doi:10.1017/9781108854399.010 · Cited by 5
Complete linear Weingarten spacelike submanifolds with higher codimension in the de Sitter space
Araújo, J. G., de Lima, H. F., dos Santos, F. R., & Velásquez, M. A. L. (2019) · International Journal of Geometric Methods in Modern Physics · doi:10.1142/s0219887819500506 · Cited by 5
Exact inner metric and microscopic state of AdS3-Schwarzschild BHs
Zeng, D.-F. (2020) · Nuclear Physics B · doi:10.1016/j.nuclphysb.2020.115001 · Cited by 5
The theory of black hole formation shares the Nobel Prize in Physics
Hill, H. M. (2020) · Physics Today · doi:10.1063/pt.3.4628 · Cited by 5
Refined inequalities for a loosely trapped surface and attractive gravity probe surface
Lee, K., Shiromizu, T., & Izumi, K. (2022) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.105.044037 · Cited by 5
The Dynamics of Spacetime Curvature: Nonlinear Aspects
Thorne, K. S. (1985) · Springer proceedings in physics · doi:10.1007/978-3-642-93289-2_11 · Cited by 5
On the geometry of trapped and marginally trapped submanifolds in Lorentzian space forms
de Lima, H. F., dos Santos, F. R., & Velásquez, M. A. L. (2015) · Communications in Contemporary Mathematics · doi:10.1142/s021919971550073x · Cited by 5
Restrictions on negative energy density for the Dirac field in flat spacetime
Wei-Xing, S., Yu, H., Fei, L., Wu, P., & Ren, Z. (2006) · Chinese Physics · doi:10.1088/1009-1963/15/5/011 · Cited by 5
SINGULARITY IN GRAVITATIONAL COLLAPSE OF PLANE SYMMETRIC CHARGED VAIDYA SPACETIME
Sharif, M., & Siddiqa, A. (2010) · Modern Physics Letters A · doi:10.1142/s0217732310033864 · Cited by 5
Consistency of the pulsating universe with Einstein’s field equations
Tangherlini, F. R. (1993) · Il Nuovo cimento della Società italiana di fisica. B/Il Nuovo cimento B · doi:10.1007/bf02828738 · Cited by 5
Violation of cosmic censorship in dynamical p -brane systems
Maeda, K., & Uzawa, K. (2016) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.93.044003 · Cited by 5
Hořava-Lifshitz bouncing Bianchi IX universes: A dynamical system analysis
Maier, R., & Soares, I. D. (2017) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.96.103532 · Cited by 6
Violation of the quantum null-energy condition in a holographic wormhole and infrared effects
Ishibashi, A., Maeda, K., & Mefford, E. (2019) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.99.026004 · Cited by 5
Theory of the classical gravitational field and Mach's principle
Логунов, А. А. (1994) · Theoretical and Mathematical Physics · doi:10.1007/bf01079252 · Cited by 5
Newtonian analysis of gravitational waves due to the formation of a naked singularity
Nakao, K.-I., Iguchi, H., & Harada, T. (2001) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.63.084003 · Cited by 5
Averaged energy conditions in 4D evaporating black hole backgrounds
Yu, H. (1998) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.58.064017 · Cited by 4
GRAVITATIONAL TUNNELLING OF RELATIVISTIC SHELLS
Ansoldi, S., & Sindoni, L. (2006) · Springer eBooks · doi:10.1007/1-4020-4339-2_11 · Cited by 5
Might black holes reveal their inner secrets?Preprint
Ted Jacobson, A., & Sotiriou, T. P. (2010) · arXiv (Cornell University) · doi:10.48550/arxiv.1006.1763 · Cited by 5
An Exploration of the Singularities in General RelativityPreprint
Stoica, O. C. (2012) · arXiv (Cornell University) · doi:10.48550/arxiv.1207.5303 · Cited by 5
Formation of Trapped Surfaces from Past Null InfinityPreprint
An, X. (2012) · arXiv (Cornell University) · doi:10.48550/arxiv.1207.5271 · Cited by 5
Gravitational Radiation from a Naked Singularity
Iguchi, H. (2000) · Institutional Repositories DataBase (IRDB) · doi:10.11501/3167089 · Cited by 5
Marginally trapped surfaces with pointwise 1-type Gauss map in Minkowski 4-spacePreprint
Milousheva, V. (2014) · arXiv (Cornell University) · doi:10.48550/arxiv.1410.6584 · Cited by 5
The Role of Metrics in the Theory of Partial Differential Equations
Giga, Y., Kubo, H., & Ozawa, T. (2020) · Advanced studies in pure mathematics · doi:10.2969/aspm/08510000 · Cited by 5
Semi-Riemannian Manifold OptimizationPreprint
Gao, T., Lim, L., & Ye, K. (2018) · arXiv (Cornell University) · doi:10.48550/arxiv.1812.07643 · Cited by 5
Reply to “Comment on ‘Quantum Raychaudhuri equation’”
Das, S. (2017) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.95.068502 · Cited by 5
Cosmology at the top of the α′ tower
Quintin, J., Bernardo, H., & Franzmann, G. (2021) · Journal of High Energy Physics · doi:10.1007/jhep07(2021)149 · Cited by 21
Hawking radiation and the quantum marginal problem
Aurell, E., Eckstein, M., & Horodecki, P. (2022) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2022/01/014 · Cited by 7
Non-topological soliton Bardeen boson stars and their frozen states
Zhao, Z., Gu, Y.-N., Liu, S.-C., Huang, L. Q., & Wang, Y. (2025) · The European Physical Journal C · doi:10.1140/epjc/s10052-025-14228-4 · Cited by 4
Generalizing Ayón-Beato–García black hole solutions to higher dimensions
Ezzaki, I., Lekbich, H., Boukili, A. E., Mansour, N., & Benami, A. (2025) · International Journal of Modern Physics A · doi:10.1142/s0217751x25501052 · Cited by 4
Can quantum gravity be both consistent and complete?
Faizal, M., Krauss, L. M., Shabir, A., Marino, F., & Pourhassan, B. (2025) · International Journal of Modern Physics D · doi:10.1142/s0218271825440171 · Cited by 7
Chakraborty, M., & Chakraborty, S. (2025) · Annals of Physics · doi:10.1016/j.aop.2025.170230 · Cited by 4
Geodesic completeness from string T-duality
Jusufi, K., & Nicolini, P. (2025) · The European Physical Journal C · doi:10.1140/epjc/s10052-025-15018-8 · Cited by 4
Hairy black holes via gravitational decoupling: Light rings, absorption and spectral lines
Ribeiro, G. P., Magalhães, R. B., & Crispino, L. C. B. (2025) · Physical review. D/Physical review. D. · doi:10.1103/lkgq-8zf5 · Cited by 4
Gravitational collapse: Generalizing Oppenheimer-Snyder and a conjecture on horizon formation time
Khodabakhshi, H., Lü, H., & Shojai, F. (2025) · Physical review. D/Physical review. D. · doi:10.1103/dhkq-w5pc · Cited by 4
General framework for the spontaneous scalarization of regular black holes
Contreras, E., Carrasco-Hidalgo, M., Bargueño, P., & Suvorov, A. G. (2025) · Physical review. D/Physical review. D. · doi:10.1103/9st9-ys67 · Cited by 4
Gulia, H., Singh, J. K., Atamurotov, F., & Ghosh, S. G. (2025) · Physics of the Dark Universe · doi:10.1016/j.dark.2025.102203 · Cited by 4
Errehymy, A., Khedif, Y., Mohammed Daoud, A., Myrzakulov, Y., Dönmez, O., & Turimov, B. (2026) · Physics Letters B · doi:10.1016/j.physletb.2026.140168 · Cited by 4
Thin-shell wormhole from modified Bardeen AdS black hole
Sarkar, B., Debnath, U., & Pradhan, A. (2026) · The European Physical Journal C · doi:10.1140/epjc/s10052-025-15249-9 · Cited by 4
Polarization images of solitonic boson stars
Zeng, X.-X., Yang, C.-Y., Yu, H., & He, K.-J. (2026) · The European Physical Journal C · doi:10.1140/epjc/s10052-026-15373-0 · Cited by 4
Babaei-Aghbolagh, H., Velni, K. B., He, S., & Isapour, F. (2026) · Physical review. D/Physical review. D. · doi:10.1103/zfc2-52md · Cited by 4
Zi, T., Li, P.-C., Gu, B.-M., & Shu, F.-W. (2026) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2026/04/077 · Cited by 4
Borissova, J. N., & Magueijo, J. (2026) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2026/07/045 · Cited by 13
Energy conditions in static, spherically symmetric spacetimes and effective geometries
Wang, Z.-L., & Battista, E. (2026) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2026/07/106 · Cited by 4
B, S. G. A., & Thébault, K. P. Y. (2023) · doi:10.1093/oso/9780198822066.001.0001 · Cited by 4
Yao, J.-T., Zhu, Q.-H., & Li, X. (2025) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.111.084083 · Cited by 4
Ahmed, F., Al‐Badawi, A., & Sakallı, İ. (2025) · Annalen der Physik · doi:10.1002/andp.202500087 · Cited by 4
Quasinormal modes and Hawking radiation of a non-minimal Einstein-Yang-Mills regular black hole
Ji, Y. Y. (2025) · Physica Scripta · doi:10.1088/1402-4896/adeede · Cited by 4
Why did the dark matter hypothesis supersede modified gravity in the 1980s?
Antoniou, A. (2025) · Studies in History and Philosophy of Science Part A · doi:10.1016/j.shpsa.2025.06.006 · Cited by 4
Ma, D., Huo, T., & Liu, C. (2025) · Nuclear Physics B · doi:10.1016/j.nuclphysb.2025.117077 · Cited by 4
Zhao, L., Tang, M., & Xu, Z. (2025) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2025/10/002 · Cited by 11
Mukuno, J.-I. (2015) · Differential Geometry and its Applications · doi:10.1016/j.difgeo.2015.04.002 · Cited by 4
Vasconcellos, C. A. Z. (2018) · WORLD SCIENTIFIC eBooks · doi:10.1142/11186 · Cited by 4
Persistence in black hole lattice cosmological models
Coley, A. A. (2020) · Classical and Quantum Gravity · doi:10.1088/1361-6382/abbf31 · Cited by 4
Samuel, J. (2021) · Resonance · doi:10.1007/s12045-020-1104-x · Cited by 4
Implications of the singularity theorem for the size of a nonsingular universe
Nomura, K., & Yoshida, D. (2022) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.106.124016 · Cited by 4
Metadata
- Authors
- Penrose, R.
- Affiliations
- Birkbeck, University of London (GB)
- Corresponding author
- Penrose, Roger
- Venue
- Physical Review Letters
- Publisher
- American Physical Society (APS)
- Published
- 1965-01-18
- Volume
- 14
- Issue
- 3
- Pages
- 57-59
- ISSN
- 0031-9007 (ISSN-L)
- OpenAlex
- W2052045615
- Semantic Scholar
- 16e21b5e29346e9413274a9051c44888943c274a
- Cited by
- 2,977
- References
- 11
- Citations by year
- 2026: 270 · 2025: 357 · 2024: 300 · 2023: 277 · 2022: 173 · 2021: 202 · 2020: 148 · 2019: 165 · 2018: 108 · 2017: 93 · 2016: 82 · 2015: 69 · 2014: 55 · 2013: 49 · 2012: 36
- FWCI
- 16.61
- Type
- journal article
- Language
- en
- Open access
- bronze
- doi.org
- Locations
- Physical Review Letters (publishedVersion)
- Topics
- Physical Sciences › Physics and Astronomy › Astronomy and Astrophysics › Relativity and Gravitational Theory
- Physical Sciences › Physics and Astronomy › Astronomy and Astrophysics › Cosmology and Gravitation Theories
- Physical Sciences › Physics and Astronomy › Nuclear and High Energy Physics › Black Holes and Theoretical Physics
- Keywords
- gravitational collapse, spacetime singularities, blast wave, cosmic ray observation
About these checks
Registry, retraction, Cites and statistics results are computed, not judged, with one exception: a printed reference that no index lists is read once by a model before it counts as a citation error. Claims are extracted by a model and kept only when their quote appears verbatim in the text; each cited source is then checked, with a model’s help, for whether it says what the claim relies on. Those verdicts can be wrong — read the claim’s quote and the cited source before relying on one.
A language model drew the claims from the paper on 2026-10-30, under version 3 of the claim definition (model deepseek-v4.1-flash, prompt extract-v3).
A second model labelled each claim on 2026-10-30 (model jev-1.13-20260917, definition revision gold-guideline-v0.2).
Statistics and arithmetic are recomputed, not judged.
Confidence bands are shown only for fields calibrated on our annotated test set. None is calibrated yet, so no band is shown.
What counts as a claim ›How we measure confidence ›How we check this ›
Are you an author, or do you see a problem with this page? Request a review