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
0 of 2 cited sources checked · 0 supported · 0 flagged
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
Tests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes✓ Based: passesThe 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
Tests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes✓ Based: passes- 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
Tests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes✓ Based: passes- 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
Tests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes✓ Based: passes- 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
Strength:hedged· not yet calibratedCausal:direct· not yet calibratedTests✓ Asserted: passes✓ Checkable: passes? Load-bearing: unclear? Based: unclearA 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
Tests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes✓ Based: passes- 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
Load-bearingStrength:boosted· not yet calibratedTests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes✓ Based: passes- 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
Tests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes? Based: unclearA 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
Load-bearingStrength:plain· not yet calibratedTests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes✓ Based: passesIn 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.
Load-bearingStrength:plain· not yet calibratedTests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes✓ Based: passes- 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
Tests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes✓ Based: passesIt 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
Load-bearingStrength:plain· not yet calibratedTests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes✓ Based: passesProbably 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
Tests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes✓ Based: passesThe 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
Tests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes? Based: unclearIt 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
Load-bearingStrength:plain· not yet calibratedTests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes✓ Based: passesThe 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
Tests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes✓ Based: passesIt 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
Load-bearingStrength:plain· not yet calibratedTests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes✓ Based: passesIt 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
Tests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes✓ Based: passesIt 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.
Tests✓ Asserted: passes✓ Checkable: passes✓ Load-bearing: passes✓ Based: passesIt 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
Flagged first, then by citations
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 1,001–1,100 of 2,958
Destroying charged black holes in higher dimensions with test particles
Wu, B., Liu, W.-Y., Tang, H., & Yue, R. (2017) · International Journal of Modern Physics A · doi:10.1142/s0217751x17501251 · Cited by 13
The Singularity Problem of Gravitation
Fuchs, H., Kasper, U., Liebscher, D. E., Müller, V., & Schmidt, H. (1988) · Fortschritte der Physik/Progress of Physics · doi:10.1002/prop.2190360603 · Cited by 12
An exact tilted Bianchi II cosmology
Hewitt, C. G. (1991) · Classical and Quantum Gravity · doi:10.1088/0264-9381/8/5/004 · Cited by 13
Numerical modeling of black holes as sources of gravitational waves in a nutshell
Husa, S. (2007) · The European Physical Journal Special Topics · doi:10.1140/epjst/e2007-00381-6 · Cited by 13
The Kähler cone as cosmic censor
Mayer, C., & Thomas Mohaupt, A. (2004) · Classical and Quantum Gravity · doi:10.1088/0264-9381/21/7/010 · Cited by 13
Singularity free dilaton-driven cosmologies and pre-little-bangs
Massimo Giovannini, A. (1999) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.59.083511 · Cited by 13
Compact astrophysical objects in modified gravityPreprint
Lehébel, A. (2018) · arXiv (Cornell University) · doi:10.48550/arxiv.1810.04434 · Cited by 18
Imprints of holographic dark energy and minimally deformed wormholes in general relativity
Alshammari, M., Rizwan, M., Almatroud, O. A., Bhatti, M. Z., Alshammari, S., & Yousaf, Z. (2026) · Physics of the Dark Universe · doi:10.1016/j.dark.2026.102219 · Cited by 12
Zare, S., Zhu, T., Nieto, L. M., Lu, S., & HASSANABADI, H. (2026) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2026/01/059 · Cited by 12
Gravitational collapse of quantum fields and Choptuik scaling
Berczi, B., Saffin, P. M., & Zhou, S.-Y. (2022) · Journal of High Energy Physics · doi:10.1007/jhep02(2022)183 · Cited by 12
Deciphering signatures of Bardeen black holes from the observed quasi-periodic oscillations
Banerjee, I. (2022) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2022/05/020 · Cited by 12
Bound orbits around charged black strings
Habibina, A. S., & Ramadhan, H. S. (2022) · Annals of Physics · doi:10.1016/j.aop.2022.169169 · Cited by 12
Irrefutable Proof of The Non-Existence of a Gravitational Singularity at The Centre of a Black Hole
Šorli, A. (2023) · International Journal of Fundamental Physical Sciences · doi:10.14331/ijfps.2023.330156 · Cited by 12
Energy nonconservation and relativistic trajectories: Unimodular gravity and beyond
Bonder, Y., Herrera, J. E., & Rubiol, A. M. (2023) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.107.084032 · Cited by 13
Black Holes as Frozen Stars: Regular Interior Geometry
Brustein, R., Medved, A. J. M., Shindelman, T., & Simhon, T. (2023) · Fortschritte der Physik · doi:10.1002/prop.202300188 · Cited by 12
Tawfik, A. N., & Dabash, T. F. (2023) · International Journal of Modern Physics D · doi:10.1142/s0218271823500979 · Cited by 12
Entanglement entropy for spherically symmetric regular black holes
Luongo, O., Mancini, S., & Pierosara, P. (2023) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.108.104059 · Cited by 12
The inheritance of energy conditions: Revisiting no-go theorems in string compactifications
Bernardo, H., Brahma, S., & Faruk, M. M. (2023) · SciPost Physics · doi:10.21468/scipostphys.15.6.225 · Cited by 12
Geodesic Structure of Generalized Vaidya Spacetime through the K-Essence
Majumder, B., Khlopov, M., Ray, S., & Manna, G. (2023) · Universe · doi:10.3390/universe9120510 · Cited by 12
Accretion disk around regular black holes
Akbarieh, A. R., Khoshragbaf, M., & Atazadeh, M. (2024) · International Journal of Geometric Methods in Modern Physics · doi:10.1142/s0219887824503237 · Cited by 12
Escrivà, A., Tada, Y., & Yoo, C. (2024) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.110.063521 · Cited by 17
Power law cosmology in modified theory with thermodynamics analysis
Singh, J. K., Shaily, Pradhan, A., & Beesham, A. (2024) · Physics of the Dark Universe · doi:10.1016/j.dark.2024.101658 · Cited by 13
Yang, X., Tang, M., & Xu, Z. (2024) · The European Physical Journal C · doi:10.1140/epjc/s10052-024-13343-y · Cited by 12
Generalized symmetry in dynamical gravity
Cheung, C., Derda, M., Kim, J.-H., Nevoa, V., Rothstein, I. Z., & Shah, N. (2024) · Journal of High Energy Physics · doi:10.1007/jhep10(2024)007 · Cited by 12
Anchordoqui, L. A., Ignatios Antoniadis, A., Lüst, D., & Castillo, K. P. (2024) · Physics of the Dark Universe · doi:10.1016/j.dark.2024.101681 · Cited by 13
Shadow of a renormalization group improved rotating black hole
Sánchez, L. A. (2024) · The European Physical Journal C · doi:10.1140/epjc/s10052-024-13398-x · Cited by 12
Filippo, F. D. (2024) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.110.084026 · Cited by 25
Strong gravitational lensing by Bardeen black hole in cloud of strings
Vishvakarma, B. K., Kala, S., & Siwach, S. (2025) · Annals of Physics · doi:10.1016/j.aop.2025.169957 · Cited by 12
Harada, T., Chen, C.-M., & Mandal, R. (2025) · Physical review. D/Physical review. D. · doi:10.1103/pt9s-jqjz · Cited by 12
Spherically symmetric analytic solutions and naked singularities in Einstein–Aether theory
Chan, R., da Silva, M. F. A., & Satheeshkumar, V. H. (2021) · The European Physical Journal C · doi:10.1140/epjc/s10052-021-09120-w · Cited by 12
Holography abhors visible trapped surfaces
Engelhardt, N., & Folkestad, Å. (2021) · Journal of High Energy Physics · doi:10.1007/jhep07(2021)066 · Cited by 11
Geometry near the inner horizon of a rotating, accreting black hole
McMaken, T., & Hamilton, A. J. S. (2021) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.103.084014 · Cited by 12
The thermodynamics of black holes: from Penrose process to Hawking radiation
Almeida, C. R. (2021) · The European Physical Journal H · doi:10.1140/epjh/s13129-021-00022-9 · Cited by 12
Semiclassical black holes and horizon singularities
Dahal, P. K., Murk, S., & Terno, D. R. (2022) · AVS Quantum Science · doi:10.1116/5.0073598 · Cited by 12
The double smeared null energy condition
Fliss, J. R., Freivogel, B., & Kontou, E.-A. (2023) · SciPost Physics · doi:10.21468/scipostphys.14.2.024 · Cited by 12
Identifying Riemannian Singularities with Regular Non-Riemannian Geometry
Morand, K., Park, J.-H., & Park, M. (2022) · Physical Review Letters · doi:10.1103/physrevlett.128.041602 · Cited by 12
Is “dark energy” a quantum vacuum energy?
Adler, S. L. (2021) · Modern Physics Letters A · doi:10.1142/s0217732321300275 · Cited by 14
Shaymatov, S., & Ahmedov, B. J. (2023) · General Relativity and Gravitation · doi:10.1007/s10714-023-03082-y · Cited by 12
Asymptotically flat vacuum solutions in order-reduced semiclassical gravity
Arrechea, J., Barceló, C., Carballo-Rubio, R., & Garay, L. J. (2023) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.107.085005 · Cited by 13
Gómez, G., & Rodríguez, J. F. (2023) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.108.024069 · Cited by 15
Gravito-electromagnetic perturbations and QNMs of regular black holes
Meng, K., & Zhang, S.-J. (2023) · Classical and Quantum Gravity · doi:10.1088/1361-6382/acf3c6 · Cited by 12
Geodetic precession and shadow of quantum extended black holes
Saadati, R., & Shojai, F. (2023) · Classical and Quantum Gravity · doi:10.1088/1361-6382/ad13c3 · Cited by 12
The Ultimate Question of Origins: God and the Beginning of the Universe
Craig, W. L. (1999) · Astrophysics and Space Science · doi:10.1023/a:1017083700096 · Cited by 13
Chen, B. (2010) · Kyushu Journal of Mathematics · doi:10.2206/kyushujm.64.261 · Cited by 12
Quantum interest in two dimensions
Teo, E., & Wong, K. F. (2002) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.66.064007 · Cited by 12
Is general relativity ‘essentially understood’?
Friedrich, H. (2005) · Annalen der Physik · doi:10.1002/andp.200510173 · Cited by 19
Simple regular black hole with logarithmic entropy correction
Morales-Durán, N., Vargas, A. F., Restrepo, P. H., & Bargueño, P. (2016) · The European Physical Journal C · doi:10.1140/epjc/s10052-016-4417-x · Cited by 12
Resolving the Schwarzschild singularity in both classic and quantum gravity
Zeng, D.-F. (2017) · Nuclear Physics B · doi:10.1016/j.nuclphysb.2017.02.005 · Cited by 12
Anomalous Galactic Dynamics by Collusion of Rindler and Cosmological Horizons
van Putten, M. H. P. M. (2017) · The Astrophysical Journal · doi:10.3847/1538-4357/aa5da9 · Cited by 12
Spectroscopy of quantum-corrected Schwarzschild black hole
Shahjalal, M. (2019) · Nuclear Physics B · doi:10.1016/j.nuclphysb.2019.01.010 · Cited by 12
A gravitational collapse singularity theorem consistent with black hole evaporation
Minguzzi, E. (2020) · Letters in Mathematical Physics · doi:10.1007/s11005-020-01295-9 · Cited by 12
Hu, S.-Q., Liu, B., Kuang, X.-M., & Yue, R.-H. (2020) · Chinese Physics C · doi:10.1088/1674-1137/abab8a · Cited by 12
Scalar hairy black holes in the presence of nonlinear electrodynamics
Tahamtan, T. (2020) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.101.124023 · Cited by 12
A generalized form of the Raychaudhuri equation
Bhattacharyya, I., & Ray, S. (2021) · International Journal of Modern Physics D · doi:10.1142/s0218271821500929 · Cited by 12
Gaiseanu, F. (2021) · Philosophy study · doi:10.17265/2159-5313/2021.08.003 · Cited by 12
Dyonically charged black holes arising in generalized Born–Infeld theory of electromagnetism
Yang, Y. (2022) · Annals of Physics · doi:10.1016/j.aop.2022.168996 · Cited by 12
Classification of Lorentzian surfaces with parallel mean curvature vector in pseudo-Euclidean spaces
Fu, Y., & Hou, Z. (2010) · Journal of Mathematical Analysis and Applications · doi:10.1016/j.jmaa.2010.04.022 · Cited by 12
Singularity, initial conditions, quantum tunneling and scalar field in modern cosmology
Khalatnikov, I. M., & Kamenshchik, A. Y. (1997) · Physics Reports · doi:10.1016/s0370-1573(97)00039-2 · Cited by 12
John Jungkeun, O. H., & Chanyong Park, B. (2010) · Journal of High Energy Physics · doi:10.1007/jhep03(2010)086 · Cited by 12
The theory of the classical gravitational field
Логунов, А. А. (1995) · Physics-Uspekhi · doi:10.1070/pu1995v038n02abeh000070 · Cited by 12
Semiclassical collapse with tachyon field and barotropic fluid
Tavakoli, Y., Marto, J., Ziaie, A. H., & Moniz, P. V. (2013) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.87.024042 · Cited by 12
Weak and strong sources of gravity: An SO(1,3)-gauge theory of gravity
Camenzind, M. (1978) · Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields · doi:10.1103/physrevd.18.1068 · Cited by 12
Globally regular solutions of a schwarzschild black hole and a Reissner-Nordstr�m black hole
WEN-DA, S., & SHI-TONG, Z. (1985) · General Relativity and Gravitation · doi:10.1007/bf00762623 · Cited by 12
On the initial value problem in general relativity and wave propagation in black-hole spacetimes
Sbierski, J. (2014) · Apollo (University of Cambridge) · doi:10.17863/cam.16140 · Cited by 12
Causal anomalies in the extended Schwarzschild manifold
Israel, W. (1966) · Physics Letters · doi:10.1016/0031-9163(66)91336-9 · Cited by 12
Singularities in general relativity
Pachner, J. (1971) · General Relativity and Gravitation · doi:10.1007/bf00759539 · Cited by 12
Gravitational waves from regular black holes in extreme mass-ratio inspirals
Kumar, S., & Zi, T. (2025) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2025/10/108 · Cited by 11
Through a black hole into a new universe
Brandenberger, R., Heisenberg, L., & Robnik, J. (2021) · International Journal of Modern Physics D · doi:10.1142/s0218271821420013 · Cited by 11
On black hole thermodynamics, singularity, and gravitational entropy
Ong, Y. C. (2022) · General Relativity and Gravitation · doi:10.1007/s10714-022-03008-0 · Cited by 13
Gravitational collapse of scalar and vector fields
Mosani, K., Koushiki, Joshi, P. S., Trivedi, J. V., & Bhanja, T. (2023) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.108.044049 · Cited by 11
Stress-energy tensor correlations across regular black holes horizons
Fontana, M., & Rinaldi, M. (2023) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.108.125003 · Cited by 13
Kinematic and energy properties of dynamical regular black holes
Murk, S., & Soranidis, I. (2023) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.108.124007 · Cited by 13
A Synthetic Null Energy Condition
McCann, R. J. (2024) · Communications in Mathematical Physics · doi:10.1007/s00220-023-04908-1 · Cited by 11
Raychaudhuri equation and the dynamics of cosmic evolution
Chakraborty, M., & Chakraborty, S. (2024) · Physica Scripta · doi:10.1088/1402-4896/ad2c4c · Cited by 11
Universality on thermodynamic relation with corrections in de Sitter black holes
Ko, J., & Gwak, B. (2024) · Journal of High Energy Physics · doi:10.1007/jhep03(2024)072 · Cited by 11
Observational appearances of hairy black holes in the framework of gravitational decoupling
Liang, Y., Lyu, X., & Tao, J. (2024) · Communications in Theoretical Physics · doi:10.1088/1572-9494/ad4ce0 · Cited by 11
Quantum nature of spacetime near the black hole singularity
Singh, H., & Nandy, M. K. (2024) · The European Physical Journal C · doi:10.1140/epjc/s10052-024-13041-9 · Cited by 11
Xie, Y., Chatterjee, D., Narayan, G., & Yunes, N. (2024) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.110.024036 · Cited by 19
Spherically symmetric configurations in the quadratic f ( R ) gravity
Zhdanov, V. I., Stashko, O. S., & Shtanov, Y. (2024) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.110.024056 · Cited by 11
Cosmology from Schwarzschild black hole revisited
Roberto Casadio, A., Kamenshchik, A. Y., & Ovalle, J. (2024) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.110.044001 · Cited by 11
Classical and quantum analysis of gravitational singularity from Raychaudhuri equation
Chakraborty, M., & Chakraborty, M. (2024) · Physics Letters A · doi:10.1016/j.physleta.2024.129883 · Cited by 11
Implications of Tarski's undefinability theorem on the Theory of Everything
Faizal, M., Shabir, A., & Khan, A. K. (2024) · Europhysics Letters (EPL) · doi:10.1209/0295-5075/ad80c2 · Cited by 11
Charged gravastar model in noncommutative geometry under f(T) gravity
Mohanty, D., Ghosh, S., & Sahoo, P. K. (2024) · Physics of the Dark Universe · doi:10.1016/j.dark.2024.101692 · Cited by 11
Exploring Tsallis thermodynamics for boundary conformal field theories in gauge/gravity duality
Sekhmani, Y., Luciano, G. G., Maurya, S. K., Rayimbaev, J., Pourhassan, B., Jasim, M. K., & Rincón, Á. (2024) · Chinese Journal of Physics · doi:10.1016/j.cjph.2024.10.015 · Cited by 11
Faizal, M., Shabir, A., & Khan, A. K. (2024) · Nuclear Physics B · doi:10.1016/j.nuclphysb.2024.116774 · Cited by 11
Non-isometry, state dependence and holography
Antonini, S., Balasubramanian, V., Bao, N., Cao, C., & Chemissany, W. A. (2025) · Journal of High Energy Physics · doi:10.1007/jhep02(2025)150 · Cited by 12
Felice, A. D., & Tsujikawa, S. (2025) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.111.064051 · Cited by 11
Are regular black holes from pure gravity classified within the same thermodynamical topology?
Wang, S., Wu, S.-P., & Wei, S.-W. (2025) · Physics Letters B · doi:10.1016/j.physletb.2025.139402 · Cited by 11
Liu, H., & Yunes, N. (2025) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.111.084049 · Cited by 21
Shadows aspect of rotating black holes in the Einstein-AdS SU(N)-nonlinear sigma model
Fathi, M., & Sekhmani, Y. (2025) · The European Physical Journal C · doi:10.1140/epjc/s10052-025-14153-6 · Cited by 11
Could planck star remnants be dark matter?
Trivedi, O., & Loeb, A. (2025) · Physics of the Dark Universe · doi:10.1016/j.dark.2025.102003 · Cited by 11
Easson, D. A., & Lesnefsky, J. E. (2025) · Physical review. D/Physical review. D. · doi:10.1103/5mhz-m8bg · Cited by 20
Cisterna, A., Hassaı̈ne, M., & Hernandez-Vera, U. (2025) · Physical review. D/Physical review. D. · doi:10.1103/6f3b-8794 · Cited by 11
Unified Field Theory and the Hierarchical Universe
Cao, Z., & Cao, H. G. (2013) · The International Journal of Physics · doi:10.12691/ijp-1-6-5 · Cited by 12
Towards wormhole beyond Horndeski
Mironov, S. A., Rubakov, V. A., & Volkova, V. E. (2018) · EPJ Web of Conferences · doi:10.1051/epjconf/201819107014 · Cited by 11
Singularity theorems and the inclusion of torsion in affine theories of gravity
Luz, P., & Mena, F. C. (2020) · Journal of Mathematical Physics · doi:10.1063/1.5126220 · Cited by 16
Nonsingular black holes and nonsingular universes in the regularized Lovelock gravity
Gao, C., Yu, S., & Qiu, J. (2020) · Physics of the Dark Universe · doi:10.1016/j.dark.2020.100754 · Cited by 11
Thermodynamic geometry of static and rotating regular black holes in conformal massive gravity
Soroushfar, S., Saffari, R., Abebe, A., & Sheikhahmadi, H. (2021) · The European Physical Journal Plus · doi:10.1140/epjp/s13360-021-02236-8 · Cited by 11
Introduction to Hamiltonian formulation of general relativity and homogeneous cosmologies
Jha, R. (2023) · SciPost Physics Lecture Notes · doi:10.21468/scipostphyslectnotes.73 · Cited by 17
Defrosting frozen stars: Spectrum of internal fluid modes
Brustein, R., Medved, A. J. M., & Shindelman, T. (2023) · Physical review. D/Physical review. D. · doi:10.1103/physrevd.108.044058 · Cited by 11
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