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 2,901–2,958 of 2,958
Holographic dark energy with quantum decoherence: a conservative cosmological model
Salih, M. A. (2026) · Indian Journal of Physics · doi:10.1007/s12648-026-04135-z
Chakraborty, M. (2026) · Modern Physics Letters A · doi:10.1142/s0217732326502226
Screened Simpson–Visser black holes with asymptotically de Sitter core
Ahmed, F., Al‐Badawi, A., & Silva, E. O. (2026) · Annals of Physics · doi:10.1016/j.aop.2026.170648
A modified gravitational theory of the matter sector of the type $$\phi (R,T)\mathcal {L}_{m}$$
Teruel, G. R. P., & PEÑA, A. P. (2026) · The European Physical Journal Plus · doi:10.1140/epjp/s13360-026-08103-8
Singh, J. P., & Jaswant (2026) · The European Physical Journal C · doi:10.1140/epjc/s10052-026-16321-8
Shaukat, S., Waseem, A., Javed, F., Gul, M. Z., Rayimbaev, J., Sirajiddin, O., & Rahmatov, B. (2026) · Annals of Physics · doi:10.1016/j.aop.2026.170659
Gravitational-Wave Echoes from a Hayward Black Hole under Minimal Geometric Deformation
Farooq, O. (2026) · International Journal of Theoretical Physics · doi:10.1007/s10773-026-06417-y
Matter-Only Cosmology: A Unified Origin for Inflation and Dark EnergyPreprint
Choi, H. (2026) · SSRN Electronic Journal · doi:10.2139/ssrn.6804638
Gauge-covariant Raychaudhuri dynamics for spin-nondegenerate Lorentz-violating congruences
Filho, A. A. A., Santos, A. F., Reis, J. A. A. S., Lisboa-Santos, L., & Bezerra, V. B. (2026) · The European Physical Journal C · doi:10.1140/epjc/s10052-026-16150-9
On the role of the Weyl tensor within the framework of Einstein-Cartan's theory
Cardoso, J. G. (2026) · Europhysics Letters (EPL) · doi:10.1209/0295-5075/ae933b
Black Hole Singularity and the Fate of Black Holes
Lin, K.-N. (2026) · Springer theses · doi:10.1007/978-981-95-8719-3_4
Pradhan, A., Ghaderi, K., & Zeyauddin, M. (2026) · Chinese Journal of Physics · doi:10.1016/j.cjph.2026.07.049
Wuebben, B. J. (2026) · SSRN Electronic Journal · doi:10.2139/ssrn.7151179
Geometrically significant surfaces of black holes from a single scalar
Anonymous, & Tekin, B. (2026) · Physical review. D/Physical review. D. · doi:10.1103/rz6d-3yj8
Signatures of greybody factor for a black hole coupled with the electromagnetic field
Naseer, T., Sharif, M., & Raza, A. (2026) · Annals of Physics · doi:10.1016/j.aop.2026.170658
Filho, A. A. A., Kumar, A., Heidari, N., Pereira, C. F. S., de Queiroz, A. R., & Bezerra, V. B. (2026) · Physics of the Dark Universe · doi:10.1016/j.dark.2026.102420
Mehmood, A., Alkaoud, A., Shahzad, M. U., Rafiq, R., Sultan, A. M., & Eid, A. (2026) · General Relativity and Gravitation · doi:10.1007/s10714-026-03597-0
Gulomov, A., Atamurotov, F., Abdujabbarov, A., Khan, I., & Yuan, C. (2026) · The European Physical Journal Plus · doi:10.1140/epjp/s13360-026-08123-4
Singularity Regularization and the Emergent Planck Scale in the Logarithmic Superfluid VacuumPreprint
Kulangiev, B. (2026) · Qeios · doi:10.32388/2dou67.3
Cosmic inflation from regular black holes
Anonymous, Yoshimoto, R., & Cano, P. A. (2026) · Physical review. D/Physical review. D. · doi:10.1103/3cy6-p27c
A generalized class of Taub-NUT-scalar metrics
Bakherad, F., Mirza, B., Bahani, R., Kachi, M. T., & Derekeh, A. (2026) · Annals of Physics · doi:10.1016/j.aop.2026.170673
Smooth Cores to Sharp Cusps in Complexity-free Regular Wormhole Geometries
Ganesan, T., Abdalgadir, L. M., Rizwan, M., Mahmoud, H. M. A., Bhatti, M. Z., & Yousaf, Z. (2026) · Chinese Journal of Physics · doi:10.1016/j.cjph.2026.08.011
Kaykı, D., Yildiz, L., & Güdekli, E. (2026) · The European Physical Journal Plus · doi:10.1140/epjp/s13360-026-08155-w
Decoding the greybody factor and potential barriers in a static black hole with quantum corrections
Sharif, M., Naseer, T., & Raza, A. (2026) · The European Physical Journal C · doi:10.1140/epjc/s10052-026-16248-0
On the Complementarity of the Speed of Light and Gravitational SingularitiesPreprint
Radcliffe, B. K. (2026) · SSRN Electronic Journal · doi:10.2139/ssrn.7308660
Regular black holes violating the GHP strong cosmic censorship hypothesis
Fenoll, D., & Bargueño, P. (2026) · Physics Letters B · doi:10.1016/j.physletb.2026.140887
Spherically symmetric quintessential black holes in antisymmetric tensor gravity
Al‐Badawi, A., Ahmed, F., & Sakallı, İ. (2026) · The European Physical Journal Plus · doi:10.1140/epjp/s13360-026-08189-0
Faizal, M., & Shabir, A. (2026) · Metaphysica · doi:10.1515/mp-2026-0028
A Way to Complete General Relativity
Mardan, S. A., & Steinvorth, R. (2026) · Scientific Inquiry and Review · doi:10.32350/sir.101.01
Interior evolution of regular Schwarzschild black holes
Ovalle, J. (2026) · Physics Letters B · doi:10.1016/j.physletb.2026.140912
Can finite-density QCD matter support a regular black-hole core?
Lambiase, G., Övgün, A., & Vertogradov, V. (2026) · Journal of Cosmology and Astroparticle Physics · doi:10.1088/1475-7516/2026/09/029
Gulia, H., Singh, J. K., & Ghosh, S. G. (2026) · Physics of the Dark Universe · doi:10.1016/j.dark.2026.102454
Exact d’Alembertian for Lorentz distance functions
Braun, M. (2026) · Calculus of Variations and Partial Differential Equations · doi:10.1007/s00526-026-03429-8
CHAPTER 9: NUCLEAR FUSION ENERGY
Singal, R. K., & Tabatabaian, M. (2019) · De Gruyter eBooks · doi:10.1515/9781683924548-009
Pradhan, A., Ghaderi, K., Zeyauddin, M., & Kumar, A. (2026) · Modern Physics Letters A · doi:10.1142/s0217732326502561
Regular black holes from anisotropic source with hydrodynamic equation of state
Anonymous (2026) · Physical review. D/Physical review. D. · doi:10.1103/v97v-2z4h
Power‐Law Cosmology in Non‐Minimally Coupled f(Q,LM) Gravity: Misner–Sharp Thermodynamic Analysis
Singh, J. K., Aggarwal, S., Sangeeta, Sahoo, P. K., & Pawar, D. D. (2026) · Annalen der Physik · doi:10.1002/andp.70297
Oscillatory Spacelike Singularities: The Bianchi Type $$\textrm{VI}_{-1/9}$$ Vacuum Models
Lappicy, P., & Uggla, C. (2026) · Annales Henri Poincaré · doi:10.1007/s00023-026-01744-6
Geodesic congruences and stability of spacetimes with specifically warped extra dimension
Gayen, P., & Koley, R. (2026) · General Relativity and Gravitation · doi:10.1007/s10714-026-03612-4
Untraversable by Construction: Three Pathologies of Wormhole Physics as One Threshold LawPreprint
Zhong, J. (2026) · SSRN Electronic Journal · doi:10.2139/ssrn.7476460
Jarra, I., Bolle, R. M., Furst, B. R., Conroy, J. M., & Secrest, J. A. (2026) · Universe · doi:10.3390/universe12100288
Anonymous, Giesel, K., & Rullit, E. (2026) · Physical review. D/Physical review. D. · doi:10.1103/5nry-t25l
Scale-invariant non-collapse from Raychaudhuri comparison
Dhormare, R. (2026) · Physics Letters B · doi:10.1016/j.physletb.2026.140987
Null Rigidity and Wave-Sector Reduction of Conformally Deformed Black Holes
Alshehri, A. A. (2026) · Universe · doi:10.3390/universe12100292
Errehymy, A., Khedif, Y., Mohammed Daoud, A., Turimov, B., Usanov, S., Yasakov, Z., & Turaev, F. (2026) · Physics Letters B · doi:10.1016/j.physletb.2026.141015
The Time Horizon: Tempodynamics as a Unified Ontology of the Time FieldPreprint
Raum, A. (2026) · doi:10.24108/preprints-3116561
Censura cósmica más allá de los agujeros negros: singularidades ocultas sin horizonte
Bixano, L. D. L. C., & Matos, T. (2026) · EPISTEMUS · doi:10.36790/epistemus.v20.510
Beckwith, A. W. (2026) · Journal of High Energy Physics Gravitation and Cosmology · doi:10.4236/jhepgc.2026.124111
Photon Dynamics and Frequency Shift in a Regular Magnetic Black Hole
Komilov, U. (2026) · Turanian Journal · doi:10.65910/turanianj.020305
Do frozars exist? Coordinate time, proper time and the formation of black-hole horizons
Toshmatov, B., Isamadinova, N., & Boydedayev, A. (2026) · Turanian Journal · doi:10.65910/turanianj.020206
CONTROLLED VACUUM PHASE TRANSITION AND ENERGY EXTRACTION FROM DISSIPATIVE STRUCTUREPreprint
Nitsberg, M. (2026) · doi:10.24108/preprints-3116661
Bounce Solutions with Quantum Vacuum Effects of Massive Fields and Subsequent Starobinsky Inflation
Silva, W. C. E., Oliveira, S. W. P., & Shapiro, I. L. (2026) · Fundamental theories of physics · doi:10.1007/978-3-032-15703-4_6
Free Particles and Light Rays as Basic Elements of General Relativity
Pfister, H., & King, M. (2014) · Lecture notes in physics · doi:10.1007/978-3-319-15036-9_2
Aspects of higher dimensional Einstein theory and M-theory
Godazgar, M. (2012) · Apollo (University of Cambridge) · doi:10.17863/cam.16128
RECENT DEVELOPMENTS IN NONLINEAR HYPERBOLIC PDE
Christodoulou, D. (2001) · Journal of the Korean Mathematical Society
Hawking radiation in NS5 and little string theory
Lorente-Espín, O. (2012) · doi:10.5821/dissertation-2117-94690
Pfister, H., & King, M. (2014) · Lecture notes in physics · doi:10.1007/978-3-319-15036-9_3
Merger Timescales in Hierarchical Triple Black Hole Systems
Lam, H. H. (2013) · Utrecht University Repository (Utrecht University)
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