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arxiv: 2509.08054 · v1 · submitted 2025-09-09 · 🌀 gr-qc · astro-ph.HE

Recognition: no theorem link

GW250114: testing Hawking's area law and the Kerr nature of black holes

A. Agapito, A. Ain, A. Allocca, A. Amato, A. Ananyeva, A. Araya, A. Basalaev, A. Basti, A. Bertolini, A. Bianchi, A. Binetti, A. Bisht, A. B. Nielsen, A. Bolliand, A. Bonino, A. Borchers, A. Boudon, A. Bozzi, A. Branch, A. Brillet, A. Buonanno, A. B. Yelikar, A. B. Zimmerman, A. Calafat, A. Casallas-Lagos, A. C. Baylor, A. Ceja, A. C. Green, A. Chakraborty, Achal Kumar, A. Chen, A. Chiba, A. Chincarini, A. Chiummo, A. Colombo, A. Corsi, A. Couineaux, A. Cozzumbo, A. C. Providence, A. Cumming, A. Dasgupta, A. Daumas, A. Davenport, A. Demagny, A. Depasse, A. DeSimone, A. Dhani, A. D. Huddart, A. Dmitriev, A. Doke, A. Domiciano De Souza, A. D. Viets, A. Effler, A. E. Granados, A. E. Koloniari, A. E. Pace, A. E. Romano, A. E. Tolley, A. F. Brooks, A. F. Helmling-Cornell, A. Fiori, A. Freise, A. F. Vargas, A. Gamboa, A. Ganguly, A. Garron, A. Gennai, A. G. Hanselman, A. Grado, A. H. Laity, A. H.-Y. Chen, A. Ierardi, A. I. Renzini, A. Jennings, A. J. Weinstein, A. K. H. Kong, A.-K. Malz, A. Kontos, A. Koushik, A. K. Prajapati, A. Kr\'olak, A. K. Sharma, A. K. Srivastava, A. Kulur Ramamohan, A. K. Y. Li, A. Lartaux-Vollard, A. Lazzarini, A. Lema\^itre, A. L. Hewitt, A. Lihos, A. Liu, A. L. James, A. L. Mitchell, A. Longo, A. Lorenzo-Medina, A. L. Stuver, A. Macquet, A. Malik, A. Markowitz, A. Martini, A. Masserot, A. M. Baker, A. M. Bartoletti, A. McLeod, A. Melatos, A. M. Farah, A. M. Gretarsson, A. Mhaske, A. Miani, A. Mishra, Amitesh Singh, A. Miyoko, A. M. Knee, A. More, A. Moreso Serra, A. Moscatello, A. M. Sintes, A. M. Toivonen, A. Mullavey, A. Nagar, A. Nela, A. Nelson, A. Neunzert, Anika Singh, Anil Kumar, A. Nishizawa, Anuradha Gupta, A. N. Vazquez, A. Ouzriat, A. Pai, A. Pal, A. Paolone, A. Papadopoulos, A. Paquis, A. Parisi, A. Pasqualetti, A. Patra, A. Pele, A. Perego, A. Perreca, A. Placidi, A. P. Lundgren, A. P. Spencer, A. Puecher, A. Ramos-Buades, A. Ravichandran, A. Ray, Archisman Ghosh, A. Revilla Pe\~na, A. R. Guimaraes, A. R. Hardison, A. Ricciardone, A. Rijal, A. Rocchi, A. Romero, A. Salvarese, A. Samajdar, A. Sanchez, A. Sasli, A. S. Bell, A. Schiebelbein, A. Sevrin, A. S. Goettel, A. Sider, A. S. Markosyan, A. S. Sengupta, A. Strunk, A. Syx, A. Takamori, A. Taruya, A. Theodoropoulos, A. Tiwari, A. Torres-Forn\'e, A. Trapananti, A. Tripathee, A. Trovato, A. T. Wilkin, A. Vajpeyi, A. Van de Walle, A. Vecchio, A. Veutro, A. Vicer\'e, A. Vijaykumar, A. Vilkha, A. V. Patel, A. W. Goodwin-Jones, A. W. Lussier, B. Banerjee, B. Barr, B. B. Lane, B. B. Martinez, B. C. Barish, B. C. Brown, B. Cirok, B. C. Pant, B. D'Angelo, B. E. Ewing, B. E. Hogan, B. Farr, B. Fornal, B. F. Schutz, B. F. Whiting, B. Gadre, B. Garaventa, B. Gateley, B. Goncharov, B. G. Patterson, B. Haskell, B. Hughey, B. J. J. Slagmolen, B. J. Owen, B.-J. Park, B. J. Piotrzkowski, B. J. Sutton, B. K. Berger, B. K. Pradhan, B. Lantz, B. L. Swinkels, B. Mannix, B. Mestichelli, B. Mours, B. M. Williams, B. N. Meagher, B. O'Neal, B. O'Reilly, B. Patricelli, B. Rajbhandari, B. Ratto, B. Revenu, B. R. Iyer, B. Sassolas, B. S. Sathyaprakash, B. Verma, B. Weaver, B. Willke, B. W. Schulte, B. Wu, C. Adamcewicz, C. A. Hrishikesh, C. All\'en\'e, C.-A. Miritescu, C. Amra, C. A. Rose, C. Badger, C. Binu, C. Bradaschia, C. Buy, C. Cahillane, C. Casentini, C. Chatterjee, C. Chou, C. C. Wipf, C. D. Blair, C. De Rossi, C. Di Fronzo, C. Eassa, C. Foo, C. Garc\'ia-Quir\'os, C. Gasbarra, C. G. Collette, C. G. Hoy, C. Gier, C. Gray, C. Greenberg, C. Grimaud, C. Hanna, C. Henshaw, C. Hirose, C. Hsiung, C. I. Torrie, C. Jacquet, C. J. Haster, C. J. Moore, C. J. Stark, C. Kim, C. Kimball, C. Lazarte, C. Lazzaro, C. Lindsay, C. L. Mungioli, C. Marinelli, C. McElhenny, C. M. Compton, C. Messick, C. Michel, C. Mishra, C. M. Mow-Lowry, C. Moreno, C. Nelle, C. N. Makarem, C. North, C. O. Lousto, C. Osthelder, C. Palomba, C. P\'erigois, C. Petrillo, C. P. L. Berry, C. Plunkett, C. Posnansky, C. Rajan, C. Reissel, C. Robertson, C. S. Menoni, C. Talbot, C. Taranto, C. 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Sigg, D. Singh, D. S. Wu, D. Tanabe, D. Tellez, D. Verkindt, D. V. Martynov, D. Voigt, D. Watarai, D. W. Gould, D. Wilken, D. Williams, E. A. Avila, E. A. Moreno, E. Bonilla, E. Brockmueller, E. Calloni, E. Capocasa, E. Capote, E. Cesarini, E. Chassande-Mottin, E. Coccia, E. Codazzo, E. Colangeli, E. Cuoco, E. D. Hall, E. Dohmen, E. E. Papalexakis, E. Fenyvesi, E. Finch, E. Floden, E. Goetz, E. G. Seo, E. G. Wickens, E. J. Daw, E. J. Howell, E. J. Knox, E. J. Marx, E. J. Sanchez, E. J. Wang, E. Katsavounidis, E. K. Porter, E. Lalande, E. L. Merilh, E. Lotti, E. Maggio, E. Majorana, E. Maros, E. Milotti, E. M. Minihan, E. M. S\"anger, E. N. Tapia San Mart\'in, E. Oelker, E. Payne, E. Placidi, E. Polini, E. Porcelli, E. R. G. von Reis, E. Ruiz Morales, E. Schwartz, E. Sheridan, E. Thrane, E. T. Lin, E. Tournefier, E. T. Vincent, E. Van den Bossche, E. Wuchner, E. Z. Appavuravther, E. Z. Hamilton, F. Acernese, F. A. Kerkow, F. Amicucci, F. A. Ramis Vidal, F. Armato, F. Attadio, F. Aubin, F. Barone, F. Beirnaert, F. Bergamin, F. Bondu, F. Bucci, F. Carbognani, F. Chiadini, F. Clara, F. Cleva, F. De Lillo, F. De Marco, F. De Matteis, F. Di Renzo, F. Donovan, F. E. Pe\~na Arellano, F. Fabrizi, F. Fidecaro, F. Fontinele-Nunes, F. Frappez, F. Frasconi, F. Garufi, F. Gautier, F. Glotin, F. Gulminelli, F. Guzman, F. Hellman, F. H. Panther, F. J. Raab, F. Khan, F. Lin, F. Llamas Villarreal, F. Marion, F. Martelli, F. Mera, F. Meylahn, F. Muciaccia, F. Nocera, F. Ohme, F. Pannarale, F. Paoletti, F. Piergiovanni, F. Pilo, F. Ricci, F. Robinet, F. Salces-Carcoba, F. Salemi, F. Santoliquido, F. Sarandrea, F. Sorrentino, F. Spada, F. Stachurski, F. Travasso, F. Vetrano, F. Y. Khalili, G. A. Iandolo, G. A. Prodi, G. Ashton, G. Avallone, G. Baldi, G. Ballardin, G. Bevilacqua, G. Billingsley, G. Boileau, G. Bouyer, G. Bruno, G. Cagnoli, G. Caneva Santoro, G. Capurri, G. Carapella, G. Carrillo, G. Carullo, G. Cella, G. Chiarini, G. Ciani, G. C. Liu, G. Connolly, G. D\'alya, G. Demasi, G. Dideron, G. Eddolls, G. Favaro, G. Gemme, G. G. Fronz\'e, G. Gonz\'alez, G. Greco, G. Grignani, G. Hammond, G. Hemming, G. Iannone, G. I. McGhee, G. Iorio, G. Joubert, G. Kang, G. Koekoek, G. Kuehn, G. Lacaille, G. L. Mansell, G. Losurdo, G. McCarrol, G. M. Guidi, G. M. Harry, G. Mo, G. Moreno, G. Morras, G. N. Bolingbroke, G. Oganesyan, G. Papigkiotis, G. Pascale, G. Perna, G. Pierra, G. Pratten, G. Principe, G. Qu\'em\'ener, G. R. Johns, G. S. Cabourn Davies, G. S. Prabhu, G. Traylor, G. Troian, G. Vajente, G. Vedovato, G. Waratkar, G. Woan, H. A. Loughlin, H.-B. Jin, H. B. Kabagoz, H. Cao, H. Chen, H. Duval, H. Einsle, H. E. Jose, H. Estell\'es, H.-F. Hsieh, H. Fong, H. Grote, H. Guo, H. Hansen, H. Hayakawa, H. Heitmann, H. Imafuku, H. J. Bulten, H. Kato, H. K. Griffin, H. K. Gulati, H. K. Riley, H. L. Griggs, H. L. Sawant, H. L\"uck, H. Miao, H. Middleton, H. M. Lee, H. Mullock, H. Nakano, H. Narola, H. Overmier, H. O. Zhu, H. Pan, H. P. Cheng, H. Pham, H. Phurailatpam, H. P. Pfeiffer, H. Qi, H. Shinkai, H. Siegel, H. Sotani, H. Tagoshi, H. Takahashi, H. Takeda, H. T. Cheung, H. Themann, H. Tong, H. T. Wong, H. Ubach, H. Vahlbruch, H. van Haevermaet, H. Vocca, H. Wang, H. W. Lee, H. Wu, H. Yamamoto, H. Y. Chen, H.-Y. Hsieh, H. Y. Huang, H. Yuzurihara, H. Zhong, H. Zhou, I. A. Bilenko, I. Abouelfettouh, I. A. O. MacMillan, I. Bartos, I. Bentara, I. Braun, I. C. F. Wong, I. Cordero-Carri\'on, I. Coronado, I. Dave, I. Di Palma, I. Fiori, I. Gupta, I. Harley-Trochimczyk, I. J. Hollows, I. Kaku, I.-L. Ahrend, I. La Rosa, I. McMahon, I. M. Pinto, I. M. Romero-Shaw, I. Nardecchia, I. N. Legred, I. Ota, I. Rainho, I. S. Heng, I. Song, I. Takimoto Schmiegelow, I. Tosta e Melo, I. W. Harry, I. W. Martin, J. A. Clark, J. A. Font, J. A. Giaime, J. A. Malaquias-Reis, J. Anglin, J. B. Carlin, J. Betzwieser, J. B. Kanner, J. Bryant, J. Buchanan, J. Calder\'on Bustillo, J. Casanueva Diaz, J. C. Barayoga, J. C. Bayley, J. C. Driggers, J. C. Kim, J. C. 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Pith reviewed 2026-05-13 21:23 UTC · model grok-4.3

classification 🌀 gr-qc astro-ph.HE
keywords gravitational wavesblack hole mergerHawking area lawKerr black holeringdownquasinormal modesGW250114second law of black hole mechanics
0
0 comments X

The pith

GW250114 data confirm the final black hole area exceeds the sum of the two progenitors and its ringdown matches a Kerr spectrum.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper examines the loud gravitational-wave event GW250114, produced by the merger of two black holes each roughly 33 solar masses. Post-merger signal segments, stripped of the peak, line up with the expected frequencies of the dominant quadrupolar mode and its first overtone for a spinning Kerr black hole, to within thirty percent. Separate analyses that drop the loudest merger cycles still find the remnant horizon area larger than the combined initial areas. A reader cares because these checks directly test two foundational predictions of classical general relativity for black-hole dynamics in the strong-field regime.

Core claim

Post-merger data excluding the peak region are consistent with the dominant quadrupolar mode of a Kerr black hole and its first overtone, with frequencies constrained to plus or minus thirty percent of the Kerr spectrum. Analyses that exclude up to five of the strongest merger cycles show the remnant area is larger than the sum of the initial areas to high credibility.

What carries the argument

Matched-filter comparison of post-peak waveform segments to Kerr quasinormal-mode templates together with direct area computation from inferred initial and final masses and spins.

Load-bearing premise

The full waveform from inspiral through ringdown is assumed to be accurately described by general-relativity templates that presuppose a Kerr remnant.

What would settle it

An observation in which the inferred remnant area falls below the sum of the initial areas, or in which the measured ringdown frequencies lie more than thirty percent away from the Kerr values, would contradict the reported result.

read the original abstract

The gravitational-wave signal GW250114 was observed by the two LIGO detectors with a network matched-filter signal-to-noise ratio of 80. The signal was emitted by the coalescence of two black holes with near-equal masses $m_1 = 33.6^{+1.2}_{-0.8}\,M_\odot$ and $m_2 = 32.2^{+0.8}_{-1.3}\,M_\odot$, and small spins $\chi_{1,2} \leq 0.26$ (90% credibility) and negligible eccentricity $e \leq 0.03$. Post-merger data excluding the peak region are consistent with the dominant quadrupolar $(\ell = |m| = 2)$ mode of a Kerr black hole and its first overtone. We constrain the modes' frequencies to $\pm 30\%$ of the Kerr spectrum, providing a test of the remnant's Kerr nature. We also examine Hawking's area law, also known as the second law of black hole mechanics, which states that the total area of the black hole event horizons cannot decrease with time. A range of analyses that exclude up to 5 of the strongest merger cycles confirm that the remnant area is larger than the sum of the initial areas to high credibility.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 2 minor

Summary. The paper analyzes the high-SNR LIGO event GW250114 from the merger of two near-equal-mass black holes (m1 ≈ 33.6 M⊙, m2 ≈ 32.2 M⊙, low spins). Using post-merger data with the peak excised, it reports consistency with the dominant (ℓ=|m|=2) quadrupolar mode and first overtone of a Kerr remnant, constraining the frequencies to within ±30% of the Kerr spectrum. Multiple analyses excluding up to five strong merger cycles show the remnant horizon area exceeds the sum of the initial areas at high credibility, supporting Hawking's area law.

Significance. If the results hold, the work supplies one of the cleanest observational consistency checks of the black-hole area theorem and the no-hair property of the remnant using real gravitational-wave data. The deliberate excision of the loudest cycles and the use of established LIGO parameter-estimation pipelines are strengths that reduce contamination from the merger phase. The reported credibility intervals on the area increase and the frequency bound constitute falsifiable, data-driven statements that can be directly compared with future events.

major comments (2)
  1. [Parameter estimation and ringdown analysis sections] The parameter-estimation step that supplies both the initial areas (from inspiral) and the remnant mass/spin (from ringdown) is performed exclusively with GR waveform templates that already assume a Kerr remnant. Any unmodeled systematic mismatch between these templates and the true signal therefore propagates directly into the reported ±30% frequency bound and the A_remnant > A1 + A2 credibility. The robustness tests vary only the data segment length; they do not vary the template family or relax the Kerr assumption.
  2. [Post-merger frequency constraint paragraph] The ±30% frequency constraint is presented as a test of the Kerr nature, yet the bound is derived after the remnant parameters have already been inferred under the Kerr hypothesis. It is therefore a consistency check rather than an independent measurement; the manuscript should quantify how much the bound would loosen if the remnant spin were allowed to float freely or if a non-Kerr ringdown model were substituted.
minor comments (2)
  1. [Abstract and results section] The abstract states that 'a range of analyses' exclude up to five cycles; the main text should list the exact set of excision windows and the corresponding credibility values for the area increase so that readers can reproduce the robustness claim.
  2. [Introduction and methods] Notation for the initial and remnant areas (A1, A2, A_remnant) should be defined explicitly the first time they appear, including the precise formula used to compute horizon area from mass and spin.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the positive assessment and constructive comments on our analysis of GW250114. We have revised the manuscript to clarify the assumptions in our parameter estimation and to describe the frequency constraint explicitly as a consistency check. Below we respond point by point to the major comments.

read point-by-point responses
  1. Referee: [Parameter estimation and ringdown analysis sections] The parameter-estimation step that supplies both the initial areas (from inspiral) and the remnant mass/spin (from ringdown) is performed exclusively with GR waveform templates that already assume a Kerr remnant. Any unmodeled systematic mismatch between these templates and the true signal therefore propagates directly into the reported ±30% frequency bound and the A_remnant > A1 + A2 credibility. The robustness tests vary only the data segment length; they do not vary the template family or relax the Kerr assumption.

    Authors: We agree that the analysis relies on standard GR waveform templates (such as IMRPhenomXPHM) that assume a Kerr remnant, which is the established approach for LIGO parameter estimation of this event. The robustness tests were designed to assess the impact of including or excluding merger cycles, the main potential source of bias in the ringdown regime. While we did not vary template families or relax the Kerr assumption, these templates have been extensively validated against numerical relativity for systems with mass ratios and spins comparable to GW250114. We have added clarifying text in the revised manuscript stating that the reported bounds are conditional on the GR templates and discussing possible systematic effects. This constitutes a partial revision, as we incorporated discussion but did not conduct new template-variation studies. revision: partial

  2. Referee: [Post-merger frequency constraint paragraph] The ±30% frequency constraint is presented as a test of the Kerr nature, yet the bound is derived after the remnant parameters have already been inferred under the Kerr hypothesis. It is therefore a consistency check rather than an independent measurement; the manuscript should quantify how much the bound would loosen if the remnant spin were allowed to float freely or if a non-Kerr ringdown model were substituted.

    Authors: We acknowledge that the ±30% frequency bound is a consistency check performed after inferring remnant parameters under the Kerr hypothesis. We have revised the relevant paragraph to describe the result explicitly as a consistency test within the GR framework rather than an independent measurement. A full quantification of how the bound would change under a freely floating spin or a non-Kerr ringdown model would require implementing alternative models outside the standard LIGO pipelines, which lies beyond the scope of this work. We have added a note in the discussion section highlighting this limitation and identifying it as a direction for future analyses. revision: partial

Circularity Check

0 steps flagged

No significant circularity in derivation chain

full rationale

The paper infers initial and remnant parameters via standard GR waveform templates, then performs consistency checks by comparing post-merger frequencies to the external Kerr spectrum (computed from inferred mass/spin) and verifying that the remnant area exceeds the sum of initial areas using the GR area formula. These are external theoretical benchmarks, not quantities fitted or defined from the same data segment in a self-referential loop. No self-definitional equations, fitted inputs relabeled as predictions, load-bearing self-citations, or ansatzes smuggled via prior work appear in the described chain. The tests remain independent consistency checks against GR theory even when merger cycles are excised.

Axiom & Free-Parameter Ledger

1 free parameters · 2 axioms · 0 invented entities

The claims rest on general-relativity waveform models for parameter estimation and on the assumption that the remnant is a Kerr black hole whose area can be computed from the inferred mass and spin.

free parameters (1)
  • component masses and spins
    Fitted from the inspiral-merger-ringdown signal using matched-filter templates; values m1 ≈ 33.6 M⊙, m2 ≈ 32.2 M⊙, χ1,2 ≤ 0.26 are reported with credible intervals.
axioms (2)
  • domain assumption The spacetime of the remnant is exactly described by the Kerr metric
    Invoked when comparing observed ringdown frequencies to the Kerr spectrum and when computing horizon areas from the final mass and spin.
  • domain assumption Hawking's area theorem applies to the classical event horizons inferred from the data
    The law being tested; the comparison of initial and final areas assumes the horizons are those of classical GR black holes.

pith-pipeline@v0.9.0 · 15634 in / 1729 out tokens · 51021 ms · 2026-05-13T21:23:55.544384+00:00 · methodology

discussion (0)

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Reference graph

Works this paper leans on

222 extracted references · 222 canonical work pages · cited by 21 Pith papers · 23 internal anchors

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