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arxiv: 2603.19020 · v1 · submitted 2026-03-19 · 🌀 gr-qc · astro-ph.HE

Recognition: 2 theorem links

· Lean Theorem

GWTC-4.0: Tests of General Relativity. II. Parameterized Tests

The LIGO Scientific Collaboration , the Virgo Collaboration , the KAGRA Collaboration: A. G. Abac , I. Abouelfettouh , F. Acernese , K. Ackley , C. Adamcewicz , S. Adhicary
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Bonilla M. S. Bonilla A. Bonino R. Bonnand A. Borchers V. Boschi S. Bose V. Bossilkov Y. Bothra A. Boudon L. Bourg M. Boyle A. Bozzi C. Bradaschia P. R. Brady A. Branch M. Branchesi I. Braun T. Briant A. Brillet M. Brinkmann P. Brockill E. Brockmueller A. F. Brooks B. C. Brown D. D. Brown M. L. Brozzetti S. Brunett G. Bruno R. Bruntz J. Bryant Y. Bu F. Bucci J. Buchanan O. Bulashenko T. Bulik H. J. Bulten A. Buonanno K. Burtnyk R. Buscicchio D. Buskulic C. Buy R. L. Byer G. S. Cabourn Davies R. Cabrita V. C\'aceres-Barbosa L. Cadonati G. Cagnoli C. Cahillane A. Calafat T. A. Callister E. Calloni S. R. Callos M. Canepa G. Caneva Santoro K. C. Cannon H. Cao L. A. Capistran E. Capocasa E. Capote G. Capurri G. Carapella F. Carbognani M. Carlassara J. B. Carlin T. K. Carlson M. F. Carney M. Carpinelli G. Carrillo J. J. Carter G. Carullo A. Casallas-Lagos J. Casanueva Diaz C. Casentini S. Y. Castro-Lucas S. Caudill M. Cavagli\`a R. Cavalieri A. Ceja G. Cella P. Cerd\'a-Dur\'an E. Cesarini N. Chabbra W. Chaibi A. Chakraborty P. Chakraborty S. Chakraborty S. Chalathadka Subrahmanya J. C. L. Chan M. Chan K. Chang S. Chao P. Charlton E. Chassande-Mottin C. Chatterjee Debarati Chatterjee Deep Chatterjee M. Chaturvedi S. Chaty K. Chatziioannou A. Chen A. H.-Y. Chen D. Chen H. Chen H. Y. Chen S. Chen Yanbei Chen Yitian Chen H. P. Cheng P. Chessa H. T. Cheung S. Y. Cheung F. Chiadini G. Chiarini A. Chiba A. Chincarini M. L. Chiofalo A. Chiummo C. Chou S. Choudhary N. Christensen S. S. Y. Chua G. Ciani P. Ciecielag M. Cie\'slar M. Cifaldi B. Cirok F. Clara J. A. Clark T. A. Clarke P. Clearwater S. Clesse F. Cleva E. Coccia E. Codazzo P.-F. Cohadon S. Colace E. Colangeli M. Colleoni C. G. Collette J. Collins S. Colloms A. Colombo C. M. Compton G. Connolly L. Conti T. R. Corbitt I. Cordero-Carri\'on S. Corezzi M. Corman N. J. Cornish I. Coronado A. Corsi R. Cottingham M. W. Coughlin A. Couineaux P. Couvares D. M. Coward R. Coyne A. Cozzumbo J. D. E. Creighton T. D. Creighton P. Cremonese S. Crook R. Crouch J. Csizmazia J. R. Cudell T. J. Cullen A. Cumming E. Cuoco M. Cusinato L. V. Da Concei\c{c}\~ao T. Dal Canton S. Dal Pra G. D\'alya O. Dan B. D'Angelo S. Danilishin S. D'Antonio K. Danzmann K. E. Darroch L. P. Dartez R. Das A. Dasgupta V. Dattilo A. Daumas N. Davari I. Dave A. Davenport M. Davier T. F. Davies D. Davis L. Davis M. C. Davis P. Davis E. J. Daw M. Dax J. De Bolle M. Deenadayalan J. Degallaix M. De Laurentis F. De Lillo S. Della Torre W. Del Pozzo A. Demagny F. De Marco G. Demasi F. De Matteis N. Demos T. Dent A. Depasse N. DePergola R. De Pietri R. De Rosa C. De Rossi M. Desai R. DeSalvo A. DeSimone R. De Simone A. Dhani R. Diab M. C. D\'iaz M. Di Cesare G. Dideron T. Dietrich L. Di Fiore C. Di Fronzo M. Di Giovanni T. Di Girolamo D. Diksha J. Ding S. Di Pace I. Di Palma D. Di Piero F. Di Renzo Divyajyoti A. Dmitriev J. P. Docherty Z. Doctor N. Doerksen E. Dohmen A. Doke A. Domiciano De Souza L. D'Onofrio F. Donovan K. L. Dooley T. Dooney S. Doravari O. Dorosh W. J. D. Doyle M. Drago J. C. Driggers L. Dunn U. Dupletsa P.-A. Duverne D. D'Urso P. Dutta Roy H. Duval S. E. Dwyer C. Eassa W. East M. Ebersold T. Eckhardt G. Eddolls A. Effler J. Eichholz H. Einsle M. Eisenmann M. Emma K. Endo R. Enficiaud L. Errico R. Espinosa M. Esposito R. C. Essick H. Estell\'es T. Etzel M. Evans T. Evstafyeva B. E. Ewing J. M. Ezquiaga F. Fabrizi V. Fafone S. Fairhurst A. M. Farah B. Farr W. M. Farr G. Favaro M. Favata M. Fays M. Fazio J. Feicht M. M. Fejer R. Felicetti E. Fenyvesi J. Fernandes T. Fernandes D. Fernando S. Ferraiuolo T. A. Ferreira F. Fidecaro A. Fienga P. Figura A. Fiori I. Fiori M. Fishbach R. P. Fisher R. Fittipaldi V. Fiumara R. Flaminio S. M. Fleischer L. S. Fleming E. Floden H. Fong J. A. Font F. Fontinele-Nunes C. Foo B. Fornal K. Franceschetti F. Frappez S. Frasca F. Frasconi J. P. Freed Z. Frei A. Freise O. Freitas R. Frey W. Frischhertz P. Fritschel V. V. Frolov G. G. Fronz\'e M. 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Sharma Preeti Sharma Prianka Sharma Ritwik Sharma S. Sharma Chaudhary P. Shawhan N. S. Shcheblanov E. Sheridan Z.-H. Shi M. Shikauchi R. Shimomura H. Shinkai S. Shirke D. H. Shoemaker D. M. Shoemaker R. W. Short S. ShyamSundar A. Sider H. Siegel D. Sigg L. Silenzi L. Silvestri M. Simmonds L. P. Singer Amitesh Singh Anika Singh D. Singh N. Singh S. Singh A. M. Sintes V. Sipala V. Skliris B. J. J. Slagmolen D. A. Slater T. J. Slaven-Blair J. Smetana J. R. Smith L. Smith R. J. E. Smith W. J. Smith S. Soares de Albuquerque Filho M. Soares-Santos K. Somiya I. Song S. Soni V. Sordini F. Sorrentino H. Sotani F. Spada V. Spagnuolo A. P. Spencer P. Spinicelli A. K. Srivastava F. Stachurski C. J. Stark D. A. Steer J. Steinhoff N. Steinle J. Steinlechner S. Steinlechner N. Stergioulas P. Stevens M. StPierre M. D. Strong A. Strunk A. L. Stuver M. Suchenek S. Sudhagar Y. Sudo N. Sueltmann L. Suleiman K. D. Sullivan J. Sun L. Sun S. Sunil J. Suresh B. J. Sutton P. J. Sutton K. Suzuki M. Suzuki S. Swain B. L. Swinkels A. Syx M. J. Szczepa\'nczyk P. Szewczyk M. Tacca H. Tagoshi S. C. Tait K. Takada H. Takahashi R. Takahashi A. Takamori S. Takano H. Takeda K. Takeshita I. Takimoto Schmiegelow M. Takou-Ayaoh C. Talbot M. Tamaki N. Tamanini D. Tanabe K. Tanaka S. J. Tanaka S. Tanioka D. B. Tanner W. Tanner L. Tao R. D. Tapia E. N. Tapia San Mart\'in C. Taranto A. Taruya J. D. Tasson J. G. Tau D. Tellez R. Tenorio H. Themann A. Theodoropoulos M. P. Thirugnanasambandam L. M. Thomas M. Thomas P. Thomas J. E. Thompson S. R. Thondapu K. A. Thorne E. Thrane J. Tissino A. Tiwari Pawan Tiwari Praveer Tiwari S. Tiwari V. Tiwari M. R. Todd M. Toffano A. M. Toivonen K. Toland A. E. Tolley T. Tomaru V. Tommasini T. Tomura H. Tong C. Tong-Yu A. Torres-Forn\'e C. I. Torrie I. Tosta e Melo E. Tournefier M. Trad Nery K. Tran A. Trapananti R. Travaglini F. Travasso G. Traylor M. Trevor M. C. Tringali A. Tripathee G. Troian A. Trovato L. Trozzo R. J. Trudeau T. Tsang S. Tsuchida L. Tsukada K. Turbang M. Turconi C. Turski H. Ubach N. Uchikata T. Uchiyama R. P. Udall T. Uehara K. Ueno V. Undheim L. E. Uronen T. Ushiba M. Vacatello H. Vahlbruch N. Vaidya G. Vajente A. Vajpeyi J. Valencia M. Valentini S. A. Vallejo-Pe\~na S. Vallero V. Valsan M. van Dael E. Van den Bossche J. F. J. van den Brand C. Van Den Broeck M. van der Sluys A. Van de Walle J. van Dongen K. Vandra M. VanDyke H. van Haevermaet J. V. van Heijningen P. Van Hove J. Vanier M. VanKeuren J. Vanosky N. van Remortel M. Vardaro A. F. Vargas V. Varma A. N. Vazquez A. Vecchio G. Vedovato J. Veitch P. J. Veitch S. Venikoudis R. C. Venterea P. Verdier M. Vereecken D. Verkindt B. Verma Y. Verma S. M. Vermeulen F. Vetrano A. Veutro A. Vicer\'e S. Vidyant A. D. Viets A. Vijaykumar A. Vilkha N. Villanueva Espinosa V. Villa-Ortega E. T. Vincent J.-Y. Vinet S. Viret S. Vitale H. Vocca D. Voigt E. R. G. von Reis J. S. A. von Wrangel W. E. Vossius L. Vujeva S. P. Vyatchanin J. Wack L. E. Wade M. Wade K. J. Wagner R. M. Wald L. Wallace E. J. Wang H. Wang J. Z. Wang W. H. Wang Y. F. Wang G. Waratkar J. Warner M. Was T. Washimi N. Y. Washington D. Watarai B. Weaver S. A. Webster N. L. Weickhardt M. Weinert A. J. Weinstein R. Weiss L. Wen K. Wette J. T. Whelan B. F. Whiting C. Whittle E. G. Wickens D. Wilken A. T. Wilkin B. M. Williams D. Williams M. J. Williams N. S. Williams J. L. Willis B. Willke M. Wils L. Wilson C. W. Winborn J. Winterflood C. C. Wipf G. Woan J. Woehler N. E. Wolfe H. T. Wong I. C. F. Wong K. Wong T. Wouters J. L. Wright M. Wright B. Wu C. Wu D. S. Wu H. Wu K. Wu Q. Wu Y. Wu Z. Wu E. Wuchner D. M. Wysocki V. A. Xu Y. Xu N. Yadav H. Yamamoto K. Yamamoto T. S. Yamamoto T. Yamamoto R. Yamazaki T. Yan K. Z. Yang Y. Yang Z. Yarbrough J. Yebana S.-W. Yeh A. B. Yelikar X. Yin J. Yokoyama T. Yokozawa S. Yuan H. Yuzurihara M. Zanolin M. Zeeshan T. Zelenova J.-P. Zendri M. Zeoli M. Zerrad M. Zevin L. Zhang N. Zhang R. Zhang T. Zhang C. Zhao J. Zhao Yue Zhao Yuhang Zhao Z.-C. Zhao Y. Zheng H. Zhong H. Zhou H. O. Zhu Z.-H. Zhu A. B. Zimmerman L. Zimmermann M. E. Zucker J. Zweizig
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Pith reviewed 2026-05-16 16:42 UTC · model grok-4.3

classification 🌀 gr-qc astro-ph.HE
keywords gravitational wavesgeneral relativity testsblack hole mergersparameterized post-Newtonian testsgraviton massGWTC-4.0LIGO-Virgo-KAGRAcompact binary coalescences
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The pith

Gravitational-wave signals from 91 events show no deviations from general relativity in parameterized tests of post-Newtonian coefficients, quadrupole moments, and propagation effects.

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

The paper applies eight parameterized tests to the 91 confident compact binary coalescence signals in GWTC-4.0. These tests modify post-Newtonian coefficients, spin-induced quadrupole moments, and wave propagation to look for departures from the values expected in general relativity. The analysis finds that the null result of no deviation lies inside the 90 percent credible interval for more than 90 percent of the events. Bounds on deviations from general-relativity post-Newtonian coefficients are tightened by factors between 1.2 and 5.5, and the upper limit on the graviton mass is updated to 1.92 times 10 to the minus 23 electronvolts over c squared.

Core claim

We find no evidence for physics beyond GR, for spin-induced quadrupole moments different from those of a Kerr black hole in GR, or for line of sight acceleration, with more than 90 percent of the events including the null result within their 90 percent credible intervals. We improve the bounds on deviations from the GR PN coefficients by factors of 1.2-5.5 and update the bound on the mass of the graviton to m_g less than or equal to 1.92 times 10 to the minus 23 eV per c squared.

What carries the argument

Parameterized deviation forms applied to the post-Newtonian coefficients, spin-induced quadrupole moments, and dispersive or birefringent propagation effects in the gravitational-wave waveforms.

If this is right

  • Tighter numerical limits now exist on the size of any post-Newtonian deviations in binary mergers.
  • The updated graviton-mass bound rules out a larger range of massive-graviton models.
  • Spin-induced quadrupole moments of the observed black holes remain consistent with the Kerr values expected in general relativity.
  • No line-of-sight acceleration is detected for any of the 91 sources.
  • The same parameterized framework can be reapplied to future catalogs with higher signal-to-noise events.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • Continued accumulation of events will push the same tests to even smaller deviation amplitudes.
  • The approach could be combined with other tests of general relativity on the same events to cross-check for hidden systematics.
  • If deviations appear in a later catalog, the current bounds provide a quantitative baseline for measuring the size of the new effect.
  • The consistency with Kerr quadrupole moments adds one more data point to the empirical case that astrophysical black holes match the general-relativity prediction.

Load-bearing premise

The eight chosen parameterized deviation forms are sufficient to capture any possible departures from general relativity without missing qualitatively different effects or being biased by waveform model inaccuracies.

What would settle it

A single event in which the posterior distribution for any one deviation parameter excludes the general-relativity value of zero at greater than three-sigma significance would falsify the central claim for that test.

read the original abstract

In this second of three papers on tests of general relativity (GR) applied to the compact binary coalescence signals in the fourth Gravitational-Wave Transient Catalog (GWTC-4.0), we present the results of the parameterized tests of GR and constraints on line-of-sight acceleration. We include events up to and including the first part of the fourth observing run (O4a) of the LIGO Virgo KAGRA detectors. As in the other two papers in this series, we restrict our analysis to the 42 confident signals, measured by at least two detectors, that have false alarm rates $\le 10^{-3} \mathrm{yr}^{-1}$ from O4a, in addition to the 49 such events from previous observing runs. This paper focuses on the eight tests that constrain parameterized deviations from the expected GR (or unaccelerated) values. These include modifications of post-Newtonian (PN) parameters, spin-induced quadrupole moments different from those of a binary black hole, and possible dispersive or birefringent propagation effects. Overall, we find no evidence for physics beyond GR, for spin-induced quadrupole moments different from those of a Kerr black hole in GR, or for line of sight acceleration, with more than 90% of the events including the null result (no deviation) within their 90% credible intervals. We discuss possible systematics affecting the other events and tests, even though they are statistically not surprising, given noise. We improve the bounds on deviations from the GR PN coefficients by factors of 1.2-5.5 and provide illustrative translations to constraints on some modified theories. Also, we update the bound on the mass of the graviton, at 90% credibility, to $m_g \leq 1.92\times 10^{-23} \mathrm{eV}/c^2$. Thus, we see that GR holds, and many of the bounds on possible deviations derived from our events are the best to date.

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

1 major / 2 minor

Summary. This paper presents parameterized tests of general relativity applied to the 91 confident compact binary coalescence events in GWTC-4.0, including 42 from O4a. It examines eight specific forms of deviations: modifications to post-Newtonian phase coefficients, spin-induced quadrupole moments for black holes, and dispersive or birefringent propagation effects. Using Bayesian inference with standard waveform models, the analysis finds that the GR null values are consistent with the data for the majority of events, with over 90% of events having the null result within their 90% credible intervals. The work improves previous bounds on PN deviations by factors between 1.2 and 5.5 and updates the upper limit on the graviton mass to m_g ≤ 1.92 × 10^{-23} eV/c² at 90% credibility. No evidence for line-of-sight acceleration or deviations from Kerr quadrupole moments is found.

Significance. Should the findings hold upon detailed review, this manuscript represents a significant contribution to the field of gravitational-wave tests of GR. By incorporating the latest O4a data, it provides updated and tighter constraints on possible deviations, serving as a key reference for the community. The use of consistent methods across the catalog and the provision of illustrative mappings to modified gravity theories enhance its utility. The null results reinforce the validity of GR in the strong-field, dynamical regime probed by these mergers.

major comments (1)
  1. [§4.2] §4.2: The statement that bounds on PN deviations are improved by factors of 1.2-5.5 is presented without a per-test or per-event breakdown; identifying which coefficients or events drive the largest gains is needed to assess whether the improvement is robust to waveform model uncertainties or data selection.
minor comments (2)
  1. [Abstract] Abstract: The phrasing 'no evidence for physics beyond GR' should be qualified explicitly as applying to the eight parameterized forms tested, consistent with the paper's own note on illustrative translations to modified theories.
  2. [Table 2] Table 2: The table summarizing credible intervals for each test would benefit from an additional column indicating the fraction of events consistent with the GR null at 90% credibility to facilitate quick assessment of the 'more than 90%' claim.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their thoughtful review and positive assessment of the manuscript. We address the single major comment below and have revised the text accordingly to improve clarity and transparency.

read point-by-point responses
  1. Referee: [§4.2] §4.2: The statement that bounds on PN deviations are improved by factors of 1.2-5.5 is presented without a per-test or per-event breakdown; identifying which coefficients or events drive the largest gains is needed to assess whether the improvement is robust to waveform model uncertainties or data selection.

    Authors: We agree that a per-coefficient and per-event breakdown would strengthen the presentation. In the revised manuscript we have added a new table (Table 4) in §4.2 that lists the improvement factor for each PN coefficient (φ0, φ1, φ2, φ3, φ4, φ5, φ6, φ7, φ8, and the two higher-order terms) relative to the GWTC-3.0 results. The table also flags the subset of events (primarily the highest-SNR O4a detections such as GW230529_000000 and GW231123_000000) that dominate the tightened constraints. The largest gains (factors of 4–5.5) occur for φ2 and φ3 and are driven by the increased number and quality of events rather than any single outlier. We have additionally verified that the quoted improvement range remains unchanged when the analysis is repeated with the alternative waveform models IMRPhenomXPHM and SEOBNRv4PHM, confirming robustness to waveform systematics and data-selection choices. revision: yes

Circularity Check

0 steps flagged

No significant circularity; results are direct statistical outputs from data fits

full rationale

The paper's central results consist of Bayesian posterior constraints on eight parameterized deviation coefficients (PN terms, quadrupole moments, dispersion relations) fitted directly to the GWTC-4.0 strain data against standard GR waveform templates. No derivation step reduces a reported bound or null result to a prior fitted constant or self-citation by algebraic identity; the graviton-mass limit and PN-coefficient improvements are explicit outputs of the likelihood evaluation on new O4a events. References to the companion papers in the series supply only shared data-selection criteria and waveform models, which remain externally verifiable and do not carry the load-bearing inference. The analysis therefore contains independent empirical content and exhibits no self-definitional, fitted-input-renamed-as-prediction, or uniqueness-imported circularity.

Axiom & Free-Parameter Ledger

1 free parameters · 1 axioms · 0 invented entities

The central claim rests on fitting a finite set of deviation parameters to the data; the baseline GR waveform models are taken as given from prior literature.

free parameters (1)
  • Parameterized deviation coefficients (delta phi_i, delta beta_i, etc.)
    These coefficients are allowed to deviate from their GR values and are fitted to each event or combined posterior.
axioms (1)
  • domain assumption GR-based waveform models accurately describe the signals when deviation parameters are zero
    Invoked as the baseline for all parameterized tests in the abstract.

pith-pipeline@v0.9.0 · 15760 in / 1368 out tokens · 41921 ms · 2026-05-16T16:42:10.580181+00:00 · methodology

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Lean theorems connected to this paper

Citations machine-checked in the Pith Canon. Every link opens the source theorem in the public Lean library.

  • IndisputableMonolith/Foundation/RealityFromDistinction.lean reality_from_one_distinction unclear
    ?
    unclear

    Relation between the paper passage and the cited Recognition theorem.

    This paper focuses on the eight tests that constrain parameterized deviations from the expected GR (or unaccelerated) values. These include modifications of post-Newtonian (PN) parameters, spin-induced quadrupole moments different from those of a binary black hole, and possible dispersive or birefringent propagation effects.

  • IndisputableMonolith/Cost/FunctionalEquation.lean washburn_uniqueness_aczel unclear
    ?
    unclear

    Relation between the paper passage and the cited Recognition theorem.

    We improve the bounds on deviations from the GR PN coefficients by factors of 1.2-5.5 and update the bound on the mass of the graviton to m_g ≤ 1.92×10^{-23} eV/c².

What do these tags mean?
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The paper's claim is directly supported by a theorem in the formal canon.
supports
The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
extends
The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
uses
The paper appears to rely on the theorem as machinery.
contradicts
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unclear
Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.

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