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arxiv: 2605.11703 · v1 · submitted 2026-05-12 · 🌀 gr-qc · astro-ph.HE· astro-ph.IM

Recognition: 2 theorem links

· Lean Theorem

GW240925 and GW250207: Astrophysical Calibration of Gravitational-wave Detectors

The LIGO Scientific Collaboration , the Virgo Collaboration , the KAGRA Collaboration: A. G. Abac , I. Abouelfettouh , F. Acernese , K. Ackley , A. Adam , C. Adamcewicz
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S. Adhicary D. Adhikari N. Adhikari R. X. Adhikari V. K. Adkins S. Afroz A. Agapito D. Agarwal M. Agathos N. Aggarwal S. Aggarwal O. D. Aguiar I.-L. Ahrend L. Aiello A. Ain P. Ajith T. Akutsu S. Albanesi L. Albers W. Ali S. Al-Kershi C. All\'en\'e A. Allocca S. Al-Shammari P. A. Altin S. Alvarez-Lopez W. Amar O. Amarasinghe A. Amato F. Amicucci C. Amra C. Anand A. Ananyeva S. B. Anderson W. G. Anderson M. Andia M. Ando M. Andr\'es-Carcasona J. L. Andrey T. Andri\'c J. Anglin J. Anna S. Ansoldi J. M. Antelis S. Antier M. Aoumi E. Z. Appavuravther S. Appert S. K. Apple K. Arai A. Araya M. C. Araya M. Arca Sedda F. Arciprete J. S. Areeda N. Aritomi F. Armato S. Armstrong N. Arnaud M. Arogeti S. M. Aronson K. G. Arun G. Ashton Y. Aso L. Asprea M. Assiduo S. Assis de Souza Melo S. M. Aston P. Astone F. Attadio F. Aubin K. AultONeal G. Avallone E. A. Avila S. Babak C. Badger S. Bae S. Bagnasco L. Baiotti R. Bajpai T. Baka K. A. Baker T. Baker G. Balbi G. Baldi N. Baldicchi M. Ball G. 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Bogdan G. Boileau M. Boldrini G. N. Bolingbroke A. Bolliand L. D. Bonavena R. Bondarescu F. Bondu V. A. Bonhomme E. Bonilla M. S. Bonilla A. Bonino R. Bonnand A. Borchers N. Borghi V. Boschi S. Bose V. Bossilkov Y. Bothra A. Boudon M. Boyle A. Bozzi C. Bradaschia M. J. Brady P. R. Brady A. Branch M. Branchesi 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 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 G. Capoccia E. Capote G. Capurri G. Carapella F. Carbognani K. J. Cardona-Mart\'inez M. Carlassara J. B. Carlin T. K. Carlson M. F. Carney M. Carpinelli G. Carrillo J. J. Carter G. Carullo A. 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Cordero-Carri\'on S. Corezzi N. J. Cornish I. Coronado A. Corsi L. A. Corubolo L. Cotnoir R. Cottingham M. W. Coughlin P. Couvares D. M. Coward D. C. Coyne R. Coyne A. Cozzumbo J. D. E. Creighton T. D. Creighton 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. Dall'Osso S. Dal Pra G. D\'alya O. Dan Y. Dang B. D'Angelo S. Danilishin S. D'Antonio K. Danzmann K. E. Darroch L. P. Dartez R. Das A. Dasgupta V. Dattilo A. Daumas 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 C. J. Delgado Mendez F. De Lillo S. Della Torre W. Del Pozzo O. M. del Rio 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 V. Deshmukh R. De Simone S. Determan A. Dhani R. Dhurkunde R. Diab C. Diaz 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 F. Dosopoulou W. J. D. Doyle M. Drago J. C. Driggers M. Dubois R. R. Dumbreck L. Dunn U. Dupletsa D. D'Urso P. Dutta Roy H. Duval P.-A. Duverne S. E. Dwyer C. Eassa M. Eberhardt M. Ebersold T. Eckhardt G. Eddolls A. Effler J. Eichholz H. Einsle M. Eisenmann R. A. Eisenstein 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 X. Fan A. M. Farah B. Farr W. M. Farr M. Favata M. Fays M. Fazio J. Feicht M. M. Fejer J.-N. Feldhusen E. Fenyvesi J. Fernandes T. Fernandes D. Fernando S. Ferraiuolo T. A. Ferreira M. Ferrer F. Fidecaro P. Figura E. Finch A. Fiori I. Fiori M. 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Authors on Pith no claims yet

Pith reviewed 2026-05-13 05:21 UTC · model grok-4.3

classification 🌀 gr-qc astro-ph.HEastro-ph.IM
keywords gravitational wavesdetector calibrationbinary black holesLIGOVirgoastrophysical calibrationgeneral relativity
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The pith

Binary black hole signals enable the first astrophysical calibration of gravitational-wave detectors.

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

The paper demonstrates that loud gravitational-wave signals from binary black hole coalescences can constrain detector calibration directly by comparing the observed data against general relativity predictions for signal phase and amplitude. This supplies an independent check on traditional in-situ calibration methods. For GW240925 the astrophysical approach verifies the Hanford detector calibration through cross-checks with known errors. For GW250207, where Hanford was unstable and calibration uncertainties were elevated, the method becomes essential for accurate data and source localization. As detector sensitivity rises, this technique will complement in-situ measurements and support more precise science with the signals.

Core claim

GW240925 and GW250207 are two loud gravitational-wave signals from binary black hole coalescences observed with network signal-to-noise ratios of approximately 32 and 69. Gravitational-wave signals from coalescing binaries have characteristic phase and amplitude evolution predicted by general relativity. These signal waveforms, together with measured instrumental calibration uncertainties, are used to infer source parameters. For sufficiently loud detections it is possible to constrain the calibration of the detectors directly using the signals themselves. The authors present the first informative astrophysical measurements of gravitational-wave detector calibration.

What carries the argument

General-relativity waveform templates for binary black hole coalescences, employed as absolute references to infer detector amplitude and phase calibration parameters directly from the observed signals.

If this is right

  • The well-localized high signal-to-noise observations enable precise measurements of source properties.
  • Stringent tests of general relativity become feasible with these events.
  • Informative dark siren measurements for cosmology are supported once calibration uncertainties are properly incorporated.
  • Astrophysical calibration will become an increasingly valuable complement to in-situ calibration measurements as detector sensitivity improves.

Where Pith is reading between the lines

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

  • This technique could maintain usable calibration during periods when one or more detectors experience transient instability.
  • It may lower systematic errors in luminosity-distance estimates that affect multi-messenger follow-up and cosmological inference.
  • Routine application to future loud events could reduce overall reliance on hardware-based calibration across the global network.

Load-bearing premise

The phase and amplitude evolution of the signals from binary black hole coalescences matches general relativity predictions closely enough to serve as an absolute calibration reference.

What would settle it

A statistically significant discrepancy between the calibration parameters inferred from the astrophysical signals and those obtained from independent in-situ measurements or hardware injections for these events or similar future loud detections.

Figures

Figures reproduced from arXiv: 2605.11703 by A. Adam, A. Agapito, A. Ain, A. Allocca, A. Amato, A. Ananyeva, A. Araya, A. Basalaev, A. Basti, A. Bertolini, A. Bhattacharjee, 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. C. Green, A. Chakraborty, Achal Kumar, A. Chen, A. Chiba, A. Chincarini, A. Chiummo, A. Colombo, A. Corsi, A. Cozzumbo, A. Cumming, A. Dasgupta, A. Daumas, A. Davenport, A. Demagny, A. Depasse, 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. Franco-Ordovas, A. Freise, A. F. Vargas, A. Gamboa, A. Ganguly, A. Garron, A. Gennai, A. G. Guerrero, A. Goodwin-Jones, A. Grado, A. Heffernan, A. H. Laity, A. H.-Y. Chen, A. Ierardi, A. I. 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Figure 1
Figure 1. Figure 1: FIG. 1. Time–frequency spectrograms [46] showing data from LIGO Hanford (left), LIGO Livingston (middle) and Virgo (right) for [PITH_FULL_IMAGE:figures/full_fig_p014_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. LIGO Hanford calibration as a function of frequency over the analysis band for each signal. The top and bottom panels show the [PITH_FULL_IMAGE:figures/full_fig_p015_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. Sky localization for GW240925 (left) and GW250207 (right) from analyses using data from all three detectors (HLV) and just [PITH_FULL_IMAGE:figures/full_fig_p016_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. Inferred (2 [PITH_FULL_IMAGE:figures/full_fig_p018_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5. ASD of the LIGO Hanford detector one day before the arrival [PITH_FULL_IMAGE:figures/full_fig_p027_5.png] view at source ↗
Figure 7
Figure 7. Figure 7: FIG. 7. Similar to Fig. 6, real-time calibration monitoring for Han [PITH_FULL_IMAGE:figures/full_fig_p027_7.png] view at source ↗
Figure 8
Figure 8. Figure 8: The detector-frame masses have a unimodal distribu [PITH_FULL_IMAGE:figures/full_fig_p030_8.png] view at source ↗
Figure 8
Figure 8. Figure 8: FIG. 8. Inferred component masses for GW240925 (left) and GW250207 (right). Results are shown for analyses that neglect calibration [PITH_FULL_IMAGE:figures/full_fig_p031_8.png] view at source ↗
Figure 9
Figure 9. Figure 9: FIG. 9. Inferred e [PITH_FULL_IMAGE:figures/full_fig_p032_9.png] view at source ↗
Figure 10
Figure 10. Figure 10: FIG. 10. Sky localization for GW240925 from the low-latency [PITH_FULL_IMAGE:figures/full_fig_p032_10.png] view at source ↗
Figure 11
Figure 11. Figure 11: FIG. 11. Posteriors on the sky location together with rings corresponding to the inferred time delays between detector pairs for GW240925 [PITH_FULL_IMAGE:figures/full_fig_p033_11.png] view at source ↗
Figure 12
Figure 12. Figure 12: FIG. 12. Sky localization for GW250207 from four di [PITH_FULL_IMAGE:figures/full_fig_p033_12.png] view at source ↗
Figure 13
Figure 13. Figure 13: FIG. 13. Time–frequency spectrograms [46] showing residual data from LIGO Hanford (left), LIGO Livingston (middle) and Virgo (right) [PITH_FULL_IMAGE:figures/full_fig_p035_13.png] view at source ↗
Figure 14
Figure 14. Figure 14: FIG. 14. Illustrative results from the FTI (top, middle) and TIGER [PITH_FULL_IMAGE:figures/full_fig_p036_14.png] view at source ↗
Figure 15
Figure 15. Figure 15: FIG. 15. The 90% credible contours for the leading two PCA pa [PITH_FULL_IMAGE:figures/full_fig_p037_15.png] view at source ↗
read the original abstract

GW240925 and GW250207 are two loud gravitational-wave signals from binary black hole coalescences observed with network signal-to-noise ratios $\sim 32$ and $\sim 69$, respectively, by the LIGO Hanford--LIGO Livingston--Virgo network. Gravitational-wave signals from coalescing binaries have characteristic phase and amplitude evolution predicted by general relativity. These signal waveforms, together with measured instrumental calibration uncertainties, are used to infer source parameters. However, for sufficiently loud detections it is possible to constrain the calibration of the detectors directly using the signals themselves. We present the first informative astrophysical measurements of gravitational-wave detector calibration. For GW240925, we verify the inference of Hanford calibration from the astrophysical signal through cross-checks with known calibration errors obtained from in-situ measurements. At the time of GW250207, the Hanford detector was not fully stabilized, leading to elevated calibration uncertainties; thus, astrophysical calibration is essential to obtain accurate data and to enable source localization. These well-localized, high signal-to-noise observations have the potential to offer precise measurements of source properties, stringent tests of general relativity, and informative dark siren measurements, provided that calibration uncertainties are properly incorporated. As detector sensitivity improves, astrophysical calibration will become an increasingly valuable complement to in-situ calibration measurements. Obtaining accurate calibration will be essential for precision gravitational-wave science.

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 manuscript reports two high-SNR binary black hole events (GW240925 with network SNR ~32 and GW250207 with ~69) observed by the LIGO-Virgo network. It claims these signals enable the first informative astrophysical calibration of the detectors by using their characteristic phase and amplitude evolution (assumed to follow general relativity) to directly constrain calibration parameters, with an in-situ cross-check for GW240925 and necessity for GW250207 due to elevated uncertainties from detector instability. The work positions the events for improved source localization, GR tests, and dark siren measurements once calibration uncertainties are incorporated.

Significance. If the results hold after addressing model dependence, the paper demonstrates a valuable complementary calibration technique using astrophysical sources that will grow in importance with detector sensitivity. The concrete cross-check for one event and identification of the practical need for the second provide useful examples. This strengthens the case for treating calibration as part of the data analysis pipeline rather than a fixed input.

major comments (2)
  1. [Abstract] Abstract: The central claim of 'first informative astrophysical measurements' of calibration rests on fitting signals to GR waveform templates. No procedure is described for jointly sampling calibration corrections together with parameterized post-Einsteinian (ppE) deviations to demonstrate that the two can be separated; any GR deviation could be absorbed into the calibration parameters, undermining the independence of the calibration reference.
  2. [GW250207 discussion] GW250207 discussion: The statement that astrophysical calibration 'is essential to obtain accurate data and to enable source localization' is load-bearing for the necessity claim, yet no quantitative comparison (e.g., change in calibration uncertainty budget or localization area before/after the astrophysical constraint) is provided to support the magnitude of the improvement.
minor comments (2)
  1. [Abstract] The abstract supplies network SNRs but omits individual detector SNRs, the explicit form of the calibration error model, or the resulting posterior widths on calibration parameters; these details are required to judge whether the constraints are genuinely informative.
  2. [GW240925 cross-check] The manuscript would benefit from a short table comparing the in-situ calibration uncertainties to the astrophysically inferred corrections for GW240925.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful and constructive review. The comments highlight important considerations for strengthening the claims regarding astrophysical calibration. We address each major point below and indicate the revisions we will make.

read point-by-point responses
  1. Referee: [Abstract] Abstract: The central claim of 'first informative astrophysical measurements' of calibration rests on fitting signals to GR waveform templates. No procedure is described for jointly sampling calibration corrections together with parameterized post-Einsteinian (ppE) deviations to demonstrate that the two can be separated; any GR deviation could be absorbed into the calibration parameters, undermining the independence of the calibration reference.

    Authors: We acknowledge the potential for parameter degeneracies between calibration corrections and possible GR deviations. Our analysis assumes general relativity, consistent with standard practice for detector calibration using astrophysical signals. Calibration parameters are modeled as specific frequency-dependent amplitude and phase corrections, distinct from the waveform modifications introduced by ppE parameters. We will add a dedicated discussion in the revised manuscript explaining the expected separability for these high-SNR events and noting that a full joint sampling analysis, while feasible, lies beyond the scope of the present work focused on demonstrating the calibration technique itself. This addition will clarify the assumptions without altering the core results. revision: partial

  2. Referee: [GW250207 discussion] GW250207 discussion: The statement that astrophysical calibration 'is essential to obtain accurate data and to enable source localization' is load-bearing for the necessity claim, yet no quantitative comparison (e.g., change in calibration uncertainty budget or localization area before/after the astrophysical constraint) is provided to support the magnitude of the improvement.

    Authors: We agree that quantitative support would strengthen the necessity claim for GW250207. In the revised manuscript, we will include explicit comparisons of the calibration uncertainty budgets and the resulting 90% credible localization areas computed with and without the astrophysical calibration constraints. These additions will provide a direct measure of the improvement and better substantiate the statement regarding the essential role of astrophysical calibration for this event. revision: yes

Circularity Check

1 steps flagged

Astrophysical calibration 'measurement' reduces to fitting data to GR waveform templates by construction

specific steps
  1. fitted input called prediction [Abstract]
    "Gravitational-wave signals from coalescing binaries have characteristic phase and amplitude evolution predicted by general relativity. These signal waveforms, together with measured instrumental calibration uncertainties, are used to infer source parameters. However, for sufficiently loud detections it is possible to constrain the calibration of the detectors directly using the signals themselves. We present the first informative astrophysical measurements of gravitational-wave detector calibration."

    Calibration parameters are inferred by fitting the high-SNR signals to GR-predicted waveforms (adjusting for phase/amplitude evolution). The resulting 'measurement' is the fitted correction that forces agreement with GR, so the output calibration is statistically equivalent to the input assumption that the signals match GR exactly. This is not an independent derivation but a reparameterization of the fit.

full rationale

The paper's core claim of 'first informative astrophysical measurements of gravitational-wave detector calibration' is obtained by constraining calibration parameters directly from the observed signals using the characteristic phase and amplitude evolution predicted by general relativity. This creates a direct model dependence: the inferred calibration corrections are the adjustments needed to align the data with GR templates. No explicit separation (e.g., joint marginalization over post-Einsteinian parameters) is demonstrated, so any GR deviation would be absorbed into the calibration result. This is a partial circularity of the fitted-input-called-prediction type, but the paper still provides independent cross-checks for one event and acknowledges the assumption, preventing a higher score.

Axiom & Free-Parameter Ledger

1 free parameters · 1 axioms · 0 invented entities

The method rests on the assumption that GR binary black hole waveforms are known to sufficient accuracy to act as calibration standards; no new entities are introduced.

free parameters (1)
  • detector calibration corrections
    Amplitude and phase correction factors inferred directly from the astrophysical signals for each detector.
axioms (1)
  • domain assumption Gravitational-wave signals from binary black hole coalescences have phase and amplitude evolution accurately predicted by general relativity
    Invoked to use the signals as calibration references.

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