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The response of the Advanced LIGO interferometers is known to vary with time [arXiv:1608.05134]. Accurate calibration of the interferometers must therefore track and compensate for temporal variations in calibration model parameters. These…

Instrumentation and Methods for Astrophysics · Physics 2023-01-11 Madeline Wade , Aaron D. Viets , Theresa Chmiel , Madeline Stover , Leslie Wade

We present a frequency modulation technique for calibration of the displacement actuators of the LIGO 4-km-long interferometric gravitational-wave detectors. With the interferometer locked in a single-arm configuration, we modulate the…

General Relativity and Quantum Cosmology · Physics 2015-03-17 E. Goetz , R. L. Savage

Precise calibration of kilometer-scale interferometric gravitational wave detectors is crucial for source localization and waveform reconstruction. A technique that uses the radiation pressure of a power-modulated auxiliary laser to induce…

General Relativity and Quantum Cosmology · Physics 2010-02-23 E. Goetz , P. Kalmus , S. Erickson , R. L. Savage , G. Gonzalez , K. Kawabe , M. Landry , S. Marka , B. O'Reilly , K. Riles , D. Sigg , P. Willems

Calibration of the Advanced LIGO detectors is the quantification of the detectors' response to gravitational waves. Gravitational waves incident on the detectors cause phase shifts in the interferometer laser light which are read out as…

The two interferometers of the Laser Interferometry Gravitaional-wave Observatory (LIGO) recently detected gravitational waves from the mergers of binary black hole systems. Accurate calibration of the output of these detectors was crucial…

Interferometric gravitational-wave detectors like LIGO need to be able to measure changes in their arm lengths of order $10^{-18}~$m or smaller. This requires very high laser power in order to raise the signal above shot noise. One…

Applied Physics · Physics 2019-12-11 S. Biscans , S. Gras , C. D. Blair , J. Driggers , M. Evans , P. Fritschel , T. Hardwick , G. Mansell

A network of three or more gravitational wave detectors simultaneously taking data is required to generate a well-localized sky map for gravitational wave sources, such as GW170817. Local seismic disturbances often cause the LIGO and Virgo…

Instrumentation and Methods for Astrophysics · Physics 2020-08-10 Ayon Biswas , Jess McIver , Ashish Mahabal

The raw outputs of the detectors within the Advanced Laser Interferometer Gravitational-Wave Observatory need to be calibrated in order to produce the estimate of the dimensionless strain used for astrophysical analyses. The two detectors…

We describe three fundamentally different methods we have applied to calibrate the test mass displacement actuators to search for systematic errors in the calibration of the LIGO gravitational-wave detectors. The actuation frequencies…

General Relativity and Quantum Cosmology · Physics 2010-04-29 E. Goetz , R. L. Savage , J. Garofoli , G. Gonzalez , E. Hirose , P. Kalmus , K. Kawabe , J. Kissel , M. Landry , B. O'Reilly , X. Siemens , A. Stuver , M. Sung

Although there have now been hundreds of transient gravitational-wave detections of merging compact stars by the LIGO-Virgo-KAGRA (LVK) detector network, no continuous-wave (CW) signals have yet been discovered. To ensure that such signals,…

Instrumentation and Methods for Astrophysics · Physics 2026-01-16 Preet Baxi , Jessica Leviton , Eilam Morag , Matthew Pitkin , Keith Riles

Accurate and reliable calibration of the Advanced LIGO detectors has enabled a plethora of gravitational-wave discoveries in the detectors' first decade of operation, starting with the ground-breaking discovery, GW150914. In the first…

General Relativity and Quantum Cosmology · Physics 2025-10-10 M. Wade , J. Betzwieser , D. Bhattacharjee , L. Dartez , E. Goetz , J. Kissel , L. Sun , A. Viets , M. Carney , E. Makelele , L. Wade

Hardware injections are simulated gravitational-wave signals added to the Laser Interferometer Gravitational-wave Observatory (LIGO). The detectors' test masses are physically displaced by an actuator in order to simulate the effects of a…

The Laser Interferometer Gravitational Wave Observatory (LIGO) is a network of three detectors built to detect local perturbations in the space-time metric from astrophysical sources. These detectors, two in Hanford, WA and one in…

General Relativity and Quantum Cosmology · Physics 2010-12-09 LIGO Scientific Collaboration , J. Abadie , B. P. Abbott , R. Abbott , M , Abernathy , C. Adams , R. Adhikari , P. Ajith , B. Allen , G. Allen , E. Amador Ceron , R. S. Amin , S. B. Anderson , W. G. Anderson , M. A. Arain , M. Araya , M. Aronsson , Y. Aso , S. Aston , D. E. Atkinson , P. Aufmuth , C. Aulbert , S. Babak , P. Baker , S. Ballmer , D. Barker , S. Barnum , B. Barr , P. Barriga , L. Barsotti , M. A. Barton , I. Bartos , R. Bassiri , M. Bastarrika , J. Bauchrowitz , B. Behnke , M. Benacquista , A. Bertolini , J. Betzwieser , N. Beveridge , P. T. Beyersdorf , I. A. Bilenko , G. Billingsley , J. Birch , R. Biswas , E. Black , J. K. Blackburn , L. Blackburn , D. Blair , B. Bland , O. Bock , T. P. Bodiya , R. Bondarescu , R. Bork , M. Born , S. Bose , M. Boyle , P. R. Brady , V. B. Braginsky , J. E. Brau , J. Breyer , D. O. Bridges , M. Brinkmann , M. Britzger , A. F. Brooks , D. A. Brown , A. Buonanno , J. Burguet--Castell , O. Burmeister , R. L. Byer , L. Cadonati , J. B. Camp , P. Campsie , J. Cannizzo , K. C. Cannon , J. Cao , C. Capano , S. Caride , S. Caudill , M. Cavaglià , C. Cepeda , T. Chalermsongsak , E. Chalkley , P. Charlton , S. Chelkowski , Y. Chen , N. Christensen , S. S. Y. Chua , C. T. Y. Chung , D. Clark , J. Clark , J. H. Clayton , R. Conte , D. Cook , T. R. Corbitt , N. Cornish , C. A. Costa , D. Coward , D. C. Coyne , J. D. E. Creighton , T. D. Creighton , A. M. Cruise , R. M. Culter , A. Cumming , L. Cunningham , K. Dahl , S. L. Danilishin , R. Dannenberg , K. Danzmann , K. Das , B. Daudert , G. Davies , A. Davis , E. J. Daw , T. Dayanga , D. DeBra , J. Degallaix , V. Dergachev , R. DeRosa , R. DeSalvo , P. Devanka , S. Dhurandhar , I. Di Palma , M. Díaz , F. Donovan , K. L. Dooley , E. E. Doomes , S. Dorsher , E. S. D. Douglas , R. W. P. Drever , J. C. Driggers , J. Dueck , J. -C. Dumas , T. Eberle , M. Edgar , M. Edwards , A. Effler , P. Ehrens , R. Engel , T. Etzel , M. Evans , T. Evans , S. Fairhurst , Y. Fan , B. F. Farr , D. Fazi , H. Fehrmann , D. Feldbaum , L. S. Finn , M. Flanigan , K. Flasch , S. Foley , C. Forrest , E. Forsi , N. Fotopoulos , M. Frede , M. Frei , Z. Frei , A. Freise , R. Frey , T. T. Fricke , D. Friedrich , P. Fritschel , V. V. Frolov , P. Fulda , M. Fyffe , J. A. Garofoli , I. Gholami , S. Ghosh , J. A. Giaime , S. Giampanis , K. D. Giardina , C. Gill , E. Goetz , L. M. Goggin , G. González , M. L. Gorodetsky , S. Goßler , C. Graef , A. Grant , S. Gras , C. Gray , R. J. S. Greenhalgh , A. M. Gretarsson , R. Grosso , H. Grote , S. Grunewald , E. K. Gustafson , R. Gustafson , B. Hage , P. Hall , J. M. Hallam , D. Hammer , G. Hammond , J. Hanks , C. Hanna , J. Hanson , J. Harms , G. M. Harry , I. W. Harry , E. D. Harstad , K. Haughian , K. Hayama , J. Heefner , I. S. Heng , A. Heptonstall , M. Hewitson , S. Hild , E. Hirose , D. Hoak , K. A. Hodge , K. Holt , D. J. Hosken , J. Hough , E. Howell , D. Hoyland , B. Hughey , S. Husa , S. H. Huttner , T. Huynh--Dinh , D. R. Ingram , R. Inta , T. Isogai , A. Ivanov , W. W. Johnson , D. I. Jones , G. Jones , R. Jones , L. Ju , P. Kalmus , V. Kalogera , S. Kandhasamy , J. Kanner , E. Katsavounidis , K. Kawabe , S. Kawamura , F. Kawazoe , W. Kells , D. G. Keppel , A. Khalaidovski , F. Y. Khalili , E. A. Khazanov , H. Kim , P. J. King , D. L. Kinzel , J. S. Kissel , S. Klimenko , V. Kondrashov , R. Kopparapu , S. Koranda , D. Kozak , T. Krause , V. Kringel , S. Krishnamurthy , B. Krishnan , G. Kuehn , J. Kullman , R. Kumar , P. Kwee , M. Landry , M. Lang , B. Lantz , N. Lastzka , A. Lazzarini , P. Leaci , J. Leong , I. Leonor , J. Li , H. Lin , P. E. Lindquist , N. A. Lockerbie , D. Lodhia , M. Lormand , P. Lu , J. Luan , M. Lubinski , A. Lucianetti , H. Lück , A. Lundgren , B. Machenschalk , M. MacInnis , M. Mageswaran , K. Mailand , C. Mak , I. Mandel , V. Mandic , S. Márka , Z. Márka , E. Maros , I. W. Martin , R. M. Martin , J. N. Marx , K. Mason , F. Matichard , L. Matone , R. A. Matzner , N. Mavalvala , R. McCarthy , D. E. McClelland , S. C. McGuire , G. McIntyre , G. McIvor , D. J. A. McKechan , G. Meadors , M. Mehmet , T. Meier , A. Melatos , A. C. Melissinos , G. Mendell , D. F. Menéndez , R. A. Mercer , L. Merill , S. Meshkov , C. Messenger , M. S. Meyer , H. Miao , J. Miller , Y. Mino , S. Mitra , V. P. Mitrofanov , G. Mitselmakher , R. Mittleman , B. Moe , S. D. Mohanty , S. R. P. Mohapatra , D. Moraru , G. Moreno , T. Morioka , K. Mors , K. Mossavi , C. MowLowry , G. Mueller , S. Mukherjee , A. Mullavey , H. Müller-Ebhardt , J. Munch , P. G. Murray , T. Nash , R. Nawrodt , J. Nelson , G. Newton , A. Nishizawa , D. Nolting , E. Ochsner , J. O'Dell , G. H. Ogin , R. G. Oldenburg , B. O'Reilly , R. O'Shaughnessy , C. Osthelder , D. J. Ottaway , R. S. Ottens , H. Overmier , B. J. Owen , A. Page , Y. Pan , C. Pankow , M. A. Papa , M. Pareja , P. Patel , M. Pedraza , L. Pekowsky , S. Penn , C. Peralta , A. Perreca , M. Pickenpack , I. M. Pinto , M. Pitkin , H. J. Pletsch , M. V. Plissi , F. Postiglione , V. Predoi , L. R. Price , M. Prijatelj , M. Principe , R. Prix , L. Prokhorov , O. Puncken , V. Quetschke , F. J. Raab , T. Radke , H. Radkins , P. Raffai , M. Rakhmanov , B. Rankins , V. Raymond , C. M. Reed , T. Reed , S. Reid , D. H. Reitze , R. Riesen , K. Riles , P. Roberts , N. A. Robertson , C. Robinson , E. L. Robinson , S. Roddy , C. Röver , J. Rollins , J. D. Romano , J. H. Romie , S. Rowan , A. Rüdiger , K. Ryan , S. Sakata , M. Sakosky , F. Salemi , L. Sammut , L. Sancho de la Jordana , V. Sandberg , V. Sannibale , L. Santamaría , G. Santostasi , S. Saraf , B. S. Sathyaprakash , S. Sato , M. Satterthwaite , P. R. Saulson , R. Savage , R. Schilling , R. Schnabel , R. Schofield , B. Schulz , B. F. Schutz , P. Schwinberg , J. Scott , S. M. Scott , A. C. Searle , F. Seifert , D. Sellers , A. S. Sengupta , A. Sergeev , D. Shaddock , B. Shapiro , P. Shawhan , D. H. Shoemaker , A. Sibley , X. Siemens , D. Sigg , A. Singer , A. M. Sintes , G. Skelton , B. J. J. Slagmolen , J. Slutsky , J. R. Smith , M. R. Smith , N. D. Smith , K. Somiya , B. Sorazu , F. C. Speirits , A. J. Stein , L. C. Stein , S. Steinlechner , S. Steplewski , A. Stochino , R. Stone , K. A. Strain , S. Strigin , A. Stroeer , A. L. Stuver , T. Z. Summerscales , M. Sung , S. Susmithan , P. J. Sutton , D. Talukder , D. B. Tanner , S. P. Tarabrin , J. R. Taylor , R. Taylor , P. Thomas , K. A. Thorne , K. S. Thorne , E. Thrane , A. Thüring , C. Titsler , K. V. Tokmakov , C. Torres , C. I. Torrie , G. Traylor , M. Trias , K. Tseng , D. Ugolini , K. Urbanek , H. Vahlbruch , B. Vaishnav , M. Vallisneri , C. Van Den Broeck , M. V. van der Sluys , A. A. van Veggel , S. Vass , R. Vaulin , A. Vecchio , J. Veitch , P. J. Veitch , C. Veltkamp , A. Villar , C. Vorvick , S. P. Vyachanin , S. J. Waldman , L. Wallace , A. Wanner , R. L. Ward , P. Wei , M. Weinert , A. J. Weinstein , R. Weiss , L. Wen , S. Wen , P. Wessels , M. West , T. Westphal , K. Wette , J. T. Whelan , S. E. Whitcomb , D. J. White , B. F. Whiting , C. Wilkinson , P. A. Willems , L. Williams , B. Willke , L. Winkelmann , W. Winkler , C. C. Wipf , A. G. Wiseman , G. Woan , R. Wooley , J. Worden , I. Yakushin , H. Yamamoto , K. Yamamoto , D. Yeaton-Massey , S. Yoshida , P. P. Yu , M. Zanolin , L. Zhang , Z. Zhang , C. Zhao , N. Zotov , M. E. Zucker , J. Zweizig

The LIGO observatories detect gravitational waves through monitoring changes in the detectors' length down to below $10^{-19}$\,$m/\sqrt{Hz}$ variation---a small fraction of the size of the atoms that make up the detector. To achieve this…

Instrumentation and Methods for Astrophysics · Physics 2020-05-27 Robert E. Colgan , K. Rainer Corley , Yenson Lau , Imre Bartos , John N. Wright , Zsuzsa Marka , Szabolcs Marka

The waveform of a compact binary coalescence is predicted by general relativity. It is therefore possible to directly constrain the response of a gravitational-wave (GW) detector by analyzing a signal's observed amplitude and phase…

Instrumentation and Methods for Astrophysics · Physics 2019-09-04 Reed Essick , Daniel E. Holz

Gravitational wave signals from coalescing compact binaries in the LIGO and Virgo interferometers are primarily detected by the template based matched filtering method. While this method is optimal for stationary and Gaussian data…

General Relativity and Quantum Cosmology · Physics 2024-09-16 Chayan Chatterjee , Karan Jani

Improved low-frequency sensitivity of gravitational wave observatories would unlock study of intermediate-mass black hole mergers, binary black hole eccentricity, and provide early warnings for multi-messenger observations of binary neutron…

Advanced gravitational-wave detectors such as the Laser Interferometer Gravitational-Wave Observatories (LIGO) require an unprecedented level of isolation from the ground. When in operation, they are expected to observe changes in the…

Instrumentation and Detectors · Physics 2019-12-10 S. Biscans , J. Warner , R. Mittleman , C. Buchanan , M. Coughlin , M. Evans , H. Gabbard , J. Harms , B. Lantz , N. Mukund , A. Pele , C. Pezerat , P. Picart , H. Radkins , T. Shaffer

The data from ground based gravitational-wave detectors such as Advanced LIGO and Virgo must be calibrated to convert the digital output of photodetectors into a relative displacement of the test masses in the detectors, producing the…

General Relativity and Quantum Cosmology · Physics 2021-03-24 Salvatore Vitale , Carl-Johan Haster , Ling Sun , Ben Farr , Evan Goetz , Jeff Kissel , Craig Cahillane

LIGO, the Laser Interferometer Gravitational-wave Observatory, has been designed and constructed to measure gravitational wave strain via differential arm length. The LIGO 4-km Michelson arms with Fabry-Perot cavities have auxiliary length…

Instrumentation and Methods for Astrophysics · Physics 2016-04-28 Grant David Meadors , Keita Kawabe , Keith Riles
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