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For broadband quantum noise reduction of gravitational-wave detectors, frequency-dependent squeezed vacuum states realized using a filter cavity is a mature technique and will be implemented in Advanced LIGO and Advanced Virgo from the…

Instrumentation and Detectors · Physics 2020-08-11 Naoki Aritomi , Matteo Leonardi , Eleonora Capocasa , Yuhang Zhao , Raffaele Flaminio

A major barrier to improving the quantum-limited sensitivity of gravitational-wave observatories is the thermal distortions of the test masses which arise at megawatt laser power. Recent advances in a new form of higher-order wavefront…

Instrumentation and Methods for Astrophysics · Physics 2025-09-30 Liu Tao , Pooyan Goodarzi , Jonathan W. Richardson

Einstein Telescope (ET) is a planned third generation gravitational waves detector located in Europe. Its design will be different from currently build interferometers, because ET will consist of three interferometers rotated by a 60 deg…

Cosmology and Nongalactic Astrophysics · Physics 2015-05-25 I. Kowalska-Leszczynska , T. Bulik

This paper presents an adaptable, parallelizable method for subtracting linearly coupled noise from Advanced LIGO data. We explain the features developed to ensure that the process is robust enough to handle the variability present in…

Instrumentation and Methods for Astrophysics · Physics 2019-06-27 D. Davis , T. J. Massinger , A. P. Lundgren , J. C. Driggers , A. L. Urban , L. K. Nuttall

Einstein Telescope (ET) is a third-generation gravitational wave (GW) detector with tenfold better sensitivity compared to the advanced LIGO detectors. It will be capable of observing copious stellar mass binary black hole mergers up to a…

Cosmology and Nongalactic Astrophysics · Physics 2026-04-30 Pinaki Roy , Tomasz Bulik

Gravitational Wave interferometers achieve their profound sensitivity by combining a Michelson interferometer with optical cavities, suspended masses, and now, squeezed quantum states of light. These states modify the measurement process of…

Instrumentation and Detectors · Physics 2021-09-22 L. McCuller , S. E. Dwyer , A. C. Green , Haocun Yu , L. Barsotti , C. D. Blair , D. D. Brown , A. Effler , M. Evans , A. Fernandez-Galiana , P. Fritschel , V. V. Frolov , N. Kijbunchoo , G. L. Mansell , F. Matichard , N. Mavalvala , D. E. McClelland , T. McRae , A. Mullavey , D. Sigg , B. J. J. Slagmolen , M. Tse , T. Vo , R. L. Ward , C. Whittle , R. Abbott , C. Adams , R. X. Adhikari , A. Ananyeva , S. Appert , K. Arai , J. S. Areeda , Y. Asali , 0 S. M. Aston , C. Austin , A. M. Baer , M. Ball , S. W. Ballmer , S. Banagiri , D. Barker , J. Bartlett , B. K. Berger , J. Betzwieser , D. Bhattacharjee , G. Billingsley , S. Biscans , R. M. Blair , N. Bode , P. Booker , R. Bork , A. Bramley , A. F. Brooks , A. Buikema , C. Cahillane , K. C. Cannon , X. Chen , 0 A. A. Ciobanu , F. Clara , C. M. Compton , S. J. Cooper , K. R. Corley , 0 S. T. Countryman , 0 P. B. Covas , D. C. Coyne , L. E. H. Datrier , D. Davis , C. Di Fronzo , K. L. Dooley , J. C. Driggers , T. Etzel , T. M. Evans , J. Feicht , P. Fulda , M. Fyffe , J. A. Giaime , K. D. Giardina , P. Godwin , E. Goetz , S. Gras , C. Gray , R. Gray , E. K. Gustafson , R. Gustafson , J. Hanks , J. Hanson , T. Hardwick , R. K. Hasskew , M. C. Heintze , A. F. Helmling-Cornell , N. A. Holland , J. D. Jones , S. Kandhasamy , S. Karki , M. Kasprzack , K. Kawabe , P. J. King , J. S. Kissel , Rahul Kumar , M. Landry , B. B. Lane , B. Lantz , M. Laxen , Y. K. Lecoeuche , J. Leviton , J. Liu , M. Lormand , A. P. Lundgren , 0 R. Macas , M. MacInnis , D. M. Macleod , S. Marka , 0 Z. Marka , 0 D. V. Martynov , K. Mason , T. J. Massinger , R. McCarthy , S. McCormick , J. McIver , G. Mendell , K. Merfeld , E. L. Merilh , F. Meylahn , T. Mistry , R. Mittleman , G. Moreno , C. M. Mow-Lowry , S. Mozzon , 0 T. J. N. Nelson , P. Nguyen , L. K. Nuttall , 0 J. Oberling , Richard J. Oram , C. Osthelder , D. J. Ottaway , H. Overmier , J. R. Palamos , W. Parker , E. Payne , A. Pele , R. Penhorwood , C. J. Perez , M. Pirello , H. Radkins , K. E. Ramirez , J. W. Richardson , K. Riles , N. A. Robertson , J. G. Rollins , C. L. Romel , J. H. Romie , M. P. Ross , K. Ryan , T. Sadecki , E. J. Sanchez , L. E. Sanchez , T. R. Saravanan , R. L. Savage , D. Schaetzl , R. Schnabel , R. M. S. Schofield , E. Schwartz , D. Sellers , T. Shaffer , J. R. Smith , S. Soni , B. Sorazu , A. P. Spencer , K. A. Strain , L. Sun , M. J. Szczepanczyk , M. Thomas , P. Thomas , K. A. Thorne , K. Toland , C. I. Torrie , G. Traylor , A. L. Urban , G. Vajente , G. Valdes , D. C. Vander-Hyde , P. J. Veitch , K. Venkateswara , G. Venugopalan , A. D. Viets , C. Vorvick , M. Wade , J. Warner , B. Weaver , R. Weiss , B. Willke , C. C. Wipf , L. Xiao , H. Yamamoto , Hang Yu , L. Zhang , M. E. Zucker , J. Zweizig

The next generation of large ground-based optical and infrared telescopes will provide new challenges for designers of astronomical instrumentation. The varied science cases for these extremely large telescopes (ELTs) require a large range…

Astrophysics · Physics 2009-11-13 Colin Cunningham , Chris Evans , Guy Monnet , Miska Le Louarn

We propose an upgrade to Advanced LIGO (aLIGO), named LIGO-LF, that focuses on improving the sensitivity in the 5-30 Hz low-frequency band, and we explore the upgrade's astrophysical applications. We present a comprehensive study of the…

The Einstein Telescope (ET) is a third-generation underground gravitational-wave observatory designed to extend the detection sensitivity down to a few Hertz. Newtonian noise is expected to limit the low-frequency sensitivity of ET,…

Instrumentation and Methods for Astrophysics · Physics 2026-03-17 Patrick Schillings , Shi Yao , Johannes Erdmann , Andreas Rietbrock

Interferometric gravitational-wave detectors like LIGO, GEO600 and Virgo record a surplus of information above and beyond possible gravitational-wave events. These auxiliary channels capture information about the state of the detector and…

Instrumentation and Methods for Astrophysics · Physics 2014-07-29 Reed Essick , Lindy Blackburn , Erik Katsavounidis

A conservative constraint on the Einstein Weak Equivalence Principle (WEP) can be obtained under the assumption that the observed time delay between correlated particles from astronomical sources is dominated by the gravitational fields…

High Energy Astrophysical Phenomena · Physics 2016-08-03 Xue-Feng Wu , He Gao , Jun-Jie Wei , Xi-Long Fan , Peter Mészáros , Bing Zhang , Zi-Gao Dai , Shuang-Nan Zhang , Zong-Hong Zhu

Significant progress has been made in recent years on the development of gravitational wave detectors. Sources such as coalescing compact binary systems, neutron stars in low-mass X-ray binaries, stellar collapses and pulsars are all…

Instrumentation and Methods for Astrophysics · Physics 2015-05-27 Matthew Pitkin , Stuart Reid , Sheila Rowan , Jim Hough

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

The Advanced LIGO gravitational wave detectors are nearing their design sensitivity and should begin taking meaningful astrophysical data in the fall of 2015. These resonant optical interferometers will have unprecedented sensitivity to the…

Based on the prior O1-O2 observing runs, about 30% of the data collected by Advanced LIGO and Virgo in the next observing runs are expected to be single-interferometer data, i.e., they will be collected at times when only one detector in…

Instrumentation and Methods for Astrophysics · Physics 2020-06-14 Marco Cavaglia , Sergio Gaudio , Travis Hansen , Kai Staats , Marek Szczepanczyk , Michele Zanolin

Teleseismic, or distant, earthquakes regularly disrupt the operation of ground--based gravitational wave detectors such as Advanced LIGO. Here, we present \emph{EQ mode}, a new global control scheme, consisting of an automated sequence of…

Instrumentation and Detectors · Physics 2020-12-02 Eyal Schwartz , A Pele , J Warner , B Lantz , J Betzwieser , K L Dooley , S Biscans , M Coughlin , N Mukund , R Abbott , C Adams , R X Adhikari , A Ananyeva , S Appert , K Arai , J S Areeda , Y Asali , S M Aston , C Austin , A M Baer , M Ball , S W Ballmer , S Banagiri , D Barker , L Barsotti , J Bartlett , B K Berger , D Bhattacharjee , G Billingsley , C D Blair , R M Blair , N Bode , P Booker , R Bork , A Bramley , A F Brooks , D D Brown , A Buikema , C Cahillane , K C Cannon , X Chen , A A Ciobanu , F Clara , S J Cooper , K R Corley , S T Countryman , P B Covas , D C Coyne , L E H Datrier , D Davis , C Di Fronzo , J C Driggers , P Dupej , S E Dwyer , A Effler , T Etze , M Evans , T M Evans , J Feicht , A Fernandez-Galiana , P Fritschel , V V Frolov , P Fulda , M Fyffe , J A Giaime , K D Giardina , P Godwin , E Goetz , S Gras , C Gray , R Gray , A C Green , Anchal Gupta , E K Gustafson , R Gustafson , J Hanks , J Hanson , T Hardwick , R K Hasskew , M C Heintze , A F Helmling-Cornell , N A Holland , J D Jones , S Kandhasamy , S Karki , M Kasprzack , K Kawabe , N Kijbunchoo , P J King , J S Kissel , Rahul Kumar , M Landry , B B Lane , M Laxen , Y K Lecoeuche , J Leviton , J Liu , M Lormand , A P Lundgren , R Macas , M MacInnis , D M Macleod , G L Mansell , S M arka , Z M arka , D V Martynov , K Mason , T J Massinger , F Matichard , N Mavalvala1 , R McCarthy , D E McClelland , S McCormick , L McCuller , J McIver , T McRae , G Mendell , K Merfeld , E L Merilh , F Meylahn , T Mistry , R Mittleman , G Moreno , C M Mow-Lowry , S Mozzon , A Mullavey , T J N Nelson , P Nguyen , L K Nuttall , J Oberling , Richard J Oram , C Osthelder , D J Ottaway , H Overmier , J R Palamos , W Parker , E Payne , C J Perez , M Pirello , H Radkins , K E Ramirez , J W Richardson , K Riles , N A Robertson , J G Rollins , C L Romel , J H Romie1 , M P Ross , K Ryan , T Sadecki , E J Sanchez , L E Sanchez , T R Saravanan , R L Savage , D Schaetzl , R Schnabel , R M S Schofield , D Sellers , T Shaffer , D Sigg , B J J Slagmolen , J R Smith , S Soni , B Sorazu , A P Spencer , K A Strain , L Sun , M J Szczepanczyk , M Thomas , P Thomas , K A Thorne , K Toland , C I Torrie , G Traylor , M Tse , A L Urban , G Vajente , G Valdes , D C Vander-Hyde , P J Veitch , K Venkateswara , G Venugopalan , A D Viets , T Vo , C Vorvick , M Wade , R L Ward , B Weaver , R Weiss , C Whittle , B Willke , C C Wipf , L Xiao , H Yamamoto , Hang Yu , Haocun Yu , L Zhang , M E Zucker , J Zweizig

One of the key science goals of advanced gravitational-wave detectors is to observe a stochastic gravitational-wave background. However, recent work demonstrates that correlated magnetic fields from Schumann resonances can produce…

Instrumentation and Methods for Astrophysics · Physics 2015-06-19 Eric Thrane , Nelson Christensen , Robert M. S. Schofield , Anamaria Effler

The sensitivity of ground-based gravitational wave (GW) detectors will be improved in the future via the injection of frequency-dependent squeezed vacuum. The achievable improvement is ultimately limited by losses of the interferometer…

Instrumentation and Detectors · Physics 2020-06-10 Antonio Perreca , Aidan Brooks , Jonathan Richardson , Daniel Toyra , Rory Smith

Gravitational-wave echoes in the post-merger ringdown phase are under intense scrutiny as probes of near-horizon quantum structures and as signatures of exotic states of matter in ultracompact stars. We present an analytical template that…

General Relativity and Quantum Cosmology · Physics 2018-09-18 Adriano Testa , Paolo Pani

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
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