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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

The time delay of light as it passes by a massive object, first calculated by Shapiro in 1964, is a hallmark of the curvature of space-time. To date, all measurements of the Shapiro time delay have been made over solar-system distance…

General Relativity and Quantum Cosmology · Physics 2014-11-18 S. Ballmer , S. Márka , P. Shawhan

The first detection of gravitational waves by the Laser Interferometer Gravitational-wave Observatory (LIGO) in 2015 launched the era of gravitational wave astronomy. The quest for gravitational wave signals from objects that are fainter or…

Advanced LIGO data contains numerous noise transients, or "glitches", that have been shown to reduce the sensitivity of matched filter searches for gravitational waves from compact binaries by increasing the rate at which random…

General Relativity and Quantum Cosmology · Physics 2020-08-26 Derek Davis , Laurel V. White , Peter R. Saulson

We propose a method for filling gaps and removing interferences in time series for applications involving continuous monitoring of environmental variables. The approach is non-parametric and based on an iterative pattern-matching between…

Geophysics · Physics 2015-08-11 Gregoire Mariethoz , Niklas Linde , Damien Jougnot , Hassan Rezaee

The characterization of the Advanced LIGO detectors in the second and third observing runs has increased the sensitivity of the instruments, allowing for a higher number of detectable gravitational-wave signals, and provided confirmation of…

Instrumentation and Methods for Astrophysics · Physics 2021-07-12 D. Davis , J. S. Areeda , B. K. Berger , R. Bruntz , A. Effler , R. C. Essick , R. P. Fisher , P. Godwin , E. Goetz , A. F. Helmling-Cornell , B. Hughey , E. Katsavounidis , A. P. Lundgren , D. M. Macleod , Z. Márka , T. J. Massinger , A. Matas , J. McIver , G. Mo , K. Mogushi , P. Nguyen , L. K. Nuttall , R. M. S. Schofield , D. H. Shoemaker , S. Soni , A. L. Stuver , A. L. Urban , G. Valdes , M. Walker , R. Abbott , C. Adams , R. X. Adhikari , A. Ananyeva , S. Appert , K. Arai , Y. Asali , S. M. Aston , C. Austin , A. M. Baer , M. Ball , S. W. Ballmer , S. Banagiri , D. Barker , C. Barschaw , L. Barsotti , J. Bartlett , J. Betzwieser , R. Beda , D. Bhattacharjee , J. Bidler , G. Billingsley , S. Biscans , C. D. Blair , R. M. Blair , N. Bode , P. Booker , R. Bork , A. Bramley , A. F. Brooks , D. D. Brown , A. Buikema , C. Cahillane , T. A. Callister , G. Caneva Santoro , K. C. Cannon , J. Carlin , K. Chandra , X. Chen , N. Christensen , A. A. Ciobanu , F. Clara , C. M. Compton , S. J. Cooper , K. R. Corley , M. W. Coughlin , S. T. Countryman , P. B. Covas , D. C. Coyne , S. G. Crowder , T. Dal Canton , B. Danila , L. E. H. Datrier , G. S. Davies , T. Dent , N. A. Didio , C. Di Fronzo , K. L. Dooley , J. C. Driggers , P. Dupej , S. E. Dwyer , T. Etzel , M. Evans , T. M. Evans , S. Fairhurst , J. Feicht , A. Fernandez-Galiana , R. Frey , P. Fritschel , V. V. Frolov , P. Fulda , M. Fyffe , B. U. Gadre , J. A. Giaime , K. D. Giardina , G. González , S. Gras , C. Gray , R. Gray , A. C. Green , A. Gupta , E. K. Gustafson , R. Gustafson , J. Hanks , J. Hanson , T. Hardwick , I. W. Harry , R. K. Hasskew , M. C. Heintze , J. Heinzel , N. A. Holland , I. J. Hollows , C. G. Hoy , S. Hughey , S. J. Jadhav , K. Janssens , G. Johns , J. D. Jones , S. Kandhasamy , S. Karki , M. Kasprzack , K. Kawabe , D. Keitel , N. Kijbunchoo , Y. M. Kim , P. J. King , J. S. Kissel , S. Kulkarni , Rahul Kumar , M. Landry , B. B. Lane , B. Lantz , M. Laxen , Y. K. Lecoeuche , J. Leviton , J. Liu , M. Lormand , R. Macas , A. Macedo , M. MacInnis , V. Mandic , G. L. Mansell , S. Márka , B. Martinez , K. Martinovic , D. V. Martynov , K. Mason , F. Matichard , N. Mavalvala , R. McCarthy , D. E. McClelland , S. McCormick , L. McCuller , C. McIsaac , T. McRae , G. Mendell , K. Merfeld , E. L. Merilh , P. M. Meyers , F. Meylahn , I. Michaloliakos , H. Middleton , J. C. Mills , T. Mistry , R. Mittleman , G. Moreno , C. M. Mow-Lowry , S. Mozzon , L. Mueller , N. Mukund , A. Mullavey , J. Muth , T. J. N. Nelson , A. Neunzert , S. Nichols , E. Nitoglia , J. Oberling , J. J. Oh , S. H. Oh , Richard J. Oram , R. G. Ormiston , N. Ormsby , C. Osthelder , D. J. Ottaway , H. Overmier , A. Pai , J. R. Palamos , F. Pannarale , W. Parker , O. Patane , M. Patel , E. Payne , A. Pele , R. Penhorwood , C. J. Perez , K. S. Phukon , M. Pillas , M. Pirello , H. Radkins , K. E. Ramirez , J. W. Richardson , K. Riles , K. Rink , N. A. Robertson , J. G. Rollins , C. L. Romel , J. H. Romie , M. P. Ross , K. Ryan , T. Sadecki , M. Sakellariadou , E. J. Sanchez , L. E. Sanchez , L. Sandles , T. R. Saravanan , R. L. Savage , D. Schaetzl , R. Schnabel , E. Schwartz , D. Sellers , T. Shaffer , D. Sigg , A. M. Sintes , B. J. J. Slagmolen , J. R. Smith , K. Soni , B. Sorazu , A. P. Spencer , K. A. Strain , D. Strom , L. Sun , M. J. Szczepańczyk , J. Tasson , R. Tenorio , M. Thomas , P. Thomas , K. A. Thorne , K. Toland , C. I. Torrie , A. Tran , G. Traylor , M. Trevor , M. Tse , G. Vajente , N. van Remortel , D. C. Vander-Hyde , A. Vargas , J. Veitch , P. J. Veitch , K. Venkateswara , G. Venugopalan , A. D. Viets , V. Villa-Ortega , T. Vo , C. Vorvick , M. Wade , G. S. Wallace , R. L. Ward , J. Warner , B. Weaver , A. J. Weinstein , R. Weiss , K. Wette , D. D. White , L. V. White , C. Whittle , A. R. Williamson , B. Willke , C. C. Wipf , L. Xiao , R. Xu , H. Yamamoto , Hang Yu , Haocun Yu , L. Zhang , Y. Zheng , M. E. Zucker , J. Zweizig

Heterodyne interferometry for precision science often comes with an optical phase modulation, for example, for intersatellite clock noise transfer for gravitational wave (GW) detectors in space, exemplified by the Laser Interferometer Space…

Instrumentation and Methods for Astrophysics · Physics 2025-12-22 Kohei Yamamoto , Olaf Hartwig , Lennart Wissel , Holly Leopardi , Kenji Numata , Ryan Derosa

Calibration is a key step in the signal processing pipeline of any radio astronomical instrument. The required sky, ionospheric and instrumental models for this step can suffer from various kinds of incompleteness. In this paper we analyze…

Instrumentation and Methods for Astrophysics · Physics 2019-02-08 A. Mouri Sardarabadi , L. V. E. Koopmans

Light travel time changes due to gravitational waves may be detected within the next decade through precision timing of millisecond pulsars. Removal of frequency-dependent interstellar medium (ISM) delays due to dispersion and scattering is…

Instrumentation and Methods for Astrophysics · Physics 2015-12-16 Nipuni Palliyaguru , Daniel Stinebring , Maura McLaughlin , Paul Demorest , Glenn Jones

We present the details of predicting atmospheric turbulence by mining Zernike moment data obtained from simulations as well as experiments. Temporally correlated optical wave-fronts were simulated such that they followed Kolmogorov phase…

Instrumentation and Methods for Astrophysics · Physics 2011-09-14 Akondi Vyas , M. B. Roopashree , B. Raghavendra Prasad

An analytical expression is given for the minimum of the time-delay induced wavefront error (also known as the servo-lag error) in Adaptive Optics systems under temporal prediction filtering. The analysis is based on the von K\'arm\'an…

Instrumentation and Methods for Astrophysics · Physics 2020-06-22 Niek Doelman

To meet the stringent time calibration requirements for the Belle II experiment upgrade, particularly for its large-size KL and Muon Detector comprising tens of thousands of scintillator channels with time resolutions better than 100 ps, we…

Instrumentation and Detectors · Physics 2026-02-23 Ziyu Liu , Xiyang Wang , Shiming Zou , Xiaolong Wang , Junhao Yin , Minggang Zhao

In wave propagation theories, many problems of multi-sensor systems utilize time delay in their solution in signal processing. This technique finds great utility in seismic exploration and static correction (low-velocity weathering), which…

Computational Physics · Physics 2018-01-25 Ashraf H. Yahia , El-Sayed El-Dahshan , Albert K. Guirguis

In many practical applications, signals and environments are time- varying, which makes fixed filters unreliable. Adaptive filtering, on the other hand, updates in real time to suppress noise, track nonstationary signals, and identify…

General Mathematics · Mathematics 2026-03-12 Keshav Raj Acharya , Pitambar Acharya

We investigate methods to calibrate the non-common path aberrations at an adaptive optics system having a wavefront-correcting device working at an extremely high resolution (larger than 150x150). We use focal-plane images collected…

Instrumentation and Methods for Astrophysics · Physics 2015-06-22 Visa Korkiakoski , Christoph U. Keller , Niek Doelman , Matthew Kenworthy , Gilles Otten , Michel Verhaegen

Upgrades to improve the sensitivity of gravitational wave detectors enable more frequent detections and more precise source parameter estimation. Unlike other advanced interferometric detectors such as Advanced LIGO and Advanced Virgo,…

A new method of polarimetric calibration is presented in which the instrumental response is derived from regular observations of PSR J0437-4715 based on the assumption that the mean polarized emission from this millisecond pulsar remains…

Instrumentation and Methods for Astrophysics · Physics 2013-01-14 W. van Straten

Uncertainty in the calibration of gravitational-wave (GW) detector data leads to systematic errors which must be accounted for in setting limits on the strength of GW signals. When cross-correlation measurements are made using data from a…

General Relativity and Quantum Cosmology · Physics 2014-03-07 John T. Whelan , Emma L. Robinson , Joseph D. Romano , Eric H. Thrane

On May 24th, 2023, the Advanced Laser Interferometer Gravitational-Wave Observatory (LIGO), joined by the Advanced Virgo and KAGRA detectors, began the fourth observing run for a two-year-long dedicated search for gravitational waves. The…

General Relativity and Quantum Cosmology · Physics 2025-03-05 E. Capote , W. Jia , N. Aritomi , M. Nakano , V. Xu , R. Abbott , I. Abouelfettouh , R. X. Adhikari , A. Ananyeva , S. Appert , S. K. Apple , K. Arai , S. M. Aston , M. Ball , S. W. Ballmer , D. Barker , L. Barsotti , B. K. Berger , J. Betzwieser , D. Bhattacharjee , G. Billingsley , S. Biscans , C. D. Blair , N. Bode , E. Bonilla , V. Bossilkov , A. Branch , A. F. Brooks , D. D. Brown , J. Bryant , C. Cahillane , H. Cao , F. Clara , J. Collins , C. M. Compton , R. Cottingham , D. C. Coyne , R. Crouch , J. Csizmazia , A. Cumming , L. P. Dartez , D. Davis , N. Demos , E. Dohmen , J. C. Driggers , S. E. Dwyer , A. Effler , A. Ejlli , T. Etzel , M. Evans , J. Feicht , R. Frey , W. Frischhertz , P. Fritschel , V. V. Frolov , M. Fuentes-Garcia , P. Fulda , M. Fyffe , D. Ganapathy , B. Gateley , T. Gayer , J. A. Giaime , K. D. Giardina , J. Glanzer , E. Goetz , R. Goetz , A. W. Goodwin-Jones , S. Gras , C. Gray , D. Griffith , H. Grote , T. Guidry , J. Gurs , E. D. Hall , J. Hanks , J. Hanson , M. C. Heintze , A. F. Helmling-Cornell , N. A. Holland , D. Hoyland , H. Y. Huang , Y. Inoue , A. L. James , A. Jamies , A. Jennings , D. H. Jones , H. B. Kabagoz , S. Karat , S. Karki , M. Kasprzack , K. Kawabe , N. Kijbunchoo , P. J. King , J. S. Kissel , K. Komori , A. Kontos , Rahul Kumar , K. Kuns , M. Landry , B. Lantz , M. Laxen , K. Lee , M. Lesovsky , F. Llamas Villarreal , M. Lormand , H. A. Loughlin , R. Macas , M. MacInnis , C. N. Makarem , B. Mannix , G. L. Mansell , R. M. Martin , K. Mason , F. Matichard , N. Mavalvala , N. Maxwell , G. McCarrol , R. McCarthy , D. E. McClelland , S. McCormick , T. McRae , F. Mera , E. L. Merilh , F. Meylahn , R. Mittleman , D. Moraru , G. Moreno , A. Mullavey , T. J. N. Nelson , A. Neunzert , J. Notte , J. Oberling , T. OHanlon , C. Osthelder , D. J. Ottaway , H. Overmier , W. Parker , O. Patane , A. Pele , H. Pham , M. Pirello , J. Pullin , V. Quetschke , K. E. Ramirez , K. Ransom , J. Reyes , J. W. Richardson , M. Robinson , J. G. Rollins , C. L. Romel , J. H. Romie , M. P. Ross , K. Ryan , T. Sadecki , A. Sanchez , E. J. Sanchez , L. E. Sanchez , R. L. Savage , D. Schaetzl , M. G. Schiworski , R. Schnabel , R. M. S. Schofield , E. Schwartz , D. Sellers , T. Shaffer , R. W. Short , D. Sigg , B. J. J. Slagmolen , C. Soike , S. Soni , V. Srivastava , L. Sun , D. B. Tanner , M. Thomas , P. Thomas , K. A. Thorne , M. R. Todd , C. I. Torrie , G. Traylor , A. S. Ubhi , G. Vajente , J. Vanosky , A. Vecchio , P. J. Veitch , A. M. Vibhute , E. R. G. von Reis , J. Warner , B. Weaver , R. Weiss , C. Whittle , B. Willke , C. C. Wipf , J. L. Wright , H. Yamamoto , L. Zhang , M. E. Zucker

Precise mode matching is needed to maximize performance in coupled cavity interferometers such as Advanced LIGO. In this paper we present a new mode matching sensing scheme that uses a single radio frequency higher order mode sideband and…