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We study the thermal-noise spectrum of multi-loop pendulum suspensions for test masses in interferometric gravitational-wave detectors. The dependence of the thermal noise on suspension parameters and on properties of the wire material is…

Instrumentation and Detectors · Physics 2007-05-23 Constantin Brif

An analysis is given of thermoelastic noise (thermal noise due to thermoelastic dissipation) in finite sized test masses of laser interferometer gravitational-wave detectors. Finite-size effects increase the thermoelastic noise by a modest…

General Relativity and Quantum Cosmology · Physics 2009-10-31 Yuk Tung Liu , Kip S. Thorne

The suspension noise in interferometric gravitational wave detectors is caused by losses at the top and the bottom attachments of each suspension fiber. We use the Fluctuation-Dissipation theorem to argue that by careful positioning of the…

General Relativity and Quantum Cosmology · Physics 2008-11-26 Vladimir B. Braginsky , Yuri Levin , Sergey Vyatchanin

The use of fused-silica ribbons as suspensions in gravitational wave interferometers can result in significant improvements in pendulum mode thermal noise. Surface loss sets a lower bound to the level of noise achievable, at what level…

General Relativity and Quantum Cosmology · Physics 2009-10-31 Andri M. Gretarsson , Sheila Rowan , Geppo Cagnoli , Gregory M. Harry , Jim Hough , Steven D. Penn , Peter R. Saulson , William J. Startin

Thermal distortion of test masses, as well as thermal drift of their vibrational mode frequencies, present a major challenge for operation of the Advanced LIGO and Advanced VIRGO interferometers, reducing optical efficiency, which limits…

Instrumentation and Methods for Astrophysics · Physics 2021-01-27 Carl D Blair , Yuri Levin , Eric Thrane

We present a calculation of the maximum sensitivity achievable by the LIGO Gravitational wave detector in construction, due to limiting thermal noise of its suspensions. We present a method to calculate thermal noise that allows the…

General Relativity and Quantum Cosmology · Physics 2009-10-31 Gabriela González

Seismic noise will be the dominant source of noise at low frequencies for ground based gravitational wave detectors, such as LIGO now under construction. Future interferometers installed at LIGO plan to use at least a double pendulum…

General Relativity and Quantum Cosmology · Physics 2009-10-31 Mark A. Beilby , Gabriela Gonzalez , Michelle Duffy , Amber Stuver , Jennifer Poker

The operation of an interferometer for gravitational waves detection requires sophisticated feedback controls in many parts of the apparatus. The aim of this lecture is to introduce the types of problems to be faced in this line of…

General Relativity and Quantum Cosmology · Physics 2017-08-23 Giovanni Losurdo

Interferometric gravitational wave detectors are devoted to pick up the effect induced on masses by gravitational waves. The variations of the length dividing two mirrors is measured through a laser interferometric technique. The Brownian…

Classical Physics · Physics 2009-10-31 Giseppe Curci , Erika D'Ambrosio

We present measurements of thermal noise in niobium and aluminium flexures. Our measurements cover the audio frequency band from 10Hz to 10kHz, which is of particular relevance to ground-based interferometric gravitational wave detectors,…

We present a theoretical estimate of the atmospheric Newtonian noise due to fluctuations of atmospheric mass densities generated by acoustic and turbulent phenomena and we determine the relevance of such noise in the laser-interferometric…

General Relativity and Quantum Cosmology · Physics 2009-12-16 Carlo Cafaro , S. A. Ali

Mirror thermal noise is and will remain one of the main limitations to the sensitivity of gravitational wave detectors based on laser interferometers. We report about projected mirror thermal noise due to losses in the mirror coatings and…

General Relativity and Quantum Cosmology · Physics 2009-12-02 Janyce Franc , Nazario Morgado , Raffaele Flaminio , Ronny Nawrodt , Iain Martin , Liam Cunningham , Alan Cumming , Sheila Rowan , James Hough

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

We have developed a scheme for reducing LIGO suspension thermal noise close to violin-mode resonances. The idea is to monitor directly the thermally-induced motion of a small portion of (a ``point'' on) each suspension fiber, thereby…

General Relativity and Quantum Cosmology · Physics 2009-12-31 D. H. Santamore , Yuri Levin

When ambient seismic waves pass near an interferometric gravitational-wave detector, they induce density perturbations in the earth which produce fluctuating gravitational forces on the interferometer's test masses. These forces mimic a…

General Relativity and Quantum Cosmology · Physics 2009-12-30 Scott A. Hughes , Kip S. Thorne

Gravitational-wave detectors are sensitive not only to astrophysical gravitational waves, but also to the fluctuating Newtonian gravitational forces of moving masses in the ground and air around the detector. This paper studies the…

General Relativity and Quantum Cosmology · Physics 2008-11-26 Teviet Creighton

Current terrestrial gravitational-wave detectors operate at frequencies above 10 Hz. There is strong astrophysical motivation to construct low-frequency gravitational-wave detectors capable of observing 10 mHz - 10Hz signals. While…

General Relativity and Quantum Cosmology · Physics 2017-03-27 Eric Thrane , Russell P Anderson , Yuri Levin , Lincoln D Turner

Quantum fluctuations in the phase and amplitude quadratures of light set limitations on the sensitivity of modern optical instruments. The sensitivity of the interferometric gravitational wave detectors, such as the Advanced Laser…

Optics · Physics 2017-04-26 D. V. Martynov , V. V. Frolov , S. Kandhasamy , K. Izumi , H. Miao , N. Mavalvala , E. D. Hall , R. Lanza , B. P. Abbott , R. Abbott , T. D. Abbott , C. Adams , R. X. Adhikari , S. B. Anderson , A. Ananyeva , S. Appert , K. Arai , S. M. Aston , S. W. Ballmer , D. Barker , B. Barr , L. Barsotti , J. Bartlett , I. Bartos , J. C. Batch , A. S. Bell , J. Betzwieser , G. Billingsley , J. Birch , S. Biscans , C. Biwer , C. D. Blair , R. Bork , A. F. Brooks , G. Ciani , F. Clara , S. T. Countryman , M. J. Cowart , D. C. Coyne , A. Cumming , L. Cunningham , K. Danzmann , C. F. Da Silva Costa , E. J. Daw , D. DeBra , R. T. DeRosa , R. DeSalvo , K. L. Dooley , S. Doravari , J. C. Driggers , S. E. Dwyer , A. Effler , T. Etzel , M. Evans , T. M. Evans , M. Factourovich , H. Fair , A. Fernández Galiana , R. P. Fisher , P. Fritschel , P. Fulda , M. Fyffe , J. A. Giaime , K. D. Giardina , E. Goetz , R. Goetz , S. Gras , C. Gray , H. Grote , K. E. Gushwa , E. K. Gustafson , R. Gustafson , G. Hammond , J. Hanks , J. Hanson , T. Hardwick , G. M. Harry , M. C. Heintze , A. W. Heptonstall , J. Hough , R. Jones , S. Karki , M. Kasprzack , S. Kaufer , K. Kawabe , N. Kijbunchoo , E. J. King , P. J. King , J. S. Kissel , W. Z. Korth , G. Kuehn , M. Landry , B. Lantz , N. A. Lockerbie , M. Lormand , A. P. Lundgren , M. MacInnis , D. M. Macleod , S. Márka , Z. Márka , A. S. Markosyan , E. Maros , I. W. Martin , K. Mason , T. J. Massinger , F. Matichard , R. McCarthy , D. E. McClelland , S. McCormick , G. McIntyre , J. McIver , G. Mendell , E. L. Merilh , P. M. Meyers , J. Miller , R. Mittleman , G. Moreno , G. Mueller , A. Mullavey , J. Munch , L. K. Nuttall , J. Oberling , P. Oppermann , Richard J. Oram , B. O'Reilly , D. J. Ottaway , H. Overmier , J. R. Palamos , H. R. Paris , W. Parker , A. Pele , S. Penn , M. Phelps , V. Pierro , I. Pinto , M. Principe , L. G. Prokhorov , O. Puncken , V. Quetschke , E. A. Quintero , F. J. Raab , H. Radkins , P. Raffai , S. Reid , D. H. Reitze , N. A. Robertson , J. G. Rollins , V. J. Roma , J. H. Romie , S. Rowan , K. Ryan , T. Sadecki , E. J. Sanchez , V. Sandberg , R. L. Savage , R. M. S. Schofield , D. Sellers , D. A. Shaddock , T. J. Shaffer , B. Shapiro , P. Shawhan , D. H. Shoemaker , D. Sigg , B. J. J. Slagmolen , B. Smith , J. R. Smith , B. Sorazu , A. Staley , K. A. Strain , D. B. Tanner , R. Taylor , M. Thomas , P. Thomas , K. A. Thorne , E. Thrane , C. I. Torrie , G. Traylor , G. Vajente , G. Valdes , A. A. van Veggel , A. Vecchio , P. J. Veitch , K. Venkateswara , T. Vo , C. Vorvick , M. Walker , R. L. Ward , J. Warner , B. Weaver , R. Weiss , P. Weßels , B. Willke , C. C. Wipf , J. Worden , G. Wu , H. Yamamoto , C. C. Yancey , Hang Yu , Haocun Yu , L. Zhang , M. E. Zucker , J. Zweizig

Among all forms of routine human activity, the one which produces the strongest gravity-gradient noise in interferometric gravitational-wave detectors (e.g. LIGO) is the beginning and end of weight transfer from one foot to the other during…

General Relativity and Quantum Cosmology · Physics 2009-12-30 Kip S. Thorne , Carolee J. Winstein

We consider a recent scheme of gravitational wave detection using atomic interferometers as inertial sensors, and reinvestigate its configuration using the concept of sensitivity functions. We show that such configuration can suppress noise…

General Relativity and Quantum Cosmology · Physics 2015-10-20 Biao Tang , Baocheng Zhang , Lin Zhou , Jin Wang , Mingsheng Zhan
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