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Related papers: Control System Design for the LIGO Pre-stabilized …

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We report long-term laser frequency stabilization using only the target laser and a pair of 5 m fiber interferometers, one as a frequency reference and the second as a sensitive thermometer to stabilize the frequency reference. When used to…

Instrumentation and Detectors · Physics 2015-09-10 Jia Kong , Vito Giovanni Lucivero , Ricardo Jimenez-Martinez , Morgan W. Mitchell

We describe the angular sensing and control of the 4 km detectors of the Laser Interferometer Gravitational-wave Observatory (LIGO). The culmination of first generation LIGO detectors, Enhanced LIGO operated between 2009 and 2010 with about…

Parametric instabilities have long been studied as a potentially limiting effect in high-power interferometric gravitational wave detectors. Until now, however, these instabilities have never been observed in a kilometer-scale…

Arm locking is one of the key technologies to suppress the laser phase noise in spaced-based gravitational waves observatories. Since arm locking was proposed, phase margin criterion was always used as the fundamental design strategy for…

General Relativity and Quantum Cosmology · Physics 2023-09-12 Yi Zhang , Mingzhe Li , Tong Wang , Xinyi Zhao , Long Ma , Shaobo Fang , Ming Xin

The goal of the Laser Interferometric Gravitational-Wave Observatory (LIGO) is to detect and study gravitational waves of astrophysical origin. Direct detection of gravitational waves holds the promise of testing general relativity in the…

General Relativity and Quantum Cosmology · Physics 2009-09-29 The LIGO Scientific Collaboration , B. Abbott

Laser frequency stabilization is a critical part of the interferometry measurement system of space-based gravitational wave observatories such as the Laser Interferometer Space Antenna (LISA). Arm locking as a proposed frequency…

General Relativity and Quantum Cosmology · Physics 2015-06-18 Yinan Yu , Shawn Mitryk , Guido Mueller

The ISAC polarized beam facility uses a Ti:Sapphire laser for producing spin-polarized beams of short-lived radioactive isotopes, initially 7Li. The laser power and spectral content must be tightly controlled and monitored. The control…

Accelerator Physics · Physics 2007-05-23 R. Nussbaumer , D. Dale , H. Hui , J. Richards , P. Levy

An inexpensive, easily programmed microcontroller is demonstrated for the fast frequency stabilization of an infrared fiber laser. The microcontroller manages all digitalization and processing, with external circuitry only providing…

Atomic Physics · Physics 2009-05-18 M. R. Dietrich , B. B. Blinov

Metrology experiments can be limited by the noise produced by the laser involved via small fluctuations in the laser's power or frequency. Typically, active power stabilization schemes consisting of an in-loop sensor and a feedback control…

Laser frequency noise suppression is a critical requirement for the Laser Interferometer Space Antenna (LISA) mission to detect gravitational waves. The baseline laser stabilization is achieved using cavity pre-stabilization and a…

General Relativity and Quantum Cosmology · Physics 2024-06-05 Jobin Thomas Valliyakalayil , Andrew Wade , David Rabeling , Jue Zhang , Daniel Shaddock , Kirk McKenzie

Laser frequency stabilization is notably one of the major challenges on the way to a space-borne gravitational wave observatory. The proposed Laser Interferometer Space Antenna (LISA) is presently under development in an ESA, NASA…

General Relativity and Quantum Cosmology · Physics 2015-06-25 Markus Herz

For the laser interferometer space antenna (LISA) to reach it's design sensitivity, the coupling of the free running laser frequency noise to the signal readout must be reduced by more than 14 orders of magnitude. One technique employed to…

General Relativity and Quantum Cosmology · Physics 2009-12-17 Kirk McKenzie , Robert E. Spero , Daniel A. Shaddock

Currently planned second-generation gravitational-wave laser interferometers such as Advanced LIGO exploit the extensively investigated signal-recycling (SR) technique. Candidate Advanced LIGO configurations are usually designed to have two…

General Relativity and Quantum Cosmology · Physics 2009-02-23 Henning Rehbein , Helge Mueller-Ebhardt , Kentaro Somiya , Stefan L. Danilishin , Roman Schnabel , Karsten Danzmann , Yanbei Chen

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

As the first generation of laser interferometric gravitational wave detectors near operation, research and development has begun on increasing the instrument's sensitivity while utilizing the existing infrastructure. In the Laser…

General Relativity and Quantum Cosmology · Physics 2009-11-07 Ryan Lawrence , Michael Zucker , Peter Fritschel , Phil Marfuta , David Shoemaker

Gravitational waves produced at kilohertz frequencies in the aftermath of a neutron star collision can shed light on the behavior of matter at extreme temperatures and densities that are inaccessible to laboratory experiments.…

Instrumentation and Methods for Astrophysics · Physics 2021-01-20 Dhruva Ganapathy , Lee McCuller , Jameson Graef Rollins , Evan D. Hall , Lisa Barsotti , Matthew Evans

High-power ultra-low noise single-mode single-frequency lasers are in great demand for interferometric metrology. Robust, compact all-fiber lasers represent one of the most promising technologies to replace the current laser sources in use…

We demonstrate a Raman laser system based on phase modulation technology and phase feedback control. The two laser beams with frequency difference of 6.835 GHz are modulated using electro-optic and acousto-optic modulators, respectively.…

Optics · Physics 2017-03-08 Wei Li , Xiong Pan , Ningfang Song , Xiaobin Xu , Xiangxiang Lu

The Laser Interferometer Gravitational-wave Observatory (LIGO) consists of two identical yet independent, widely-separated, long-baseline gravitational-wave detectors. Each Advanced LIGO detector consists of complex optical-mechanical…

Instrumentation and Methods for Astrophysics · Physics 2016-08-12 Jameson Graef Rollins

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