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All gravitational-wave observatories (GWOs) have been using the laser wavelength of 1064 nm. Ultra-stable laser devices are at the sites of GEO 600, Kagra, LIGO and Virgo. Since 2019, not only GEO 600 but also LIGO and Virgo have been using…

Thermal noise of the dielectric mirror coatings can limit laser-optical high-precision measurements. Coatings made of amorphous silicon and silicon nitride could provide a remedy for both gravitational-wave detectors and optical clocks.…

Current interferometric gravitational wave detectors use the combination of quasi-monochromatic, continuous-wave laser light at 1064 nm and fused silica test masses at room temperature. Detectors of the third generation, such as the…

Ultra-stable laser light is essential for high-precision interferometric measurements, in particular for the next generation of gravitational wave detectors, where high power lasers with unprecedented low power and frequency noise are…

Optics · Physics 2025-11-11 Henning Vahlbruch , Fabian Meylahn , Benno Willke

We have developed a Watt-level single-frequency tunable fiber laser in the 915-937 nm spectral window. The laser is based on a neodymium-doped fiber master oscillator power amplifier architecture, with two amplification stages using a 20 mW…

Future ground-based gravitational-wave detectors are slated to detect black hole and neutron star collisions from the entire stellar history of the universe. To achieve the designed detector sensitivities, frequency noise from the laser…

Instrumentation and Detectors · Physics 2021-12-07 Craig Cahillane , Georgia Mansell , Daniel Sigg

We report on the high power amplification of 1064nm linearly-polarized laser in all-fiber polarization-maintained MOPA, which can operate at output power level of 1.3kW. The main amplifier was pumped with six 915nm laser diodes, and the…

Optics · Physics 2015-05-29 Rumao Tao , Pengfei Ma , Xiaolin Wang , Pu Zhou , Zejin Liu

We demonstrate the potential of new adaptive optical technology to expand the detection horizon of gravitational-wave observatories. Achieving greater quantum-noise-limited sensitivity to spacetime strain hinges on achieving higher…

The Laser Interferometer Gravitational Wave Observatory (LIGO) consists of two widely separated 4 km laser interferometers designed to detect gravitational waves from distant astrophysical sources in the frequency range from 10 Hz to 10…

Instrumentation and Methods for Astrophysics · Physics 2018-02-13 D. V. Martynov , E. D. Hall , B. P. Abbott , R. Abbott , T. D. Abbott , C. Adams , R. X. Adhikari , R. A. Anderson , S. B. Anderson , K. Arai , M. A. Arain , S. M. Aston , L. Austin , S. W. Ballmer , M. Barbet , D. Barker , B. Barr , L. Barsotti , J. Bartlett , M. A. Barton , I. Bartos , J. C. Batch , A. S. Bell , I. Belopolski , J. Bergman , J. Betzwieser , G. Billingsley , J. Birch , S. Biscans , C. Biwer , E. Black , C. D. Blair , C. Bogan , C. Bond , R. Bork , D. O. Bridges , A. F. Brooks , D. D. Brown , L. Carbone , C. Celerier , G. Ciani , F. Clara , D. Cook , S. T. Countryman , M. J. Cowart , D. C. Coyne , A. Cumming , L. Cunningham , M. Damjanic , R. Dannenberg , 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 , D. Feldbaum , R. P. Fisher , S. Foley , M. Frede , A. Freise , P. Fritschel , V. V. Frolov , P. Fulda , M. Fyffe , V. Galdi , J. A. Giaime , K. D. Giardina , J. R. Gleason , R. Goetz , S. Gras , C. Gray , R. J. S. Greenhalgh , H. Grote , C. J. Guido , K. E. Gushwa , E. K. Gustafson , R. Gustafson , G. Hammond , J. Hanks , J. Hanson , T. Hardwick , G. M. Harry , K. Haughian , J. Heefner , M. C. Heintze , A. W. Heptonstall , D. Hoak , J. Hough , A. Ivanov , K. Izumi , M. Jacobson , E. James , R. Jones , S. Kandhasamy , S. Karki , M. Kasprzack , S. Kaufer , K. Kawabe , W. Kells , N. Kijbunchoo , E. J. King , P. J. King , D. L. Kinzel , J. S. Kissel , K. Kokeyama , W. Z. Korth , G. Kuehn , P. Kwee , M. Landry , B. Lantz , A. Le Roux , B. M. Levine , J. B. Lewis , V. Lhuillier , N. A. Lockerbie , M. Lormand , M. J. Lubinski , A. P. Lundgren , T. MacDonald , M. MacInnis , D. M. Macleod , M. Mageswaran , K. Mailand , S. M'arka , Z. M'arka , A. S. Markosyan , E. Maros , I. W. Martin , R. M. Martin , J. N. Marx , K. Mason , T. J. Massinger , F. Matichard , N. Mavalvala , R. McCarthy , D. E. McClelland , S. McCormick , G. McIntyre , J. McIver , E. L. Merilh , M. S. Meyer , P. M. Meyers , J. Miller , R. Mittleman , G. Moreno , C. L. Mueller , G. Mueller , A. Mullavey , J. Munch , P. G. Murray , L. K. Nuttall , J. Oberling , J. O'Dell , P. Oppermann , Richard J. Oram , B. O'Reilly , C. Osthelder , D. J. Ottaway , H. Overmier , J. R. Palamos , H. R. Paris , W. Parker , Z. Patrick , A. Pele , S. Penn , M. Phelps , M. Pickenpack , V. Piero , I. Pinto , J. Poeld , M. Principe , L. Prokhorov , O. Puncken , V. Quetschke , E. A. Quintero , F. J. Raab , H. Radkins , P. Raffai , C. R. Ramet , C. M. Reed , 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 , V. Sannibale , R. L. Savage , R. M. S. Schofield , B. Schultz , P. Schwinberg , D. Sellers , A. Sevigny , D. A. Shaddock , Z. Shao , B. Shapiro , P. Shawhan , D. H. Shoemaker , D. Sigg , B. J. J. Slagmolen , J. R. Smith , M. R. Smith , N. D. Smith-Lefebvre , B. Sorazu , A. Staley , A. J. Stein , A. Stochino , K. A. Strain , R. Taylor , M. Thomas , P. Thomas , K. A. Thorne , E. Thrane , K. V. Tokmakov , C. I. Torrie , G. Traylor , G. Vajente , G. Valdes , A. A. van Veggel , M. Vargas , A. Vecchio , P. J. Veitch , K. Venkateswara , T. Vo , C. Vorvick , S. J. Waldman , M. Walker , R. L. Ward , J. Warner , B. Weaver , R. Weiss , T. Welborn , P. Wessels , C. Wilkinson , P. A. Willems , L. Williams , B. Willke , I. Wilmut , L. Winkelmann , C. C. Wipf , J. Worden , G. Wu , H. Yamamoto , C. C. Yancey , H. Yu , L. Zhang , M. E. Zucker , J. Zweizig

Twenty years ago, construction began on the Laser Interferometer Gravitational-wave Observatory (LIGO). Advanced LIGO, with a factor of ten better design sensitivity than Initial LIGO, will begin taking data this year, and should soon make…

Instrumentation and Methods for Astrophysics · Physics 2015-05-15 Sheila E. Dwyer , Daniel Sigg , Stefan Ballmer , Lisa Barsotti , Nergis Mavalvala , Matthew Evans

Ultra-stable, quasi-monochromatic laser light forms the basis for high-precision interferometric measurements, e.g. for observing gravitational waves and for time keeping with optical clocks. Optical frequency conversion enables access to…

A universal amplification scheme of ultra-small phase based on weak measurements is given and a weak measurements amplification based laser interferometer gravitational-wave observatory (WMA-LIGO) is suggested. The WMA-LIGO has potential to…

Quantum Physics · Physics 2017-11-03 Meng-Jun Hu , Yong-Sheng Zhang

Thin-disk lasers (TDLs) have made spectacular progress in the last decades both in continuous-wave and ultrafast operation. Nowadays, single thin-disk oscillators with > 16 kW of continuous-wave (CW)-power have been demonstrated and…

Optics · Physics 2021-11-29 Sergei Tomilov , Martin Hoffmann , Yicheng Wang , Clara J. Saraceno

This article reviews current efforts and plans for gravitational-wave detection, the gravitational-wave sources that might be detected, and the information that the detectors might extract from the observed waves. Special attention is paid…

General Relativity and Quantum Cosmology · Physics 2007-05-23 Kip S. Thorne

Achieving the quantum noise targets of third-generation detectors will require 10 dB of squeezed-light enhancement as well as megawatt laser power in the interferometer arms - both of which require unprecedented control of the internal…

Instrumentation and Methods for Astrophysics · Physics 2022-05-31 Jonathan W. Richardson , Swadha Pandey , Edita Bytyqi , Tega Edo , Rana X. Adhikari

We present a narrow linewidth continuous laser source with over 11 Watts of output power at 780nm, based on single-pass frequency doubling of an amplified 1560nm fibre laser with 36% efficiency. This source offers a combination of high…

Gravitational wave (GW) detection in space is aimed at low frequency band (100 nHz - 100 mHz) and middle frequency band (100 mHz - 10 Hz). The science goals are the detection of GWs from (i) Supermassive Black Holes; (ii) Extreme-Mass-Ratio…

Instrumentation and Methods for Astrophysics · Physics 2016-12-06 Wei-Tou Ni

We report the development of a tunable, low-noise, all-fiber, single-frequency, linearly polarized high-power master oscillator power amplifier operating over 20 nm, from 1017 nm down to 997 nm. Using Ytterbium highly-doped silica fiber…

We report the operation of an optical parametric amplifier (OPA) capable of producing gigawatt peak-power laser pulses with tunable wavelength in either the visible or near-infrared spectrum. The OPA has two distinct operation modes (i)…

TAMA300, an interferometric gravitational-wave detector with 300-m baseline length, has been developed and operated with sufficient sensitivity to detect gravitational-wave events within our galaxy and sufficient stability for observations;…

Astrophysics · Physics 2009-07-09 Masaki Ando , the TAMA collaboration
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