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KAGRA is the first km-scale gravitational wave detector to be constructed underground and employ cryogenics to cool down its test masses. While the underground location provides a quiet site with low seismic noise, the cooling…

Instrumentation and Detectors · Physics 2023-02-15 Rishabh Bajpai , Takayuki Tomaru , Toshikazu Suzuki , Kazuhiro Yamamoto , Takafumi Ushiba , Tohru Honda

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

This paper presents an analysis of the conceptual design of a novel silicon suspension for the cryogenic test-mass mirrors of the low-frequency detector of the Einstein Telescope gravitational-wave observatory. In traditional suspensions,…

KAGRA uses cryogenics to cool its sapphire test masses down to 20 K to reduce the thermal noise. However, cryocooler vibration and structural resonances of the cryostat couple to test mass and can contaminate the detector sensitivity. We…

Instrumentation and Detectors · Physics 2022-07-05 Rishabh Bajpai , Takayuki Tomaru , Nobuhiro Kimura , Takafumi Ushiba , Kazuhiro Yamamoto , Toshikazu Suzuki , Tohru Honda

KAGRA is a second-generation interferometric gravitational-wave detector with 3-km arms constructed at Kamioka, Gifu in Japan. It is now in its final installation phase, which we call bKAGRA (baseline KAGRA), with scientific observations…

Instrumentation and Methods for Astrophysics · Physics 2019-10-16 KAGRA Collaboration , T. Akutsu , M. Ando , K. Arai , Y. Arai , S. Araki , A. Araya , N. Aritomi , H. Asada , Y. Aso , S. Atsuta , K. Awai , S. Bae , L. Baiotti , M. A. Barton , K. Cannon , E. Capocasa , C-S. Chen , T-W. Chiu , K. Cho , Y-K. Chu , K. Craig , W. Creus , K. Doi , K. Eda , Y. Enomoto , R. Flaminio , Y. Fujii , M. -K. Fujimoto , M. Fukunaga , M. Fukushima , T. Furuhata , A. Hagiwara , S. Haino , K. Hasegawa , K. Hashino , K. Hayama , S. Hirobayashi , E. Hirose , B. H. Hsieh , C-Z. Huang , B. Ikenoue , Y. Inoue , K. Ioka , Y. Itoh , K. Izumi , T. Kaji , T. Kajita , M. Kakizaki , M. Kamiizumi , S. Kanbara , N. Kanda , S. Kanemura , M. Kaneyama , G. Kang , J. Kasuya , Y. Kataoka , N. Kawai , S. Kawamura , T. Kawasaki , C. Kim , J. Kim , J. C. Kim , W. S. Kim , Y. -M. Kim , N. Kimura , T. Kinugawa , S. Kirii , Y. Kitaoka , H. Kitazawa , Y. Kojima , K. Kokeyama , K. Komori , A. K. H. Kong , K. Kotake , R. Kozu , R. Kumar , H-S. Kuo , S. Kuroyanagi , H. K. Lee , H. M. Lee , H. W. Lee , M. Leonardi , C-Y. Lin , F-L. Lin , G. C. Liu , Y. Liu , E. Majorana , S. Mano , M. Marchio , T. Matsui , F. Matsushima , Y. Michimura , N. Mio , O. Miyakawa , A. Miyamoto , T. Miyamoto , K. Miyo , S. Miyoki , W. Morii , S. Morisaki , Y. Moriwaki , T. Morozumi , I. Murakami , M. Musha , K. Nagano , S. Nagano , K. Nakamura , T. Nakamura , H. Nakano , M. Nakano , K. Nakao , Y. Namai , T. Narikawa , L. Naticchioni , L. Nguyen Quynh , W. -T. Ni , A. Nishizawa , Y. Obuchi , T. Ochi , J. J. Oh , S. H. Oh , M. Ohashi , N. Ohishi , M. Ohkawa , K. Okutomi , K. Ono , K. Oohara , C. P. Ooi , S-S. Pan , J. Park , F. E. Peña Arellano , I. Pinto , N. Sago , M. Saijo , Y. Saito , S. Saitou , K. Sakai , Y. Sakai , Y. Sakai , M. Sasai , M. Sasaki , Y. Sasaki , N. Sato , S. Sato , T. Sato , Y. Sekiguchi , N. Seto , M. Shibata , T. Shimoda , H. Shinkai , T. Shishido , A. Shoda , K. Somiya , E. J. Son , A. Suemasa , T. Suzuki , T. Suzuki , H. Tagoshi , H. Tahara , H. Takahashi , R. Takahashi , A. Takamori , H. Takeda , H. Tanaka , K. Tanaka , T. Tanaka , S. Tanioka , E. N. Tapia San Martin , D. Tatsumi , S. Terashima , T. Tomaru , T. Tomura , F. Travasso , K. Tsubono , S. Tsuchida , N. Uchikata , T. Uchiyama , A. Ueda , T. Uehara , S. Ueki , K. Ueno , F. Uraguchi , T. Ushiba , M. H. P. M. van Putten , H. Vocca , S. Wada , T. Wakamatsu , Y. Watanabe , W-R. Xu , T. Yamada , A. Yamamoto , K. Yamamoto , K. Yamamoto , S. Yamamoto , T. Yamamoto , K. Yokogawa , J. Yokoyama , T. Yokozawa , T. H. Yoon , T. Yoshioka , H. Yuzurihara , S. Zeidler , Z. -H. Zhu

Thermal noise from the suspension fibres used in the mirror pendulums in current gravitational wave detectors is a critical noise source. Future detectors will require improved suspension performance with the specific ability to suspend…

Instrumentation and Methods for Astrophysics · Physics 2021-11-18 A. V. Cumming , R. Jones , G. D. Hammond , J. Hough , I. W. Martin , S. Rowan

KAGRA is the first large-scale gravitational-wave detector with cryogenic test masses. Its target sensitivity is limited mostly by quantum noise in the observation frequency band owing to the remarkable reduction of thermal noise at…

Optics · Physics 2020-05-13 Kentaro Somiya

The thermal fluctuation of mirror surfaces is the fundamental limitation for interferometric gravitational wave (GW) detectors. Here, we experimentally demonstrate for the first time a reduction in a mirror's thermal fluctuation in a GW…

Gravitational wave detectors, such as KAGRA, require complex mirror suspension systems to reach high sensitivity. One particular concern in these suspensions is the presence of crackling noise, where motion of the steel crystal structure…

Instrumentation and Detectors · Physics 2021-10-04 Yuhang Zhao , Shin Kirii , Yingtao Liu , Takashi Uchiyama , Ryutaro Takahashi , Seiji Kawamura

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

KAGRA is a new gravitational wave detector which aims to begin joint observation with Advanced LIGO and Advanced Virgo from late 2019. Here, we present KAGRA's possible upgrade plans to improve the sensitivity in the decade ahead. Unlike…

We present the design and commissioning of a cryogenic low-vibration test facility that measures displacement noise from a gram-scale silicon cantilever at the level of 10$^{-16}\, \mathrm{m/\sqrt{Hz}}$ at 1kHz. A volume of $\sim$36 litres…

Instrumentation and Detectors · Physics 2025-08-28 D. P. Kapasi , T. G. McRae , J. Eichholz , P. A. Altin , D. E. McClelland , B. J. J. Slagmolen

It has been reported that treating music wire (high carbon steel wire) by cooling to cryogenic temperatures can enhance its mechanical properties with particular reference to those properties important for musical performance. We use such…

Instrumentation and Methods for Astrophysics · Physics 2015-09-30 A. Heptonstall , M. Waller , N. A. Robertson

Thermodynamically induced length fluctuations of high-reflectivity mirror coatings put a fundamental limit on sensitivity and stability of precision optical interferometers like gravitational wave detectors and ultra-stable lasers. The main…

Cooling down test masses to cryogenic temperatures is a way to reduce the thermal noise of gravitational wave detectors. Crystalline materials are considered the most promising materials for fabricating cryogenic test masses and their…

We report on the current status of CLIO (Cryogenic Laser Interferometer Observatory), which is a prototype interferometer for LCGT (Large Scale Cryogenic Gravitational-Wave Telescope). LCGT is a Japanese next-generation interferometric…

Suspension thermal modes in interferometric gravitational-wave detectors produce narrow, high-Q spectral lines that can contaminate gravitational searches and bias parameter estimation. In KAGRA, cryogenic mirrors are held by thick…

General Relativity and Quantum Cosmology · Physics 2025-10-09 Lucas Moisset , Marco Meyer-Conde , Christopher Allene , Yusuke Sakai , Dan Chen , Nobuyuki Kanda , Hirotaka Takahashi

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

Future gravitational wave detectors (GWDs) such as Advanced LIGO upgrades and the Einstein Telescope are planned to operate at cryogenic temperatures using crystalline silicon (cSi) test-mass mirrors at an operation wavelength of 1550 nm.…

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