Details
Originalsprache | Englisch |
---|---|
Aufsatznummer | 135001 |
Fachzeitschrift | Classical and quantum gravity |
Jahrgang | 39 |
Ausgabenummer | 13 |
Frühes Online-Datum | 31 Mai 2022 |
Publikationsstatus | Veröffentlicht - 7 Juli 2022 |
Extern publiziert | Ja |
Abstract
With a relative length measurement precision of better than 10-23, gravitational wave interferometers are the most precise instruments that have ever been built. With this enormous sensitivity many noise sources potentially effect gravitational wave detector sensitivity, each of which must be investigated to ensure confidence in design sensitivity. We present calculations of photoelastic noise as well as thermo refractive noise in the beam splitter and the input test masses in Einstein telescope (ET). It turns out that the amplitude of the photoelastic noise in the ET low-frequency detector is about five orders of magnitude below the maximum design sensitivity and five orders of magnitude below that of the ET high-frequency detector, whereas thermo refractive noise impairs the design sensitivity by approximately 20%.
ASJC Scopus Sachgebiete
- Physik und Astronomie (insg.)
- Physik und Astronomie (sonstige)
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in: Classical and quantum gravity, Jahrgang 39, Nr. 13, 135001, 07.07.2022.
Publikation: Beitrag in Fachzeitschrift › Artikel › Forschung › Peer-Review
}
TY - JOUR
T1 - Thermally induced refractive index fluctuations in transmissive optical components and their influence on the sensitivity of Einstein telescope
AU - Meyer, Jan
AU - Dickmann, Walter
AU - Kroker, Stefanie
AU - Gaedtke, Mika
AU - Dickmann, Johannes
N1 - Funding Information: This work is partially funded by the Project 17FUN05 ‘PhotOQuant’ within the Programme EMPIR. The EMPIR initiative is co-founded by the European Union’s Horizon 2020 Research and Innovation Program and the EMPIR Participating Countries. The authors also acknowledge support by the Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) under Germanys Excellence Strategy—EXC-2123 QuantumFrontiers—390837967.
PY - 2022/7/7
Y1 - 2022/7/7
N2 - With a relative length measurement precision of better than 10-23, gravitational wave interferometers are the most precise instruments that have ever been built. With this enormous sensitivity many noise sources potentially effect gravitational wave detector sensitivity, each of which must be investigated to ensure confidence in design sensitivity. We present calculations of photoelastic noise as well as thermo refractive noise in the beam splitter and the input test masses in Einstein telescope (ET). It turns out that the amplitude of the photoelastic noise in the ET low-frequency detector is about five orders of magnitude below the maximum design sensitivity and five orders of magnitude below that of the ET high-frequency detector, whereas thermo refractive noise impairs the design sensitivity by approximately 20%.
AB - With a relative length measurement precision of better than 10-23, gravitational wave interferometers are the most precise instruments that have ever been built. With this enormous sensitivity many noise sources potentially effect gravitational wave detector sensitivity, each of which must be investigated to ensure confidence in design sensitivity. We present calculations of photoelastic noise as well as thermo refractive noise in the beam splitter and the input test masses in Einstein telescope (ET). It turns out that the amplitude of the photoelastic noise in the ET low-frequency detector is about five orders of magnitude below the maximum design sensitivity and five orders of magnitude below that of the ET high-frequency detector, whereas thermo refractive noise impairs the design sensitivity by approximately 20%.
KW - photoelasticity
KW - gravitational wave detection
KW - thermal noise
KW - Einstein telescope
UR - http://www.scopus.com/inward/record.url?scp=85131693025&partnerID=8YFLogxK
U2 - 10.1088/1361-6382/ac6e21
DO - 10.1088/1361-6382/ac6e21
M3 - Article
VL - 39
JO - Classical and quantum gravity
JF - Classical and quantum gravity
SN - 0264-9381
IS - 13
M1 - 135001
ER -