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  5. Tunable coherence laser interferometry: Demonstrating 40 dB of stray light suppression and compatibility with resonant optical cavities

Tunable coherence laser interferometry: Demonstrating 40 dB of stray light suppression and compatibility with resonant optical cavities

Publication date
2025-05-28
Document type
Forschungsartikel
Author
Voigt, Daniel
Eggers, Leonie
Isleif, Katharina-Sophie  
Koehlenbeck, S. M.
Ast, M.
Gerberding, Oliver
Organisational unit
Messtechnik  
DOI
10.1103/physrevlett.134.213802
URI
https://openhsu.ub.hsu-hh.de/handle/10.24405/23054
Publisher
American Physical Society
Series or journal
Physical Review Letters
ISSN
0031-9007
Periodical volume
134
Periodical issue
21
Article ID
213802
Peer-reviewed
✅
Part of the university bibliography
✅
Additional Information
Language
English
Abstract
A major limitation of laser interferometers using continuous wave lasers are parasitic light fields, such as ghost beams, scattered or stray light, that can cause nonlinear noise. This is especially relevant for laser interferometric ground-based gravitational wave detectors. Increasing their sensitivity, particularly at frequencies below 10 Hz, is threatened by the influence of parasitic photons. These can up-convert low-frequency disturbances into phase and amplitude noise inside the relevant measurement band. By artificially tuning the coherence of the lasers, using pseudo-random-noise (PRN) phase modulations, this influence of parasitic fields can be suppressed. As it relies on these fields traveling different paths, it does not sacrifice the coherence for the intentional interference. We demonstrate the feasibility of this technique experimentally, achieving noise suppression levels of 40 dB in a Michelson interferometer with an artificial coherence length below 30 cm. We probe how the suppression depends on the delay mismatch and length of the PRN sequence. We also prove that optical resonators can be operated in the presence of PRN modulation by measuring the behavior of a linear cavity with and without such a modulation. By matching the resonators round-trip length and the PRN sequence repetition length, the classic response is recovered.
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Published version
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