Residual amplitude modulation at the \(10^{-7}\) level for ultra-stable lasers

The stabilization of lasers on ultra-stable optical cavities by the Pound-Drever-Hall (PDH) technique is a widely used method. The PDH method relies on the phase-modulation of the laser, which is usually performed by an electro-optic modulator (EOM). When approaching the \(10^{-16}\) level, this tec...

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Published inarXiv.org
Main Authors Gillot, Jonathan, Santerelli Falzon Tetsing-Talla, Denis, Séverine, Goavec-Merou, Gwenhaël, Millo, Jacques, Lacroûte, Clément, Kersalé, Yann
Format Paper
LanguageEnglish
Published Ithaca Cornell University Library, arXiv.org 07.06.2022
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Summary:The stabilization of lasers on ultra-stable optical cavities by the Pound-Drever-Hall (PDH) technique is a widely used method. The PDH method relies on the phase-modulation of the laser, which is usually performed by an electro-optic modulator (EOM). When approaching the \(10^{-16}\) level, this technology requires an active control of the residual amplitude modulation (RAM) generated by the EOM in order to bring the frequency stability of the laser down to the thermal noise limit of the ultra-stable cavity. In this article, we report on the development of an active system of RAM reduction based on a free space EOM, which is used to perform PDH-stabilization of a laser on a cryogenic silicon cavity. A RAM stability of \(1.4 \times 10^{-7}\) is obtained by employing a digital servo that stabilizes the EOM DC electric field, the crystal temperature and the laser power. Considering an ultra-stable cavity with a finesse of \(2.5\times 10^5\), this RAM level would contribute to the fractional frequency instability at the level of about \(5\times 10^{-19}\), well below the state of the art thermal noise limit of a few \( 10^{-17}\).
ISSN:2331-8422
DOI:10.48550/arxiv.2206.03332