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Springer proceedings in physics

Modulation Spectroscopy and Cavity QED

Mark G. Raizen, Robert J. Thompson, Robert J. Brecha, Harry J. Kimble, H. J. Carmichael

Published Jan 1, 1989• 0 citations
Publisher
DOI
10.1007/978-3-642-74951-3_17

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We study the nonlinear interaction of a cold sample of 88Sr^{88}\mathrm{Sr}88Sr atoms coupled to a single mode of a low finesse optical cavity in the so-called bad cavity limit, and we investigate the implications for applications to laser stabilization. The atoms are probed on the weak intercombination line $|5{s}^{2}{\phantom{\rule{0.16em}{0ex}}}^{1}{S}_{0}\ensuremath{\rangle}\phantom{\rule{0.16em}{0ex}}\ensuremath{-}\phantom{\rule{0.16em}{0ex}}|5s5p{\phantom{\rule{0.16em}{0ex}}}^{3}{P}_{1}\ensuremath{\rangle}$ at 689 nm in a strongly saturated regime. Our measured observables include the atomic induced phase shift and absorption of the light field transmitted through the cavity represented by the complex cavity transmission coefficient. We demonstrate high signal-to-noise-ratio measurements of both quadratures---the cavity transmitted phase and absorption---by employing frequency modulation (FM) spectroscopy (noise-immune cavity-enhanced optical-heterodyne molecular spectroscopy). We also show that when FM spectroscopy is employed in connection with a cavity locked to the probe light, observables are substantially modified compared to the free-space situation in which no cavity is present. Furthermore, the nonlinear dynamics of the phase dispersion slope is experimentally investigated, and the optimal conditions for laser stabilization are established. Our experimental results are compared to state-of-the-art cavity QED theoretical calculations.