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Physical Review A

Temperature sensitivity of the cavity scale factor enhancement for a Gaussian absorption resonance

Krishna Myneni, David D. Smith, Hongrok Chang, H. A. Luckay

Published Nov 19, 2015• 11 citations
Publisher

Abstract

We derive analytic expressions for the on-resonant cavity scale factor enhancement dependence on temperature, ${S}_{0}(T)$, for an intracavity medium with a Gaussian absorption resonance. Results are expressed as functions of the cavity parameters and the two resonance parameters: ${\ensuremath{\alpha}}_{0}(T)$, the peak absorption coefficient, and ${\mathrm{\ensuremath{\Gamma}}}_{\ensuremath{\alpha}}^{R}(T)$, the resonance width. A semiempirical model is developed for the temperature-dependent absorption coefficient, ${\ensuremath{\alpha}}_{F}(\mathrm{\ensuremath{\Delta}},T)$, in an alkali-metal-atom vapor cell, and is used to compare the predicted behavior of ${\ensuremath{\alpha}}_{0}(T)$ and ${\mathrm{\ensuremath{\Gamma}}}_{\ensuremath{\alpha}}^{R}(T)$ with the measured values for the $D{}_{2}\phantom{\rule{0.28em}{0ex}}F=2\ensuremath{\rightarrow}{F}^{\ensuremath{'}}$ resonance in $^{87}\mathrm{Rb}$, over the temperature range 298--325 K. Measurements of ${S}_{0}(T)$ in a low-finesse ring cavity, using the same vapor cell as the intracavity dispersive medium, were performed and found to be in agreement with the temperature-dependent behavior predicted by our theory, with quantitative agreement to 2 K for the critical temperature. The practical range of ${S}_{0}$ is found to be limited by the achievable temperature stability of the resonance parameters of the dispersive medium.

DOI
10.1103/physreva.92.053845

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We derive analytic expressions for the on-resonant cavity scale factor enhancement dependence on temperature, S0(T){S}_{0}(T)S0​(T), for an intracavity medium with a Gaussian absorption resonance. Results are expressed as functions of the cavity parameters and the two resonance parameters: \ensuremathα0(T){\ensuremath{\alpha}}_{0}(T)\ensuremathα0​(T), the peak absorption coefficient, and \ensuremathΓ\ensuremathαR(T){\mathrm{\ensuremath{\Gamma}}}_{\ensuremath{\alpha}}^{R}(T)\ensuremathΓ\ensuremathαR​(T), the resonance width. A semiempirical model is developed for the temperature-dependent absorption coefficient, \ensuremathαF(\ensuremathΔ,T){\ensuremath{\alpha}}_{F}(\mathrm{\ensuremath{\Delta}},T)\ensuremathαF​(\ensuremathΔ,T), in an alkali-metal-atom vapor cell, and is used to compare the predicted behavior of \ensuremathα0(T){\ensuremath{\alpha}}_{0}(T)\ensuremathα0​(T) and \ensuremathΓ\ensuremathαR(T){\mathrm{\ensuremath{\Gamma}}}_{\ensuremath{\alpha}}^{R}(T)\ensuremathΓ\ensuremathαR​(T) with the measured values for the D2F=2\ensuremath→F\ensuremath′D{}_{2}\phantom{\rule{0.28em}{0ex}}F=2\ensuremath{\rightarrow}{F}^{\ensuremath{'}}D2​F=2\ensuremath→F\ensuremath′ resonance in 87Rb^{87}\mathrm{Rb}87Rb, over the temperature range 298--325 K. Measurements of S0(T){S}_{0}(T)S0​(T) in a low-finesse ring cavity, using the same vapor cell as the intracavity dispersive medium, were performed and found to be in agreement with the temperature-dependent behavior predicted by our theory, with quantitative agreement to 2 K for the critical temperature. The practical range of S0{S}_{0}S0​ is found to be limited by the achievable temperature stability of the resonance parameters of the dispersive medium.
Enhancement of the response of an optical cavity to a change in optical path length, through the use of an intracavity fast-light medium, has previously been demonstrated experimentally and described theoretically for an atomic vapor cell as the intracavity resonant absorber. This phenomenon may be used to enhance both the scale factor and sensitivity of an optical cavity mode to the change in path length, e.g. in gyroscopic applications. We study the temperature sensitivity of the on-resonant scale factor enhancement, S(sub o), due to the thermal sensitivity of the lower-level atom density in an atomic vapor cell, specifically for the case of the Rb-87 D(sub 2) transition. A semi-empirical model of the temperature-dependence of the absorption profile, characterized by two parameters, a(sub o)(T) and gamma(sub a)(T) allows the temperature-dependence of the cavity response, S(sub o)(T) and dS(sub o)/dT to be predicted over a range of temperature. We compare the predictions to experiment. Our model will be useful in determining the useful range for S(sub o), given the practical constraints on temperature stability for an atomic vapor cell.
We demonstrate for a passive optical cavity containing a dispersive atomic medium, the increase in scale factor near the critical anomalous dispersion is not cancelled by mode broadening or attenuation, resulting in an overall increase in the predicted quantum-noise-limited sensitivity. Enhancements of over two orders of magnitude are measured in the scale factor, which translates to greater than an order-of-magnitude enhancement in the predicted quantum-noise-limited measurement precision, by temperature tuning a low-pressure vapor of non-interacting atoms in a low-finesse cavity close to the critical anomalous dispersion condition. The predicted enhancement in sensitivity is confirmed through Monte-Carlo numerical simulations.
The pushing of the modes of a Fabry-Perot cavity by an intracavity rubidium cell is measured. The scale factor of the modes is increased by the anomalous dispersion and is inversely proportional to the sum of the effective group index and an additional cavity delay factor that arises from the variation of the Rb absorption over a free spectral range. This additional positive feedback further increases the effect of the anomalous dispersion and goes to zero at the lasing threshold. The mode width does not grow as fast as the scale factor as the intracavity absorption is increased resulting in enhanced measurement sensitivities. For absorptions larger than the scale factor pole, the atom-cavity response is multivalued and mode splitting occurs.
This paper presents a theoretical analysis of the optical properties of an optical cavity with both one- and two-photon intracavity absorption loss, without saturation. The cavity two-photon absorption loss per pass is assumed to be small, but otherwise the analysis is general. Analytical results for the cavity transmission as a function of cavity parameters, linear and two-photon intracavity loss, and detuning from resonance are derived and limiting cases discussed. Extraction of the two-photon loss from both cavity ring-down and cavity-enhanced absorption spectroscopy methods is analyzed and the predicted shot-noise limited sensitivities derived and compared. Numerical results are computed using the parameters of a recent experimental intracavity measurement of two-photon absorption of nitrous oxide. The results will be useful in the design and interpretation of cavity-enhanced, two-photon absorption spectroscopy.
We demonstrate the operation of a closed-loop fast-light cavity that allows rapid (~10 ms) measurements of the cavity mode frequency and its uncertainty. We vary the scale factor by temperature tuning the atomic density of an intracavity vapor cell. The cavity remains locked even as the system passes through the critical anomalous dispersion where a pole is observed in the scale factor. Positive and negative scale-factor enhancements as large as |S| ≈70 were obtained. To our knowledge, these are the first experiments that demonstrate a scale-factor enhancement in a closed-loop fast-light device by changing the optical path length, laying the groundwork for the improvement of cavity-based metrology instruments such as optical gyroscopes.