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Bulletin of the American Physical Society

Transient enhancement of the nonlinear atom-photon coupling via recoil-induced resonances

Joel A. Greenberg, Daniel J. Gauthier

Published May 22, 2009• 0 citations
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Transient dynamics and momentum redistribution in cold atoms via recoil-induced resonances

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We use an optically dense anisotropic magneto-optical trap to study recoil-induced resonances (RIRs) in the transient high-gain regime. We find that two distinct mechanisms govern the atomic dynamics: the finite, frequency-dependent atomic response time and momentum-space population redistribution. At low input probe intensities, the residual Doppler width of the atoms, combined with the finite atomic response time, result in a linear transient hysteretic effect that modifies the locations, widths, and magnitudes of the resulting gain spectra depending on the sign of the scan chirp. When larger intensities (i.e., greater than a few $\ensuremath{\mu}\text{W}/{\text{cm}}^{2}$) are incident on the atomic sample for several $\ensuremath{\mu}\text{s}$, hole burning in the atomic sample momentum distribution leads to a coherent population redistribution that persists for approximately $100\text{ }\ensuremath{\mu}\text{s}$. We propose using RIRs to engineer the atomic momentum distribution to enhance the nonlinear atom-photon coupling. We present a numerical model and compare the calculated and experimental results to verify our interpretation.

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We use an optically dense anisotropic magneto-optical trap to study recoil-induced resonances (RIRs) in the transient high-gain regime. We find that two distinct mechanisms govern the atomic dynamics: the finite, frequency-dependent atomic response time and momentum-space population redistribution. At low input probe intensities, the residual Doppler width of the atoms, combined with the finite atomic response time, result in a linear transient hysteretic effect that modifies the locations, widths, and magnitudes of the resulting gain spectra depending on the sign of the scan chirp. When larger intensities (i.e., greater than a few $\ensuremath{\mu}\text{W}/{\text{cm}}^{2}$) are incident on the atomic sample for several $\ensuremath{\mu}\text{s}$, hole burning in the atomic sample momentum distribution leads to a coherent population redistribution that persists for approximately $100\text{ }\ensuremath{\mu}\text{s}$. We propose using RIRs to engineer the atomic momentum distribution to enhance the nonlinear atom-photon coupling. We present a numerical model and compare the calculated and experimental results to verify our interpretation.
We demonstrate a method to directly observe the dynamics of motion of cold atoms in an optical standing wave using a recoil-induced resonance. By detecting a transient response of this resonance, we observed the interaction between an atomic population grating and a periodic optical potential. Using this method, we investigated the lifetime of the atomic grating under various conditions in the optical potential. As a result, we obtained the appropriate conditions for the long lifetime and observed the narrowest linewidth in the recoil-induced resonance corresponding to the atomic temperature of 4.4\ifmmode\pm\else\textpm\fi{}0.3 \ensuremath{\mu}K for 87Rb^{87}\mathrm{Rb}87Rb atoms.