Abstract

In a recent paper [Gorshkov et al., Phys. Rev. Lett. 98, 123601 (2007)], we used a universal physical picture to optimize and demonstrate equivalence between a wide range of techniques for storage and retrieval of photon wave packets in $\ensuremath{\Lambda}$-type atomic media in free space, including the adiabatic reduction of the photon group velocity, pulse-propagation control via off-resonant Raman techniques, and photon-echo-based techniques. In the present paper, we perform the same analysis for the cavity model. In particular, we show that the retrieval efficiency is equal to $C∕(1+C)$ independent of the retrieval technique, where $C$ is the cooperativity parameter. We also derive the optimal strategy for storage and, in particular, demonstrate that at any detuning one can store, with the optimal efficiency of $C∕(1+C)$, any smooth input mode satisfying $TC\ensuremath{\gamma}⪢1$ and a certain class of resonant input modes satisfying $TC\ensuremath{\gamma}\ensuremath{\sim}1$, where $T$ is the duration of the input mode and $2\ensuremath{\gamma}$ is the transition linewidth. In the two subsequent papers of the series, we present the full analysis of the free-space model and discuss the effects of inhomogeneous broadening on photon storage.

Highlights

  • The faithful storage of a traveling light pulse in an atomic memory and the subsequent retrieval of the state are currently being pursued in a number of laboratories around the world [1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12, 13, 14, 15]

  • We have treated in detail the storage and retrieval of photons in homogeneously broadened Λ-type atomic media enclosed in a running-wave cavity

  • We have shown that, provided that no excitations are left in the atoms at the end of the retrieval process, the retrieval efficiency is independent of the control and the detuning and is equal to C/(1 + C)

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Summary

INTRODUCTION

The faithful storage of a traveling light pulse in an atomic memory and the subsequent retrieval of the state are currently being pursued in a number of laboratories around the world [1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12, 13, 14, 15]. We show in the present paper how, for the case of a single incoming spatiotemporal field mode, proper control field shaping can be used to achieve the same optimal efficiency independent of detuning This effectively makes the Raman, the resonant, and the intermediate regimes all exhibit reduced sensitivity to spontaneous emission. [21], in the present paper, and in papers II and III by demonstrating that the ideas of time reversal can be used to optimize photon storage even when the dynamics of the system are not completely reversible and when the ideal unit efficiency cannot be achieved This is the case for finite cooperativity parameter C in the cavity model and for finite optical depth d in the free-space model. In the Appendixes, we present some details omitted in the main text

FIGURE OF MERIT
OPTIMAL STRATEGY FOR STORAGE AND RETRIEVAL
Adiabatic retrieval
Adiabatic storage
Adiabaticity conditions
FAST RETRIEVAL AND STORAGE
SUMMARY
VIII. ACKNOWLEDGMENTS
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