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arXiv:quant-ph/0202073 · Physical Review A

Entangling atoms in bad cavities

Anders Søndberg Sørensen, Klaus Mølmer

Published Aug 27, 2002• 102 citations
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Abstract

We propose a method to produce entangled spin squeezed states of a large number of atoms inside an optical cavity. By illuminating the atoms with bichromatic light, the coupling to the cavity induces pairwise exchange of excitations which entangles the atoms. Unlike most proposals for entangling atoms by cavity QED, our proposal does not require the strong coupling regime ${g}^{2}/\ensuremath{\kappa}\ensuremath{\Gamma}\ensuremath{\gg}1,$ where g is the atom cavity coupling strength, $\ensuremath{\kappa}$ is the cavity decay rate, and $\ensuremath{\Gamma}$ is the decay rate of the atoms. In this work the important parameter is ${\mathrm{Ng}}^{2}/\ensuremath{\kappa}\ensuremath{\Gamma},$ where N is the number of atoms, and our proposal permits the production of entanglement in bad cavities as long as they contain a large number of atoms.

DOI
10.1103/physreva.66.022314

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We propose a method to produce entangled spin squeezed states of a large number of atoms inside an optical cavity. By illuminating the atoms with bichromatic light, the coupling to the cavity induces pairwise exchange of excitations which entangles the atoms. Unlike most proposals for entangling atoms by cavity QED, our proposal does not require the strong coupling regime g2/\ensuremathκ\ensuremathΓ\ensuremath≫1,{g}^{2}/\ensuremath{\kappa}\ensuremath{\Gamma}\ensuremath{\gg}1,g2/\ensuremathκ\ensuremathΓ\ensuremath≫1, where g is the atom cavity coupling strength, \ensuremathκ\ensuremath{\kappa}\ensuremathκ is the cavity decay rate, and \ensuremathΓ\ensuremath{\Gamma}\ensuremathΓ is the decay rate of the atoms. In this work the important parameter is Ng2/\ensuremathκ\ensuremathΓ,{\mathrm{Ng}}^{2}/\ensuremath{\kappa}\ensuremath{\Gamma},Ng2/\ensuremathκ\ensuremathΓ, where N is the number of atoms, and our proposal permits the production of entanglement in bad cavities as long as they contain a large number of atoms.
A scheme is presented for generation of entangled states for two atoms trapped in two distant bad cavities. The scheme can work with bad cavities with the coupling strength smaller than the cavity decay rate, which is important from the viewpoint of experiment. In the scheme the atoms have no probability of being populated in the excited state and thus the atomic spontaneous emission is suppressed, which increases the probability of success. The fidelity of the entangled state is not affected by the detection efficiency. Furthermore, the scheme does not require the detection of the left-polarized photon and right-polarized photon at the same time.
We present a scheme for generation of two-atomic entangled state by using the interference of polarized photons. The scheme does not require complete mapping between the atomic state and the photonic state, nor does it require the establishment of maximal entanglement between the atom and the cavity. And the atom-cavity coupling strength is smaller than the cavity decay rate. This greatly relaxes the requirement on the cavity quality. The scheme is for non-post-selection results and all the steps of the scheme are within the current technologies.
We theoretically investigate the entangled states of an atomic ensemble that can be obtained via cavity feedback, varying the atom-light coupling from weak to strong, and including a systematic treatment of decoherence. In the strong-coupling regime for small atomic ensembles, the system is driven by cavity losses into a long-lived, highly entangled many-body state that we characterize analytically. In the weak-coupling regime for large ensembles, we find analytically the maximum spin-squeezing that can be achieved by optimizing both the coupling and the atom number. This squeezing is fundamentally limited by spontaneous emission to a constant value, which is independent of the atom number.
We theoretically investigate the entangled states of an atomic ensemble that can be obtained via cavity feedback, varying the atom-light coupling from weak to strong, and including a systematic treatment of decoherence. In the strong-coupling regime for small atomic ensembles, the system is driven by cavity losses into a long-lived, highly entangled many-body state that we characterize analytically. In the weak-coupling regime for large ensembles, we find analytically the maximum spin-squeezing that can be achieved by optimizing both the coupling and the atom number. This squeezing is fundamentally limited by spontaneous emission to a constant value, which is independent of the atom number.
We propose an optical cavity-QED scheme for the deterministic generation of polarization entangled photon pairs that operates with high fidelity even in the bad cavity limit. The scheme is based on the interaction of an excited four-level atom with two empty optical cavity modes via an adiabatic passage process. Monte-Carlo wave function simulations are used to evaluate the fidelity of the cavity-QED source and its entanglement capability in the presence of decoherence. In the bad cavity limit, fidelities close to one are predicted for state-of-the-art experimental parameter values.