Collective quantum dynamics of an atomic lattice coupled to an optical resonator

S. Zippilli, G. Morigi, J. Asbóth, H. Ritsch
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Abstract

We study the quantum dynamics of an array of coherently driven two-level atoms coupled to an optical resonator. In the strong coupling regime the cavity field generated by atomic scattering interferes destructively with the pump on the atoms. In this configuration atomic excitation is suppressed even for strong driving fields, while the stationary intracavity field amplitude is almost independent of the atom number. The magnitude of this interference effect depends on the detuning between laser and cavity field and on the relative atomic positions and is strongest when the atoms are ordered in a wavelength spaced lattice placed at the antinodes of the cavity mode. In this case three dimensional intensity minima are created in the vicinity of each atom. We analyze the mechanical forces in the regime where the interference condition is fulfilled, and show that the atomic pattern is mechanically stable whenever the driving frequency is red detuned with respect to the cavity frequency, irrespective of the atomic transition frequency
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耦合到光学谐振器的原子晶格的集体量子动力学
我们研究了一组相干驱动的二能级原子与光学谐振器耦合的量子动力学。在强耦合状态下,原子散射产生的腔场对原子上的泵浦产生破坏性干扰。在这种结构中,即使在强驱动场下,原子激发也被抑制,而腔内固定场的振幅几乎与原子数无关。这种干涉效应的大小取决于激光和腔场之间的失谐以及原子的相对位置,当原子排列在位于腔模式反端的波长间隔晶格中时,这种干涉效应最强。在这种情况下,三维强度最小值是在每个原子附近产生的。我们分析了在满足干涉条件的状态下的机械力,并表明无论原子跃迁频率如何,当驱动频率相对于腔频率发生红失谐时,原子图案都是机械稳定的
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