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Bose-Glass Phases of Ultracold Atoms due to Cavity Backaction

机译:腔反向作用导致超冷原子的玻色玻璃相

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We determine the quantum ground-state properties of ultracold bosonic atoms interacting with the mode of a high-finesse resonator. The atoms are confined by an external optical lattice, whose period is incommensurate with the cavity mode wavelength, and are driven by a transverse laser, which is resonant with the cavity mode. While for pointlike atoms photon scattering into the cavity is suppressed, for sufficiently strong lasers quantum fluctuations can support the buildup of an intracavity field, which in turn amplifies quantum fluctuations. The dynamics is described by a Bose-Hubbard model where the coefficients due to the cavity field depend on the atomic density at all lattice sites. Quantum Monte Carlo simulations and mean-field calculations show that, for large parameter regions, cavity backaction forces the atoms into clusters with a checkerboard density distribution. Here, the ground state lacks superfluidity and possesses finite compressibility, typical of a Bose glass. This system constitutes a novel setting where quantum fluctuations give rise to effects usually associated with disorder.
机译:我们确定与高精细共振器的模式相互作用的超冷硼原子的量子基态性质。原子受外部光学晶格限制,外部晶格的周期与腔模波长不匹配,并由与腔模共振的横向激光器驱动。虽然对于点状原子,光子散射到空腔中是受到抑制的,但对于足够强的激光器,量子涨落可以支持腔内场的建立,这反过来会放大量子涨落。动力学由Bose-Hubbard模型描述,其中由腔场引起的系数取决于所有晶格位置的原子密度。量子蒙特卡洛模拟和均值场计算表明,对于较大的参数区域,腔背作用迫使原子成具有棋盘密度分布的簇。在这里,基态缺乏超流动性,并且具有有限的可压缩性,这是玻色玻璃的典型特征。该系统构成了一种新颖的环境,其中量子涨落引起通常与无序有关的效应。

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