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arXiv 1003.4005cond-mat.quant-gas
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用陷阱压缩研究光晶格中相互作用玻色子的巨正则phase diagram

Exploring the grand-canonical phase diagram of interacting bosons in optical lattices by trap squeezing

Tommaso Roscilde

摘要:

本文从理论上讨论了基于光晶格中囚禁冷玻色子的量子模拟器如何通过独立于所有其他实验参数(陷阱压缩)控制囚禁势来探索均匀晶格玻色子模型的巨正则相图。基于量子MonteCarlo方法,建立了描述光晶格中冷玻色子的抛物阱中玻色-哈伯德模型的整体化学势与哈密顿参量之间的一般标度关系;我们发现,在足够高的密度和/或足够弱的相互作用的情况下,以及在更大的参数范围内由平均场GutzwillerAncillor确定。上述标度关系允许实验控制的化学势,独立于所有其他的哈密顿参数,通过陷阱压缩;考虑到全局化学势与局部化学势在陷阱中心重合,作为化学势的函数的中心密度的测量提供了访问的信息的玻色-哈伯德模型的体积压缩性。与相干性的飞行时间测量补充,压缩性的测量使人们能够辨别各种可能的相位之间实现的玻色子在光晶格与或没有外部(周期性或随机)的潜力-例如超流体,莫特绝缘体,带绝缘体,玻色玻璃。我们从理论上证明了一维光晶格和一维无公度超晶格中玻色子的陷阱压缩效应。

英文摘要:

In this paper we theoretically discuss how quantum simulators based on trapped cold bosons in optical lattices can explore the grand-canonical phase diagram of homogeneous lattice boson models, via control of the trapping potential independently of all other experimental parameters (trap squeezing). Based on quantum Monte Carlo, we establish the general scaling relation linking the global chemical potential to the Hamiltonian parameters of the Bose-Hubbard model in a parabolic trap, describing cold bosons in optical lattices; we find that this scaling relation is well captured by a modified Thomas-Fermi scaling behavior - corrected for quantum fluctuations - in the case of high enough density and/or weak enough interactions, and by a mean-field Gutzwiller Ansatz over a much larger parameter range. The above scaling relation allows to control experimentally the chemical potential, independently of all other Hamiltonian parameters, via trap squeezing; given that the global chemical potential coincides with the local chemical potential in the trap center, measurements of the central density as a function of the chemical potential gives access to the information on the bulk compressibility of the Bose-Hubbard model. Supplemented with time-of-flight measurements of the coherence properties, the measurement of compressibility enables one to discern among the various possible phases realized by bosons in an optical lattice with or without external (periodic or random) potentials -- e.g. superfluid, Mott insulator, band insulator, and Bose glass. We theoretically demonstrate the trap-squeezing investigation of the above phases in the case of bosons in a one-dimensional optical lattice, and in a one-dimensional incommensurate superlattice.

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