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arXiv 0811.4515cond-mat.str-el
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光晶格中硬核玻色-费米混合物的相位和集体模

Phases and collective modes of hardcore Bose-Fermi mixture in an optical lattice

S. Sinha, K. Sengupta

摘要:

利用从玻色子平均场论,得到了具有最近邻种内相互作用和就地种间排斥的无自旋玻色子和自旋极化费米子的玻色-费米混合体在半填充光晶格中的相图.我们证明了这样一个系统可以有四种可能的相:a)超固态玻色子与处于Mott态的费米子共存,b)玻色子的Mott态与处于金属态或电荷密度波态的费米子共存,c)金属费米子态与玻色子的超流相共存,d)费米子和玻色子的Mott绝缘态。我们绘制了系统的相图,并提供了平均场论中相边界的解析表达式。我们证明了除了超固态和Mott态之间的相变是连续的量子相变之外,这些相变一般都是一级相变。我们还得到了系统在这些阶段的低能集体激发。最后,我们研究了Mott绝缘相的粒子-空穴激发,并利用它确定了超固态-莫特绝缘体相变的动力学临界指数$z$。我们讨论可以检验我们理论的实验。

英文摘要:

We obtain the phase diagram of a Bose-Fermi mixture of hardcore spinless Bosons and spin-polarized Fermions with nearest neighbor intra-species interaction and on-site inter-species repulsion in an optical lattice at half-filling using a slave-boson mean-field theory. We show that such a system can have four possible phases which are a) supersolid Bosons coexisting with Fermions in the Mott state, b) Mott state of Bosons coexisting with Fermions in a metallic or charge-density wave state, c) a metallic Fermionic state coexisting with superfluid phase of Bosons, and d) Mott insulating state of Fermions and Bosons. We chart out the phase diagram of the system and provide analytical expressions for the phase boundaries within mean-field theory. We demonstrate that the transition between these phases are generically first order with the exception of that between the supersolid and the Mott states which is a continuous quantum phase transition. We also obtain the low-energy collective excitations of the system in these phases. Finally, we study the particle-hole excitations in the Mott insulating phase and use it to determine the dynamical critical exponent $z$ for the supersolid-Mott insulator transition. We discuss experiments which can test our theory.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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