光晶格中多体极化子在Mott绝缘体区域的量子相

Quantum Phases of Many-Body Polaron in Mott Insulator Regime in Optical Lattice

  • 摘要: 极化子是在玻色-爱因斯坦凝聚(BEC)背景下,光晶格中的玻色子与BEC声子库耦合形成的一种准粒子。通过Lang-Firsov变换得到极化子体系的有效哈密顿量,其形式为拓展的玻色-哈伯德模型。在Mott绝缘体区域,通过直接求解体系的哈密顿量得到了单组份极化子在填充数分别为1/2和1/4时的量子相;通过Hartree-Fock近似,进一步得到了双组份极化子在填充数分别为1/2和1/4时体系的量子相。研究预测了单组份和双组份极化子体系可能存在的非平庸量子相。

     

    Abstract: The quantum phases of many-body polaron was investigated in two-dimensional optical lattices in Mott Insulator regime. The polaron is a quasi-particle formed by the coupling between bosons in optical lattices and BEC phonons. The effective Hamiltonian of polarons is derived through Lang-Firsov transformation. The system can be described by extended Bose-Hubbard Model. In Mott Insulator regime, the Hamiltonian was solved directly so that the quantum phases of the system can be obtained for single-component case with filling factors of 1/2 and 1/4. By using Hartree-Fock approximation, more quantum phases for two-component case with filling factors of 1/2 and 1/4 can be found. Non-trivial quantum phases was predicted in single-component and two-component systems of polarons.

     

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