Alon Ofir E, Streltsov Alexej I, Cederbaum Lorenz S
Theoretische Chemie, Physikalisch-Chemisches Institut, Universität Heidelberg, Im Neuenheimer Feld 229, D-69120 Heidelberg, Germany.
Phys Rev Lett. 2005 Jul 15;95(3):030405. doi: 10.1103/PhysRevLett.95.030405.
Quantum phases and phase transitions of weakly to strongly interacting bosonic atoms in deep to shallow optical lattices are described by a single multiorbital mean-field approach in real space. For weakly interacting bosons in one dimension, the critical value of the superfluid to Mott insulator (MI) transition found is in excellent agreement with many-body treatments of the Bose-Hubbard model. For strongly interacting bosons, (i) additional MI phases appear, for which two (or more) atoms residing in each site undergo a Tonks-Girardeau-like transition and localize, and (ii) on-site excitation becomes the excitation lowest in energy. Experimental implications are discussed.
在实空间中,通过单一的多轨道平均场方法描述了深陷阱到浅光晶格中弱相互作用到强相互作用玻色子原子的量子相和相变。对于一维弱相互作用玻色子,所发现的超流体到莫特绝缘体(MI)转变的临界值与玻色-哈伯德模型的多体处理结果高度吻合。对于强相互作用玻色子,(i)出现了额外的MI相,其中每个格点上的两个(或更多)原子经历类汤克斯-吉拉尔代奥转变并局域化,并且(ii)在位激发成为能量最低的激发。文中讨论了实验意义。