Superfluid-Mott-insulator transition of ultracold superradiant bosons in a cavity

被引:23
|
作者
Lin, Rui [1 ]
Papariello, Luca [1 ]
Molignini, Paolo [1 ]
Chitra, R. [1 ]
Lode, Axel U. J. [2 ,3 ]
机构
[1] Swiss Fed Inst Technol, Inst Theoret Phys, CH-8093 Zurich, Switzerland
[2] Univ Vienna, Fac Math, Wolfgang Pauli Inst, Oskar Morgenstern Pl 1, A-1090 Vienna, Austria
[3] TU Wien, Atominst, Vienna Ctr Quantum Sci & Technol, Stadionallee 2, A-1020 Vienna, Austria
基金
奥地利科学基金会; 瑞士国家科学基金会;
关键词
QUANTUM PHASE-TRANSITION; BOSE-EINSTEIN CONDENSATE; OPTICAL LATTICES; GAS; ATOMS; FIELD; MODEL;
D O I
10.1103/PhysRevA.100.013611
中图分类号
O43 [光学];
学科分类号
070207 ; 0803 ;
摘要
We investigate harmonically trapped, laser-pumped bosons with infinite-range interactions induced by a dissipative high-finesse red-detuned optical cavity with numerical and analytical methods. We obtain multiple cavity and atomic observables as well as the full phase diagram of the system using the multiconfigurational time-dependent Hartree method for indistinguishable particles (MCTDH-X) approach. Besides the transition from an unorganized normal phase to a superradiant phase where the atoms self-organize, we focus on an in-depth investigation of the self-organized superfluid to self-organized Mott-insulator phase transition in the superradiant phase as a function of the cavity-atom coupling. The numerical results are substantiated by an analytical study of an effective Bose-Hubbard model. We numerically analyze cavity fluctuations and emergent strong correlations between atoms in the many-body state across the Mott transition via the atomic density distributions and Glauber correlation functions. Unexpectedly, the weak harmonic trap leads to features like a lattice switching between the two symmetry-broken Z(2) configurations of the untrapped system and a reentrance of superfluidity in the Mott-insulating phase. Our analytical considerations quantitatively explain the numerically observed correlation features.
引用
收藏
页数:15
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