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Dynamical Quasicondensation of Hard-Core Bosons at Finite Momenta
被引:82
|作者:
Vidmar, L.
[1
,2
]
Ronzheimer, J. P.
[2
,3
]
Schreiber, M.
[2
,3
]
Braun, S.
[2
,3
]
Hodgman, S. S.
[2
,3
]
Langer, S.
[4
]
Heidrich-Meisner, F.
[1
,2
]
Bloch, I.
[2
,3
]
Schneider, U.
[2
,3
,5
]
机构:
[1] Univ Munich, Arnold Sommerfeld Ctr Theoret Phys, D-80333 Munich, Germany
[2] Univ Munich, Dept Phys, D-80333 Munich, Germany
[3] Max Planck Inst Quantum Opt, D-85748 Garching, Germany
[4] Univ Pittsburgh, Dept Phys & Astron, Pittsburgh, PA 15213 USA
[5] Univ Cambridge, Cavendish Lab, Cambridge CB3 0HE, England
基金:
美国国家科学基金会;
关键词:
NONEQUILIBRIUM STEADY-STATE;
BOSE-EINSTEIN CONDENSATION;
MANY-BODY LOCALIZATION;
TONKS-GIRARDEAU GAS;
QUANTUM-SYSTEMS;
PHASE-TRANSITIONS;
OPTICAL LATTICE;
ULTRACOLD ATOMS;
CHAIN;
TEMPERATURE;
D O I:
10.1103/PhysRevLett.115.175301
中图分类号:
O4 [物理学];
学科分类号:
0702 ;
摘要:
Long-range order in quantum many-body systems is usually associated with equilibrium situations. Here, we experimentally investigate the quasicondensation of strongly interacting bosons at finite momenta in a far-from-equilibrium case. We prepare an inhomogeneous initial state consisting of one-dimensional Mott insulators in the center of otherwise empty one-dimensional chains in an optical lattice with a lattice constant d. After suddenly quenching the trapping potential to zero, we observe the onset of coherence in spontaneously forming quasicondensates in the lattice. Remarkably, the emerging phase order differs from the ground-state order and is characterized by peaks at finite momenta +/-(pi/2)((h) over bar /d) in the momentum distribution function.
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