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BCS-BEC crossover at finite temperature in the broken-symmetry phase

机译:BCS-BEC在对称破缺阶段在有限温度下的交叉

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The BCS-BEC crossover is studied in a systematic way in the broken-symmetry phase between xero temperature and the critical temperature. This study bridges two regimes where quantum and thermal fluctuations are, respectively, important. The theory is implemented on physical grounds, by adopting a fermionic self-energy in the broken-symmetry phase that represents fermions coupled to superconducting fluctuations in weak coupling and to bosons described by the Bogoliubov theory in strong coupling. This extension of the theory beyond mean field proves important at finite temperature, to connect with the results in the normal phase. The order parameter, the chemical potential, and the single-particle spectral function are calculated numerically for a wide range of coupling and temperature. This enables us to assess the quantitative importance of superconducting fluctuations in the broken-symmetry phase over the whole BCS-BEC crossover. Our results are relevant to the possible realizations of this crossover with high-temperature cuprate superconductors and with ultracold fermionic atoms in a trap.
机译:在干温度和临界温度之间的对称破缺阶段,系统地研究了BCS-BEC交叉。这项研究架起了两种机制,在这两种机制中,量子涨落和热涨落分别很重要。该理论是在物理基础上实施的,它在对称性破碎阶段采用了费米离子自能量,该能量代表与弱耦合中的超导波动耦合的费米子以及在强耦合中由Bogoliubov理论描述的玻色子。该理论超出平均场的这种扩展在有限温度下被证明很重要,以与正相结果相关。在广泛的耦合和温度范围内,通过数值计算了阶数参数,化学势和单粒子光谱函数。这使我们能够评估整个BCS-BEC分频器中在对称对称阶段中超导波动的定量重要性。我们的结果与在高温铜酸盐超导体和阱中超冷的铁离子原子的交叉可能实现有关。

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