Bistritzer R, Altman E
Department of Condensed Matter Physics, The Weizmann Institute of Science, Rehovot 76100, Israel.
Proc Natl Acad Sci U S A. 2007 Jun 12;104(24):9955-9. doi: 10.1073/pnas.0608910104. Epub 2007 Jun 4.
Quantum-phase fluctuations prevent true long-range phase order from forming in interacting 1D condensates, even at zero temperature. Nevertheless, by dynamically splitting the condensate into two parallel decoupled tubes the system can be prepared with a macroscopic relative phase, facilitating interferometric measurement. Here, we describe a dephasing mechanism whereby the quantum-phase fluctuations, which are so effective in equilibrium, act to destroy the macroscopic relative phase that was imposed as a nonequilibrium initial condition. We show that the phase coherence between the condensates decays exponentially with a dephasing time that depends on intrinsic parameters: the interaction strength, sound velocity, and density. Interestingly, significant temperature dependence appears only above a cross-over scale T*. In contrast to the usual phase diffusion, which is essentially an effect of confinement and leads to Gaussian decay, the exponential dephasing caused by fluctuations is a bulk effect that survives the thermodynamic limit.
量子相位涨落会阻止在相互作用的一维凝聚体中形成真正的长程相位有序,即使在零温度下也是如此。然而,通过动态地将凝聚体分裂成两个平行的解耦管,可以制备出具有宏观相对相位的系统,便于进行干涉测量。在这里,我们描述了一种退相机制,即在平衡状态下非常有效的量子相位涨落,会破坏作为非平衡初始条件施加的宏观相对相位。我们表明,凝聚体之间的相位相干性以退相时间呈指数衰减,退相时间取决于内在参数:相互作用强度、声速和密度。有趣的是,显著的温度依赖性仅在一个交叉尺度T*以上出现。与通常的相位扩散不同,后者本质上是一种限制效应并导致高斯衰减,由涨落引起的指数退相是一种体效应,在热力学极限下仍然存在。