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Thermodynamics, contact, and density profiles of the repulsive Gaudin-Yang model

机译:热力学,接触和令人厌恶的高文扬杨模型的密度概况

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摘要

We address the problem of computing the thermodynamic properties of the repulsive one-dimensional two-component Fermi gas with contact interaction, also known as the Gaudin-Yang model. Using a specific lattice embedding and the quantum transfer matrix we derive an exact system of only two nonlinear integral equations for the thermodynamics of the homogeneous model which is valid for all temperatures and values of the chemical potential, magnetic field, and coupling strength. This system allows for an easy and extremely accurate calculation of thermodynamic properties circumventing the difficulties associated with the truncation of the thermodynamic Bethe ansatz system of equations. We present extensive results for the densities, polarization, magnetic susceptibility, specific heat, interaction energy, Tan contact, and local correlation function of opposite spins. Our results show that at low and intermediate temperatures the experimentally accessible contact is a nonmonotonic function of the coupling strength. As a function of the temperature the contact presents a pronounced local minimum in the Tonks-Girardeau regime which signals an abrupt change of the momentum distribution in a small interval of temperature. The density profiles of the system in the presence of a harmonic trapping potential are computed using the exact solution of the homogeneous model coupled with the local density approximation. We find that at finite temperature the density profile presents a double shell structure ( partially polarized center and fully polarized wings) only when the polarization in the center of the trap is above a critical value which is monotonically increasing with temperature.
机译:我们解决了用接触相互作用计算排斥式一维双组分Fermi气体的热力学性质的问题,也称为高文阳模型。使用特定的晶格嵌入和量子传递矩阵我们从均匀模型的热力学产生的精确系统仅是两个非线性整体方程,这对于化学电位,磁场和耦合强度的所有温度和值是有效的。该系统允许容易且非常精确地计算热力学性质,避免与截断与截断等式的热力学贝尔ansatz系统相关的困难。我们对相反旋转的密度,极化,磁化率,特定的热,相互作用,棕褐色接触和局部相关函数呈现了广泛的效果。我们的研究结果表明,在低和中间温度下,实验可访问的接触是耦合强度的非单调功能。作为温度的函数,接触在TONKS-Girardeau制度中提出了发音的局部最小值,其在小的温度间隔内突然改变动量分布。使用与局部密度近似耦合的均匀模型的精确解决方案来计算系统在存在谐波捕获电位的情况下的密度分布。我们发现,在有限温度下,密度型材仅当陷阱中心的偏振高于温度时单调增加的临界值时,密度型才能占双壳结构(部分偏振中心和完全偏振翼)。

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