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Non-equilibrium dynamics of artificial quantum matter.

机译:人造量子物质的非平衡动力学。

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摘要

The rapid progress of the field of ultracold atoms during the past two decades has set new milestones in our control over matter. By cooling dilute atomic gases and molecules to nano-Kelvin temperatures, novel quantum mechanical states of matter can be realized and studied on a table-top experimental setup while bulk matter can be tailored to faithfully simulate abstract theoretical models. Two of such models which have witnessed significant experimental and theoretical attention are (1) the two-component Fermi gas with resonant s-wave interactions, and (2) the single-component Fermi gas with dipole-dipole interactions. This thesis is devoted to studying the non-equilibrium collective dynamics of these systems using the general framework of quantum kinetic theory.;We present a concise review of the utilized mathematical methods in the first two chapters, including the Schwinger-Keldysh formalism of non-equilibrium quantum fields, two-particle irreducible (2PI) effective actions and the framework of quantum kinetic theory. We study the collective dynamics of the dipolar Fermi gas in a quasi-two-dimensional optical trap in chapter 3 and provide a detailed account of its dynamical crossover from the collisionless to the hydrodynamical regime. Chapter 4 is devoted to studying the dynamics of the attractive Fermi gas in the normal phase. Starting from the self-consistent T-matrix (pairing fluctuation) approximation, we systematically derive a set of quantum kinetic equations and show that they provide a globally valid description of the dynamics of the attractive Fermi gas, ranging from the weak-coupling Fermi liquid phase to the intermediate non-Fermi liquid pairing pseudogap regime and finally the strong-coupling Bose liquid phase. The shortcomings of the self-consistent T-matrix approximation in two spatial dimensions are discussed along with a proposal to overcome its unphysical behaviors. The developed kinetic formalism is finally utilized to reproduce and interpret the findings of a recent experiment done on the collective dynamics of trapped two-dimensional ultracold gases.
机译:在过去的二十年中,超冷原子领域的快速发展为我们对物质的控制树立了新的里程碑。通过将稀释的原子气体和分子冷却到纳米开尔文温度,可以在台式实验装置上实现并研究新的物质量子力学状态,同时可以定制散装物质以忠实地模拟抽象的理论模型。这些模型中的两个已经在实验和理论上引起了广泛关注,它们是(1)具有共振s波相互作用的两组分费米气体,以及(2)具有偶极-偶极相互作用的单组分费米气体。本论文致力于利用量子动力学理论的一般框架研究这些系统的非平衡集体动力学。我们在前两章简要介绍了所用的数学方法,包括非辛格的Schwinger-Keldysh形式主义。平衡量子场,两粒子不可还原(2PI)有效作用和量子动力学理论的框架。我们将在第3章中研究准二维光学阱中偶极费米气体的集体动力学,并详细说明其从无碰撞到流体动力学状态的动力学交叉。第四章专门研究正相吸引费米气体的动力学。从自洽的T矩阵(配对波动)逼近开始,我们系统地推导了一组量子动力学方程,并表明它们提供了对吸引费米气体动力学的全局有效描述,从弱耦合费米液体开始到中间非费米液体配对拟间隙体系,最后是强耦合玻色液相。讨论了在两个空间维度上自洽T矩阵逼近的缺点以及克服其非物理行为的建议。最终,利用发达的动力学形式主义来再现和解释最近对捕获的二维超冷气体的集体动力学进行的实验的发现。

著录项

  • 作者

    Babadi, Mehrtash.;

  • 作者单位

    Harvard University.;

  • 授予单位 Harvard University.;
  • 学科 Physics Condensed Matter.;Physics Low Temperature.
  • 学位 Ph.D.
  • 年度 2013
  • 页码 351 p.
  • 总页数 351
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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