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Superfluidity in a degenerate atomic Fermi gas.

机译:简并原子费米气体中的超流。

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摘要

Dilute atomic gases have become a powerful tool for studying many-body quantum mechanics. The best example of this is the achievement of Bose-Einstein condensation in 1995 in a gas of Bose atoms, a discovery which has invoked a confluence of ideas from condensed matter, atomic and nuclear physics. Now a concerted research effort is focused on creating and studying a BCS superfluid in an atomic Fermi gas.; In the work presented here we study in detail pairing superfluidity in a Fermi gas of atoms, by self-consistently solving the Bogoliubov-de Gennes equations, both for bulk systems, and for atoms in a harmonic confining potential. A critical part of this work is the derivation of a regularized theory, which is formulated entirely in terms of physically measurable quantities, such that a quantitative comparison between theory and experiment is possible with no adjustable parameters. The resulting equations form a non-linear problem, and the accurate numerical solution of this poses a formidable challenge. A major component of this thesis is the development of efficient computational approaches to overcome these difficulties.; Based on the linear response of the gas to a twisting of the order parameter phase, the superfluid density can be defined as a generalized elasticity of the system. Using finite temperature perturbation theory we calculate the superfluid density in an inhomogeneous system.; We investigate the structure and thermodynamic properties of a singly quantized vortex line in a gas of superfluid fermionic atoms, making the first quantitative determination the critical rotation frequency for thermodynamic stability of the vortex state, and study the nature of the bound states in the vortex core. These excitations fill the core, making direct imaging of the vortex unlikely. Instead, we propose an experiment to indirectly probe the vortex density of states with laser fields, in a scheme analogous to Scanning Tunneling Microscopy. Furthermore, it is shown that the vortex state causes a shift of the superfluid transition temperature, which can be understood as a finite size effect.
机译:稀原子气体已经成为研究多体量子力学的有力工具。最好的例子是1995年在玻色原子气体中实现了玻色-爱因斯坦凝聚,这一发现唤起了凝聚态,原子和核物理学的思想汇聚。现在,一致的研究工作集中于在原子费米气体中创建和研究BCS超流体。在这里提出的工作中,我们通过自洽求解Bogoliubov-de Gennes方程,详细讨论了原子费米气体中的超流体配对,该方程既适用于本体系统,也适用于处于谐波约束势的原子。这项工作的关键部分是规则化理论的推导,该理论完全根据物理上可测量的量来制定,这样就可以在没有可调参数的情况下对理论和实验进行定量比较。由此产生的方程式构成了一个非线性问题,而对此的精确数值解决方案提出了巨大的挑战。本文的主要内容是开发有效的计算方法来克服这些困难。基于气体对阶数参数相的扭曲的线性响应,可以将超流体密度定义为系统的广义弹性。使用有限温度扰动理论,我们计算了非均匀系统中的超流体密度。我们研究了超流态铁离子原子气体中单量化涡旋线的结构和热力学性质,从而首次定量确定了涡旋态热力学稳定性的临界旋转频率,并研究了涡旋核中结合态的性质。 。这些激发充满了核,使得不可能对涡旋进行直接成像。取而代之的是,我们提出了一种类似于扫描隧道显微镜的方案,通过激光场间接探测状态的涡旋密度。此外,显示出涡流状态引起超流体转变温度的偏移,这可以理解为有限尺寸效应。

著录项

  • 作者

    Nygaard, Nicolai.;

  • 作者单位

    University of Maryland College Park.;

  • 授予单位 University of Maryland College Park.;
  • 学科 Physics Condensed Matter.; Physics Atomic.
  • 学位 Ph.D.
  • 年度 2003
  • 页码 p.4423
  • 总页数 306
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 O49;
  • 关键词

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