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Quantum Monte Carlo studies of quantum criticality in low-dimensional spin systems.

机译:量子蒙特卡洛研究低维自旋系统中的量子临界。

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摘要

Strongly correlated low-dimensional quantum spin models provide a well-established frame- work to study magnetic properties of insulators, and are of great theoretical interest and experimental relevance in condensed-matter physics. In this thesis, I use quantum Monte Carlo methods to numerically study quantum critical behavior in low-dimensional quantum spin models and wavefunctions.;First, I study spinons---emergent spin-1/2 bosonic excitations---at certain one- and two-dimensional quantum phase transitions (QPTs) in spin models, by characterizing their size and confinement length quantitatively. In particular, I focus on the QPT from an antiferromagnetic (AFM) phase into a valence-bond solid (VBS) phase, which is an example of a violation of the standard Landau-Ginzburg-Wilson paradigm for phase transitions. This transition in two dimensions (2D) is instead likely described by a novel theory called "deconfined quantum criticality" (DQC). According to the theory, spinons should be deconfined. The degree of deconfinement is quantified in my calculations.;Second, I present a comprehensive study of so-called short-bond resonating-valence-bond (RVB) spin liquids in 2D, which have been suggested as a good starting point for understanding the spin physics of high-temperature cuprates. I find that these RVB states can also be classified as quantum-critical VBS states, which indicates that RVB is less disordered than expected. This work suggests a possible mapping from the quantum RVB states to classical dimer models via a classical continuum field theory---the height model. This map explicitly bridges well-established classical results to future quantum studies.;Third, I consider 1D amplitude product (AP) states, which are generalized versions of RVB states, with different wavefunction weightings of bonds according to their lengths. AP states constitute a good ansatz for certain Hamiltonians and are of broad interest in quantum magnetism. I study phase transitions from AFM-VBS phases in AP states by tuning their amplitudes, and obtain continuously varying critical exponents. In addition, I classify the 1D AP states through entanglement entropy calculations of the central charge in (1+1)D conformal field theory. This new classification could serve as guide for AP states as trial wavefunctions to search for ground states of corresponding quantum spin models.
机译:高度相关的低维量子自旋模型为研究绝缘子的磁性能提供了完善的框架,在凝聚态物理中具有重要的理论意义和实验意义。在本文中,我使用量子蒙特卡罗方法对低维量子自旋模型和波函数中的量子临界行为进行了数值研究;首先,我研究了自旋子-发生自旋1/2玻色子激发-在某些情况下-自旋模型中的二维量子相变(QPT),通过定量表征其尺寸和约束长度。特别是,我将重点放在从反铁磁(AFM)到价键固相(VBS)的QPT,这是违反标准Landau-Ginzburg-Wilson范式进行相变的一个例子。相反,二维(2D)的这种过渡可能是由一种称为“非限定量子临界”(DQC)的新颖理论来描述的。根据该理论,应该限制棘刺。第二,我对所谓的二维短键共振价键旋转液体(RVB)进行了全面的研究,这被认为是理解该方法的一个很好的起点。高温铜酸盐的自旋物理学。我发现这些RVB状态也可以归类为量子临界VBS状态,这表明RVB的混乱程度低于预期。这项工作提出了通过经典连续场理论-高度模型从量子RVB状态到经典二聚体模型的可能映射。该图明确地将建立良好的经典结果与未来的量子研究联系起来。第三,我考虑一维振幅乘积(AP)状态,它们是RVB状态的广义形式,根据键的长度具有不同的波函数权重。 AP状态对于某些哈密顿量而言是很好的ansatz,并且在量子磁性方面引起广泛关注。我通过调整幅度来研究AP状态中AFM-VBS相的相变,并获得连续变化的临界指数。此外,我通过(1 + 1)D共形场理论中中心电荷的纠缠熵计算对一维AP状态进行分类。这种新的分类可以作为AP状态的指南,作为试探波函数来搜索相应量子自旋模型的基态。

著录项

  • 作者

    Tang, Ying.;

  • 作者单位

    Boston University.;

  • 授予单位 Boston University.;
  • 学科 Physics Quantum.
  • 学位 Ph.D.
  • 年度 2014
  • 页码 210 p.
  • 总页数 210
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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