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arXiv 1111.7174cond-mat.str-el
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Luttinger液体的局部光谱性质:标度与非普适能量标度

Local spectral properties of Luttinger liquids: scaling versus nonuniversal energy scales

D. Schuricht, S. Andergassen, V. Meden

摘要:

最近的扫描隧道和光电子能谱测量锗表面上的自组织金链的动机,我们重新调查的局部单粒子的光谱性质的Luttinger液体。在第一部分中,我们使用玻色化的方法来精确地计算一个简化的场论低能模型的局部谱函数,并仔细研究作为能量和温度之比的函数的标度特性。平移不变的Luttinger液体,以及那些与一个开放的边界(切链几何)被认为是。我们明确表明,这两种设置的尺度函数具有相同的解析形式。缩放行为表明可以对测量数据进行各种一致性检查,以实验验证Luttinger液体行为。第二部分利用泛函重整化群近似计算了一个微观格点模型--扩展哈伯德模型--在开边界附近的局部谱函数。我们表明,作为能量和温度的函数,它遵循在低能量制度的场论预测,并指出任何微观模型所固有的非普遍的能量尺度的重要性。该谱函数的空间依赖性的特征在于振荡行为和包络函数,其遵循幂律都根据场论连续模型。有趣的是,对于晶格模型,我们发现一个相移是成比例的两粒子相互作用,而不是占在标准玻色子化方法与开放边界的Luttinger液体。我们简要地评论了几个一维分支的费米能量切割和Rashba自旋轨道相互作用的影响。

英文摘要:

Motivated by recent scanning tunneling and photoemission spectroscopy measurements on self-organized gold chains on a germanium surface we reinvestigate the local single-particle spectral properties of Luttinger liquids. In the first part we use the bosonization approach to exactly compute the local spectral function of a simplified field theoretical low-energy model and take a closer look at scaling properties as a function of the ratio of energy and temperature. Translational invariant Luttinger liquids as well as those with an open boundary (cut chain geometry) are considered. We explicitly show that the scaling functions of both setups have the same analytic form. The scaling behavior suggests a variety of consistency checks which can be performed on measured data to experimentally verify Luttinger liquid behavior. In a second part we approximately compute the local spectral function of a microscopic lattice model---the extended Hubbard model---close to an open boundary using the functional renormalization group. We show that as a function of energy and temperature it follows the field theoretical prediction in the low-energy regime and point out the importance of nonuniversal energy scales inherent to any microscopic model. The spatial dependence of this spectral function is characterized by oscillatory behavior and an envelope function which follows a power law both in accordance with the field theoretical continuum model. Interestingly, for the lattice model we find a phase shift which is proportional to the two-particle interaction and not accounted for in the standard bosonization approach to Luttinger liquids with an open boundary. We briefly comment on the effects of several one-dimensional branches cutting the Fermi energy and Rashba spin-orbit interaction.

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