Quantum interference and spin-charge separation in a disordered Luttinger liquid

被引:9
|
作者
Yashenkin, A. G. [1 ,2 ]
Gornyi, I. V. [1 ,3 ]
Mirlin, A. D. [1 ,4 ]
Polyakov, D. G. [1 ]
机构
[1] Forschungszentrum Karlsruhe, Inst Nanotechnol, D-76021 Karlsruhe, Germany
[2] Petersburg Nucl Phys Inst, Div Theory, St Petersburg 188300, Russia
[3] AF Ioffe Phys Tech Inst, St Petersburg 194021, Russia
[4] Univ Karlsruhe, Inst Theorie Kondensierten Mat, D-76128 Karlsruhe, Germany
来源
PHYSICAL REVIEW B | 2008年 / 78卷 / 20期
关键词
D O I
10.1103/PhysRevB.78.205407
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
We study the influence of spin on the quantum interference of interacting electrons in a single-channel disordered quantum wire within the framework of the Luttinger liquid (LL) model. The nature of the electron interference in a spinful LL is particularly nontrivial because the elementary bosonic excitations that carry charge and spin propagate with different velocities. We extend the functional-bosonization approach to treat the fermionic and bosonic degrees of freedom in a disordered spinful LL on an equal footing. We analyze the effect of spin-charge separation at finite temperature both on the spectral properties of single-particle fermionic excitations and on the conductivity of a disordered quantum wire. We demonstrate that the notion of weak localization, related to the interference of multiple-scattered electron waves and their decoherence due to electron-electron scattering, remains applicable to the spin-charge separated system. The relevant dephasing length, governed by the interplay of inelastic electron-electron interactions and spin-charge separation, is found to be parametrically shorter than in a spinless LL. We calculate both the quantum (weak localization) and classical (memory effect) corrections to the conductivity of a disordered spinful LL. The classical correction is shown to dominate in the limit of high temperature.
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页数:21
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