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Metal-insulator transition in a weakly interacting many-electron system with localized single-particle states

机译:具有局部单粒子态的弱相互作用多电子系统中的金属-绝缘体跃迁

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We consider low-temperature behavior of weakly interacting electrons in disordered conductors in the regime when all single-particle eigenstates are localized by the quenched disorder. We prove that in the absence of coupling of the electrons to any external bath do electrical conductivity exactly vanishes as long as the temperature T does not exceed some finite value T-c. At the same time, it can be also proven that at high enough T the conductivity is finite. These two statements imply that the system undergoes a finite temperature metal-to-insulator transition, which can be viewed as Anderson-like localization of many-body wave functions in the Fock space. Metallic and insulating states are not different from each other by any spatial or discrete symmetries. We formulate the effective Hamiltonian description of the system at low energies (of the order of the level spacing in the single-particle localization volume). In the metallic phase quantum Boltzmann equation is valid, allowing to find the kinetic coefficients. In the insulating phase, T < T-c, we use Feynmann diagram technique to determine the probability distribution function for quantum-mechanical transition rates. The probability of an escape rate from a given quantum state to be finite turns out to vanish in every order of the perturbation theory in electron-electron interaction. Thus, electron-electron interaction alone is unable to cause the relaxation and establish the thermal equilibrium. As soon as some weak coupling to a bath is turned on, conductivity becomes finite even in the insulating phase. Moreover, in the vicinity of the transition temperature it is much larger than phonon-induced hopping conductivity of non-interacting electrons. The reason for this enhancement is that the stability of the insulating state is gradually decreasing as the transition point is approached. As a result, a single phonon can cause a whole cascade of electronic hops. (c) 2005 Elsevier Inc. All rights reserved.
机译:当所有单粒子本征态均被淬灭的无序态定位时,我们考虑了无序导体中弱相互作用电子的低温行为。我们证明,在没有电子耦合到任何外部浴的情况下,只要温度T不超过某个有限值T-c,导电性就会完全消失。同时,还可以证明,在足够高的T下,电导率是有限的。这两个陈述暗示该系统经历了有限的金属到绝缘体的转变,这可以看作是Fock空间中多体波函数的安德森式局部化。金属状态和绝缘状态在任何空间或离散对称性上都没有不同。我们在低能量(单粒子定位体积中的水平间距的数量级)下制定了系统的有效哈密顿量描述。在金属相中,量子玻尔兹曼方程是有效的,从而可以找到动力学系数。在绝缘阶段,T

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