Titlebook: Quantum Many-Body Physics; A Perspective on Str Yoshio Kuramoto Book 2020 Springer Japan KK, part of Springer Nature 2020 3d and 4f Electro

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書目名稱Quantum Many-Body Physics影響因子(影響力)




書目名稱Quantum Many-Body Physics影響因子(影響力)學(xué)科排名




書目名稱Quantum Many-Body Physics網(wǎng)絡(luò)公開度




書目名稱Quantum Many-Body Physics網(wǎng)絡(luò)公開度學(xué)科排名




書目名稱Quantum Many-Body Physics被引頻次




書目名稱Quantum Many-Body Physics被引頻次學(xué)科排名




書目名稱Quantum Many-Body Physics年度引用




書目名稱Quantum Many-Body Physics年度引用學(xué)科排名




書目名稱Quantum Many-Body Physics讀者反饋




書目名稱Quantum Many-Body Physics讀者反饋學(xué)科排名

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Fermi Liquid Theory,he theory is the concept of quasi-particles. This chapter explains how the Fermi liquid theory accounts for interaction effects taking examples such as specific heat and magnetic susceptibility. Also discussed is the dynamical response of Fermi liquid against slowly varying external fields.

Congregate

JAUNT

Kondo Effect, speaking, the exchange interaction between the impurity and conduction electrons becomes endlessly large in the effective Hamiltonian, even though its magnitude is originally tiny. As a result, the impurity spin is completely screened in the ground state, resulting in a local Fermi liquid. However,

ADOPT

One-Dimensional Fermions and Bosonization,er than in higher dimensional systems. Detailed treatment is provided for a powerful method called bosonization, which regards density fluctuation of 1D fermions as a bosonic object. In terms of bosonization, it is possible to discuss such interesting states as non-Fermi liquid with power-law decay

GROUP

六邊形

Many-Body Perturbation Theory,umbers. Green function appears as a natural element in Feynman diagram that represents a group of terms in many-body perturbation theory. The graphical method appeals to intuition, and is convenient to reorganize the perturbation series to infinite order. The discussion in this chapter is rather tec

aerial

Dynamical Mean Field Theory,corresponding field can be included. The correlation problem in a large system is then replaced by a single-site problem surrounded by a dynamical effective medium. The effective impurity system is regarded as zero-dimensional. It can be shown that the replacement by an effective impurity is exact i