Unified theory of quantum many-particle systems

dc.creatorLiu, Yu-Liang
dc.date2001-03-06
dc.date.accessioned2026-07-07T02:40:40Z
dc.date.available2026-07-07T02:40:40Z
dc.descriptionUsing eigen-functional bosonization method, we study quantum many-particle systems, and show that the quantum many-particle problems end in to solve the differential equation of the phase fields which represent the particle correlation strength. Thus, the physical properties of these systems are completely determined by the differential equation of the phase fields. We mainly focus on the study of D-dimensional electron gas with/without transverse gauge fields, two-dimensional electron gas under an external magnetic field, D-dimensional boson systems, a D-dimensional Heisenberg model and a one-band Hubbard model on a square lattice, and give their exact (accurate for Heisenberg model) functional expressions of the ground state energy and action, and the eigen-functional wave functions of the fermions/bosons. With them, we can calculate a variety of correlation functions of the systems, such as single particle Green's functions and their ground state wave functions. In present theoretical framework, we can unifiably represent the Landau Fermi liquid, non-Fermi liquid ($D\geq 2$) and Tomonaga-Luttinger liquid.
dc.description38 pages, RevTex, no figure
dc.identifierhttps://arxiv.org/abs/cond-mat/0103124
dc.identifierhttp://arxiv.org/abs/cond-mat/0103124
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/17454
dc.subjectStrongly Correlated Electrons
dc.subjectMesoscale and Nanoscale Physics
dc.titleUnified theory of quantum many-particle systems
dc.typetext

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