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Effects of phonons in the spin-boson model and the Hubbard-Holstein model =: 自旋 : 玻色子模型及Hubbard-Holstein模型中之聲子效應. / 自旋 : 玻色子模型及Hubbard-Holstein模型中之聲子效應 / Effects of phonons in the spin-boson model and the Hubbard-Holstein model =: Zi xuan : bo se zi mo xing ji Hubbard-Holstein mo xing zhong zhi sheng zi xiao ying. / Zi xuan : bo se zi mo xing ji Hubbard-Holstein mo xing zhong zhi sheng zi xiao ying

by Wong Wing Hung. / Thesis (Ph.D.)--Chinese University of Hong Kong, 1996. / Includes bibliographical references (leaves 127-129). / by Wong Wing Hung. / Acknowledgments --- p.v / Abstract --- p.vii / Chapter 1 --- Introduction - Charming simple harmonic oscillator --- p.1 / Chapter 1.1 --- High school physics --- p.1 / Chapter 1.2 --- Quantum mechanics --- p.2 / Chapter 1.3 --- Quantum dissipative systems and harmonic oscillator --- p.3 / Chapter 1.4 --- Electron-phonon interaction --- p.3 / Chapter 2 --- Dissipative two-state system 一 Spin-boson model --- p.5 / Chapter 2.1 --- Introduction --- p.5 / Chapter 2.2 --- "An ""isolated"" two-state system" --- p.6 / Chapter 2.3 --- Coupling to the environment --- p.7 / Chapter 2.4 --- Derivation of the spin-boson Hamiltonian for an extended system --- p.8 / Chapter 2.5 --- Path integral result (optional) --- p.9 / Chapter 2.5.1 --- "Ohmic, unbiased case (s =1,E= 0)" --- p.9 / Chapter 2.5.2 --- "Nonohmic, unbiased case (s≠1,E = 0)" --- p.12 / Chapter 2.5.3 --- Biased case (E ≠0) --- p.12 / Chapter 2.6 --- Our scope --- p.13 / Chapter 3 --- Correlated squeezed-state approach --- p.14 / Chapter 3.1 --- Introduction --- p.14 / Chapter 3.2 --- Coherent-state and squeezed-state approach --- p.15 / Chapter 3.3 --- Correlated squeezed-state approach --- p.16 / Chapter 3.4 --- Tunneling system coupled to two identical phonon modes --- p.19 / Chapter 3.5 --- Tunneling system coupled to a dispersionless phonon bath --- p.23 / Chapter 3.6 --- Conclusion --- p.27 / Chapter 4 --- Exact result for a two-state system coupled to a dispersionless boson bath --- p.28 / Chapter 4.1 --- The decoupling transformation --- p.28 / Chapter 4.2 --- Exact diagonalization result --- p.30 / Chapter 5 --- A variational coupled-cluster approach --- p.38 / Chapter 5.1 --- Introduction --- p.38 / Chapter 5.2 --- """Traditional"" coupled-cluster method" --- p.39 / Chapter 5.2.1 --- Zeroth level --- p.40 / Chapter 5.2.2 --- First level --- p.40 / Chapter 5.2.3 --- Second to fourth levels --- p.41 / Chapter 5.3 --- Variational coupled-cluster method --- p.43 / Chapter 5.3.1 --- Zeroth level --- p.44 / Chapter 5.3.2 --- First level --- p.44 / Chapter 5.3.3 --- Second to fourth levels --- p.45 / Chapter 5.4 --- Traditional CCA based on VCCA --- p.46 / Chapter 5.5 --- Numerical results and discussion --- p.47 / Chapter 5.6 --- Conclusion --- p.56 / Chapter 6 --- A two-state system coupled to an ohmic phonon bath ´ؤ a variational coupled-cluster approach --- p.57 / Chapter 6.1 --- A variable displacement transformation --- p.57 / Chapter 6.2 --- The zeroth level --- p.58 / Chapter 6.3 --- The first level --- p.58 / Chapter 6.4 --- The second level --- p.59 / Chapter 6.5 --- The third level --- p.61 / Chapter 6.6 --- Numerical results and discussions --- p.63 / Chapter 6.7 --- Conclusion --- p.66 / Chapter 7 --- Hubbard-Holstein model --- p.67 / Chapter 7.1 --- The Hubbard model --- p.67 / Chapter 7.2 --- The Hubbard-Holstein model --- p.68 / Chapter 8 --- Heat capacity and spin susceptibility of the Hubbard-Holstein model --- p.69 / Chapter 8.1 --- Grand partition function of the model --- p.69 / Chapter 8.1.1 --- Unperturbed grand partition function --- p.70 / Chapter 8.1.2 --- Second-order correction to grand partition function --- p.72 / Chapter 8.1.3 --- Fourth-order correction to grand partition function --- p.74 / Chapter 8.1.4 --- Third-order correction to the grand partition function --- p.75 / Chapter 8.2 --- One- and two-dimensional regular lattices --- p.76 / Chapter 8.2.1 --- Linear chain --- p.76 / Chapter 8.2.2 --- Square lattice --- p.81 / Chapter 8.3 --- Amorphous models --- p.84 / Chapter 8.3.1 --- One-dimensional model --- p.85 / Chapter 8.3.2 --- Two-dimensional model --- p.88 / Chapter 8.4 --- Conclusion --- p.90 / Chapter 9 --- Nuclear spin-lattice relaxation of the Hubbard-Holstein model --- p.92 / Chapter 9.1 --- Formalism --- p.92 / Chapter 9.2 --- One-dimensional systems --- p.100 / Chapter 9.2.1 --- Regular linear chain --- p.100 / Chapter 9.2.2 --- Amorphous linear chain --- p.102 / Chapter 9.3 --- Three-dimensional systems --- p.103 / Chapter 9.3.1 --- Simple cubic lattice --- p.103 / Chapter 9.3.2 --- Three-dimensional amorphous structure --- p.104 / Chapter 9.4 --- Conclusion --- p.106 / Chapter A --- Coherent state and squeezed state --- p.107 / Chapter A.1 --- Coherent state --- p.107 / Chapter A.2 --- Single-mode squeezed state --- p.109 / Chapter A.3 --- Generalized multimode squeezing --- p.109 / Chapter B --- Construction of a rotation transformation --- p.110 / Chapter C --- Perturbation series for the grand partition function --- p.114 / Chapter D --- Propagator of simple harmonic oscillator --- p.116 / Chapter E --- Derivation of the nuclear spin-lattice relaxation time --- p.118 / Bibliography --- p.127

Identiferoai:union.ndltd.org:cuhk.edu.hk/oai:cuhk-dr:cuhk_321584
Date January 1996
ContributorsWong, Wing Hung., Chinese University of Hong Kong Graduate School. Division of Physics.
PublisherChinese University of Hong Kong
Source SetsThe Chinese University of Hong Kong
LanguageEnglish
Detected LanguageEnglish
TypeText, bibliography
Formatprint, viii, 129 leaves : ill. ; 30 cm.
RightsUse of this resource is governed by the terms and conditions of the Creative Commons “Attribution-NonCommercial-NoDerivatives 4.0 International” License (http://creativecommons.org/licenses/by-nc-nd/4.0/)

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