
eBook - PDF
Nonequilibrium Many-Body Theory of Quantum Systems
A Modern Introduction
- 620 pages
- English
- PDF
- Available on iOS & Android
eBook - PDF
Nonequilibrium Many-Body Theory of Quantum Systems
A Modern Introduction
About this book
The Green's function method is one of the most powerful and versatile formalisms in physics, and its nonequilibrium version has proved invaluable in many research fields. This book provides a unique, self-contained introduction to nonequilibrium many-body theory. Starting with basic quantum mechanics, the authors introduce the equilibrium and nonequilibrium Green's function formalisms within a unified framework called the contour formalism. The physical content of the contour Green's functions and the diagrammatic expansions are explained with a focus on the time-dependent aspect. Every result is derived step-by-step, critically discussed and then applied to different physical systems, ranging from molecules and nanostructures to metals and insulators. With an abundance of illustrative examples, this accessible book is ideal for graduate students and researchers who are interested in excited state properties of matter and nonequilibrium physics.
Trusted by 375,005 students
Access to over 1.5 million titles for a fair monthly price.
Study more efficiently using our study tools.
Information
Table of contents
- Contents
- Preface
- List of abbreviations and acronyms
- Fundamental constants and basic relations
- 1 Second quantization
- 1.1 Quantum mechanics of one particle
- 1.2 Quantum mechanics of many particles
- 1.3 Quantum mechanics of many identical particles
- 1.4 Field operators
- 1.5 General basis states
- 1.6 Hamiltonian in second quantization
- 1.7 Density matrices and quantum averages
- 2 Getting familiar with second quantization: model Hamiltonians
- 2.1 Model Hamiltonians
- 2.2 PariserâParrâPople model
- 2.3 Noninteracting models
- 2.3.1 Bloch theorem and band structure
- 2.3.2 Fano model
- 2.4 Hubbard model
- 2.4.1 Particleâhole symmetry: application to the Hubbard dimer
- 2.5 Heisenberg model
- 2.6 BCS model and the exact Richardson solution
- 2.7 Holstein model
- 2.7.1 Peierls instability
- 2.7.2 LangâFirsov transformation: the heavy polaron
- 3 Time-dependent problems and equations of motion
- 3.1 Introduction
- 3.2 Evolution operator
- 3.3 Equations of motion for operators in the Heisenberg picture
- 3.4 Continuity equation: paramagnetic and diamagnetic currents
- 3.5 Lorentz Force
- 4 The contour idea
- 4.1 Time-dependent quantum averages
- 4.2 Time-dependent ensemble averages
- 4.3 Initial equilibrium and adiabatic switching
- 4.4 Equations of motion on the contour
- 4.5 Operator correlators on the contour
- 5 Many-particle Greenâs functions
- 5.1 MartinâSchwinger hierarchy
- 5.2 Truncation of the hierarchy
- 5.3 Exact solution of the hierarchy from Wickâs theorem
- 5.4 Finite and zero-temperature formalism from the exact solution
- 5.5 Langreth rules
- 6 One-particle Greenâs function
- 6.1 What can we learn from G?
- 6.1.1 The inevitable emergence of memory
- 6.1.2 Matsubara Greenâs function and initial preparations
- 6.1.3 Lesser/greater Greenâs function: relaxation and quasi-particles
- 6.2 Noninteracting Greenâs function
- 6.2.1 Matsubara component
- 6.2.2 Lesser and greater components
- 6.2.3 All other components and a useful exercise
- 6.3 Interacting Greenâs function and Lehmann representation
- 6.3.1 Steady-states, persistent oscillations,initial-state dependence
- 6.3.2 Fluctuationâdissipation theorem and otherexact properties
- 6.3.3 Spectral function and probability interpretation
- 6.3.4 Photoemission experiments and interaction effects
- 6.4 Total energy from the GalitskiiâMigdal formula
- 7 Mean field approximations
- 7.1 Introduction
- 7.2 Hartree approximation
- 7.2.1 Hartree equations
- 7.2.2 Electron gas
- 7.2.3 Quantum discharge of a capacitor
- 7.3 HartreeâFock approximation
- 7.3.1 HartreeâFock equations
- 7.3.2 Coulombic electron gas and spin-polarized solutions
- 8 Conserving approximations: two-particle Greenâs function
- 8.1 Introduction
- 8.2 Conditions on the approximate G2
- 8.3 Continuity equation
- 8.4 Momentum conservation law
- 8.5 Angular momentum conservation law
- 8.6 Energy conservation law
- 9 Conserving approximations: self-energy
- 9.1 Self-energy and Dyson equations I
- 9.2 Conditions on the approximate ÎŁ
- 9.3 ÎŚ functional
- 9.4 KadanoffâBaym equations
- 9.5 Fluctuationâdissipation theorem for the self-energy
- 9.6 Recovering equilibrium from the KadanoffâBaym equations
- 9.7 Formal solution of the KadanoffâBaym equations
- 10 MBPT for the Greenâs function
- 10.1 Getting started with Feynman diagrams
- 10.2 Loop rule
- 10.3 Cancellation of disconnected diagrams
- 10.4 Summing only the topologically inequivalent diagrams
- 10.5 Self-energy and Dyson equations II
- 10.6 G-skeleton diagrams
- 10.7 W-skeleton diagrams
- 10.8 Summary and Feynman rules
- 11 MBPT and variational principles for the grand potential
- 11.1 Linked cluster theorem
- 11.2 Summing only the topologically inequivalent diagrams
- 11.3 How to construct the ÎŚ functional
- 11.4 Dressed expansion of the grand potential
- 11.5 LuttingerâWard and Klein functionals
- 11.6 LuttingerâWard theorem
- 11.7 Relation between the reducible polarizability and the ÎŚ functional
- 11.8 Ψ functional
- 11.9 Screened functionals
- 12 MBPT for the two-particle Greenâs function
- 12.1 Diagrams for G2 and loop rule
- 12.2 BetheâSalpeter equation
- 12.3 Excitons
- 12.4 Diagrammatic proof of K = ¹δΣ/δG
- 12.5 Vertex function and Hedin equations
- 13 Applications of MBPT to equilibrium problems
- 13.1 Lifetimes and quasi-particles
- 13.2 Fluctuationâdissipation theorem for P and W
- 13.3 Correlations in the second-Born approximation
- 13.3.1 Polarization effects
- 13.4 Ground-state energy and correlation energy
- 13.5 GW correlation energy of a Coulombic electron gas
- 13.6 T-matrix approximation
- 13.6.1 Formation of a Cooper pair
- 14 Linear response theory: preliminaries
- 14.1 Introduction
- 14.2 Shortcomings of the linear response theory
- 14.2.1 Discreteâdiscrete coupling
- 14.2.2 Discreteâcontinuum coupling
- 14.2.3 Continuumâcontinuum coupling
- 14.3 Fermi golden rule
- 14.4 Kubo formula
- 15 Linear response theory: many-body formulation
- 15.1 Current and density response function
- 15.2 Lehmann representation
- 15.2.1 Analytic structure
- 15.2.2 The f-sum rule
- 15.2.3 Noninteracting fermions
- 15.3 BetheâSalpeter equation from the variation of a conserving G
- 15.4 Ward identity and the f-sum rule
- 15.5 Time-dependent screening in an electron gas
- 15.5.1 Noninteracting density response function
- 15.5.2 RPA density response function
- 15.5.3 Sudden creation of a localized hole
- 15.5.4 Spectral properties in the G0W0 approximation
- 16 Applications of MBPT to nonequilibrium problems
- 16.1 KadanoffâBaym equations for open systems
- 16.2 Time-dependent quantum transport: an exact solution
- 16.2.1 LandauerâBĂźttiker formula
- 16.3 Implementation of the KadanoffâBaym equations
- 16.3.1 Time-stepping technique
- 16.3.2 Second-Born and GW self-energies
- 16.4 Initial-state and history dependence
- 16.5 Charge conservation
- 16.6 Time-dependent GW approximation in open systems
- 16.6.1 Keldysh Greenâs functions in the double-time plane
- 16.6.2 Time-dependent current and spectral function
- 16.6.3 Screened interaction and physical interpretation
- 16.7 Inbedding technique: how to explore the reservoirs
- 16.8 Response functions from time-propagation
- Appendices
- A Fromthe N roots of 1 to the Dirac δ-function
- B Graphical approach to permanents and determinants
- C Density matrices and probability interpretation
- D Thermodynamics and statistical mechanics
- E Greenâs functions and lattice symmetry
- F Asymptotic expansions
- G Wickâs theorem for general initial states
- H BBGKY hierarchy
- I Fromδ-like peaks to continuous spectral functions
- J Virial theorem for conserving approximations
- K Momentum distribution and sharpness of the Fermi surface
- L Hedin equations from a generating functional
- M LippmannâSchwinger equation and cross-section
- N Why the name Random Phase Approximation?
- O KramersâKronig relations
- P Algorithm for solving the KadanoffâBaym equations
- References
- Index
Frequently asked questions
Yes, you can cancel anytime from the Subscription tab in your account settings on the Perlego website. Your subscription will stay active until the end of your current billing period. Learn how to cancel your subscription
No, books cannot be downloaded as external files, such as PDFs, for use outside of Perlego. However, you can download books within the Perlego app for offline reading on mobile or tablet. Learn how to download books offline
We are an online textbook subscription service, where you can get access to an entire online library for less than the price of a single book per month. With over 1.5 million books across 990+ topics, weâve got you covered! Learn about our mission
Look out for the read-aloud symbol on your next book to see if you can listen to it. The read-aloud tool reads text aloud for you, highlighting the text as it is being read. You can pause it, speed it up and slow it down. Learn more about Read Aloud
Yes! You can use the Perlego app on both iOS and Android devices to read anytime, anywhere â even offline. Perfect for commutes or when youâre on the go.
Please note we cannot support devices running on iOS 13 and Android 7 or earlier. Learn more about using the app
Please note we cannot support devices running on iOS 13 and Android 7 or earlier. Learn more about using the app
Yes, you can access Nonequilibrium Many-Body Theory of Quantum Systems by Gianluca Stefanucci,Robert van Leeuwen in PDF and/or ePUB format, as well as other popular books in Physical Sciences & Physics. We have over 1.5 million books available in our catalogue for you to explore.