A guide to. Feynman diagrams in the many-body problem

Size: px
Start display at page:

Download "A guide to. Feynman diagrams in the many-body problem"

Transcription

1 A guide to. Feynman diagrams in the many-body problem Richard D. Mattuck SECOND EDITION

2

3 PAGE Preface to second edition v Preface to first edition. vi i 0. The Many-Body Problem for Everybody What the many-body problem is about Simple example of non-interacting fictitious bodies Quasi particles and quasi horses Collective excitations Feynman Diagrams, or how to Solve the Many-Body Problem by means o f Pictures Propagators-the heroes of the many-body problem Calculating propagators by Feynman diagrams : the drunken man propagator Propagator for single electron moving through a metal Single-particle propagator for system of many interacting particles The two-particle propagator and the particle-hole propagator The no-particle propagator (` vacuum amplitude') Classical Quasi Particles and the Pinball Propagator Physical picture of quasi particle The classical quasi particle propagator Calculation of the propagator by means of diagrams Quantum Quasi Particles and the Quantum Pinball Propagator The quantum mechanical propagator The quantum pinball game Disappearance of disagreeable divergences Where the diagram expansion of the propagator really comes from Energy and lifetime of an electron in an impure metal Quasi Particles in Fermi Systems Propagator method in many-body systems Non-interacting Fermi system in external potential ; particle-hole picture A primer of occupation number formalism (second quantization) Propagator for non-interacting Fermi system in external perturbin g potential Interacting Fermi system The `quasi-physical' nature of Feynman diagrams Hartree and Hartree-Fock quasi particles Hartree-Fock quasi particles in nuclear matter Quasi particles in the electron gas, and the random phase approxima - tion 94

4 YAVt: 5. Ground State Energy and the Vacuum Amplitude or `No-particle Propagator' Meaning of the vacuum amplitude The pinball machine vacuum amplitude Quantum vacuum amplitude for one-particle system Linked cluster theorem for one-particle system Finding the ground state energy in one-particle system The many-body case Bird's-Eye View of Diagram Methods in the Many-Body Problem Occupation Number Formalism (Second Quantization) The advantages of occupation number formalism Many-body wave function in occupation number formalism Operators in occupation number formalism Hamiltonian and Schrödinger equation in occupation number formalism Particle-hole formalism Occupation number formalism based on single-particle positio n eigenstates Bosons More about Quasi Particles Introduction A soluble fermion system : the pure Hartree model Crude calculation of quasi particle lifetime General form of quasi particle propagator The Single-Particle Propagator Re-visited Second quantization and the propagator Mathematical expression for the single-particle Green's functio n propagator Spectral density function Derivation of the propagator expansion in the many-body case Topology of diagrams Diagram rules for single-particle propagator Modified propagator formalism using chemical potential, Beyond Hartree-Fock : the single pair-bubble approximation Dyson's Equation, Renormalization, RPA and Ladder Approximations General types of partial sums Dyson's equation Quasi particles in low-density Fermi system (ladder approximation) Quasi particles in high-density electron gas (random phase approxi - mation) The general `dressed' or `effective' interaction The scattering amplitude Evaluation of the pair bubble ; Friedel oscillations. 197

5 PAGE 11. Self-Consistent Renormalization and the Existence of the Fermi Surface Dressed particle and hole lines, or `clothed skeletons' Existence of quasi particles when the perturbation expansion is valid Existence of the Fermi surface in an interacting system Dressed vertices Ground State Energy of Electron Gas and Nuclear Matter Review Diagrams for the ground state energy Ground state energy of high-density electron gas : theory of Gell-Mann and Brueckner Brief view of Brueckner theory of nuclear matter Collective Excitations and the Two-Particle Propagator Introduction The two-particle Green's function propagator Polarization (` density fluctuation ') propagator Retarded polarization propagator and linear response The collective excitation propagator Plasmons and quasi plasmons Expressing the two-particle propagator in terms of the scattering amplitude Fermi Systems at Finite Temperature Generalization of the T=0 case Statistical mechanics in occupation number formalism The finite temperature propagator The finite temperature vacuum amplitude The pair-bubble at finite temperature Diagram Methods in Superconductivity Introduction Hamiltonian for coupled electron-phonon system Short review of BCS theory Breakdown of the perturbation expansion in a superconductor A brief look at Nambu formalism Treatment of retardation effects by Nambu formalism Transition temperature of a superconductor Phonons From a Many-Body Viewpoint (Reprint) 275

6 17. Quantum Field Theory of Phase Transitions in Fermi Systems Introduction Qualitative theory of phase transitions Anomalous propagators and the breakdown of the perturbation serie s in the condensed phase The generalized matrix propagator Application to ferromagnetic phase in system with 8-function inter - action Divergence of the two-particle propagator and scattering amplitud e at the transition point Feynman Diagrams in the Kondo Problem Introduction Second-order (Born) approximation Parquet approximation with bare propagators Self-consistently renormalized s-electrons Strong-coupling approximation with self-consistently renormalized pseudofermions and vertices The Renormalization Group Introduction Review of effective interaction in the high-density electron gas Renormalization group for interaction propagators in the high-densit y electron gas Transforming from one transformed quantity to another : the functional equation of the renormalization group Lie equation for the renormalization group Solution of the Lie equation Appendices d. Finding fictitious particles with the canonical transformation A. Dirac formalism. 345 B. The time development operator, U(t) C. Finding the ground state energy from the vacuum amplitude D. The 17(t) operator and its expansion E. Expansion of the single-particle propagator and vacuum amplitude F. Evaluating matrix elements by Wick's theorem G. Derivation of the graphical expansion for propagator and vacuu m amplitude H. The spectral density function. 372 I. How the i8 factor is used J. Electron propagator in normal electron-phonon system K. Spin wave functions L. Summary of different kinds of propagators and their spectral representations and analytic properties M. The decoupled equations of motion for the Green's function expresse d as a partial sum of Feyman diagrams. 391 N. The reduced graph expansion. 395

7 Answers to Exercises. 402 References 414 Index 422

A guide to Feynman diagrams in the many-body Problem

A guide to Feynman diagrams in the many-body Problem A guide to Feynman diagrams in the many-body Problem Second edition Richard D.[Mattuck H. C. ßrsted Institute University of Copenhagen, Denmark ausgesondert am 2 h. April \%%' McGraw-Hill International

More information

Many-Body Problems and Quantum Field Theory

Many-Body Problems and Quantum Field Theory Philippe A. Martin Francois Rothen Many-Body Problems and Quantum Field Theory An Introduction Translated by Steven Goldfarb, Andrew Jordan and Samuel Leach Second Edition With 102 Figures, 7 Tables and

More information

Green's Function in. Condensed Matter Physics. Wang Huaiyu. Alpha Science International Ltd. SCIENCE PRESS 2 Beijing \S7 Oxford, U.K.

Green's Function in. Condensed Matter Physics. Wang Huaiyu. Alpha Science International Ltd. SCIENCE PRESS 2 Beijing \S7 Oxford, U.K. Green's Function in Condensed Matter Physics Wang Huaiyu SCIENCE PRESS 2 Beijing \S7 Oxford, U.K. Alpha Science International Ltd. CONTENTS Part I Green's Functions in Mathematical Physics Chapter 1 Time-Independent

More information

Preface Introduction to the electron liquid

Preface Introduction to the electron liquid Table of Preface page xvii 1 Introduction to the electron liquid 1 1.1 A tale of many electrons 1 1.2 Where the electrons roam: physical realizations of the electron liquid 5 1.2.1 Three dimensions 5 1.2.2

More information

Part I. Many-Body Systems and Classical Field Theory

Part I. Many-Body Systems and Classical Field Theory Part I. Many-Body Systems and Classical Field Theory 1. Classical and Quantum Mechanics of Particle Systems 3 1.1 Introduction. 3 1.2 Classical Mechanics of Mass Points 4 1.3 Quantum Mechanics: The Harmonic

More information

Quantum Field Theory. Kerson Huang. Second, Revised, and Enlarged Edition WILEY- VCH. From Operators to Path Integrals

Quantum Field Theory. Kerson Huang. Second, Revised, and Enlarged Edition WILEY- VCH. From Operators to Path Integrals Kerson Huang Quantum Field Theory From Operators to Path Integrals Second, Revised, and Enlarged Edition WILEY- VCH WILEY-VCH Verlag GmbH & Co. KGaA I vh Contents Preface XIII 1 Introducing Quantum Fields

More information

Summary of Mattuck Chapters 16 and 17

Summary of Mattuck Chapters 16 and 17 Summary of Mattuck Chapters 16 and 17 Tomas Petersson Växjö university 2008-02-05 1 Phonons form a Many-Body Viewpoint Hamiltonian for coupled Einstein phonons Definition of Einstein phonon propagator

More information

MANY BODY PHYSICS - HT Meeting 3 pt.1: Mattuck Chapter 0-2

MANY BODY PHYSICS - HT Meeting 3 pt.1: Mattuck Chapter 0-2 MANY BODY PHYSICS - HT 2007 Meeting 3 pt.1: Mattuck Chapter 0-2 1 1 The Many-Body Problem for Everybody 1.1 The many body problem Systems of many interacting bodies. Examples: Nucleons in a nucleus Electrons

More information

Quantum Field Theory 2 nd Edition

Quantum Field Theory 2 nd Edition Quantum Field Theory 2 nd Edition FRANZ MANDL and GRAHAM SHAW School of Physics & Astromony, The University of Manchester, Manchester, UK WILEY A John Wiley and Sons, Ltd., Publication Contents Preface

More information

Andrea Marini. Introduction to the Many-Body problem (I): the diagrammatic approach

Andrea Marini. Introduction to the Many-Body problem (I): the diagrammatic approach Introduction to the Many-Body problem (I): the diagrammatic approach Andrea Marini Material Science Institute National Research Council (Monterotondo Stazione, Italy) Zero-Point Motion Many bodies and

More information

Quantum Mechanics: Fundamentals

Quantum Mechanics: Fundamentals Kurt Gottfried Tung-Mow Yan Quantum Mechanics: Fundamentals Second Edition With 75 Figures Springer Preface vii Fundamental Concepts 1 1.1 Complementarity and Uncertainty 1 (a) Complementarity 2 (b) The

More information

Quantum Field Theory. and the Standard Model. !H Cambridge UNIVERSITY PRESS MATTHEW D. SCHWARTZ. Harvard University

Quantum Field Theory. and the Standard Model. !H Cambridge UNIVERSITY PRESS MATTHEW D. SCHWARTZ. Harvard University Quantum Field Theory and the Standard Model MATTHEW D. Harvard University SCHWARTZ!H Cambridge UNIVERSITY PRESS t Contents v Preface page xv Part I Field theory 1 1 Microscopic theory of radiation 3 1.1

More information

Lecture notes for QFT I (662)

Lecture notes for QFT I (662) Preprint typeset in JHEP style - PAPER VERSION Lecture notes for QFT I (66) Martin Kruczenski Department of Physics, Purdue University, 55 Northwestern Avenue, W. Lafayette, IN 47907-036. E-mail: markru@purdue.edu

More information

MASTER OF SCIENCE IN PHYSICS

MASTER OF SCIENCE IN PHYSICS MASTER OF SCIENCE IN PHYSICS The Master of Science in Physics program aims to develop competent manpower to fill the demands of industry and academe. At the end of the program, the students should have

More information

1 The Quantum Anharmonic Oscillator

1 The Quantum Anharmonic Oscillator 1 The Quantum Anharmonic Oscillator Perturbation theory based on Feynman diagrams can be used to calculate observables in Quantum Electrodynamics, like the anomalous magnetic moment of the electron, and

More information

QUANTUM MECHANICS. Franz Schwabl. Translated by Ronald Kates. ff Springer

QUANTUM MECHANICS. Franz Schwabl. Translated by Ronald Kates. ff Springer Franz Schwabl QUANTUM MECHANICS Translated by Ronald Kates Second Revised Edition With 122Figures, 16Tables, Numerous Worked Examples, and 126 Problems ff Springer Contents 1. Historical and Experimental

More information

The Advent of Quantum Field Theoretical Methods in Solid State Physics. Christian Joas MPIWG

The Advent of Quantum Field Theoretical Methods in Solid State Physics. Christian Joas MPIWG The Advent of Quantum Field Theoretical Methods in Solid State Physics Christian Joas MPIWG Overview λ general claims λ case study in postwar theoretical physics: the quantum plasma from early theories

More information

QUANTUM FIELD THEORY IN CONDENSED MATTER PHYSICS. Wolfgang Belzig

QUANTUM FIELD THEORY IN CONDENSED MATTER PHYSICS. Wolfgang Belzig QUANTUM FIELD THEORY IN CONDENSED MATTER PHYSICS Wolfgang Belzig FORMAL MATTERS Wahlpflichtfach 4h lecture + 2h exercise Lecture: Mon & Thu, 10-12, P603 Tutorial: Mon, 14-16 (P912) or 16-18 (P712) 50%

More information

Static and covariant meson-exchange interactions in nuclear matter

Static and covariant meson-exchange interactions in nuclear matter Workshop on Relativistic Aspects of Two- and Three-body Systems in Nuclear Physics - ECT* - 19-23/10/2009 Static and covariant meson-exchange interactions in nuclear matter Brett V. Carlson Instituto Tecnológico

More information

TENTATIVE SYLLABUS INTRODUCTION

TENTATIVE SYLLABUS INTRODUCTION Physics 615: Overview of QFT Fall 2010 TENTATIVE SYLLABUS This is a tentative schedule of what we will cover in the course. It is subject to change, often without notice. These will occur in response to

More information

Contents. Appendix A Strong limit and weak limit 35. Appendix B Glauber coherent states 37. Appendix C Generalized coherent states 41

Contents. Appendix A Strong limit and weak limit 35. Appendix B Glauber coherent states 37. Appendix C Generalized coherent states 41 Contents Preface 1. The structure of the space of the physical states 1 1.1 Introduction......................... 1 1.2 The space of the states of physical particles........ 2 1.3 The Weyl Heisenberg algebra

More information

Lecture 5. Hartree-Fock Theory. WS2010/11: Introduction to Nuclear and Particle Physics

Lecture 5. Hartree-Fock Theory. WS2010/11: Introduction to Nuclear and Particle Physics Lecture 5 Hartree-Fock Theory WS2010/11: Introduction to Nuclear and Particle Physics Particle-number representation: General formalism The simplest starting point for a many-body state is a system of

More information

Lecture 1: The Equilibrium Green Function Method

Lecture 1: The Equilibrium Green Function Method Lecture 1: The Equilibrium Green Function Method Mark Jarrell April 27, 2011 Contents 1 Why Green functions? 2 2 Different types of Green functions 4 2.1 Retarded, advanced, time ordered and Matsubara

More information

Lecture Models for heavy-ion collisions (Part III): transport models. SS2016: Dynamical models for relativistic heavy-ion collisions

Lecture Models for heavy-ion collisions (Part III): transport models. SS2016: Dynamical models for relativistic heavy-ion collisions Lecture Models for heavy-ion collisions (Part III: transport models SS06: Dynamical models for relativistic heavy-ion collisions Quantum mechanical description of the many-body system Dynamics of heavy-ion

More information

The very basic: QF methods and many body perturbation theory

The very basic: QF methods and many body perturbation theory The very basic: QF methods and many body perturbation theory Georg Kresse, Felix Hummel Faculty of Physics, Universität Wien Funded by the Austrian FWF SFB ViCoM FOR 1346 Outline Intro 2nd PT Diag. Introduction

More information

Introduction to particle physics Lecture 2

Introduction to particle physics Lecture 2 Introduction to particle physics Lecture 2 Frank Krauss IPPP Durham U Durham, Epiphany term 2009 Outline 1 Quantum field theory Relativistic quantum mechanics Merging special relativity and quantum mechanics

More information

Strongly correlated Cooper pair insulators and superfluids

Strongly correlated Cooper pair insulators and superfluids Strongly correlated Cooper pair insulators and superfluids Predrag Nikolić George Mason University Acknowledgments Collaborators Subir Sachdev Eun-Gook Moon Anton Burkov Arun Paramekanti Affiliations and

More information

Field Theories in Condensed Matter Physics. Edited by. Sumathi Rao. Harish-Chandra Research Institute Allahabad. lop

Field Theories in Condensed Matter Physics. Edited by. Sumathi Rao. Harish-Chandra Research Institute Allahabad. lop Field Theories in Condensed Matter Physics Edited by Sumathi Rao Harish-Chandra Research Institute Allahabad lop Institute of Physics Publishing Bristol and Philadelphia Contents Preface xiii Introduction

More information

Electrical Transport in Nanoscale Systems

Electrical Transport in Nanoscale Systems Electrical Transport in Nanoscale Systems Description This book provides an in-depth description of transport phenomena relevant to systems of nanoscale dimensions. The different viewpoints and theoretical

More information

Quantum Physics II (8.05) Fall 2002 Outline

Quantum Physics II (8.05) Fall 2002 Outline Quantum Physics II (8.05) Fall 2002 Outline 1. General structure of quantum mechanics. 8.04 was based primarily on wave mechanics. We review that foundation with the intent to build a more formal basis

More information

Contents. 1.1 Prerequisites and textbooks Physical phenomena and theoretical tools The path integrals... 9

Contents. 1.1 Prerequisites and textbooks Physical phenomena and theoretical tools The path integrals... 9 Preface v Chapter 1 Introduction 1 1.1 Prerequisites and textbooks......................... 1 1.2 Physical phenomena and theoretical tools................. 5 1.3 The path integrals..............................

More information

PRINCIPLES OF PHYSICS. \Hp. Ni Jun TSINGHUA. Physics. From Quantum Field Theory. to Classical Mechanics. World Scientific. Vol.2. Report and Review in

PRINCIPLES OF PHYSICS. \Hp. Ni Jun TSINGHUA. Physics. From Quantum Field Theory. to Classical Mechanics. World Scientific. Vol.2. Report and Review in LONDON BEIJING HONG TSINGHUA Report and Review in Physics Vol2 PRINCIPLES OF PHYSICS From Quantum Field Theory to Classical Mechanics Ni Jun Tsinghua University, China NEW JERSEY \Hp SINGAPORE World Scientific

More information

Molecular Electronics

Molecular Electronics Molecular Electronics An Introduction to Theory and Experiment Juan Carlos Cuevas Universidad Autönoma de Madrid, Spain Elke Scheer Universität Konstanz, Germany 1>World Scientific NEW JERSEY LONDON SINGAPORE

More information

2 Canonical quantization

2 Canonical quantization Phys540.nb 7 Canonical quantization.1. Lagrangian mechanics and canonical quantization Q: How do we quantize a general system?.1.1.lagrangian Lagrangian mechanics is a reformulation of classical mechanics.

More information

Landau-Fermi liquid theory

Landau-Fermi liquid theory Landau-Fermi liquid theory Shreyas Patankar Chennai Mathematical Institute Abstract We study the basic properties of Landau s theory of a system of interacting fermions (a Fermi liquid). The main feature

More information

in-medium pair wave functions the Cooper pair wave function the superconducting order parameter anomalous averages of the field operators

in-medium pair wave functions the Cooper pair wave function the superconducting order parameter anomalous averages of the field operators (by A. A. Shanenko) in-medium wave functions in-medium pair-wave functions and spatial pair particle correlations momentum condensation and ODLRO (off-diagonal long range order) U(1) symmetry breaking

More information

Chapter 10 Dyson s equation, RPA and Ladder Approximations

Chapter 10 Dyson s equation, RPA and Ladder Approximations Chapter 1 Dyson s euation RPA and Ladder Approximations Dyson s euation low-high density fermion gases Summation tris to deal with divergent series. Conept of renormalization i.e. dressed partile is bare

More information

Dirac-Brueckner mean fields and an effective* density-dependent DiracHartree-Fock interaction in nuclear. matter

Dirac-Brueckner mean fields and an effective* density-dependent DiracHartree-Fock interaction in nuclear. matter Dirac-Brueckner mean fields and an effective* density-dependent DiracHartree-Fock interaction in nuclear matter Brett V. Carlson Instituto Tecnológico de Aeronáutica, São José dos Campos Brazil and Daisy

More information

arxiv:cond-mat/ v1 [cond-mat.supr-con] 11 Dec 1997

arxiv:cond-mat/ v1 [cond-mat.supr-con] 11 Dec 1997 Anderson Model in a Superconductor: Φ-Derivable Theory arxiv:cond-mat912118v1 [cond-matsupr-con] 11 Dec 199 Ari T Alastalo (a), Robert J Joynt (b) and Martti M Salomaa (a,b) (a) Materials Physics Laboratory,

More information

Condensed matter physics FKA091

Condensed matter physics FKA091 Condensed matter physics FKA091 Ermin Malic Department of Physics Chalmers University of Technology Henrik Johannesson Department of Physics University of Gothenburg Teaching assistants: Roland Jago &

More information

2.1 Green Functions in Quantum Mechanics

2.1 Green Functions in Quantum Mechanics Chapter 2 Green Functions and Observables 2.1 Green Functions in Quantum Mechanics We will be interested in studying the properties of the ground state of a quantum mechanical many particle system. We

More information

Euclidean path integral formalism: from quantum mechanics to quantum field theory

Euclidean path integral formalism: from quantum mechanics to quantum field theory : from quantum mechanics to quantum field theory Dr. Philippe de Forcrand Tutor: Dr. Marco Panero ETH Zürich 30th March, 2009 Introduction Real time Euclidean time Vacuum s expectation values Euclidean

More information

FRG approach to interacting fermions with partial bosonization: from weak to strong coupling

FRG approach to interacting fermions with partial bosonization: from weak to strong coupling FRG approach to interacting fermions with partial bosonization: from weak to strong coupling Talk at conference ERG08, Heidelberg, June 30, 2008 Peter Kopietz, Universität Frankfurt collaborators: Lorenz

More information

Quantum Algorithms for Quantum Field Theories

Quantum Algorithms for Quantum Field Theories Quantum Algorithms for Quantum Field Theories Stephen Jordan Joint work with Keith Lee John Preskill Science, 336:1130 (2012) Jan 24, 2012 The full description of quantum mechanics for a large system with

More information

The Physics of Nanoelectronics

The Physics of Nanoelectronics The Physics of Nanoelectronics Transport and Fluctuation Phenomena at Low Temperatures Tero T. Heikkilä Low Temperature Laboratory, Aalto University, Finland OXFORD UNIVERSITY PRESS Contents List of symbols

More information

LECTURES ON QUANTUM MECHANICS

LECTURES ON QUANTUM MECHANICS LECTURES ON QUANTUM MECHANICS GORDON BAYM Unitsersity of Illinois A II I' Advanced Bock Progrant A Member of the Perseus Books Group CONTENTS Preface v Chapter 1 Photon Polarization 1 Transformation of

More information

Aditi Mitra New York University

Aditi Mitra New York University Superconductivity following a quantum quench Aditi Mitra New York University Supported by DOE-BES and NSF- DMR 1 Initially system of free electrons. Quench involves turning on attractive pairing interactions.

More information

P. W. Atkins and R. S. Friedman. Molecular Quantum Mechanics THIRD EDITION

P. W. Atkins and R. S. Friedman. Molecular Quantum Mechanics THIRD EDITION P. W. Atkins and R. S. Friedman Molecular Quantum Mechanics THIRD EDITION Oxford New York Tokyo OXFORD UNIVERSITY PRESS 1997 Introduction and orientation 1 Black-body radiation 1 Heat capacities 2 The

More information

5. Superconductivity. R(T) = 0 for T < T c, R(T) = R 0 +at 2 +bt 5, B = H+4πM = 0,

5. Superconductivity. R(T) = 0 for T < T c, R(T) = R 0 +at 2 +bt 5, B = H+4πM = 0, 5. Superconductivity In this chapter we shall introduce the fundamental experimental facts about superconductors and present a summary of the derivation of the BSC theory (Bardeen Cooper and Schrieffer).

More information

Monday, April 13. Today: equation of motion method (EOM) Dyson equation and Self-energy. Many-Body Green s Functions

Monday, April 13. Today: equation of motion method (EOM) Dyson equation and Self-energy. Many-Body Green s Functions Monday, April 13 Today: equation of motion method (EOM) Dyson equation and Self-energy Unperturbed propagator Take a system of non interacting fermions The unperturbed propagator is: ( ) or Unperturbed

More information

Lecture 6. Fermion Pairing. WS2010/11: Introduction to Nuclear and Particle Physics

Lecture 6. Fermion Pairing. WS2010/11: Introduction to Nuclear and Particle Physics Lecture 6 Fermion Pairing WS2010/11: Introduction to Nuclear and Particle Physics Experimental indications for Cooper-Pairing Solid state physics: Pairing of electrons near the Fermi surface with antiparallel

More information

On the Higgs mechanism in the theory of

On the Higgs mechanism in the theory of On the Higgs mechanism in the theory of superconductivity* ty Dietrich Einzel Walther-Meißner-Institut für Tieftemperaturforschung Bayerische Akademie der Wissenschaften D-85748 Garching Outline Phenomenological

More information

Study Plan for Ph.D in Physics (2011/2012)

Study Plan for Ph.D in Physics (2011/2012) Plan Study Plan for Ph.D in Physics (2011/2012) Offered Degree: Ph.D in Physics 1. General Rules and Conditions:- This plan conforms to the regulations of the general frame of the higher graduate studies

More information

Green Functions in Many Body Quantum Mechanics

Green Functions in Many Body Quantum Mechanics Green Functions in Many Body Quantum Mechanics NOTE This section contains some advanced material, intended to give a brief introduction to methods used in many body quantum mechanics. The material at the

More information

Dynamic properties of interacting bosons and magnons

Dynamic properties of interacting bosons and magnons Ultracold Quantum Gases beyond Equilibrium Natal, Brasil, September 27 October 1, 2010 Dynamic properties of interacting bosons and magnons Peter Kopietz, Universität Frankfurt collaboration: A. Kreisel,

More information

The 4th Windsor Summer School on Condensed Matter Theory Quantum Transport and Dynamics in Nanostructures Great Park, Windsor, UK, August 6-18, 2007

The 4th Windsor Summer School on Condensed Matter Theory Quantum Transport and Dynamics in Nanostructures Great Park, Windsor, UK, August 6-18, 2007 The 4th Windsor Summer School on Condensed Matter Theory Quantum Transport and Dynamics in Nanostructures Great Park, Windsor, UK, August 6-18, 2007 Kondo Effect in Metals and Quantum Dots Jan von Delft

More information

BETHE - SALPETER EQUATION THE ORIGINS Edwin E. Salpeter October 2008

BETHE - SALPETER EQUATION THE ORIGINS Edwin E. Salpeter October 2008 1. INTRODUCTION BETHE - SALPETER EQUATION THE ORIGINS Edwin E. Salpeter October 2008 The Bethe-Salpeter equation was first given at an American Physical Society meeting at the beginning of 1951 (Bethe-Salpeter

More information

Summary lecture II. Graphene exhibits a remarkable linear and gapless band structure

Summary lecture II. Graphene exhibits a remarkable linear and gapless band structure Summary lecture II Bloch theorem: eigen functions of an electron in a perfectly periodic potential have the shape of plane waves modulated with a Bloch factor that possess the periodicity of the potential

More information

Part III. Interacting Field Theory. Quantum Electrodynamics (QED)

Part III. Interacting Field Theory. Quantum Electrodynamics (QED) November-02-12 8:36 PM Part III Interacting Field Theory Quantum Electrodynamics (QED) M. Gericke Physics 7560, Relativistic QM 183 III.A Introduction December-08-12 9:10 PM At this point, we have the

More information

International Journal of Scientific Engineering and Applied Science (IJSEAS) - Volume-1, Issue-8,November 2015 ISSN:

International Journal of Scientific Engineering and Applied Science (IJSEAS) - Volume-1, Issue-8,November 2015 ISSN: International Journal of Scientific Engineering and Applied Science (IJSEAS) - Volume-1, Issue-8,November 015 ISSN: 395-3470 Electron Phonon Interactions under the External Applied Electric Fields in the

More information

Tunneling Into a Luttinger Liquid Revisited

Tunneling Into a Luttinger Liquid Revisited Petersburg Nuclear Physics Institute Tunneling Into a Luttinger Liquid Revisited V.Yu. Kachorovskii Ioffe Physico-Technical Institute, St.Petersburg, Russia Co-authors: Alexander Dmitriev (Ioffe) Igor

More information

WORLD SCIENTIFIC (2014)

WORLD SCIENTIFIC (2014) WORLD SCIENTIFIC (2014) LIST OF PROBLEMS Chapter 1: Magnetism of Free Electrons and Atoms 1. Orbital and spin moments of an electron: Using the theory of angular momentum, calculate the orbital

More information

Lecture 2: Ultracold fermions

Lecture 2: Ultracold fermions Lecture 2: Ultracold fermions Fermions in optical lattices. Fermi Hubbard model. Current state of experiments Lattice modulation experiments Doublon lifetimes Stoner instability Ultracold fermions in optical

More information

FEYNMAN DIAGRAM TECHNIQUES IN CONDENSED MATTER PHYSICS

FEYNMAN DIAGRAM TECHNIQUES IN CONDENSED MATTER PHYSICS FEYNMAN DIAGRAM TECHNIQUES IN CONDENSED MATTER PHYSICS A concise introduction to Feynman diagram techniques, this book shows how they can be applied to the analysis of complex many-particle systems, and

More information

Summary lecture IX. The electron-light Hamilton operator reads in second quantization

Summary lecture IX. The electron-light Hamilton operator reads in second quantization Summary lecture IX The electron-light Hamilton operator reads in second quantization Absorption coefficient α(ω) is given by the optical susceptibility Χ(ω) that is determined by microscopic polarization

More information

Condensed matter theory Lecture notes and problem sets 2012/2013

Condensed matter theory Lecture notes and problem sets 2012/2013 Condensed matter theory Lecture notes and problem sets 2012/2013 Dmitri Ivanov Recommended books and lecture notes: [AM] N. W. Ashcroft and N. D. Mermin, Solid State Physics. [Mar] M. P. Marder, Condensed

More information

Introduction to Modern Quantum Optics

Introduction to Modern Quantum Optics Introduction to Modern Quantum Optics Jin-Sheng Peng Gao-Xiang Li Huazhong Normal University, China Vfe World Scientific» Singapore* * NewJerseyL Jersey* London* Hong Kong IX CONTENTS Preface PART I. Theory

More information

Summary lecture VI. with the reduced mass and the dielectric background constant

Summary lecture VI. with the reduced mass and the dielectric background constant Summary lecture VI Excitonic binding energy reads with the reduced mass and the dielectric background constant Δ Statistical operator (density matrix) characterizes quantum systems in a mixed state and

More information

8.3. Feynman diagram. Phys620.nb multi-particle Green s functions the equations of motion of the Green s functions

8.3. Feynman diagram. Phys620.nb multi-particle Green s functions the equations of motion of the Green s functions Phys60.nb 0 8.3. Feynman diagram 8.3.. multi-particle Green s functions Single particle Green s function: G, ' ' (8.7) Two-particle Green s function: G, ; ', ' ' ' (8.73) three-particle Green s function:

More information

Universal theory of complex SYK models and extremal charged black holes

Universal theory of complex SYK models and extremal charged black holes HARVARD Universal theory of complex SYK models and extremal charged black holes Subir Sachdev Jerusalem Winter School, December 31, 2018 HARVARD Wenbo Fu Yingfei Gu Grigory Tarnopolsky 1. Quantum matter

More information

Lecture Notes. Quantum Theory. Prof. Maximilian Kreuzer. Institute for Theoretical Physics Vienna University of Technology. covering the contents of

Lecture Notes. Quantum Theory. Prof. Maximilian Kreuzer. Institute for Theoretical Physics Vienna University of Technology. covering the contents of Lecture Notes Quantum Theory by Prof. Maximilian Kreuzer Institute for Theoretical Physics Vienna University of Technology covering the contents of 136.019 Quantentheorie I and 136.027 Quantentheorie II

More information

Lectures on Quantum Mechanics

Lectures on Quantum Mechanics Lectures on Quantum Mechanics Steven Weinberg The University of Texas at Austin CAMBRIDGE UNIVERSITY PRESS Contents PREFACE page xv NOTATION xviii 1 HISTORICAL INTRODUCTION 1 1.1 Photons 1 Black-body radiation

More information

Preface. Preface to the Third Edition. Preface to the Second Edition. Preface to the First Edition. 1 Introduction 1

Preface. Preface to the Third Edition. Preface to the Second Edition. Preface to the First Edition. 1 Introduction 1 xi Contents Preface Preface to the Third Edition Preface to the Second Edition Preface to the First Edition v vii viii ix 1 Introduction 1 I GENERAL THEORY OF OPEN QUANTUM SYSTEMS 5 Diverse limited approaches:

More information

Physics of atoms and molecules

Physics of atoms and molecules Physics of atoms and molecules 2nd edition B.H. Bransden and C.J. Joachain Prentice Hall An imprint of Pearson Education Harlow, England London New York Boston San Francisco Toronto Sydney Singapore Hong

More information

Solid State Physics. GIUSEPPE GROSSO Professor of Solid State Physics, Department of Physics, University of Pavia, and INFM

Solid State Physics. GIUSEPPE GROSSO Professor of Solid State Physics, Department of Physics, University of Pavia, and INFM Solid State Physics GIUSEPPE GROSSO Professor of Solid State Physics, Department of Physics, University of Pisa, and INFM GIUSEPPE PASTORI PARRAVICINI Professor of Solid State Physics, Department of Physics,

More information

1 Equal-time and Time-ordered Green Functions

1 Equal-time and Time-ordered Green Functions 1 Equal-time and Time-ordered Green Functions Predictions for observables in quantum field theories are made by computing expectation values of products of field operators, which are called Green functions

More information

Quantum Theory of Low Dimensional Systems: Bosonization. Heung-Sun Sim

Quantum Theory of Low Dimensional Systems: Bosonization. Heung-Sun Sim PSI 2014 Quantum Theory of Many Particles ( 평창, 2014 년 8 월 28-29 일 ) Quantum Theory of Low Dimensional Systems: Bosonization Heung-Sun Sim Physics, KAIST Overview Target of this lecture: low dimension

More information

Lattice modulation experiments with fermions in optical lattices and more

Lattice modulation experiments with fermions in optical lattices and more Lattice modulation experiments with fermions in optical lattices and more Nonequilibrium dynamics of Hubbard model Ehud Altman Weizmann Institute David Pekker Harvard University Rajdeep Sensarma Harvard

More information

The Gutzwiller Density Functional Theory

The Gutzwiller Density Functional Theory The Gutzwiller Density Functional Theory Jörg Bünemann, BTU Cottbus I) Introduction 1. Model for an H 2 -molecule 2. Transition metals and their compounds II) Gutzwiller variational theory 1. Gutzwiller

More information

Conference on Superconductor-Insulator Transitions May 2009

Conference on Superconductor-Insulator Transitions May 2009 2035-10 Conference on Superconductor-Insulator Transitions 18-23 May 2009 Phase transitions in strongly disordered magnets and superconductors on Bethe lattice L. Ioffe Rutgers, the State University of

More information

MESOSCOPIC QUANTUM OPTICS

MESOSCOPIC QUANTUM OPTICS MESOSCOPIC QUANTUM OPTICS by Yoshihisa Yamamoto Ata Imamoglu A Wiley-Interscience Publication JOHN WILEY & SONS, INC. New York Chichester Weinheim Brisbane Toronto Singapore Preface xi 1 Basic Concepts

More information

Fermi liquid theory Can we apply the free fermion approximation to a real metal? Phys540.nb Strong interaction vs.

Fermi liquid theory Can we apply the free fermion approximation to a real metal? Phys540.nb Strong interaction vs. Phys540.nb 7 Fermi liquid theory.. Can we apply the free fermion approximation to a real metal? Can we ignore interactions in a real metal? Experiments says yes (free fermion models work very well), but

More information

Non-equilibrium time evolution of bosons from the functional renormalization group

Non-equilibrium time evolution of bosons from the functional renormalization group March 14, 2013, Condensed Matter Journal Club University of Florida at Gainesville Non-equilibrium time evolution of bosons from the functional renormalization group Peter Kopietz, Universität Frankfurt

More information

Shigeji Fujita and Salvador V Godoy. Mathematical Physics WILEY- VCH. WILEY-VCH Verlag GmbH & Co. KGaA

Shigeji Fujita and Salvador V Godoy. Mathematical Physics WILEY- VCH. WILEY-VCH Verlag GmbH & Co. KGaA Shigeji Fujita and Salvador V Godoy Mathematical Physics WILEY- VCH WILEY-VCH Verlag GmbH & Co. KGaA Contents Preface XIII Table of Contents and Categories XV Constants, Signs, Symbols, and General Remarks

More information

Renormalization Group and Fermi Liquid. Theory. A.C.Hewson. Dept. of Mathematics, Imperial College, London SW7 2BZ. Abstract

Renormalization Group and Fermi Liquid. Theory. A.C.Hewson. Dept. of Mathematics, Imperial College, London SW7 2BZ. Abstract Renormalization Group and Fermi Liquid Theory A.C.Hewson Dept. of Mathematics, Imperial College, London SW7 2BZ. Abstract We give a Hamiltonian based interpretation of microscopic Fermi liquid theory within

More information

Excited states and tp propagator for fermions

Excited states and tp propagator for fermions Excited states and tp propagator for fermions So far sp propagator gave access to E 0 Ground-state energy and all expectation values of 1-body operators E +1 Energies in +1 relative to ground state n E0

More information

Medium polarization effects and pairing interaction in finite nuclei

Medium polarization effects and pairing interaction in finite nuclei Medium polarization effects and pairing interaction in finite nuclei S. Baroni, P.F. Bortignon, R.A. Broglia, G. Colo, E. Vigezzi Milano University and INFN F. Barranco Sevilla University Commonly used

More information

Springer Series in Solid-State Sciences. Edited by Peter Fulde

Springer Series in Solid-State Sciences. Edited by Peter Fulde 7 Springer Series in Solid-State Sciences Edited by Peter Fulde Springer Series in Solid-State Sciences Editors: M. Cardona P. Fulde H.-J. Queisser Volume 1 Principles of Magnetic Resonance By C. P. Slichter

More information

7.1 Creation and annihilation operators

7.1 Creation and annihilation operators Chapter 7 Second Quantization Creation and annihilation operators. Occupation number. Anticommutation relations. Normal product. Wick s theorem. One-body operator in second quantization. Hartree- Fock

More information

Optics and Response Functions

Optics and Response Functions Theory seminar: Electronic and optical properties of graphene Optics and Response Functions Matthias Droth, 04.07.2013 Outline: Light absorption by Dirac fermions Intro: response functions The optics of

More information

MOTTNESS AND STRONG COUPLING

MOTTNESS AND STRONG COUPLING MOTTNESS AND STRONG COUPLING ROB LEIGH UNIVERSITY OF ILLINOIS Rutgers University April 2008 based on various papers with Philip Phillips and Ting-Pong Choy PRL 99 (2007) 046404 PRB 77 (2008) 014512 PRB

More information

DR.RUPNATHJI( DR.RUPAK NATH )

DR.RUPNATHJI( DR.RUPAK NATH ) 11 Perturbation Theory and Feynman Diagrams We now turn our attention to interacting quantum field theories. All of the results that we will derive in this section apply equally to both relativistic and

More information

Metals: the Drude and Sommerfeld models p. 1 Introduction p. 1 What do we know about metals? p. 1 The Drude model p. 2 Assumptions p.

Metals: the Drude and Sommerfeld models p. 1 Introduction p. 1 What do we know about metals? p. 1 The Drude model p. 2 Assumptions p. Metals: the Drude and Sommerfeld models p. 1 Introduction p. 1 What do we know about metals? p. 1 The Drude model p. 2 Assumptions p. 2 The relaxation-time approximation p. 3 The failure of the Drude model

More information

Landau-Fermi liquid theory

Landau-Fermi liquid theory Landau- 1 Chennai Mathematical Institute April 25, 2011 1 Final year project under Prof. K. Narayan, CMI Interacting fermion system I Basic properties of metals (heat capacity, susceptibility,...) were

More information

Reference for most of this talk:

Reference for most of this talk: Cold fermions Reference for most of this talk: W. Ketterle and M. W. Zwierlein: Making, probing and understanding ultracold Fermi gases. in Ultracold Fermi Gases, Proceedings of the International School

More information

1 Fluctuations of the number of particles in a Bose-Einstein condensate

1 Fluctuations of the number of particles in a Bose-Einstein condensate Exam of Quantum Fluids M1 ICFP 217-218 Alice Sinatra and Alexander Evrard The exam consists of two independant exercises. The duration is 3 hours. 1 Fluctuations of the number of particles in a Bose-Einstein

More information

MAGNETISM MADE SIMPLE. An Introduction to Physical Concepts and to Some Useful Mathematical Methods. Daniel C. Mattis

MAGNETISM MADE SIMPLE. An Introduction to Physical Concepts and to Some Useful Mathematical Methods. Daniel C. Mattis THE THEORY OF MAGNETISM MADE SIMPLE An Introduction to Physical Concepts and to Some Useful Mathematical Methods Daniel C. Mattis Department of Physics, University of Utah lb World Scientific NEW JERSEY

More information

The Mott Metal-Insulator Transition

The Mott Metal-Insulator Transition Florian Gebhard The Mott Metal-Insulator Transition Models and Methods With 38 Figures Springer 1. Metal Insulator Transitions 1 1.1 Classification of Metals and Insulators 2 1.1.1 Definition of Metal

More information

List of Comprehensive Exams Topics

List of Comprehensive Exams Topics List of Comprehensive Exams Topics Mechanics 1. Basic Mechanics Newton s laws and conservation laws, the virial theorem 2. The Lagrangian and Hamiltonian Formalism The Lagrange formalism and the principle

More information

Madhya Pradesh Bhoj (Open) University, Bhopal. Assignment Question Paper I

Madhya Pradesh Bhoj (Open) University, Bhopal. Assignment Question Paper I Subject : I- Quantum mechanics Maximum Marks : 30 Q6 Q7 Q8 Q6 Q7 Q8 Explain Direc delta function Explain Heitler -London theory of hydrogen molecule. Explain Pauli's exclusion principle. Explain orbital

More information