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Lattice Gauge Theories: An Introduction,9789812560629
Other versions by this Author

Lattice Gauge Theories: An Introduction


Edition: 3rd
Author(s): Rothe, Heinz J.
ISBN10:  9812560629
ISBN13:  9789812560629
Format:  Hardcover
Pub. Date:  6/1/2005
Publisher(s): World Scientific Pub Co Inc


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SummaryTable of Contents
- Wherever possible simple examples, which illustrate the main ideas, are provided before embarking on the actual discussion of the problem of interest
- The book introduces the readers to problems of great current interest, like instantons, calorons, vortices, magnetic monopoles
- QCD at finite temperature is discussed at great length, both in perturbation theory and in Monte Carlo simulations
- The book contains many figures showing numerical results of pioneering work
Preface to the Third Edition vii
Preface to the Second Edition ix
Preface to the First Edition xi
1. INTRODUCTION
1(6)
2. THE PATH INTEGRAL APPROACH TO QUANTIZATION
7(29)
2.1 The Path Integral Method in Quantum Mechanics
8(7)
2.2 Path Integral Representation of Bosonic Green Functions in Field Theory
15(7)
2.3 The Transfer Matrix
22(1)
2.4 Path Integral Representation of Fermionic Green Functions
23(10)
2.5 Discretizing Space-Time. The Lattice as a Regulator of a Quantum Field Theory
33(3)
3. THE FREE SCALAR FIELD ON THE LATTICE
36(7)
4. FERMIONS ON THE LATTICE
43(34)
4.1 The Doubling Problem
43(5)
4.2 A Closer Look at Fermion Doubling
48(8)
4.3 Wilson Fermions
56(1)
4.4 Staggered Fermions
57(4)
4.5 Technical Details of the Staggered Fermion Formulation
61(8)
4.6 Staggered Fermions in Momentum Space
69(4)
4.7 Ginsparg-Wilson Fermions
73(4)
5. ABELIAN GAUGE FIELDS ON THE LATTICE AND COMPACT QED
77(10)
5.1 Preliminaries
77(3)
5.2 Lattice Formulation of QED
80(7)
6. NON-ABELIAN GAUGE FIELDS ON THE LATTICE COMPACT QCD
87(8)
7. THE WILSON LOOP AND THE STATIC QUARK-ANTIQUARK POTENTIAL
95(14)
7.1 A Look at Non-Relativistic Quantum Mechanics
96(1)
7.2 The Wilson Loop and the Static qq-Potential in QED
97(8)
7.3 The Wilson Loop in QCD
105(4)
8. THE QQ POTENTIAL IN SOME SIMPLE MODELS
109(10)
8.1 The Potential in Quenched QED
109(5)
8.2 The Potential in Quenched Compact QED2
114(5)
9. THE CONTINUUM LIMIT OF LATTICE QCD
119(11)
9.1 Critical Behaviour of Lattice QCD and the Continuum Limit
119(3)
9.2 Dependece of the Coupling Constant on the Lattice Spacing and the Renormalization Group β-Function
122(8)
10. LATTICE SUM RULES 130(21)
10.1 Energy Sum Rule for the Harmonic Oscillator
130(6)
10.2 The SU(N) Gauge Action on an Anisotropic Lattice
136(2)
10.3 Sum Rules for the Static qq-Potential
138(8)
10.4 Determination of the Electric, Magnetic and Anomalous Contribution to the qq-Potential
146(2)
10.5 Sum Rules for the Glueball Mass
148(3)
11. THE STRONG COUPLING EXPANSION 151(19)
11.1 The qq-Potential to Leading Order in Strong Coupling
151(3)
11.2 Beyond the Leading Approximation
154(4)
11.3 The Lattice Hamiltonian in the Strong Coupling Limit and the String Picture of Confinement
158(12)
12. THE HOPPING PARAMETER EXPANSION 170(22)
12.1 Path Integral Representation of Correlation Functions in Terms of Bosonic Variables
171(3)
12.2 Hopping Parameter Expansion of the Fermion Propagator in an External Field
174(5)
12.3 Hopping Parameter Expansion of the Effective Action
179(4)
12.4 The HPE and the Pauli Exclusion Principle
183(9)
13. WEAK COUPLING EXPANSION (I). THE Φ³-THEORY 192(17)
13.1 Introduction
192(3)
13.2 Weak Coupling Expansion of Correlation Functions in the φ³-Theory
195(6)
13.3 The Power Counting Theorem of Reisz
201(8)
14. WEAK COUPLING EXPANSION (II). LATTICE QED 209(33)
14.1 The Gauge Fixed Lattice Action
209(7)
14.2 Lattice Feynman Rules
216(6)
14.3 Renormalization of the Axial Vector Current in One-Loop Order
222(12)
14.4 The ABJ Anomaly
234(8)
15. WEAK COUPLING EXPANSION (III). LATTICE QCD 242(42)
15.1 The Link Integration Measure
243(4)
15.2 Gauge Fixing and the Faddeev-Popov Determinant
247(5)
15.3 The Gauge Field Action
252(5)
15.4 Propagators and Vertices
257(15)
15.5 Relation Between Λ and the Λ-Parameter of Continuum QCD
272(3)
15.6 Universality of the Axial Anomaly in Lattice QCD
275(9)
16. MONTE CARLO METHODS 284(33)
16.1 Introduction
284(2)
16.2 Construction Principles for Algorithms. Markov chains
286(5)
16.3 The Metropolis Method
291(2)
16.4 The Langevin Algorithm
293(2)
16.5 The Molecular Dynamics Method
295(6)
16.6 The Hybrid Algorithm
301(3)
16.7 The Hybrid Monte Carlo Algorithm
304(3)
16.8 The Pseudofermion Method
307(6)
16.9 Application of the Hybrid Monte Carlo Algorithm to Systems with Fermions
313(4)
17. SOME RESULTS OF MONTE CARLO CALCULATIONS 317(66)
17.1 The String Tension and the qq-Potential in the SU(3) Gauge Theory
317(7)
17.2 The qq-Potential in Full QCD
324(2)
17.3 Chiral Symmetry Breaking
326(4)
17.4 Glueballs
330(6)
17.5 Hadron Mass Spectrum
336(9)
17.6 Instantons
345(14)
17.7 Flux Tubes in the qq and qqq-Systems
359(4)
17.8 The Dual Superconductor Picture of Confinement
363(10)
17.9 Center Vortices and Confinement
373(10)
18. PATH-INTEGRAL REPRESENTATION OF THE THERMODYNAMICAL PARTITION FUNCTION FOR SOME SOLVABLE BOSONIC AND FERMIONIC SYSTEMS 383(41)
18.1 Introduction
383(1)
18.2 Path-Integral Representation of the Partition Function in Quantum Mechanics
384(2)
18.3 Sum Rule for the Mean Energy
386(3)
18.4 Test of the Energy Sum Rule. The Harmonic Oscillator
389(5)
18.5 The Free Relativistic Boson Gas in the Path Integral Appoach
394(4)
18.6 The Photon Gas in the Path Integral Approach
398(3)
18.7 Functional Methods for Fermions. Basics
401(4)
18.8 Path Integral Representation of the Partition Function for a Fermionic System valid for Arbitrary Time-Step
405(5)
18.9 A Modified Fermion Action Leading to Fermion Doubling
410(3)
18.10 The Free Dirac Gas. Continuum Approach
413(4)
18.11 Dirac Gas of Wilson Fermions on the Lattice
417(7)
19. FINITE TEMPERATURE PERTURBATION THEORY OFF AND ON THE LATTICE 424(61)
19.1 Feynman Rules For Thermal Green Functions in the λφ4-Theory
424(9)
19.2 Generation of a Dynamical Mass at T not = to 0
433(1)
19.3 Perturbative Expansion of the Thermodynamical Potential
434(6)
19.4 Feynman Rules for QED and QCD at non-vanishing Temperature and Chemical Potential in the Continuum
440(5)
19.5 Temporal Structure of the Fermion Propagator at T not = to 0 and μ not = to 0 in the Continuum
445(3)
19.6 The Electric Screening Mass in Continuum QED in One-Loop Order
448(4)
19.7 The Electric Screening Mass in Continuum QCD in One-Loop Order
452(3)
19.8 Lattice Feynman Rules for QED and QCD at T not = to 0 and μ not = to 0
455(5)
19.9 Particle-Antiparticle Spectrum of the Fermion Propagator at T not = to 0. Naive vs. Wilson Fermions
460(4)
19.10 The Electric Screening Mass for Wilson Fermions in Lattice QED to One-Loop Order
464(8)
19.11 The Electric Screening Mass for Wilson Fermions in Lattice QCD to One-Loop Order
472(10)
19.12 The Infrared Problem
482(3)
20. NON-PERTURBATIVE QCD AT FINITE TEMPERATURE 485(57)
20.1 Thermodynamics on the Lattice
485(5)
20.2 The Wilson Line or Polyakov Loop
490(5)
20.3 Spontaneous Breakdown of the Center Symmetry and the Deconfinement Phase Transition
495(1)
20.4 How to Determine the Transition Temperature
496(2)
20.5 A Two-Dimensional Model. Test of Theoretical Concepts
498(14)
20.6 Monte Carlo Study of the Deconfinement Phase Transition in the Pure SU(3) Gauge Theory
512(8)
20.7 The Chiral Phase Transition
520(4)
20.8 Some Monte Carlo Results on the High Temperature Phase of QCD
524(8)
20.9 Some Possible Signatures for Plasma Formation
532(10)
Appendix A 542(10)
Appendix B 552(2)
Appendix C 554(3)
Appendix D 557(3)
Appendix E 560(2)
Appendix F 562(2)
Appendix G 564(7)
References 571(14)
Index 585

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