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quarks.jpg (21757 bytes)Quarks, Leptons, and Gauge Fields

Second edition

(World Scientific, Singapore, 1992) 348 pages

ISBN  981-02-0695-3   981-02-0660-7 (pbk)

To order online go to World Scientific, find book under Physics, High Energy Physics.

 

FROM THE PREFACE

According to the current view, the basic building blocks of matter are 
quarks and leptons, which interact with one another through the 
intermediaries of Yang Mills gauge fields (gravity being ignored in this 
context). This means that the forms of the interactions are completely 
determined by the algebraic structure of certain internal symmetry groups. 
Thus, the strong interactions are associated with the group SU(3), and is 
described by a gauge theory called quantum chromodynamics. The 
electro-weak interactions, as described by the now standard Weinberg-
Salam model, is associated with the group SU(2) x U(l).
This book is a concise introduction to the physical motivation behind 
these ideas, and precise mathematical formulation thereof. The goal of the 
book is to explain why and how the mathematical formalism helps us to 
understand the relevant observed phenomena. The audience for which this 
book is written are graduate students in physics who have some knowledge 
of the experimental parts of particle physics, and an acquaintance with 
quantum field theory, including Feynman graphs and the notion of 
renormalization.

CONTENTS

1 INTRODUCTION
	Particles and Interactions
	Gauge Theories of Interactions
	Notations and Conventions
2 QUARKS
	Internal Symmetries
	Representation of SU(3)
	The Quark Model
	Color	
	Electromagnetic and Weak Probes
	Charm
3 MAXWELL FIELD: U(1) GAUGE THEORY
	Global and Local Gauge Invariance
	Spontaneous Breaking of Global Gauge Invariance: Goldstone Mode
	Spontaneous Breaking of Local Gauge Invariance: Higgs Mode
	Classical Finite-Energy Solutions
	Magnetic Flux Quantization
	Soliton Solutions: Vortex Lines
4 YANG-MILLS FIELDS: NON-ABELIAN GAUGE THEORIES
	Introductory Note
	Lie Groups
	The Yang-Mills Constructions
	Properties of Yang-Mills Fields
	Canonical Formalism
	Spontaneous Symmetry Breaking
5 TOPOLOGICAL SOLITONS
	Solitons
	The Instanton
	The Monopole
6 WEINBERG-SALAM MODEL	
	The Matter Fields
	The Gauge Fields	
	The General Theory
7 METHOD OF PATH INTEGRALS
	Non-Relativistic Quantum Mechanics
	Quantum Field Theory
	External Sources
	Euclidean 4-Space
	Calculation of Path Integrals
	The Feynman Propagator
	Feynman Graphs
	Boson Loops and Fermion Loops
	Fermion Fields
8 QUANTIZATION OF GAUGE FIELDS
	Canonical Quantization	
	Path Integral Method in Hamiltonian Form
	Feynman Path Integral: Fadeev-Popov Method
	Free Maxwell Field
	Pure Yang-Mills Fields
	The Theta-World and the Instanton
	Gribov Ambiguity
	Projection Operator for Gauss' Law
9 RENORMALIZATION
	Charge Renormalization
	Perturbative Renormalization in Quantum Electrodynamics
	The Renormalization Group	
	Scalar Fields
	Renormalizability
	Phi4 theory
	Triviality" and the Landau ghost
	The Physics of Renormalization
	Renormalization of QED
10 METHOD OF EFFECTIVE POTENTIAL
	Spontaneous Symmetry Breaking
	The Effective Action
	The Effective Potential
	The Loop Expansion
	One-Loop Effective Potential
	Renormalization
	Dimensional Transmutation
	A Non-Relativistic Example
	Application to Weinberg-Salam Model
11 THE AXIAL ANOMALY
	Origin of the Axial Anomaly
	The Triangle Graph
	Anomalous Divergence of the Chiral Current
	Physical Explanation of the Axial Anomaly
	cancellation of Anomalies
	't Hooft's Principle
12 QUANTUM CHROMODYNAMICS	
	General Properties
	The Color Gyromagnetic Ratio
	Asymptotic Freedom
	The Pion as Goldstone Boson
	The U(1) Puzzle
	Theta Worlds in QCD
13 LATTICE GAUGE THEORY
	Wilson's Lattice Action
	Transfer Matrix
	Lattice Hamiltonian
	Lattice Fermions
	Wilson Loop and Confinement
	Continuum Limit
	Monte Carlo Methods
14 QUARK CONFINEMENT
	Wilson Criterion and Electric Confinement
	String Model of Hadrons
	Superconductivity: Magnetic Confinement
	Electric and Magnetic Order Parameters
	Scenario for Quark Confinement
	Symmetry and Confinement

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