夸克、轻子和规范场(第2版)(QUARKS,LEPTONS＆GAUGE FIELDS)
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品牌: 黄克逊
基本信息·出版社：世界图书出版公司
·页码：333 页
·出版日期：2009年
·ISBN：7506291754
·条形码：9787506291750
·包装版本：第2版
·装帧：平装
·开本：24
·正文语种：英语
·丛书名：QUARKS,LEPTONS＆GAUGE FIELDS
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内容简介《夸克、轻子和规范场(第2版)》简明地介绍了在这些思想背后的动力，以及由此而来的严谨的数学系统表述。依据通行的观点，物质的基本彻块是夸克与轻子，它们通过杨-米尔斯规范场的媒介相互作用(在这种场合下引力被忽略了)。这就意味着相互作用的形式是完全由某些内部对称群的代数结构所决定的。于是强相互作用是与SU(3)群相关联的，它是由叫做量子色动力学的规范场理论所描述的。而电一弱相互作用则是与SU(2)XU(1)群相关联的，现在它是由标准的温伯格-萨拉姆模型来描述的。
编辑推荐《夸克、轻子和规范场(第2版)》是由世界图书出版公司出版的。
目录
PREFACE
Ⅰ.INTRODUCTION
1.1 Particles and Interactions
1.2 Gauge Theories of Interactions
1.3 Notations and Conventions
Ⅱ.QUARKS
2.1 Internal Symmetries
1 Isospin
2 The gauge groups
3 More general internal symmetries: SU(n)
4 Unitary symmetry
2.2 Representation of SU(3)
1 The basic representation
2 Young's tableaux
3 Irreducible representations
2.3 The Quark Model
1 Quarks as basic triplets
2 Quarks as building blocks
3 Weight diagrams
4 The composition of hadrons
2.4 Color
1 Independent quark model
2 Color SU(3) group
2.5 Electromagnetic and Weak Probes
1 Electromagnetic interactions
2 Parton model
3 Evidence for color
4 Weak interactions
2.6 Charm
1 The charmed quark
2 The J/φ and its family
3 Correspondence between quarks and leptons
Ⅲ.MAXWELL FIELD: U(I) GAUGE THEORY
3.1 Global and Local Gauge Invariance
3.2 Spontaneous Breaking of Global Gauge Invariance: Goldstone Mode
3.3 Spontaneous Breaking of Local Gauge Invariance: Higgs Mode
3.4 Classical Finite-Energy Solutions
3.5 Magnetic Flux Quantization
3.6 Soliton Solutions: Vortex Lines
Ⅳ. YANG-MILLS FIELDS: NON-ABELIAN GAUGE THEORIES
4.1 Introductory Note
4.2 Lie Groups
1 Structure constants
2 Matrix representations
3 Topological properties
4 General remarks
4.3 The Yang-Mills Constructions
1 Global gauge invariance
2 Local gauge invariance
4.4 Properties of Yang-Milis Fields
1 Electric and magnetic fields
2 Dual tensor
3 Path representation of the gauge group
4.5 Canonical Formalism
1 Equations of motion
2 Hamiltonian
4.6 Spontaneous Symmetry Breaking
1 The little group
2 Higgs mechanism
Ⅴ.TOPOLOGICAL SOLITONS
5.1 Solitons
5.2 The Instanton
1 Topological charge
2 Explicit solution
5.3 The Monopole
1 Topological stability
2 Flux quantization
3 Boundary conditions
4 Explicit solution
5 Physical fields
6 Spin from isospin
Ⅵ.WEINBERG-SALAM MODEL
6.1 The Matter Fields
6.2 The Gauge Fields
1 Gauging SU(2)×U(1)
2 Determination of constants
3 Interactions
6.3 The General Theory
1 Mass terms
2 Cabibbo angle
3 Kobayashi-Maskawa matrix
4 Solitons
Ⅶ.METHOD OF PATH INTEGRALS
7.1 Non-Relativistic Quantum Mechanics
7.2 Quantum Field Theory
7.3 External Sources
7.4 Euclidean 4-Space
7.5 Calculation of Path Integrals
7.6 The Feynman .Propagator
7.7 Feynman Graphs
7.8 Boson Loops and Fermion Loops
7.9 Fermion Fields
Ⅷ.QUANTIZATION OF GAUGE FIELDS
8.1 Canonical Quantization
1 Free Maxwell field
2 Pure Yang-Mills fields
8.2 Path Integral Method in Hamiltonian Form
8.3 Feynman Path Integral: Fadeev-Popov Method
8.4 Free Maxwell Field
1 Lorentz gauge
2 Coulomb gauge
3 Temporal and axial gauges
8.5 Pure Yang-Mills Fields
I Axial gauge
2 Lorentz gauge: Fadeev-Popov ghosts
8.6 The 0-World and the Instanton
1 Discovering the 0-world
2 lnstanton as tunneling solution
3 The 0-action
8.7 Gribov Ambiguity
8.8 Projection Operator for Gauss' Law
Ⅸ.RENORMALIZATION
9.1 Charge Renormalization
9.2 Perturbative Renormalization in Quantum Electredynamics
9.3 The Renormalization Group
1 Scale transformations
2 Scaling form
3 Fixed points
4 Callan-Symanzik equation
9.4 Scalar Fields
1 Renormalizability
2 Φ4 theory
3 "Triviality" and the Landau ghost
9.5 The Physics of Renormalization
1 Renormalization-group transformation
2 Real-space renormalization
3 Fixed points and relevancy
4 Renormalization and universality
Appendix to Chapter 9. Renormalization of QED
1 Vertex
2 Electron Propagator
3 Photon Propagator
4 Scaling Properties
5 Renormalization
6 Gauge Invariance and the Photon Mass
Ⅹ.METHOD OF EFFECTIVE POTENTIAL
10.1 Spontaneous Symmetry Breaking
10.2 The Effective Action
10.3 The Effective Potential
10.4 The Loop Expansion
10.5 One-Loop Effective Potential
10.6 Renormalization
1 General scheme
2 Massive case
3 Massless case
10.7 Dimensional Transmutation
10.8 A Non-Relativistic Example
10.9 Application to Weinberg-Salam Model
Ⅺ. THE AXIAL ANOMALY
11.1 Origin of the Axial Anomaly
11.2 The Triangle Graph
11.3 Anomalous Divergence of the Chiral Current
11.4 Physical Explanation of the Axial Anomaly
11.5 Cancellation of Anomalies
11.6 't Hooft's Principle
Ⅻ. QUANTUM CHROMODYNAMICS
12.1 General Properties
1 Lagrangian density
2 Feynman rules
3 Quark-gluon interactions
4 Gluon self-interactions
12.2 The Color Gyromagnetic Ratio
12.3 Asymptotic Freedom
1 The running coupling constant
2 The vacuum as magnetic medium
3 The Nielsen-Hughes formula
12.4 The Pion as Goldstone Boson
1 The low-energy domain
2 Chiral symmetry: an idealized limit
3 PCAC
4 The decay π0→2y
5 Extension to pion octet
12.5 The U(1) Puzzle
12.6 θ-Worlds in QCD
1 Euclidean action
2 The axial anomaly and the index theorem
3 Chiral limit: Collapse of the 0-worlds
4 Quark mass matrix
5 Strong CP violation
ⅩⅢ. LATTICE GAUGE THEORY
13.1 Wilson's Lattice Action
13.2 Transfer Matrix
13.3 Lattice Hamiltonian
13.4 Lattice Fermions
13.5 Wilson Loop and Confinement
13.6 Continuum Limit
13.7 Monte Carlo Methods
ⅩⅣ. QUARK CONFINEMENT
14.1 Wilson Criterion and Electric Confmement
14.2 String Model of Hadrons
14.3 Superconductivity: Magnetic Confinement
1 Experimental manifestation
2 Theory
3 Mechanism for monopole confinement
14.4 Electric and Magnetic Order Parameters
14.5 Scenario for Quark Confinement
Appendix to Chapter 14.Symmetry and Confinement
1 Quark Propagator
2 Center Symmetry
3 Confinement as Symmetry
INDEX
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序言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 start. dard Weinberg-Salam model，iS associated with the group su（2）×U（1）.
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 ale 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.This book might serve as a text for a one-semester course beyond quantum field theory.The first edition 0f mis book，which came out in 1982，was based on a course I gave at M.I.T.，and on lectures I gave in Santiago，Chile，in 1977，and in Beiiing，China.in 1979.I am indebted to I.Saavedra for the opportunity to lecture in Chile.to Chang Wen-yu and S.C.C.Ting for the inducement to give the Beijing lecture。and to M.Jacob and K.K.Phua for the encouragement to bring out the first edition. The main addition to the second edition are Wilson’S approach t0 renormaliza. tion，Iattice gauge theory，and quark confinement.I am grateful to the many readers who have pointed out ell-ors in the first edition.which I hope have been corrected in this edition.
I owe special thanks to my colleagues at M.I.T.，especially A.Guth.R. Jackiw，K.Johnson，and J.Polonyi，from whom I have Iearned much that iS being passed along in this book.
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