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By definition, gauge theories - among the cornerstones of fundamental theoretical physics - involve more degrees of freedom than required by the underlying physics. The unphysical degrees of freedom must be shown not to yield unwarranted effects at every step in the formalism where explicit Lorentz covariance is required.
The present work presents, in a rigorous way, a consistent formulation for the handling of noncovariant gauges in the quantization and renormalization of gauge theories. Though the path integral method is very convenient for the proof of unitarity and renormalizability of gauge theories, the canonical formalism is eventually necessary to to expose the issues in a self-consistent way.
These notes are written as an introduction to postgraduate students, lecturers and researchers in the field and assume prior knowledge of quantum field theory.
Industry Reviews
From the reviews:
"This book develops a consistent formulation for the handling of noncovariant gauges in the quantization process. ... provide the setting of the noncovariant gauge theories on the same levels of consistency as the covariant ones, by means of the canonical formalism. ... the author has also included a detailed and complete description of the quantization theory of constrained systems. ... All in all, this comprehensive ... monograph represents a gratifying addition for graduate students and researchers from high energy physics, gauge theories and related areas." (Vladimir Balan, Zentralblatt MATH, Vol. 1159, 2009)
"In this book the quantization of abelian and non-abelian gauge theories in non-covariant gauges in the canonical formalism is treated in detail. ... great value to anyone involved with the quantization of gauge theories, or even with gauge-fixed gauge theories in general, and provides essential knowledge. ... the book can also be highly recommended to advanced students for an extra insight into the complexities of gauge theories. ... this book is a definite must-read." (Axel Maas, Mathematical Reviews, Issue 2010 a)| Canonical Quantization for Constrained Systems | p. 1 |
| Canonical Quantization of Mechanical Unconstrained Systems | p. 1 |
| Lagrangian Formalism | p. 1 |
| Hamiltonian | p. 1 |
| Poisson Brackets | p. 2 |
| Quantization | p. 2 |
| Field Theory | p. 3 |
| Lagrangian and Lagrangian Density | p. 3 |
| Hamiltonian | p. 3 |
| Poisson Brackets | p. 4 |
| Quantization | p. 4 |
| The Free Scalar Field | p. 5 |
| Solution of the Klein-Gordon Equation | p. 5 |
| The Electromagnetic Field | p. 6 |
| Primary and Secondary Constraints | p. 8 |
| Primary Constraints | p. 8 |
| Secondary Constraints | p. 8 |
| First and Second Class Constraints | p. 9 |
| Quantization in the Presence of Second-Class Constraints | p. 10 |
| Quantization in Presence of First-Class Constraints | p. 11 |
| BRST Quantization | p. 13 |
| Summary | p. 14 |
| Back to the Free Massless Vector Field | p. 14 |
| Lagrangian and Constraints | p. 14 |
| Gauge Fixing | p. 16 |
| Covariant Gauge for the Free Massless Vector Field | p. 16 |
| Commutation Relations for Any Time | p. 18 |
| Creation and Annihilation Operators | p. 21 |
| The Gupta-Bleuler Formalism | p. 22 |
| References | p. 23 |
| Quantization of the Free Electromagnetic Field in General Class III Linear Gauges | p. 25 |
| Introduction | p. 25 |
| Lagrangian and Field Equations | p. 26 |
| The Lagrangian | p. 26 |
| Euler-Lagrange Equations | p. 26 |
| Derived Field Equations | p. 28 |
| Sketching the Solution of the Cauchy Problem | p. 28 |
| Particular Cases of Interest | p. 30 |
| Planar-Type Gauges | p. 31 |
| Constraint Analysis | p. 32 |
| Canonical Momenta and Primary Constraints | p. 32 |
| The Hamiltonian | p. 33 |
| Constraint Chains | p. 33 |
| Singular Frames | p. 33 |
| Commutation Relations for Any Time | p. 34 |
| Canonical Commutation Relations | p. 34 |
| Commutation Relations Involving the S Field | p. 34 |
| Commutation Relations Involving the S' Field | p. 36 |
| Commutation Relations Involving B = [partial differential] [middle dot] A | p. 38 |
| Commutation Relations Between A[subscript mu]'s | p. 42 |
| Summary of the Commutation Relations for Any Time | p. 44 |
| Creation and Annihilation Operators | p. 45 |
| Momentum Space Expansion of the Fields | p. 45 |
| Commutation Relations Between Creation and Annihilation Operators | p. 50 |
| Summary of the Algebra of Creation and Annihilation Operators | p. 55 |
| The Gupta-Bleuler Formalism | p. 55 |
| Covariance Problems | p. 56 |
| Translation Invariance | p. 56 |
| Lorentz Transformations | p. 58 |
| References | p. 60 |
| Quantization of the Free Electromagnetic Field in Class II Axial Gauges | p. 61 |
| Introduction | p. 61 |
| Lagrangian and Field Equations | p. 61 |
| The Lagrangian | p. 61 |
| Euler-Lagrange Equations | p. 62 |
| Derived Field Equations | p. 63 |
| Summary of the Field Equations | p. 63 |
| Constraint Analysis and Effective Hamiltonian | p. 63 |
| Solution of Field Equations | p. 65 |
| Solution of n [middle dot] [partial differential]S = 0 | p. 65 |
| Solution of (n [middle dot] [partial differential] + [kappa])S = 0 | p. 66 |
| Solution of n [middle dot] [partial differential]B = (n[superscript 2] - a)S | p. 67 |
| Elementary Solution of n [middle dot] [partial differential square]A = 0 | p. 67 |
| Solution of the Cauchy Problem for [square]A(x - z) = L[subscript x]D[subscript n](x - z) | p. 70 |
| Elementary Solution of (n [middle dot] [partial differential superscript 2 square]A = 0 | p. 70 |
| Commutation Relations | p. 71 |
| Equal Time Commutators | p. 71 |
| Commutation Relations Involving the S-Field | p. 72 |
| Commutation Relations Involving the S'-Field | p. 72 |
| Commutation Relations Involving [partial differential] [middle dot] A | p. 73 |
| Commutation Relations [A subscript mu](x), A[subscript v](z) | p. 74 |
| Association of a Feynman Propagator with the Operator n [middle dot] [partial differential] | p. 76 |
| Associating Creation and Annihilation Operators with Fields | p. 77 |
| The S-Field | p. 78 |
| Other Fields | p. 78 |
| Correct Momentum Space Expansion of the Fields | p. 80 |
| The S-Field | p. 80 |
| The B-Field | p. 80 |
| The S'-Field | p. 82 |
| The A[subscript mu]-Field | p. 83 |
| A Toy Model for the Unphysical S and B Fields | p. 84 |
| Conclusions | p. 85 |
| Interpolating Between Axial and Relativistic Gauges | p. 85 |
| Summary | p. 86 |
| References | p. 86 |
| Gauge Fields in Interaction | p. 87 |
| Introduction | p. 87 |
| General Formalism of Gauge Invariance | p. 88 |
| General Transformations | p. 88 |
| Infinitesimal Transformations | p. 89 |
| Remarks | p. 90 |
| Class III Gauges in Yang-Mills Theory | p. 91 |
| Building the Lagrangian | p. 91 |
| Field Equations | p. 94 |
| Canonical Momenta and Constraints | p. 94 |
| The Hamiltonian | p. 95 |
| The BRST Charge | p. 95 |
| Ghost Number | p. 97 |
| Global Internal Symmetry | p. 97 |
| Physical States | p. 98 |
| Problems of Covariance | p. 98 |
| References | p. 99 |
| Perturbation Theory: Renormalization and All That | p. 101 |
| Introduction | p. 101 |
| The S-Matrix | p. 101 |
| Definition and Properties | p. 101 |
| Perturbative Expansion | p. 103 |
| Expansion and Consequences of the Unitarity Condition | p. 103 |
| Consequences of the Causality Condition | p. 104 |
| The First Term T[subscript 1] | p. 106 |
| Nonunicity of the T[subscript n] | p. 108 |
| The Fixed Part of T[subscript n] | p. 108 |
| Wick's Theorem | p. 109 |
| Feynman Rules | p. 111 |
| Feynman Rules in Momentum Space | p. 113 |
| Divergences, Power Counting and Renormalizability | p. 118 |
| Example | p. 118 |
| Power Counting and Superficial Degree of Divergence | p. 118 |
| Renormalizability by Power Counting | p. 120 |
| Dimensional Regularization of Covariant Divergent Integrals | p. 120 |
| A General One-Loop Integral | p. 120 |
| Euclidean Space | p. 121 |
| Use of the Feynman Formula | p. 121 |
| Elimination of the Denominators | p. 122 |
| Complex Dimension | p. 122 |
| Tensor Integrals | p. 123 |
| Extension to General Covariant or Noncovariant Integrals in a Preferred Frame | p. 124 |
| The General One-Loop Integral | p. 124 |
| Euclidean Space | p. 125 |
| Elimination of the Denominators | p. 126 |
| Calculation of the Derivatives | p. 127 |
| Introduction of the Feynman Variables | p. 128 |
| Integration Over [lambda] | p. 129 |
| Regularization of Ultraviolet Divergences | p. 129 |
| Consequences of the Nonsingularity of the B[superscript -1] Matrix | p. 130 |
| Computation of the Ghost Loop With Two Legs | p. 131 |
| Renormalization and Counter-Terms | p. 132 |
| Various Renormalization Schemes | p. 133 |
| Multiplicative Renormalization | p. 134 |
| Summary | p. 135 |
| References | p. 136 |
| Slavnov-Taylor Identities for Yang-Mills Theory | p. 137 |
| Introduction | p. 137 |
| The Reduction Formula | p. 137 |
| One-Particle Irreducible Vertex Functions | p. 138 |
| Yang-Mills Theory in a General Class III Gauge | p. 139 |
| The Lagrangian and Superficially Divergent Processes | p. 139 |
| BRST Symmetry, Field Equations and Canonical Commutation Relations | p. 141 |
| Commuting Derivatives and Time-Ordered Products | p. 143 |
| The Ward-Takahashi-Slavnov-Taylor Identity for the Gluon Self-Energy | p. 143 |
| Covariant Gauges | p. 143 |
| General Gauges | p. 146 |
| Renormalization | p. 148 |
| Identity for the Three-Gluon Vertex Function | p. 149 |
| Derivation of the Identity | p. 150 |
| Renormalization | p. 150 |
| Ghost Propagator | p. 151 |
| Ghost-Ghost-Gluon Vertex | p. 153 |
| Identity in Coordinate Space | p. 153 |
| Momentum Space | p. 153 |
| Remark | p. 154 |
| Multiplicative Renormalization | p. 154 |
| Summary | p. 156 |
| References | p. 156 |
| Field Theory Without Infinities | p. 157 |
| Introduction | p. 157 |
| Iterative Construction of the S-Matrix Without Time-Ordering | p. 158 |
| Splitting of Causal Distributions into Advanced and Retarded Parts | p. 159 |
| Distribution and Fourier Transform | p. 159 |
| Order of Singularity of a Distribution | p. 160 |
| Splitting of Distribution with Negative Order of Singularity | p. 161 |
| Nonnegative Singularity Order | p. 162 |
| Application to Yang-Mills Theory | p. 164 |
| First Order | p. 164 |
| Example of a One-Loop Process: The Gluon Self-energy | p. 179 |
| Calculation of I[subscript 1]([xi];[kappa]) | p. 186 |
| Calculation of I[subscript 2](k;[kappa subscript 1], [kappa subscript 2]) | p. 187 |
| Calculation of the Tensor Distributions | p. 188 |
| The Final Result for the Gluon Self-energy | p. 190 |
| Summary | p. 190 |
| References | p. 191 |
| Gauges with a Singular C Matrix | p. 193 |
| Introduction | p. 193 |
| The Ghost Loop Contribution | p. 194 |
| The Leibbrandt Gauges | p. 194 |
| Interpolating Between Leibbrandt and Relativistic Gauges | p. 197 |
| Singularities Generated by the Lack of Power Counting in Ultra-Violet Divergent Perturbative Theory | p. 199 |
| The Loop Integration in a General Gauge | p. 200 |
| Restriction to Loops with Two External Particles | p. 201 |
| Further Restriction for m [greater than or equal right] 6 | p. 201 |
| Interpolating Between Leibbrandt and Relativistic Gauges | p. 205 |
| Cancellation of Divergences at [alpha] = 0 in the Self-Energy | p. 207 |
| References | p. 208 |
| Conclusion | p. 209 |
| Notations | p. 211 |
| A Useful Fourier Transform | p. 213 |
| Generalized Functions | p. 215 |
| Elementary Solutions of the Klein-Gordon Equation | p. 215 |
| The [Delta] Function | p. 215 |
| The [Delta superscript F] Function | p. 216 |
| The E Function | p. 216 |
| Definition | p. 216 |
| Derivation of the Elementary Solution | p. 216 |
| Zero-Time Properties | p. 217 |
| Integration Over k[subscript 0] | p. 218 |
| The Cauchy Problem Associated with [square superscript 2] | p. 218 |
| Generalized Functions Associated with the [square subscript C] Operator | p. 219 |
| Elementary Solution D[subscript C superscript (1)] | p. 220 |
| Positive Frequency Part | p. 221 |
| Negative Frequency Part | p. 222 |
| Elementary Solution with Causal Support | p. 222 |
| Generalization with a Mass Parameter | p. 223 |
| Analogous of the Feynman Propagator | p. 224 |
| Solution of the Cauchy Problem | p. 225 |
| Remarks | p. 226 |
| Generalized Functions Associated with [square subscript C superscript 2] | p. 226 |
| The Elementary Function with Causal Support | p. 226 |
| Zero Time Properties | p. 227 |
| Integration Over k[subscript 0] | p. 227 |
| The Cauchy Problem | p. 228 |
| Generalized Functions Associated with [square square subscript C] | p. 228 |
| Elementary Solution with Causal Support | p. 228 |
| Zero-Time Properties of F[subscript C] and its Time Derivatives | p. 230 |
| Preferred Frame | p. 231 |
| The Cauchy Problem | p. 231 |
| The G-Functions | p. 232 |
| Index | p. 235 |
| Table of Contents provided by Ingram. All Rights Reserved. |
ISBN: 9783540699200
ISBN-10: 3540699201
Series: Lecture Notes in Physics
Published: 6th October 2008
Format: Hardcover
Language: English
Number of Pages: 256
Audience: General Adult
Publisher: Springer Nature B.V.
Country of Publication: DE
Dimensions (cm): 23.5 x 15.88 x 1.91
Weight (kg): 0.5
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