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