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Relativistic Wave Equation for Spin-0 Particles: The Klein--Gordon Equation and Its Applications |
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1 | (98) |
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2 | (2) |
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The Klein--Gordon Equation |
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4 | (3) |
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The Nonrelativistic Limit |
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7 | (1) |
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8 | (4) |
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Energy-Momentum Tensor of the Klein--Gordon Field |
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12 | (9) |
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The Klein--Gordon Equation in Schrodinger Form |
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21 | (5) |
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26 | (5) |
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Free Spin-0 Particles in the Feshbach--Villars Representation |
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31 | (10) |
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The Interaction of a Spin-0 Particle with an electromagnetic Field |
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41 | (8) |
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Gauge Invariance of the Coupling |
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49 | (1) |
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The Nonrelativistic Limit with Fields |
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50 | (18) |
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Interpretation of One-Particle Operators in Relativistic Quantum Mechanics |
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68 | (29) |
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97 | (2) |
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A Wave Equation for Spin-1/2 Particles: The Dirac Equation |
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99 | (28) |
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Free Motion of a Dirac Particle |
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107 | (4) |
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Single-Particle Interpretation of the Plane (Free) Dirac Waves |
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111 | (9) |
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Nonrelativistic Limit of the Dirac Equation |
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120 | (6) |
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126 | (1) |
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Lorentz Covariance of the Dirac Equation |
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127 | (22) |
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Formulation of Covariance (Form Invariance) |
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130 | (10) |
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Construction of the S Operator for Infinitesimal Lorentz Transformations |
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140 | (3) |
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Finite Proper Lorentz Transformations |
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143 | (1) |
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The S Operator for Proper Lorentz Transformations |
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144 | (3) |
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147 | (1) |
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148 | (1) |
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Spinors Under Spatial Reflection |
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149 | (2) |
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Bilinear Covariants of the Dirac Spinors |
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151 | (6) |
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156 | (1) |
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Another Way of Constructing Solutions of the Free Dirac Equation: Construction by Lorentz Transformations |
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157 | (20) |
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Plane Waves in Arbitrary Directions |
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161 | (4) |
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The General Form of the Free Solutions and Their Properties |
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165 | (9) |
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Polarized Electrons in Relativistic Theory |
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174 | (3) |
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Projection Operators for Energy and Spin |
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177 | (6) |
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Simultaneous Projections of Energy and Spin |
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181 | (2) |
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Wave Packets of Plane Dirac Waves |
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183 | (14) |
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Dirac Particles in External Fields: Examples and Problems |
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197 | (64) |
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The Two-Centre Dirac Equation |
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261 | (16) |
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The Foldy--Wouthuysen Representation for Free Particles |
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277 | (14) |
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The Foldy--Wouthuysen Representation in the Presence of External Fields |
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285 | (6) |
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291 | (34) |
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299 | (10) |
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Charge Conjugation of Eigenstates with Arbitrary Spin and Momentum |
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309 | (1) |
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Charge Conjugation of Bound States |
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310 | (2) |
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Time Reversal and PCT Symmetry |
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312 | (11) |
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323 | (2) |
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325 | (8) |
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The Weyl Equation -- The Neutrino |
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333 | (14) |
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Wave Equations for Particles with Arbitrary Spins |
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347 | (42) |
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Particles with Finite Mass |
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347 | (8) |
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355 | (4) |
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Spin-1 Fields for Particles with Finite Mass: Proca Equations |
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359 | (2) |
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361 | (3) |
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364 | (19) |
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383 | (5) |
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388 | (1) |
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Lorentz Invariance and Relativistic Symmetry Principles |
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389 | (28) |
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Orthogonal Transformations in Four Dimensions |
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389 | (1) |
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Infinitesimal Transformations and the Proper Subgroup of O(4) |
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390 | (6) |
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Classification of the Subgroups of O(4) |
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396 | (2) |
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The Inhomogeneous Lorentz Group |
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398 | (2) |
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400 | (2) |
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Representations of the Four-Dimensional Orthogonal Group and its Subgroups |
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402 | (4) |
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Tensor Representation of the Proper Groups |
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402 | (1) |
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403 | (3) |
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Representation of SL(2,C) |
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406 | (1) |
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Representations of SO(3,R) |
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407 | (1) |
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Representations of the Lorentz Group Lp |
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408 | (2) |
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Spin and the Rotation Group |
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410 | (5) |
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415 | (2) |
| Subject Index |
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417 | |
