The Self-energy of a Dirac Particle, and its Relativistic Covariance.
スポンサーリンク
概要
著者
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Umezawa Hiroomi
Institute Of Theoretical Physics Nagoya University
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Kawabe Rokuo
Institute For Theoretical Physics Nagoya University:(present Address)physics Department Kyushu Unive
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Umezawa Hiroomi
Institute Of Theoretial Physics Nagoya University
関連論文
- On the Transition Matrix and the Green Function in the Quantum Field Theory
- On the Problem of Gauge-Invariancy and Divergence in the Theory of Elementary Particles, I
- On the Applicability of the Method of the Mixed Fields in the Theory of the Elementary Particles
- On the Structure of the Interaction of the Elementary Particles, I : The Renormalizability of the Interactions
- The Vaccum in Quantum Electrodynamics
- On the Structure of the Interaction of the Elementary Pasticles, IV : On the Interaction of the Second Kind
- On the Renormalization in Quantum Electrodynamics
- The Self-energy of a Dirac Particle, and its Relativistic Covariance.
- On the Reaction of the Mesonic Proper Field
- Vacuum Polarization due to Various Charged Particles.
- Theory of the Interaction of Elementary Particles. V. : The Problem of Vacuum Polarization(3)
- Theory of the Interaction of Elementary Particles, IV_2. : The Problem of Vacuum Polarisation. (2)
- Theory of the Interaction of Elementary Particles. IV_1. : The Problem of Vacuum Polarization(1)
- Some General Formulae relating to Vacuum Polarization
- On the Self-stress
- The General Theory of the Interaction Representation, II : General Fields and Interactions
- On the Problem of Covariance in Quantum Electrodynamics, I
- On the Structure of the Interactions of the Elementary Particles, III : On the Renormalizable Field Theory
- Some Remarks on the Goldhaber Model for Strange Particles
- On the Problem of Covariance in Quantum Electrodynamics, II
- The General Theory of the Interaction Representation, I : The Local Field
- On the Families of Spinor Fields
- On the Relativistically Improved Integration in Perturbation Theory. : Its Meaning in Feynman Theory
- An Improvement on the Integrations appearing in Perturbation Theory.