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9. Interacting Relativistic Field Theories 9.1. Asymptotic States and the Scattering Operator 9.2. Reduction Formulae 9.3. Path Integrals 9.4. Perturbation Theory 9.5. Quantization of Gauge Fields 9.6. Renormalization 9.7. Quantum Electrodynamics
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9.1. Asymptotic States and the Scattering Operator Non-relativistic quantum mechanics: Problem of single particle in external potential is always solvable. System of N non-relativistic, non-interacting particles: Creation and annihilation operators for stable single particle eigenstates. System of relativistic non-interacting particles: Number of particles not fixed even in closed, isolated systems. System of interacting particles: Ground state = vacuum state; other eigenstates: usually not known. States/particles created by field operators usually not eigenstates/stable. Exceptions: interaction removable by canonical transformation, e.g., elementary excitations such as phonons, magnon, excitons, polarons, Cooper pairs, etc. Description of free particles : Plane wave ~ wave packet. Interacting particles: Plane waves still useful unless bound states are formed.
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Scattering Problem Short-ranged interaction → free particles outside interaction region. Tricks justifying the use of plane waves instead of wave packet : 1. Replace incoming particle with a steady stream of particles. 2. Adiabatic switching: replace H = H 0 + H int with → Field operators for asymptotic states: Z = wavefunction renormalization constant ~ phase shift due to scattering.
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Incoming asymptotic state of N particles: ‘Out’ state of scattered particles: Probability amplitude = See appendix D for calculating other physical quantities of interest. If ‘in’ and ‘out’ states belong to the same multi-particle (Fock) space, S = scattering operator Conservation of probability → Normalization of asymptotic states preserved. → S is unitary. →
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9.2. Reduction Formulae
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9.3. Path Integrals
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9.4. Perturbation Theory
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9.5. Quantization of Gauge Fields
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9.6. Renormalization
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9.7. Quantum Electrodynamics
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