An Introduction to Field Quantization |
Contents
NONRELATIVISTIC FIELDS | 11 |
RELATIVISTIC FREE FIELDS | 45 |
SOME ASPECTS OF LINEAR FIELD EQUATIONS | 78 |
Copyright | |
14 other sections not shown
Other editions - View all
Common terms and phrases
antiparticles arbitrary assume Aµ(x c-number calculation Chapter charge conjugation commutation relation condition consequence conserved d(ip d¹x dªx defined denote derivative Dirac field discussed do(x do₂(x dox(x eigenvalue eigenvector equation of motion expand expectation value field equation field operator field theory field with spin follows formula free fields Hence hermitian hermitian conjugate identity implies infinitesimal integrability interacting fields invariant ju(x jµ(x Klein-Gordon divisor Klein-Gordon equation Lorentz transformation matrix mobs momentum normal obeying obtain one-particle ỗµ P₁ Pa(x particle photon Phys Pin(x prove pseudoscalar quantity quantization quantized field quantum relativistic representation right-hand side S-matrix satisfies scalar space-like surface spinor substituting substitution law Takahashi theorem tion U+(o Umezawa unitary transformation vacuum expectation value vacuum subtraction vanishes vector wave functions yields αα αμ δσ(χ μμ μν