Quantum electrodynamics of charged boson fields with a spontaneously broken symmetry. [Lorentz gauge, photon ghost modes]

Journal Article · Thu Jul 15 00:00:00 EDT 1976 · Phys. Rev., D; (United States)

DOI:https://doi.org/10.1103/PhysRevD.14.479· OSTI ID:7341065

Haller, K; Sohn, R

We describe the canonical formulation of the theory of a charged scalar field with a spontaneously broken symmetry, interacting with the electromagnetic field. The formulation is carried out in the Lorentz gauge, and the effect of the spontaneous symmetry breaking on the subsidiary condition is studied. The spectrum of states includes four massive observable modes: two that are transversely polarized and stem from the elementary excitations of the electromagnetic field, and two that originate from the excitations of the charged scalar field. There are also two zero-norm photon ''ghost'' modes which carry neither probability amplitude nor energy, and which do not in any way affect the dynamical behavior of the observable particles. (AIP)

• Research Organization: Department of Physics, University of Connecticut, Storrs, Connecticut 06268
• OSTI ID: 7341065
• Journal Information: Phys. Rev., D; (United States), Vol. 14:2
• Country of Publication: United States
• Language: English

Related Subjects

72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS
BOSONS
QUANTUM ELECTRODYNAMICS
SCALAR FIELDS
SYMMETRY BREAKING
ELECTROMAGNETIC FIELDS
EXCITATION
LAGRANGIAN FUNCTION
LORENTZ INVARIANCE
ELECTRODYNAMICS
ENERGY-LEVEL TRANSITIONS
FIELD THEORIES
FUNCTIONS
INVARIANCE PRINCIPLES
QUANTUM FIELD THEORY
645400* - High Energy Physics- Field Theory