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The Conceptual Framework of Quantum Field Theory$
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Anthony Duncan

Print publication date: 2012

Print ISBN-13: 9780199573264

Published to Oxford Scholarship Online: January 2013

DOI: 10.1093/acprof:oso/9780199573264.001.0001

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Dynamics V: Construction of local covariant ffields

Dynamics V: Construction of local covariant ffields

Chapter:
(p.171) 7 Dynamics V: Construction of local covariant ffields
Source:
The Conceptual Framework of Quantum Field Theory
Author(s):

Anthony Duncan

Publisher:
Oxford University Press
DOI:10.1093/acprof:oso/9780199573264.003.0007

In many of the standard texts on quantum field theory, the introduction of fields representing particles of low spin (zero, ½, or one — there is no direct phenomenological evidence for elementary particles of any higher spin) is a fairly ad hoc matter. Relativistic wave equations are introduced here and shown to have ‘nice’ covariance properties. A Lagrangian formalism is then constructed for which these equations are just the Euler–Lagrange equations of the theory, corresponding to the extremal condition on the classical action. Finally, a canonical quantization procedure is carried out: conjugate momentum fields are introduced, and the resultant Hamiltonian is shown to be the appropriate energy operator for particles of the desired mass and spin. This chapter eschews this ad hoc methodology in favour of a more direct, constructive approach. The relativistic wave equations satisfied by the covariant fields representing particles of low spin are shown to be automatic consequences of the representation theory of the Poincaré group, which can be used to write a completely general expression for the fields transforming according to an arbitrary finite-dimensional representation of the Lorentz group and representing particles of arbitrary mass and spin.

Keywords:   quantum field theory, low spin particles, Hamiltoninans, relativistic wave equations, covariatnt fields, Poincaré group, Lorentz group

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