Section 3 describes the Wightman theory of fields, with the main results and recent generalizations. Section 4 describes the C*-algebra approach of Haag, which follows the same physical ideas but has become an independent theory capable of explaining superselection rules.
Section 5 describes dispersion relations and the analytic properties in momentum space, with brief reference to the Froissart bound and other consequances of positivity. Finally, Section 6 describes the Euclidean approach leading to a history integral formulation.
The review as a whole is a survey of the work over the period 1954-1974. It is confined to relativistic theories, omitting applications to many-body theory and avoiding the actual solution of the field equations. That nonlinear field equations, at least in two- and three-dimensional space-time, have solutions has recently been proved by Glimm and Jaffe. This suggests that field theory will be solved and used to describe elementary particles within the next few years.
Sept. 1974.
The optimistic last sentence of the abstract has not turned out to be the case. Some people think that no scalar field theory with nontrivial S-matrix exists. The experimental difficulty in finding the Higgs particle might be said to support this. Quantum fields are still thought to describe elementary particles, but they must be gauge fields (which do not allow an easy axiomatic formulation).
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© by Ray Streater 13/10/00.