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Concepts in Hadron Physics : Proceedings of the X. Internationale Universitatswochen fur Kernphysik 1971 der Karl-Franzens-Universitat Graz, at Schladming (Steiermark, Austria), 1st March - 13th March, PDF eBook

Concepts in Hadron Physics : Proceedings of the X. Internationale Universitatswochen fur Kernphysik 1971 der Karl-Franzens-Universitat Graz, at Schladming (Steiermark, Austria), 1st March - 13th March PDF

Edited by Paul Urban

Part of the Few-Body Systems series

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Description

Soluble quantum field theory models are a rare commodity.

An infinite number of degrees of freedom and noncompact invariance groups have a nasty habit of ex- ploding in the model-makers' face.

Nevertheless, impor- tant progress has recently been made in the class of superrenormalizable relativistic theories, such as a self-interacting boson in a two-dimensional space time [ 1].

These results have been obtained starting with the free field and adding the interaction in a carefully controlled way.

Yet, the models successfully studied in this way do DQ~ have an infinite field strength renormalization, which, at least according to perturbation theory, should appear for realistic relativistic models in four-dimensional space time. ~2~!Y~~!9n_~g_~h~_~gg~1 The ultralocal scalar field theories discussed in these lecture notes are likewise motivated by relativistic theories but are based on a different approximatiGn.

This approximation formally amounts to dropping the spatial gradient term from the Hamiltonian rather than the non- linear interaction.

For a self-interacting boson field in a space-time of (s+l) dimensions (s~l), the classical ultralocal model Hamiltonian reads (1-1) The quantum theory of this model is the subject of the present paper.

This model differs formally from a rela- tivistic theory by the term f![Z~Cl(~)]2 d~ which, it is hoped, can, in one or another way, be added as a pertur- 229 bation in the quantum theory.

However, that still remains a problem for the future, and we confine our remarks to . . a careful study of the "unperturbed" model (1-1).

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