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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 1971 (Paperback, Softcover reprint of the original 1st ed. 1971)
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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 1971 (Paperback, Softcover reprint of the original 1st ed. 1971)
Series: Few-Body Systems, 8/1971
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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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