Abstract
An exact formulation of LSZ field theory is given. It is based on the Wightman axioms, asymptotic completeness, and a technical assumption stating the existence of retarded products of field operators. Reduction formulae are derived directly from the strong asymptotic condition. The GLZ-theorem, which states the conditions under which a given set of retarded functions defines a field theory, is formulated and proved in a rigorous way.
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References
Lehmann, H., K. Symanzik, andW. Zimmermann: Nuovo Cimento1, 205 (1955).
—— —— ——: Nuovo Cimento6, 319 (1957).
Glaser, V., H. Lehmann, andW. Zimmermann: Nuovo Cimento6 1122 (1957).
Streater, R. F., andA. S. Wightman: PCT, spin and statistics, and all that. New York: W. A. Benjamin Inc. 1964.
Jost, R.: The general theory of quantized fields. Providence: Am. Math. Soc. 1965.
Haag, R.: Phys. Rev.112, 669 (1958).
Ruelle, D.: Helv. Phys. Acta35, 147 (1962).
Hepp, K.: Commun. Math. Phys.1, 95 (1965).
Schneider, W.: Helv. Phys. Acta39, 81 (1966).
Nishijima, K.: Phys. Rev.111, 995 (1958).
Epstein, H.: Axiomatic field theory, ed.M. Chretien andS. Deser. New York: Gordon & Breach 1966.
Jost, R.: Helv. Phys. Acta39, 21 (1966).
Schwartz, L.: Théorie des distributions, p. 239. Paris: Hermann 1966.
Pohlmeyer, K.: Technical report DESY 66/36 (unpublished). Hamburg 1966.
Haag, R.: Dan. Mat. Fys. Medd. 29, no. 12 (1955).
Bros, J., H. Epstein, andV. Glaser: Commun. Math. Phys.6, 77 (1967).
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Steinmann, O. A rigorous formulation of LSZ field theory. Commun.Math. Phys. 10, 245–268 (1968). https://doi.org/10.1007/BF01654234
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DOI: https://doi.org/10.1007/BF01654234