Abstract
We give a simple proof of Lorentz covariance for theP(φ)2 model without using the higher order estimates: For each Poincaré transformation {a, Λ} and each bounded regionB of Minkowski space there exists a unitary operatorU which correctly transforms the Heisenberg picture field operator:U φ(f)U*=φ(f (a,↔)),f ∈C ∞0 (B).
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Cannon, J., Jaffe, A.: Commun. math. Phys.17, 261–321 (1970)
Glimm, J., Jaffe, A.: Quantum field theory models. In: 1971 Les Houches Lectures, ed. R. Stora, C. De Witt. New York: Gordon and Breach 1972
Glimm, J., Jaffe, A.: Boson quantum field models (to appear). In: Mathematics of Contemporary Physics, ed. R. Streater. New York: Academic Press 1972
Haag, R., Kastler, D.: J. Math. Phys.5, 848–861 (1964)
Hoegh-Krohn, R., Simon, B.: J. Funct. Anal.9, No. 2, 127–180 (1972)
Kato, T.: Perturbation theory for linear operators. Berlin-Heidelberg-New York: Springer 1965
Klein, A.: Quadratic expressions in a free Boson field, preprint
Rosen, L.: Comm. Pure Appl. Math.24, 417–457 (1971)
Rosen, L.: J. Math. Anal. Applic.32, No. 2, 276–311 (1972)
Simon, B.: Math. Ann.201, 211–220 (1973)
Segal, I.: Annals of Math.92, 462–481 (1970)
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Park, Y.M. Lorentz covariance of theP(φ)2 quantum field theory without higher order estimates. Commun.Math. Phys. 34, 179–192 (1973). https://doi.org/10.1007/BF01645679
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DOI: https://doi.org/10.1007/BF01645679