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SMJ's analysis of Ising model correlation functions: Leo P. Kadanoff and Mahito Kohmoto, The James Franck Institute, The University of Chicago, Chicago, Illinois 60637


Publisher
Elsevier Science
Year
1980
Tongue
English
Weight
89 KB
Volume
126
Category
Article
ISSN
0003-4916

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โœฆ Synopsis


Starting from the tensor product of N irreducible positive energy representations of the Poincare group describing N free relativistic particles with arbitrary spins and positive masses, we construct an interacting positive energy representation by modifying the total 4-momentum operator. We first make a transformation to a Hilbert space on which the free total 4-momentum operator equals the product of a dimensionless center-of-mass 4-vector ((I k 1' -l)'/?, k) and a free "reduced Hamiltonian" H,", which is a positive operator acting only on internal variables, and then replace H," by an interacting reduced Hamiltonian H? = H," + V, where V commutes with the Lorentz group and is such that H, is a positive operator. The resulting product form is shown to imply that the wave operators intertwine the free and interacting representations so that the S-operator is Lorentz invariant. From a physical point of view the scheme is related to the framework first introduced by Bakamjian and Thomas, in which the Hamiltonian and boost generators are modified, but the above procedure makes a mathematically rigorous discussion much simpler. In the spin-0 case we introduce a natural generalization of the pair potentials of nonrelativistic N-particle Schrodinger theory to the present relativistic setting, study its scattering theory, and point out some problems that do not have analogs at the nonrelativistic level. In the spin-i case we propose, inspired by the Dirac equation, explicit reduced Hamiltonians to describe atomic energy levels and present arguments making it plausible that their eigenvalues are in closer agreement with the experimental data than their nonrelativistic counterparts. We also consider extensions to arbitrary spin and, in the spin-i case, coupling of a quantized radiation field. In view of eventual applications to "completely integrable" one-dimensional field theories the case of one space dimension is studied as well, both in quantum mechanics and in classical mechanics.

Setuiclussical Electrotl Models: Casimir SelflStress in Dielectric and Corrducting Balls.


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