1997
DOI: 10.1142/s0217732397000480
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UV-Regularization of Field Discontinuities

Abstract: A nonperturbative regularization of UV-divergencies, caused by finite discontinuities in the field configuration, is discussed in the context of 1+1-dimensional kink models. The relationship between this procedure and the appearance of "quantum copies" of classical kink solutions is studied in detail and confirmed by conventional methods of soliton quantization.

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Cited by 4 publications
(3 citation statements)
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“…First, let us note, that the initial formulation of the model is a local field theory, and in spite of the variety of classical solutions one needs to deal with, the covariance is broken only spontaneously, and so can be restored by means of the methods of refs. [23] using the covariant group center-of-mass variables for a localized quantum-field system. Besides this, the positive points of this approach are: the more correct derivation of chiral boundary conditions, by which any term in the initial Lagrangian has exact physical meaning; the presence of an intermediate phase describing quasifree massive "constituent" quarks; physically acceptable behavior of the total energy of the bag as a function of it's geometry.…”
Section: Resultsmentioning
confidence: 99%
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“…First, let us note, that the initial formulation of the model is a local field theory, and in spite of the variety of classical solutions one needs to deal with, the covariance is broken only spontaneously, and so can be restored by means of the methods of refs. [23] using the covariant group center-of-mass variables for a localized quantum-field system. Besides this, the positive points of this approach are: the more correct derivation of chiral boundary conditions, by which any term in the initial Lagrangian has exact physical meaning; the presence of an intermediate phase describing quasifree massive "constituent" quarks; physically acceptable behavior of the total energy of the bag as a function of it's geometry.…”
Section: Resultsmentioning
confidence: 99%
“…One can obviously construct the Lagrangian containing as many fields θ(x) as needed with appropriate self-interaction, which will determine (almost) rectangular division of space into regions corresponding to different phases, while the Lorentz-covariance will be broken only spontaneously, namely on the level of solutions of equations of motion. The latter circumstance allows one to use the framework of covariant group variables [23] in order to restore the covariance. Assuming further that subsidiary fields θ(x) have already formed the required bag configuration, let us start with the following Lagrangian:…”
Section: Lagrangian and Equations Of Motionmentioning
confidence: 99%
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