Standard

On the correspondence between a light-front Hamiltonian approach and a Lorentz-covariant formulation for quantum gauge theories. / Paston, S. A.; Prokhvatilov, E. V.; Franke, V. A.

в: Nuclear Physics B - Proceedings Supplements, Том 108, 01.04.2002, стр. 189-193.

Результаты исследований: Научные публикации в периодических изданиях › статья › Рецензирование

Harvard

Paston, SA, Prokhvatilov, EV & Franke, VA 2002, 'On the correspondence between a light-front Hamiltonian approach and a Lorentz-covariant formulation for quantum gauge theories', Nuclear Physics B - Proceedings Supplements, Том. 108, стр. 189-193. https://doi.org/10.1016/S0920-5632(02)01327-0

APA

Paston, S. A., Prokhvatilov, E. V., & Franke, V. A. (2002). On the correspondence between a light-front Hamiltonian approach and a Lorentz-covariant formulation for quantum gauge theories. Nuclear Physics B - Proceedings Supplements, 108, 189-193. https://doi.org/10.1016/S0920-5632(02)01327-0

Vancouver

Paston SA, Prokhvatilov EV, Franke VA. On the correspondence between a light-front Hamiltonian approach and a Lorentz-covariant formulation for quantum gauge theories. Nuclear Physics B - Proceedings Supplements. 2002 Апр. 1;108:189-193. https://doi.org/10.1016/S0920-5632(02)01327-0

Author

Paston, S. A. ; Prokhvatilov, E. V. ; Franke, V. A. / On the correspondence between a light-front Hamiltonian approach and a Lorentz-covariant formulation for quantum gauge theories. в: Nuclear Physics B - Proceedings Supplements. 2002 ; Том 108. стр. 189-193.

BibTeX

@article{8e2a1e6600974097851c66fb1832c8f3,
title = "On the correspondence between a light-front Hamiltonian approach and a Lorentz-covariant formulation for quantum gauge theories",
abstract = "The problem of restoring the equivalence between Light-Front (LF) Hamiltonian and conventional Lorentz-covariant formulations of gauge theories is solved for QED(1+1) and (perturbatively to all orders) for QCD(3+1). For QED(1+1) a LF Hamiltonian is constructed which reproduces the results of a Lorentz-covariant theory. This is achieved through bosonization of the model and by analyzing the resulting bosonic theory to all orders in the fermion mass. For QCD(3+1) we describe nonstandard regularization that allows to restore the mentioned equivalence with a finite number of counterterms in the LF Hamiltonian.",
author = "Paston, {S. A.} and Prokhvatilov, {E. V.} and Franke, {V. A.}",
year = "2002",
month = apr,
day = "1",
doi = "10.1016/S0920-5632(02)01327-0",
language = "English",
volume = "108",
pages = "189--193",
journal = "Nuclear and Particle Physics Proceedings",
issn = "2405-6014",
publisher = "Elsevier",

}

RIS

TY - JOUR

T1 - On the correspondence between a light-front Hamiltonian approach and a Lorentz-covariant formulation for quantum gauge theories

AU - Paston, S. A.

AU - Prokhvatilov, E. V.

AU - Franke, V. A.

PY - 2002/4/1

Y1 - 2002/4/1

N2 - The problem of restoring the equivalence between Light-Front (LF) Hamiltonian and conventional Lorentz-covariant formulations of gauge theories is solved for QED(1+1) and (perturbatively to all orders) for QCD(3+1). For QED(1+1) a LF Hamiltonian is constructed which reproduces the results of a Lorentz-covariant theory. This is achieved through bosonization of the model and by analyzing the resulting bosonic theory to all orders in the fermion mass. For QCD(3+1) we describe nonstandard regularization that allows to restore the mentioned equivalence with a finite number of counterterms in the LF Hamiltonian.

AB - The problem of restoring the equivalence between Light-Front (LF) Hamiltonian and conventional Lorentz-covariant formulations of gauge theories is solved for QED(1+1) and (perturbatively to all orders) for QCD(3+1). For QED(1+1) a LF Hamiltonian is constructed which reproduces the results of a Lorentz-covariant theory. This is achieved through bosonization of the model and by analyzing the resulting bosonic theory to all orders in the fermion mass. For QCD(3+1) we describe nonstandard regularization that allows to restore the mentioned equivalence with a finite number of counterterms in the LF Hamiltonian.

UR - http://www.scopus.com/inward/record.url?scp=0036557391&partnerID=8YFLogxK

U2 - 10.1016/S0920-5632(02)01327-0

DO - 10.1016/S0920-5632(02)01327-0

M3 - Article

VL - 108

SP - 189

EP - 193

JO - Nuclear and Particle Physics Proceedings

JF - Nuclear and Particle Physics Proceedings

SN - 2405-6014

ER -

ID: 5144932