Standard

Quantum Field Theory in Light-Front coordinates. / Franke, V.A.; Novozhilov, Yu.V.; Paston, S.A.; Prokhvatilov, E.V.

Quantum Theory in honour of Vladimir A. Fock, Part 1. UNESCO, 1998. p. 38-97.

Research output: Chapter in Book/Report/Conference proceeding › Article in an anthology

Harvard

Franke, VA, Novozhilov, YV, Paston, SA & Prokhvatilov, EV 1998, Quantum Field Theory in Light-Front coordinates. in Quantum Theory in honour of Vladimir A. Fock, Part 1. UNESCO, pp. 38-97. <http://arxiv.org/abs/hep-th/9901029>

APA

Franke, V. A., Novozhilov, Y. V., Paston, S. A., & Prokhvatilov, E. V. (1998). Quantum Field Theory in Light-Front coordinates. In Quantum Theory in honour of Vladimir A. Fock, Part 1 (pp. 38-97). UNESCO. http://arxiv.org/abs/hep-th/9901029

Vancouver

Franke VA, Novozhilov YV, Paston SA, Prokhvatilov EV. Quantum Field Theory in Light-Front coordinates. In Quantum Theory in honour of Vladimir A. Fock, Part 1. UNESCO. 1998. p. 38-97

Author

Franke, V.A. ; Novozhilov, Yu.V. ; Paston, S.A. ; Prokhvatilov, E.V. / Quantum Field Theory in Light-Front coordinates. Quantum Theory in honour of Vladimir A. Fock, Part 1. UNESCO, 1998. pp. 38-97

BibTeX

@inbook{363149f181964ddabf6cf5d1e5775644,
title = "Quantum Field Theory in Light-Front coordinates",
abstract = "Canonical formulation of quantum field theory on the Light Front (LF) is reviewed. The problem of constructing the LF Hamiltonian which gives the theory equivalent to original Lorentz and gauge invariant one is considered. We describe possible ways of solving this problem: (a) the limiting transition from the equal-time Hamiltonian in a fastly moving Lorentz frame to LF Hamiltonian, (b) the direct comparison of LF perturbation theory in coupling constant and usual Lorentz-covariant Feynman perturbation theory. Gauge invariant regularization of LF Hamiltonian via introducing a lattice in transverse coordinates and imposing periodic boundary conditions in LF coordinate $x^-$ for gauge fields on the interval $|x^-|<L$ is considered. We find that LF canonical formalism for this regularization avoid usual most complicated constraints connecting zero and nonzero modes of gauge fields.",
author = "V.A. Franke and Yu.V. Novozhilov and S.A. Paston and E.V. Prokhvatilov",
year = "1998",
language = "English",
pages = "38--97",
booktitle = "Quantum Theory in honour of Vladimir A. Fock, Part 1",
publisher = "UNESCO",
address = "Korea, Republic of",

}

RIS

TY - CHAP

T1 - Quantum Field Theory in Light-Front coordinates

AU - Franke, V.A.

AU - Novozhilov, Yu.V.

AU - Paston, S.A.

AU - Prokhvatilov, E.V.

PY - 1998

Y1 - 1998

N2 - Canonical formulation of quantum field theory on the Light Front (LF) is reviewed. The problem of constructing the LF Hamiltonian which gives the theory equivalent to original Lorentz and gauge invariant one is considered. We describe possible ways of solving this problem: (a) the limiting transition from the equal-time Hamiltonian in a fastly moving Lorentz frame to LF Hamiltonian, (b) the direct comparison of LF perturbation theory in coupling constant and usual Lorentz-covariant Feynman perturbation theory. Gauge invariant regularization of LF Hamiltonian via introducing a lattice in transverse coordinates and imposing periodic boundary conditions in LF coordinate $x^-$ for gauge fields on the interval $|x^-|<L$ is considered. We find that LF canonical formalism for this regularization avoid usual most complicated constraints connecting zero and nonzero modes of gauge fields.

AB - Canonical formulation of quantum field theory on the Light Front (LF) is reviewed. The problem of constructing the LF Hamiltonian which gives the theory equivalent to original Lorentz and gauge invariant one is considered. We describe possible ways of solving this problem: (a) the limiting transition from the equal-time Hamiltonian in a fastly moving Lorentz frame to LF Hamiltonian, (b) the direct comparison of LF perturbation theory in coupling constant and usual Lorentz-covariant Feynman perturbation theory. Gauge invariant regularization of LF Hamiltonian via introducing a lattice in transverse coordinates and imposing periodic boundary conditions in LF coordinate $x^-$ for gauge fields on the interval $|x^-|<L$ is considered. We find that LF canonical formalism for this regularization avoid usual most complicated constraints connecting zero and nonzero modes of gauge fields.

M3 - Article in an anthology

SP - 38

EP - 97

BT - Quantum Theory in honour of Vladimir A. Fock, Part 1

PB - UNESCO

ER -

ID: 4442581