We describe a direct method for calculating the glueball mass spectrum in QCD and apply it to the SU (2) non-abelian gauge theory. The method involves the applicatio of Monte Carlo methods to the lattice regulated theory. We calculate the masses of states of various spins and parity. We check for the absence of finite size effects, for the desired renormalization group dependence and that our higher mass states do not merely reflect a continuum cut. Finally we repeat the calculation in the “Hamiltonian” limit and in the high temperature deconfining phase of QCD.
Описание
Zeitschrift für Physik C Particles and Fields, Volume 19, Number 4 - SpringerLink
%0 Journal Article
%1 springerlink:10.1007/BF01577189
%A Ishikawa, K.
%A Schierholz, G.
%A Teper, M.
%C Berlin / Heidelberg
%D 1983
%I Springer
%J Zeitschrift für Physik C Particles and Fields
%K Glueballs Reviewlike SU2 YM
%N 4
%P 327-352
%R 10.1007/BF01577189
%T Calculation of the glueball mass spectrum of<i>SU</i> (2) and<i>SU</i> (3) non-abelian lattice gauge theories I: Introduction and<i>SU</i> (2)
%U http://dx.doi.org/10.1007/BF01577189
%V 19
%X We describe a direct method for calculating the glueball mass spectrum in QCD and apply it to the SU (2) non-abelian gauge theory. The method involves the applicatio of Monte Carlo methods to the lattice regulated theory. We calculate the masses of states of various spins and parity. We check for the absence of finite size effects, for the desired renormalization group dependence and that our higher mass states do not merely reflect a continuum cut. Finally we repeat the calculation in the “Hamiltonian” limit and in the high temperature deconfining phase of QCD.
@article{springerlink:10.1007/BF01577189,
abstract = {We describe a direct method for calculating the glueball mass spectrum in QCD and apply it to the SU (2) non-abelian gauge theory. The method involves the applicatio of Monte Carlo methods to the lattice regulated theory. We calculate the masses of states of various spins and parity. We check for the absence of finite size effects, for the desired renormalization group dependence and that our higher mass states do not merely reflect a continuum cut. Finally we repeat the calculation in the “Hamiltonian” limit and in the high temperature deconfining phase of QCD.},
added-at = {2012-09-03T16:41:23.000+0200},
address = {Berlin / Heidelberg},
affiliation = {City College CUNY 10033 New York NY USA},
author = {Ishikawa, K. and Schierholz, G. and Teper, M.},
biburl = {https://www.bibsonomy.org/bibtex/200fb65288fecdbcbcfad561968c1c0a0/gber},
description = {Zeitschrift für Physik C Particles and Fields, Volume 19, Number 4 - SpringerLink},
doi = {10.1007/BF01577189},
interhash = {7a3279c740620a54c29f41e1fdc34ffe},
intrahash = {00fb65288fecdbcbcfad561968c1c0a0},
issn = {0170-9739},
journal = {Zeitschrift für Physik C Particles and Fields},
keyword = {Physics and Astronomy},
keywords = {Glueballs Reviewlike SU2 YM},
number = 4,
pages = {327-352},
publisher = {Springer},
timestamp = {2012-09-03T16:41:24.000+0200},
title = {Calculation of the glueball mass spectrum of<i>SU</i> (2) and<i>SU</i> (3) non-abelian lattice gauge theories I: Introduction and<i>SU</i> (2)},
url = {http://dx.doi.org/10.1007/BF01577189},
volume = 19,
year = 1983
}