Abstract
Monopole and photon contributions to abelian Wilson loops are calculated using Monte-Carlo simulations of finite-temperature SU(2) QCD in the maximally abelian gauge. The string tension is reproduced by monopole contribution alone also in finite temperature SU(2) QCD. The spatial string tension scales as {radical}(s){proportional_to}g{sup 2}(T)T and is reproduced almost by monopole contribution alone. Each configuration has one long monopole loop, and the long monopole loops alone are responsible for the string tension in the confinement phase. On the other hand, the spatial string tension in the deconfinement phase is reproduced by wrapped monopole loops alone. ((orig.)).
Ejiri, S;
[1]
Kitahara, S I;
[1]
Matsubara, Y;
[2]
Suzuki, T
[1]
- Kanazawa Univ. (Japan). Dept. of Physics
- Nanao Junior College, Nanao, Ishikawa 926 (Japan)
Citation Formats
Ejiri, S, Kitahara, S I, Matsubara, Y, and Suzuki, T.
String tension and monopoles in T{ne}0 SU(2) QCD.
Netherlands: N. p.,
1995.
Web.
doi:10.1016/0920-5632(95)00286-I.
Ejiri, S, Kitahara, S I, Matsubara, Y, & Suzuki, T.
String tension and monopoles in T{ne}0 SU(2) QCD.
Netherlands.
https://doi.org/10.1016/0920-5632(95)00286-I
Ejiri, S, Kitahara, S I, Matsubara, Y, and Suzuki, T.
1995.
"String tension and monopoles in T{ne}0 SU(2) QCD."
Netherlands.
https://doi.org/10.1016/0920-5632(95)00286-I.
@misc{etde_101157,
title = {String tension and monopoles in T{ne}0 SU(2) QCD}
author = {Ejiri, S, Kitahara, S I, Matsubara, Y, and Suzuki, T}
abstractNote = {Monopole and photon contributions to abelian Wilson loops are calculated using Monte-Carlo simulations of finite-temperature SU(2) QCD in the maximally abelian gauge. The string tension is reproduced by monopole contribution alone also in finite temperature SU(2) QCD. The spatial string tension scales as {radical}(s){proportional_to}g{sup 2}(T)T and is reproduced almost by monopole contribution alone. Each configuration has one long monopole loop, and the long monopole loops alone are responsible for the string tension in the confinement phase. On the other hand, the spatial string tension in the deconfinement phase is reproduced by wrapped monopole loops alone. ((orig.)).}
doi = {10.1016/0920-5632(95)00286-I}
journal = []
volume = {42}
journal type = {AC}
place = {Netherlands}
year = {1995}
month = {Apr}
}
title = {String tension and monopoles in T{ne}0 SU(2) QCD}
author = {Ejiri, S, Kitahara, S I, Matsubara, Y, and Suzuki, T}
abstractNote = {Monopole and photon contributions to abelian Wilson loops are calculated using Monte-Carlo simulations of finite-temperature SU(2) QCD in the maximally abelian gauge. The string tension is reproduced by monopole contribution alone also in finite temperature SU(2) QCD. The spatial string tension scales as {radical}(s){proportional_to}g{sup 2}(T)T and is reproduced almost by monopole contribution alone. Each configuration has one long monopole loop, and the long monopole loops alone are responsible for the string tension in the confinement phase. On the other hand, the spatial string tension in the deconfinement phase is reproduced by wrapped monopole loops alone. ((orig.)).}
doi = {10.1016/0920-5632(95)00286-I}
journal = []
volume = {42}
journal type = {AC}
place = {Netherlands}
year = {1995}
month = {Apr}
}