Abstract
We investigate the role of monopoles in the deconfinement transition of finite temperature SU(2) QCD in the maximally abelian gauge. In the confinement phase a long monopole loop exists in each configuration, whereas no long loop exists in the deep deconfinement region. Balancing of the energy and the entropy of loops of the maximally extended monopoles can explain the occurrence of the deconfinement transition. ((orig.)).
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
Kitahara, S I, Matsubara, Y, and Suzuki, T.
Monopoles and deconfinement transition in finite temperature SU(2) QCD.
Netherlands: N. p.,
1995.
Web.
doi:10.1016/0920-5632(95)00296-L.
Kitahara, S I, Matsubara, Y, & Suzuki, T.
Monopoles and deconfinement transition in finite temperature SU(2) QCD.
Netherlands.
https://doi.org/10.1016/0920-5632(95)00296-L
Kitahara, S I, Matsubara, Y, and Suzuki, T.
1995.
"Monopoles and deconfinement transition in finite temperature SU(2) QCD."
Netherlands.
https://doi.org/10.1016/0920-5632(95)00296-L.
@misc{etde_101149,
title = {Monopoles and deconfinement transition in finite temperature SU(2) QCD}
author = {Kitahara, S I, Matsubara, Y, and Suzuki, T}
abstractNote = {We investigate the role of monopoles in the deconfinement transition of finite temperature SU(2) QCD in the maximally abelian gauge. In the confinement phase a long monopole loop exists in each configuration, whereas no long loop exists in the deep deconfinement region. Balancing of the energy and the entropy of loops of the maximally extended monopoles can explain the occurrence of the deconfinement transition. ((orig.)).}
doi = {10.1016/0920-5632(95)00296-L}
journal = []
volume = {42}
journal type = {AC}
place = {Netherlands}
year = {1995}
month = {Apr}
}
title = {Monopoles and deconfinement transition in finite temperature SU(2) QCD}
author = {Kitahara, S I, Matsubara, Y, and Suzuki, T}
abstractNote = {We investigate the role of monopoles in the deconfinement transition of finite temperature SU(2) QCD in the maximally abelian gauge. In the confinement phase a long monopole loop exists in each configuration, whereas no long loop exists in the deep deconfinement region. Balancing of the energy and the entropy of loops of the maximally extended monopoles can explain the occurrence of the deconfinement transition. ((orig.)).}
doi = {10.1016/0920-5632(95)00296-L}
journal = []
volume = {42}
journal type = {AC}
place = {Netherlands}
year = {1995}
month = {Apr}
}