Gluon propagators in maximally Abelian gauge in SU(3) lattice QCD
Gluon propagators in maximally Abelian gauge in SU(3) lattice QCD
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DOI：
10.1103/physrevd.87.074506
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发表时间：
2013-02
影响因子：
5
通讯作者：
S. Gongyo;H. Suganuma
中科院分区：
文献类型：
--
作者：
S. Gongyo;H. Suganuma
In SU(3) lattice QCD, we study diagonal and off-diagonal gluon propagators in the maximally Abelian gauge with $\mathrm{U}(1{)}_{3}\ifmmode\times\else\texttimes\fi{}\mathrm{U}(1{)}_{8}$ Landau gauge fixing. These propagators are studied both in the coordinate space and in the momentum space. The Monte Carlo simulation is performed on ${16}^{4}$ at $\ensuremath{\beta}=6.0$ and ${32}^{4}$ at $\ensuremath{\beta}=5.8$ and 6.0 at the quenched level. In the four-dimensional Euclidean space-time, the effective mass of diagonal gluons is estimated as ${M}_{\mathrm{diag}}\ensuremath{\simeq}0.3\text{ }\text{ }\mathrm{GeV}$ and that of off-diagonal gluons as ${M}_{\mathrm{off}}\ensuremath{\simeq}1\text{ }\text{ }\mathrm{GeV}$ in the region of $r=0.4--1.0\text{ }\text{ }\mathrm{fm}$. In the momentum space, the effective mass of diagonal gluons is estimated as ${M}_{\mathrm{diag}}\ensuremath{\simeq}0.3\text{ }\text{ }\mathrm{GeV}$ and that of off-diagonal gluons as ${M}_{\mathrm{off}}\ensuremath{\simeq}1\text{ }\text{ }\mathrm{GeV}$ in the region of $pl1.1\text{ }\text{ }\mathrm{GeV}$. The off-diagonal gluon propagator is relatively suppressed in the infrared region and seems to be finite at zero momentum, while the diagonal gluon propagator is enhanced. Furthermore, we also study the functional form of these propagators in momentum space. These propagators are well fitted by $Z/({p}^{2}+{m}^{2}{)}^{\ensuremath{\nu}}$ with fit parameters, $Z$, $m$, and $\ensuremath{\nu}$ in the region of $pl3.0\text{ }\text{ }\mathrm{GeV}$. From the fit results and lattice calculations, all of the spectral functions of diagonal and off-diagonal gluons would have negative regions.
In SU(3) lattice QCD, we study diagonal and off-diagonal gluon propagators in the maximally Abelian gauge with $\mathrm{U}(1{)}_{3}\ifmmode\times\else\texttimes\fi{}\mathrm{U}(1{)}_{8}$ Landau gauge fixing. These propagators are studied both in the coordinate space and in the momentum space. The Monte Carlo simulation is performed on ${16}^{4}$ at $\ensuremath{\beta}=6.0$ and ${32}^{4}$ at $\ensuremath{\beta}=5.8$ and 6.0 at the quenched level. In the four-dimensional Euclidean space-time, the effective mass of diagonal gluons is estimated as ${M}_{\mathrm{diag}}\ensuremath{\simeq}0.3\text{ }\text{ }\mathrm{GeV}$ and that of off-diagonal gluons as ${M}_{\mathrm{off}}\ensuremath{\simeq}1\text{ }\text{ }\mathrm{GeV}$ in the region of $r=0.4--1.0\text{ }\text{ }\mathrm{fm}$. In the momentum space, the effective mass of diagonal gluons is estimated as ${M}_{\mathrm{diag}}\ensuremath{\simeq}0.3\text{ }\text{ }\mathrm{GeV}$ and that of off-diagonal gluons as ${M}_{\mathrm{off}}\ensuremath{\simeq}1\text{ }\text{ }\mathrm{GeV}$ in the region of $pl1.1\text{ }\text{ }\mathrm{GeV}$. The off-diagonal gluon propagator is relatively suppressed in the infrared region and seems to be finite at zero momentum, while the diagonal gluon propagator is enhanced. Furthermore, we also study the functional form of these propagators in momentum space. These propagators are well fitted by $Z/({p}^{2}+{m}^{2}{)}^{\ensuremath{\nu}}$ with fit parameters, $Z$, $m$, and $\ensuremath{\nu}$ in the region of $pl3.0\text{ }\text{ }\mathrm{GeV}$. From the fit results and lattice calculations, all of the spectral functions of diagonal and off-diagonal gluons would have negative regions.