Nucl. Phys. B435 (1995) 207-240


TITLE:

Color Confinement, Quark Pair Creation and Dynamical Chiral-Symmetry Breaki\ ng in the Dual Ginzburg-Landau Theory.

ABSTRACT:

We study the color confinement, the $q$-$\bar q$ pair creation and the dynamical chiral-symmetry breaking of nonperturbative QCD by using the dual Ginzburg-Landau theory, where the dual Higgs mechanism plays an essential role on the nonperturbative dynamics in the infrared region. As a result of the dual Meissner effect, the linear static quark potential, which characterizes the quark confinement, is obtained in the long distance within the quenched approximation. We obtain a simple expression for the string tension similar to the energy per unit length of a vortex in the superconductivity physics. The dynamical effect of light quarks on the quark confining potential is investigated in terms of the infrared screening effect due to the $q$-$\bar q$ pair creation or the cut of the hadronic string. The screening length of the potential is estimated by using the Schwinger formula for the $q$-$\bar q$ pair creation. We introduce the corresponding infrared cutoff to the strong long-range correlation factor in the gluon propagator as a dynamical effect of light quarks, and obtain a compact formula for the quark potential including the screening effect in the infrared region. We investigate the dynamical chiral-symmetry breaking by using the Schwinger-Dyson equation in the dual Ginzburg-Landau theory, where the gluon propagator includes the nonperturbative effect related to the color confinement. We find a large enhancement of the chiral-symmetry breaking by the dual Higgs mechanism, which supports the close relation between the color confinement and the chiral-symmetry breaking. The dynamical quark mass, the pion decay constant and the quark condensate are well reproduced by using the consistent values of the gauge coupling constant and the QCD scale parameter with the perturbative QCD and the quark confining potential. The light-quark confinement is also roughly examined in terms of the disappearance of physical poles in the light-quark propagator by using the smooth extrapolation of the quark mass function to the time-like momentum region.



Nucl. Phys. A577 (1994) 353c-360c


TITLE:

Magnetic Monopole Condensation for Confinement and Chiral Symmetry Breaking.

ABSTRACT:

Nonperturbative feature of QCD are investigated using the dual Ginzburg- Landau theory. The quark confinement is realized through the dual Meissner effect, when QCD monopoles are condensed. The chiral symmetry is dynamically broken due to a large contribution of QCD-monopole condensation.



Prog. Theor. Phys. 94 (1995) 373-384


TITLE:

Dual Ginzburg-Landau Theory with QCD Monopoles for Dynamical Chiral-Symmetry Breaking.

ABSTRACT:

We study dynamical chiral-symmetry breaking of non-perturbative QCD in the dual Ginzburg-Landau theory, where the QCD-monopole field is introduced as an essential field for color confinement stemming from the choice of the abelian gauge fixing {\it a la} 't Hooft. In this theory, QCD-monopole condensation causes the dual Meissner effect, which changes the gluon propagator. The dynamical chiral-symmetry breaking is investigated using the Schwinger-Dyson equation with the modified gluon propagator in the QCD-monopole condensed vacuum. We introduce the low momentum cutoff on the modified gluon propagator by considering the effects of the $q$-$\bar q$ pair creation and/or the quarks being confined in hadrons. We find that dynamical chiral- symmetry breaking is largely enhanced by QCD-monopole condensation, which suggests the close relation between the color confinement and the chiral symmetry breaking. The dynamical quark mass, the pion decay constant and the quark condensate are reproduced consistently with the confining mechanism in this theory.



Prog. Theor. Phys. Suppl. 120 (1995) 57


TITLE:

Dual Higgs Mechanism for Quarks in Hadrons.

ABSTRACT:

We study nonperturbative features of QCD using the dual Ginzburg-Landau (DGL) theory, where the color confinement is realized through the dual Higgs mechanism brought by QCD-monopole condensation. The linear confinement potential appears in the QCD-monopole condensed vacuum. We study the infrared screening effect to the confinement potential by the light-quark pair creation, and derive a compact formula for the screened quark potential. We study the dynamical chiral-symmetry breaking (D$\chi $SB) in the DGL theory by solving the Schwinger-Dyson equation. QCD-monopole condensation plays an essential role to D$\chi $SB. The QCD phase transition at finite temperature is studied using the effective potential formalism in the DGL theory. We find the reduction of QCD-monopole condensation and the string tension at high temperatures. The surface tension is calculated using the effective potential at the critical temperature. The DGL theory predicts a large mass reduction of glueballs near the critical temperature. We apply the DGL theory to the quark-gluon-plasma (QGP) physics in the ultrarelativistic heavy-ion collisions. We propose a new scenario of the QGP formation via the annihilation of color-electric flux tubes based on the attractive force between them.



Nucl. Phys. B (Proc.Suppl.) 47 (1996) 302


TITLE:

Evidence of Strong Correlation between Instanton and QCD-Monopole on SU(2) Lattice.

ABSTRACT:

The correlation between instantons and QCD-monopoles is studied both in the lattice gauge theory and in the continuum theory. An analytical study in the Polyakov-like gauge, where $A_4(x)$ is diagonalized, shows that the QCD-monopole trajectory penetrates the center of each instanton, and becomes complicated in the multi-instanton system. Using the SU(2) lattice with $16^4$, the instanton number is measured in the singular (monopole-dominating) and regular (photon-dominating) parts, respectively. The monopole dominance for the topological charge is found both in the maximally abelian gauge and in the Polyakov gauge.



Nucl. Phys. B (Proc.Suppl.) 53 (1997) 494


TITLE:

Distribution of Instanton and Monopole Clustering.

ABSTRACT:

We study the relation between the instanton distribution and the monopole loop length in the SU(2) gauge theory with the abelian gauge fixing. We measure the monopole current from the multi-instanton ensemble on the $16^4$ lattice using the maximally abelian gauge. When the instanton density is dilute, there appear only small monopole loops. On the other hand, in the dense case, there appears one very long monopole loop, which is responsible for the confinement property, in each gauge configuration. We find a clear monopole clustering in the histogram of the monopole loop length from 240 gauge configurations.



Nucl. Phys. B (Proc.Suppl.) 53 (1997) 302


TITLE:

Distribution of Instanton and Monopole Clustering.

ABSTRACT:

We study the relation between instantons and monopoles in the abelian gauge. First, we investigate the monopole in the multi-instanton solution in the continuum Yang-Mills theory using the Polyakov gauge. At a large instanton density, the monopole trajectory becomes highly complicated, which can be regarded as a signal of monopole condensation. Second, we study instantons and monopoles in the SU(2) lattice gauge theory both in the maximally abelian (MA) gauge and in the Polyakov gauge. Using the $16^3 \times 4$ lattice, we find monopole dominance for instantons in the confinement phase even at finite temperatures. A linear-type correlation is found between the total monopole-loop length and the integral of the absolute value of the topological density (the total number of instantons and anti-instantons) in the MA gauge. We conjecture that instantons enhance the monopole-loop length and promote monopole condensation.



Aust. J. Phys. 50 (1997) 199


TITLE:

Chiral Symmetry Breaking in the Dual Ginzburg-Landau Theory.

ABSTRACT:

Confinement and chiral symmetry breaking are the most fundamental phenomena in Quark Nuclear Physics, where hadrons and nuclei are described in terms of quarks and gluons. The dual Ginzburg-Landau (DGL) theory, which contains monopole fields as the most essential degrees of freedom and their condensation in the vacuum, is modeled to describe quark confinement in strong connection with QCD. We then demonstrate that the DGL theory is able to describe the spontaneous break down of the chiral symmetry.



Aust. J. Phys. 50 (1997) 233


TITLE:

Monopole Dominance for Nonperturbative QCD.

ABSTRACT:

Monopole dominance for the nonperturbative features in QCD is studied both in the continuum and the lattice gauge theories. First, we study the dynamical chiral-symmetry breaking (D$\chi $SB) in the dual Higgs theory using the effective potential formalism. We find that the main driving force for D$\chi $SB is brought from the confinement part in the nonperturbative gluon propagator rather than the short-range part, which means monopole dominance for D$\chi $SB. Second, the correlation between instantons and QCD-monopoles is studied. In the Polyakov-like gauge, where $A_4(x)$ is diagonalized, the QCD-monopole trajectory penetrates the center of each instanton, and becomes complicated in the multi-instanton system. Finally, using the SU(2) lattice gauge theory with $16^4$ and $16^3 \times 4$, the instanton number is measured in the singular (monopole-dominating) and regular (photon-dominating) sectors, respectively. Instantons and anti- instantons only exist in the monopole sector both in the maximally abelian gauge and in the Polyakov gauge, which means monopole dominance for the topological charge.



Phys. Lett. B399 (1997) 141-147.


TITLE:

Clustering of Monopoles in the Instanton Vacuum.

ABSTRACT:

We generate a random instanton vacuum with various densities and size distributions. We perform numerically the maximally abelian gauge fixing of these configurations in order to find monopole trajectories induced by instantons. We find that instanton-induced monopole loops form enormous clusters occupying the whole physical volume, provided instantons are sufficiently dense. It indicates that confinement might be caused by instantons.



Nucl. Phys. B (Proc. Suppl.) 63A-C (1998) 507-509.


TITLE:

Existence of Chiral-Asymmetric Zero Modes in the Background of QCD-Monopoles

ABSTRACT:

We study topological aspects of the QCD vacuum structure in SU(2) lattice gauge theory with the abelian ague fixing. The index of the Dirac operator is measured by using the Wilson fermion in the quenched approximation. We find chiral-asymmetric zero modes in background fields dominated by QCD-monopoles without any cooling.



Nucl. Phys. B (Proc. Suppl.) 63A-C (1998) 513-515.


TITLE:

Confinemnet Properties in the Multi-Instanton System

ABSTRACT:

We investigate the confinement properties in the multi-instanton system, where the size distribution is assumed to be $\rho^{-5}$ for the large instanton size $\rho$. We find that the instanton vacuum gives the area law behavior of the Wilson loop, which indicates existence of the linear confining potential. In the multi-instanton system, the string tension increases monotonously with the instanton density, and takes the standard value $\sigma \simeq$ 1 GeV/fm for the density $(N/V)^{1 \over 4}$ =200MeV. Thus, instantons directly relate to color confinement properties.



Prog. Theor. Phys. Suppl. 129 (1997) 227-230.


TITLE:

Confinement Mechanism and Chiral Phase Transition in the Nonperturbative vacuum of QCD.

ABSTRACT:

We study the relation between color confinement and chiral symmetry breaking in the background of condensed monopoles at $T=0$ and $T\neq0$. We formulate the Schwinger-Dyson (SD) equation including the vacuum polarization effect, which could remove the infrared singularity, in the dual Ginzburg-Landau theory. In order to solve the SD equation at $T\neq0$, we provide a new ansatz for the quark mass function in the imaginary-time formalism. We find the existence of a strong correlation between the critical temperature $T_{c}$ of the chiral symmetry restoration and the confinement quantity such as the string tension.



Physics Letters B443 (1998) 331-337.


TITLE:

Lattice Study of ${\rm U_{A}}(1)$ Anomaly: The Role of QCD-Monopoles.

ABSTRACT:

We investigate the role of QCD-monopoles for the ${\rm U}_{\rm A}(1)$ anomaly in the maximally abelian gauge within the SU(2) lattice gauge theory. The existence of the strong correlation between instantons and QCD-monopoles in the abelian gauge was already shown by both analytic and numerical works including the Monte Carlo simulation. Their interrelation brings us a conjecture that the presence of QCD-monopoles plays a considerable role on the ${\rm U}_{\rm A}(1)$ anomaly. We find an evidence for our conjecture on a determination of the fermionic zero modes of the Dirac operator in both the ``monopole removed'' gauge configuration and the ``photon removed'' gauge configuration.



Physical Review D59 (1999) 094507.


TITLE:

Topological Aspect of Abelian Projected SU(2) Lattice Gauge Theory.

ABSTRACT:

We show that the hypothesis of abelian dominance allows QCD-monopoles to preserve the topological feature of the QCD vacuum within SU(2) lattice gauge theory. An analytical study is made to find the relationship between the topological charge and QCD-monopoles in the lattice formulation. The topological charge is explicitly represented in terms of the monopole current and the abelian component of gauge fields in the abelian dominated system. We numerically examine the relation and demonstrate the abelian dominance in the topological structure by using Monte Carlo simulation.



Nucl. Phys. B (Proc. Suppl.) 73 (1999) 545-547.


TITLE:

A Conclusive Test of Abelian Dominance Hypothesis for Topological Charge in the QCD Vacuum.

ABSTRACT:

We study the topological feature in the QCD vacuum based on the hypothesis of abelian dominance. The topological charge $Q_{\rm SU(2)}$ can be explicitly represented in terms of the monopole current in the abelian dominated system. To appreciate its justification, we directly measure the corresponding topological charge $Q_{\rm Mono}$, which is reconstructed only from the monopole current and the abelian component of gauge fields, by using the Monte Carlo simulation on SU(2) lattice. We find that there exists a one-to-one correspondence between $Q_{\rm SU(2)}$ and $Q_{\rm Mono}$ in the maximally abelian gauge.Furthermore, $Q_{\rm Mono}$ is classified by approximately discrete values.