689 research outputs found

    Properties of Scalar-Quark Systems in SU(3)c Lattice QCD

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    We perform the first study for the bound states of colored scalar particles ϕ\phi ("scalar quarks") in terms of mass generation with quenched SU(3)c_c lattice QCD. We investigate the bound states of ϕ\phi, ϕϕ\phi^\dagger\phi and ϕϕϕ\phi\phi\phi ("scalar-quark hadrons"), as well as the bound states of ϕ\phi and quarks ψ\psi, i.e., ϕψ\phi^\dagger\psi, ψψϕ\psi\psi\phi and ϕϕψ\phi\phi\psi ("chimera hadrons"). All these new-type hadrons including ϕ\phi have a large mass of several GeV due to large quantum corrections by gluons, even for zero bare scalar-quark mass mϕ=0m_\phi=0 at a11GeVa^{-1}\sim 1{\rm GeV}. We find a similar mψm_\psi-dependence between ϕψ\phi^\dagger\psi and ϕϕψ\phi\phi\psi, which indicates their similar structure due to the large mass of ϕ\phi. From this study, we conjecture that all colored particles generally acquire a large effective mass due to dressed gluons

    Gluon-propagator functional form in the Landau gauge in SU(3) lattice QCD: Yukawa-type gluon propagator and anomalous gluon spectral function

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    We study the gluon propagator Dμνab(x)D_{\mu\nu}^{ab}(x) in the Landau gauge in SU(3) lattice QCD at β\beta = 5.7, 5.8, and 6.0 at the quenched level. The effective gluon mass is estimated as 400600400 \sim 600MeV for r(xαxα)1/2=0.51.0r \equiv (x_\alpha x_\alpha)^{1/2} = 0.5 \sim 1.0 fm. Through the functional-form analysis of Dμνab(x)D_{\mu\nu}^{ab}(x) obtained in lattice QCD, we find that the Landau-gauge gluon propagator Dμμaa(r)D_{\mu\mu}^{aa}(r) is well described by the Yukawa-type function emr/re^{-mr}/r with m600m \simeq 600MeV for r=0.11.0r = 0.1 \sim 1.0 fm in the four-dimensional Euclidean space-time. In the momentum space, the gluon propagator D~μμaa(p2)\tilde D_{\mu\mu}^{aa}(p^2) with (p2)1/2=0.53(p^2)^{1/2}= 0.5 \sim 3 GeV is found to be well approximated with a new-type propagator of (p2+m2)3/2(p^2+m^2)^{-3/2}, which corresponds to the four-dimensional Yukawa-type propagator. Associated with the Yukawa-type gluon propagator, we derive analytical expressions for the zero-spatial-momentum propagator D0(t)D_0(t), the effective mass Meff(t)M_{\rm eff}(t), and the spectral function ρ(ω)\rho(\omega) of the gluon field. The mass parameter mm turns out to be the effective gluon mass in the infrared region of \sim 1fm. As a remarkable fact, the obtained gluon spectral function ρ(ω)\rho(\omega) is almost negative-definite for ω>m\omega >m, except for a positive δ\delta-functional peak at ω=m\omega=m.Comment: 20 pages, 15 figure

    Dual Ginzburg-Landau Theory for Nonperturbative QCD

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    Nonperturbative QCD is studied with the dual Ginzburg-Landau theory, where color confinement is realized through the dual Higgs mechanism by QCD-monopole condensation. We obtain a general analytic formula for the string tension. A compact formula is derived for the screened inter-quark potential in the presence of light dynamical quarks. The QCD phase transition at finite temperature is studied using the effective potential formalism. The string tension and the QCD-monopole mass are largely reduced near the critical temperature, TcT_c. The surface tension is estimated from the effective potential at TcT_c. We propose also a new scenario of the quark-gluon-plasma creation through the color-electric flux-tube annihilation. Finally, we discuss a close relation between instantons and QCD-monopoles.Comment: Talk presented by H. Suganuma at the Int. Conf. ``CONFINEMENT95'', March 22-24, 1995, Osaka, Japan, 12 pages, uses PHYZZ

    Model independent approach to studies of the confining dual Abrikosov vortex in SU(2) lattice gauge theory

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    We address the problem of determining the type I, type II or borderline dual superconductor behavior in maximal Abelian gauge SU(2) through the study of the dual Abrikosov vortex. We find that significant electric currents in the simulation data call into question the use of the dual Ginzburg Landau Higgs model in interpreting the data. Further, two definitions of the penetration depth parameter take two different values. The splitting of this parameter into two is intricately connected to the existence of electric currents. It is important in our approach that we employ definitions of flux and electric and magnetic currents that respect Maxwell equations exactly for lattice averages independent of lattice spacings. Applied to specific Wilson loop sizes, our conclusions differ from those that use the dual GLH model.Comment: 18 pages, 14 figures, change title, new anaylysis with more figure

    Dark Matter Search with Direction Sensitive Scintillator

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    A direction sensitive dark matter detector using organic crystals is being developed. It exploits the anisotropic scintillation efficiency of organic crystals with respect to the direction of nuclear recoils relative to crystallographic axes. A variation of about 7% was observed in the scintillation efficiency of carbon recoils in a stilbene crystal for recoil energies of 30 keV to 1 MeV. We have performed a pilot experiment at Kamioka to prove the feasibility of this method.Comment: 6 Pages, 4 figures, To appear in the proceedings of the 5th Workshop on "Neutrino Oscillations and their Origin" (NOON2004

    Off-diagonal Gluon Mass Generation and Infrared Abelian Dominance in the Maximally Abelian Gauge in Lattice QCD

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    We study effective mass generation of off-diagonal gluons and infrared abelian dominance in the maximally abelian (MA) gauge. Using the SU(2) lattice QCD, we investigate the propagator and the effective mass of the gluon field in the MA gauge with the U(1)3_3 Landau gauge fixing. The Monte Carlo simulation is performed on the 123×2412^3 \times 24 lattice with 2.2β2.42.2 \le \beta \le 2.4, and also on the 16416^4 and 20420^4 lattices with 2.3β2.42.3 \le \beta \le 2.4. In the MA gauge, the diagonal gluon component Aμ3A_\mu^3 shows long-range propagation, and infrared abelian dominance is found for the gluon propagator. In the MA gauge, the off-diagonal gluon component Aμ±A_\mu^\pm behaves as a massive vector boson with the effective mass Moff1.2M_{\rm off} \simeq 1.2 GeV in the region of r \gsim 0.2 fm, and its propagation is limited within short range. We conjecture that infrared abelian dominance can be interpreted as infrared inactivity of the off-diagonal gluon due to its large mass generation induced by the MA gauge fixing.Comment: 31 pages, 7 figures and 2 tables included, changed title, corrected typos and updated reference, accepted for publication in Physical Review

    Three-Quark Potential in SU(3) Lattice QCD

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    The static three-quark (3Q) potential is measured in the SU(3) lattice QCD with 123×2412^3 \times 24 and β=5.7\beta=5.7 at the quenched level. From the 3Q Wilson loop, the 3Q ground-state potential V3QV_{\rm 3Q} is extracted using the smearing technique for the ground-state enhancement. With accuracy better than a few %, V3QV_{\rm 3Q} is well described by a sum of a constant, the two-body Coulomb term and the three-body linear confinement term σ3QLmin\sigma_{\rm 3Q} L_{\rm min}, where LminL_{\rm min} denotes the minimal length of the color flux tube linking the three quarks. By comparing with the Q-Qˉ\bar {\rm Q} potential, we find a universal feature of the string tension, σ3QσQQˉ\sigma_{\rm 3Q} \simeq \sigma_{\rm Q \bar Q}, as well as the one-gluon-exchange result for the Coulomb coefficient, A3Q12AQQˉA_{\rm 3Q} \simeq \frac12 A_{\rm Q \bar Q}.Comment: 7 pages, 3 figur

    Mass Generation in the Supersymmetric Nambu--Jona--Lasinio Model in an External Magnetic Field

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    The mass generation in the (3+1)-dimensional supersymmetric Nambu-Jona-Lasinio model in a constant magnetic field is studied. It is shown that the external magnetic field catalyzes chiral symmetry breaking.Comment: LaTeX file, 6 pages. Talk given at the International Seminar dedicated to the memory of Dmitrij Volkov "Supersymmetry and Quantum Field Theory", Kharkov, Ukraine, January 5-7, 199

    Exploring the inner region of Type 1 AGNs with the Keck interferometer

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    The exploration of extragalactic objects with long-baseline interferometers in the near-infrared has been very limited. Here we report successful observations with the Keck interferometer at K-band (2.2 um) for four Type 1 AGNs, namely NGC4151, Mrk231, NGC4051, and the QSO IRAS13349+2438 at z=0.108. For the latter three objects, these are the first long-baseline interferometric measurements in the infrared. We detect high visibilities (V^2 ~ 0.8-0.9) for all the four objects, including NGC4151 for which we confirm the high V^2 level measured by Swain et al.(2003). We marginally detect a decrease of V^2 with increasing baseline lengths for NGC4151, although over a very limited range, where the decrease and absolute V^2 are well fitted with a ring model of radius 0.45+/-0.04 mas (0.039+/-0.003 pc). Strikingly, this matches independent radius measurements from optical--infrared reverberations that are thought to be probing the dust sublimation radius. We also show that the effective radius of the other objects, obtained from the same ring model, is either roughly equal to or slightly larger than the reverberation radius as a function of AGN luminosity. This suggests that we are indeed partially resolving the dust sublimation region. The ratio of the effective ring radius to the reverberation radius might also give us an approximate probe for the radial structure of the inner accreting material in each object. This should be scrutinized with further observations.Comment: accepted for publication in A&A Letter
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