Thermal Width Broadening of the 0++ Glueball Spectrum near Tc

We study the 0++ glueball correlator constructed with SU(3) anisotropic quenched lattice QCD at various temperature taking into account the possible existence of the thermal width in the ground-state peak. For this purpose, we adopt the Breit-Wigner ansatz, analysing the lattice data obtained with 5,500-9,900 gauge configurations at each T. The results indicate the significant thermal width broadening as Gamma(Tc) \sim 300 MeV with a reduction in the peak center as Delta omega_0(Tc) \sim 100 MeV in the vicinity of the critical temperature Tc.Comment: Talk given at Tokyo-Adelaide Joint Workshop on Quarks, Astrophysics and Space Physics, Tokyo, Japan, 6-10 January 2003, 5 pages, Latex2e, 2 figure

Glueball properties in anisotropic SU(3) lattice QCD with improved action

We study the glueballs properties at finite temperature using SU(3) lattice QCD at the quenched level with the anisotropic lattice. We use the tree-level Symanzik O(a^2) improved action. We present our preliminary results which shows the slight reduction of the scalar glueball mass near T_cComment: 8 pages, 13 figures, Talk given at Joint Workshop of the Special Research Center for the Subatomic Structure of Matter and the National Institute for Theoretical Physics (Workshop on Lepton Scattering, Hadrons and QCD), Adelaide, Australia 26 March - 6 April 200

Properties of Thermal Glueballs

We study the properties of the 0++ glueball at finite temperature using SU(3) quenched lattice QCD. We find a significant thermal effects near T_c. We perform the \chi^2 fit analyses adopting two Ansaetze for the spectral function, i.e., the conventional narrow-peak Ansatz and an advanced Breit-Wigner Ansatz. The latter is an extension of the former, taking account of the appearance of the thermal width at T>0. We also perform the MEM analysis. These analyses indicate that the thermal effect on the glueball is a significant thermal-width broadening \Gamma(T_c) \sim 300 MeV together with a modest reduction in the peak center \Delta\omega_0(T_c) \sim 100 MeV.Comment: A talk presented at International Conference on Color Confinement and Hadrons in Quantum Chromodynamics --Confinement 2003--, Wako, Japan, 21-24 July 2003, 5 pages, 3 figure

The Thermal Width of the Glueball at Non-Zero Temperature

We use SU(3) anisotropic lattice QCD at quenched level to study the 0++ glueball correlator at various temperature taking into account the possible existence of the thermal width in the ground-state peak. For this purpose, we adopt the Breit-Wigner ansatz for the appropriate fit-function for the lattice data obtained with 5,500-9,900 gauge configurations at each T. The results show the significant thermal width broadening as Gamma(T_c) \sim 300 MeV with a reduction in the peak center as Delta omega_0(T_c) \sim 100 MeV near the critical temperature T_c.Comment: Talk given at LATTICE 2002, The XX International Symposium on Lattice Field Thoery, Massachusetts, USA, June 24-29, 2002, Lattice2001(nonzerot), 1 figure, 3 page

Rescue of Rous sarcoma virus (RSV) from RSV-transformed human embryonic cells by cell fusion with chick embryo fibroblasts using lysolecithin

Heterokaryon formation and Rous sarcoma virus (RSV)-induction were studied by fusion of RSV-transformed human embryonic cells with chick embryo fibroblasts in the presence of lysolecithin. Heterokaryon formation was observed by autoradiography. RSV-induction was identified by focus formation, electron microscopy and density gradient centrifugation of 3H-uridine-labeled particles. The most effective concentration of lysolecithin for virus induction was 10 mug/10(6) cells/0.1 ml. Efficiency of lysolecithin in virus induction was not less than that of ultraviolet-inactivated Sendai virus (UV-HVJ).</p

MEM Analysis of Glueball Correlators at T>0

Maximum Entropy Method (MEM) is applied to glueball correlators at finite temperature constructed by using 5,500-9,900 gauge field configurations generated in SU(3) quenched lattice QCD with the lattice parameter beta = 2N_c/g^2 = 6.25 and the renormalized anisotropy a_s/a_t = 4. The results support the thermal width broadening of the 0++ glueball near the critical temperature.Comment: Talk given at LATTICE 2003, The XXI International Symposium on Lattice Field Thoery, Tsukuba International Congress Center, Tsukuba, Ibaraki, Japan, July 15-19, 2003, Lattice2003(nonzerot), latex2e, 1 figure, 3 page

The Determination of the Quark-Gluon Mixed Condensate (anti-Q sigma G Q) from Lattice QCD

We study the quark-gluon mixed condensate g, using the SU(3)c lattice QCD with the Kogut-Susskind fermion at the quenched level. We generate 100 gauge configurations on the 16^4 lattice with \beta = 6.0, and perform the measurement of the mixed condensate at 16 points in each gauge configuration for each current quark mass of m_q=21, 36, 52 MeV. Using the 1600 data for each m_q, we find the ratio between the mixed condensate and the quark condensate, m_0^2 = g / \simeq 2.5 GeV^2 at the lattice scale of 1/a \simeq 2 GeV in the chiral limit. The large value of the mixed condensate suggests its importance in the operator product expansions in QCD. We study also chiral restoration at finite temperature in terms of the mixed condensate, which is another chiral order parameter. We present the lattice QCD results of the mixed condensate at finite temperature.Comment: 5 pages, Talk given at Tokyo-Adelaide Joint Workshop on Quarks, Astrophysics and Space physics, Tokyo, Japan, Jan.6 - Jan.10, 200