NSR Query Results
Output year order : Descending NSR database version of May 8, 2024. Search: Author = H.Fujii Found 39 matches. 2022FU06 Phys.Rev. C 106, 034906 (2022) H.Fujii, K.Itakura, K.Miyachi, C.Nonaka Radiative hadronization: Photon emission at hadronization from quark-gluon plasma
doi: 10.1103/PhysRevC.106.034906
2017FU08 Nucl.Phys. A967, 704 (2017) Photon emission at hadronization
doi: 10.1016/j.nuclphysa.2017.06.045
2017SA36 Phys.Rev. C 95, 064905 (2017) M.Sakaida, M.Asakawa, H.Fujii, M.Kitazawa Dynamical evolution of critical fluctuations and its observation in heavy ion collisions
doi: 10.1103/PhysRevC.95.064905
2016FU04 Nucl.Phys. A951, 45 (2016); Erratum Nucl.Phys. A961, 218 (2017) Leptons from heavy-quark semileptonic decay in pA collisions within the CGC framework
doi: 10.1016/j.nuclphysa.2016.03.045
2013AL02 Nucl.Phys. A897, 1 (2013) J.L.Albacete, A.Dumitru, H.Fujii, Y.Nara CGC predictions for p + Pb collisions at the LHC
doi: 10.1016/j.nuclphysa.2012.09.012
2013FU10 Nucl.Phys. A915, 1 (2013) Heavy quark pair production in high-energy pA collisions: Quarkonium
doi: 10.1016/j.nuclphysa.2013.06.011
2013FU13 Nucl.Phys. A920, 78(2013) Heavy quark pair production in high energy pA collisions: Open heavy flavors
doi: 10.1016/j.nuclphysa.2013.10.006
2009FU04 Phys.Rev. C 79, 024909 (2009) H.Fujii, K.Fukushima, Y.Hidaka Initial energy density and gluon distribution from the glasma in heavy-ion collisions
doi: 10.1103/PhysRevC.79.024909
2009FU08 Nucl.Phys. A828, 178 (2009) Instabilities in non-expanding glasma
doi: 10.1016/j.nuclphysa.2009.06.021
2008FU10 Nucl.Phys. A809, 88 (2008) Expanding color flux tubes and instabilities
doi: 10.1016/j.nuclphysa.2008.05.016
2007FU17 J.Phys.(London) G34, S937 (2007) H.Fujii, F.Gelis, R.Venugopalan Heavy flavour production in pA collisions
doi: 10.1088/0954-3899/34/8/S130
2006FU14 Nucl.Phys. A780, 146 (2006) H.Fujii, F.Gelis, R.Venugopalan Quark pair production in high energy pA collisions: General features
doi: 10.1016/j.nuclphysa.2006.09.012
2006FU18 Nucl.Phys. A774, 793 (2006) H.Fujii, F.Gelis, R.Venugopalan Violation of kperp factorization in quark production from the Color Glass Condensate
doi: 10.1016/j.nuclphysa.2006.06.137
2005FU09 Eur.Phys.J. C 43, 139 (2005) H.Fujii, F.Gelis, R.Venugopalan Quark production in high-energy proton-nucleus collisions
doi: 10.1140/epjc/s2005-02232-y
2005HA52 Prog.Theor.Phys.(Kyoto) 114, 595 (2005) Effective Potential Study of the Chiral Phase Transition in a QCD-Like Theory
doi: 10.1143/PTP.114.595
2004OH15 Prog.Theor.Phys.(Kyoto), Suppl. 156, 167 (2004) Sigma and Hydrodynamic Modes near the Critical End Point
doi: 10.1143/PTPS.156.167
2003FU04 Phys.Rev. C 67, 031901 (2003) J/ψ suppression in heavy ion collisions by quark momentum diffusion NUCLEAR REACTIONS Pb(Pb, X), E=high; calculated J/ψ yield. Quark momentum diffusion, comparison with data.
doi: 10.1103/PhysRevC.67.031901
2003FU20 Prog.Theor.Phys.(Kyoto), Suppl. 151, 127 (2003) Quarkonium in Heavy Ion Collisions - High-Energy Multiple Scattering of Quark Pair in Nuclei -
doi: 10.1143/PTPS.151.127
2002FU15 Nucl.Phys. A709, 236 (2002) Penetration of a High Energy Q(Q-bar) Bound State Through SU(N) Color Background
doi: 10.1016/S0375-9474(02)01072-2
1999FU11 Nucl.Phys. A661, 542c (1999) Interactions of Quarkonium at Low Energies
doi: 10.1016/S0375-9474(99)85085-4
1999MA94 Prog.Theor.Phys.(Kyoto) 102, 809 (1999) T.Maruyama, H.Shin, H.Fujii, T.Tatsumi K+(K0)-Condensation in Highly Dense Matter with the Relativistic Mean-Field Theory
doi: 10.1143/PTP.102.809
1997SH44 Prog.Theor.Phys.(Kyoto) 98, 1139 (1997) Dilepton Production from Meson Condensed Matter
doi: 10.1143/PTP.98.1139
1996FU01 Nucl.Phys. A597, 645 (1996) H.Fujii, T.Maruyama, T.Muto, T.Tatsumi Equation of State with Kaon Condensates and Neutron Stars
doi: 10.1016/0375-9474(95)00451-3
1994FU02 Nucl.Phys. A571, 758 (1994) H.Fujii, T.Muto, T.Tatsumi, R.Tamagaki Effects of Weak Interaction on Kaon Condensation and Cooling of Neutron Stars
doi: 10.1016/0375-9474(94)90719-6
1994FU10 Phys.Rev. C50, 3140 (1994) H.Fujii, T.Muto, T.Tatsumi, R.Tamagaki Effects of Symmetry Energy on the Direct URCA Process in the Kaon Condensed Phase
doi: 10.1103/PhysRevC.50.3140
1994MA49 Phys.Lett. 337B, 19 (1994) T.Maruyama, H.Fujii, T.Muto, T.Tatsumi Kaon Condensation and Equation of State in the Relativistic Mean-Field Theory
doi: 10.1016/0370-2693(94)91436-2
1991KO33 J.Phys.Soc.Jpn. 60, 2546 (1991) K.Kojima, Y.Hukuda, S.Miyata, T.Takabatake, H.Fujii, T.Hihara 119Sn NMR Study of Heavy Fermion Compound U3Ni3Sn4 NUCLEAR MOMENTS 119Sn; measured NMR; deduced Knight shift, spin-lattice relaxation time.
doi: 10.1143/JPSJ.60.2546
1989TA08 Nucl.Instrum.Methods Phys.Res. A274, 345 (1989) Nuclide Identification of β-Emitter by a Double Ratio Technique Using a Liquid Scintillation Counter RADIOACTIVITY 3H, 14C, 32P(β-); 36Cl(β-), (β+), (EC); 63Ni, 35S, 45Ca(β-); measured β-activity; deduced quenching correction role in nuclide identification. Computer aided quenching correction, liquid scintillation double ratio technique.
doi: 10.1016/0168-9002(89)90400-2
1986TA19 Nucl.Instrum.Methods Phys.Res. A251, 574 (1986) Liquid Scintillation Technique for the Determination of the Thermal Neutron Flux Density Due to 59Co and 197Au Monitors NUCLEAR REACTIONS 59Co, 197Au(n, γ), E=thermal; measured Eγ, Iγ; deduced neutron flux densities. Liquid scintillation counter, activation technique.
doi: 10.1016/0168-9002(86)90653-4
1985IW01 Nucl.Phys. A433, 580 (1985) H.Iwasaki, H.Aihara, J.Chiba, H.Fujii, T.Fujii, T.Kamae, K.Nakamura, T.Sumiyoshi, Y.Takada, T.Takeda, M.Yamauchi, H.Fukuma Small-Angle (pol)p Elastic Scattering and the Real-to-Imaginary Ratio of the Forward Amplitude between 413 and 715 MeV/c NUCLEAR REACTIONS 1H(p-bar, p-bar), E at 413-715 MeV/c; measured σ(θ≤10°); deduced real to imaginary amplitude ratio.
doi: 10.1016/0375-9474(85)90019-3
1981AI01 Nucl.Phys. A360, 291 (1981) H.Aihara, J.Chiba, H.Fujii, T.Fujii, H.Iwasaki, T.Kamae, K.Nakamura, T.Sumiyoshi, Y.Takada, T.Takeda, M.Yamauchi, H.Fukuma Absorption Cross Sections for Antiprotons on Carbon, Aluminum and Copper at 485 and 597 MeV/c NUCLEAR REACTIONS 12C, 27Al, Cu(p-bar, X), E=118, 174 MeV; measured σ(absorption). Transmission method, natural targets.
doi: 10.1016/0375-9474(81)90147-0
1980IK01 Nucl.Phys. B172, 509 (1980) H.Ikeda, I.Arai, H.Fujii, T.Fujii, H.Iwasaki, N.Kajiura, T.Kamae, K.Nakamura, T.Sumiyoshi, H.Takeda, K.Ogawa, M.Kanazawa Further Measurement of Proton Polarization in Deuteron Photodisintegration at Photon Energies between 400 and 650 MeV: Possible evidence for dibaryon resonances NUCLEAR REACTIONS 2H(γ, p), E=400-650 MeV bremsstrahlung; measured proton polarization P(θ), σ(θp); deduced possible dibaryon resonances.
doi: 10.1016/0550-3213(80)90181-9
1979BA22 Nucl.Phys. A322, 349 (1979) K.Baba, I.Endo, M.Fujisaki, S.Kadota, Y.Sumi, H.Fujii, Y.Murata, S.Noguchi, A.Murakami Quasi-Free Photoproduction of Charged Pions from Copper and Lead NUCLEAR REACTIONS Cu, Pb(γ, π+), (γ, π-), E=418-668 MeV; measured production σ.
doi: 10.1016/0375-9474(79)90430-5
1979IK01 Phys.Rev.Lett. 42, 1321 (1979) H.Ikeda, I.Arai, H.Fujii, T.Fujii, H.Iwasaki, N.Kajiura, T.Kamae, K.Nakamura, T.Sumiyoshi, H.Takeda, K.Ogawa, M.Kanazawa Angular Dependence of Proton Polarization in the Reaction γd → pn And a Partial-Wave Analysis of Possible Dibaryon Resonances NUCLEAR REACTIONS 2H(γ, p), E=400-650 MeV; measured σ(θp), P(θp); deduced possible dibaryon resonance. Partial wave analysis.
doi: 10.1103/PhysRevLett.42.1321
1979MA18 J.Phys.Soc.Jpn. 46, 1403 (1979) K.Maruyama, H.Fujii, S.Homma, H.Okuno, N.Yamashita, I.Arai, H.Ikeda, A.Itano, E.Ohshima, Y.Hoshi, T.Ishii, A.Sasaki Photoproduction of Positive and Negative Pions from Protons in the Energy Range from 710 MeV to 950 MeV NUCLEAR REACTIONS 1H(γ, 2π+), (γ, 2π-), E=710-950 MeV; measured momentum spectra; deduced production σ for Δ. Gauge invariant one pion exchange model.
doi: 10.1143/JPSJ.46.1403
1978AR08 J.Phys.Soc.Jpn. 45, 1 (1978) I.Arai, H.Fujii, S.Homma, Y.Hoshi, H.Ikeda, T.Ishii, A.Itano, K.Maruyama, E.Ohshima, H.Okuno, A.Sasaki, N.Yamashita Photoproduction of Negative Pions from Carbon in the Energy Range between 510 MeV and 750 MeV NUCLEAR REACTIONS C(γ, π-), E=510-750 MeV; measured σ(E).
doi: 10.1143/JPSJ.45.1
1978BA50 Nucl.Phys. A306, 292 (1978) K.Baba, I.Endo, M.Fujisaki, S.Kadota, Y.Sumi, H.Fujii, Y.Murata, S.Noguchi, A.Murakami Quasi-Free Pion Photoproduction from Carbon Above 300 MeV NUCLEAR REACTIONS 12C(γ, π+), (γ, π-), E=300-850 MeV; measured σ(E, Eπ, θ). PWIA calculations.
doi: 10.1016/0375-9474(78)90466-9
1977AR14 J.Phys.Soc.Jap. 43, 363 (1977) I.Arai, H.Fujii, S.Homma, Y.Hoshi, H.Ikeda, T.Ishii, A.Itano, K.Maruyama, E.Ohshima, H.Okuno, A.Sasaki, N.Yamashita Differential Cross Sections for Single Pion Photoproduction from Protons in the Energy Range between 500 MeV and 930 MeV NUCLEAR REACTIONS 1H(γ, π0p), (γ, π+n), E=500-930 MeV; measured σ.
doi: 10.1143/JPSJ.43.363
1977BA60 J.Phys.Soc.Jap. 42, 1049 (1977) K.Baba, I.Endo, H.Fujii, M.Fujisaki, S.Kadota, A.Murakami, Y.Murata, S.Noguchi, Y.Sumi Experimental Study of Inclusive Reaction 12C(γ, π-) at 44.2 Degrees NUCLEAR REACTIONS 12C(γ, π+), (γ, π-), E=300-850 MeV; measured σ(E).
doi: 10.1143/JPSJ.42.1049
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