NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = T.Maruyama Found 90 matches. 2023NA22 Phys.Rev. C 108, 024910 (2023) Y.Nara, A.Jinno, T.Maruyama, K.Murase, A.Ohnishi Poincare covariant cascade method for high-energy nuclear collisions
doi: 10.1103/PhysRevC.108.024910
2022XI02 Phys.Rev. C 105, 045803 (2022) C.-J.Xia, B.Y.Sun, T.Maruyama, W.-H.Long, A.Li Unified nuclear matter equations of state constrained by the in-medium balance in density-dependent covariant density functionals ATOMIC MASSES A=20-260; calculated binding energies, energy per baryon of finite nuclei. Thomas-Fermi approximation framework with two covariant density functionals DD-LZ1 and DD-ME2. Comparison with data from AME2016.
doi: 10.1103/PhysRevC.105.045803
2021XI04 Phys.Rev. C 103, 055812 (2021) C.-J.Xia, T.Maruyama, N.Yasutake, T.Tatsumi, Y.-X.Zhang Nuclear pasta structures and symmetry energy NUCLEAR STRUCTURE 208Pb; calculated symmetry energy and its slope of nuclear matter, neutron skin thickness, proton and neutron density profiles using Thomas-Fermi approximation. Investigated nuclear pasta structures in a three-dimensional geometry with reflection symmetry using RMF model with Thomas-Fermi approximation; deduced similarity of droplets and bubbles in body-centered cubic (bcc) and face-centered cubic (fcc) lattices, with impact on properties of neutron stars, supernova dynamics, and binary neutron star mergers.
doi: 10.1103/PhysRevC.103.055812
2020NA26 Phys.Rev. C 102, 024913 (2020) Y.Nara, T.Maruyama, H.Stoecker Momentum-dependent potential and collective flows within the relativistic quantum molecular dynamics approach based on relativistic mean-field theory
doi: 10.1103/PhysRevC.102.024913
2019MA60 Phys.Rev. C 100, 025802 (2019) K.Maslov, N.Yasutake, D.Blaschke, A.Ayriyan, H.Grigorian, T.Maruyama, T.Tatsumi, D.N.Voskresensky Hybrid equation of state with pasta phases, and third family of compact stars
doi: 10.1103/PhysRevC.100.025802
2015CH18 J.Phys.(London) G42, 345102 (2015) M.-K.Cheoun, K.S.Kim, H.Kim, W.Y.So, T.Maruyama, T.Kajino In-medium effect with muon-neutrino and anti-muon-neutrino quasi-elastic scattering from 12C nucleons
doi: 10.1088/0954-3899/42/4/045102
2014MA13 Phys.Rev. C 89, 035801 (2014) T.Maruyama, J.Hidaka, T.Kajino, N.Yasutake, T.Kuroda, T.Takiwaki, M.-K.Cheoun, C.-Y.Ryu, G.J.Mathews Rapid spin deceleration of magnetized protoneutron stars via asymmetric neutrino emission
doi: 10.1103/PhysRevC.89.035801
2014YA13 Phys.Rev. C 89, 065803 (2014) N.Yasutake, R.Lastowiecki, S.Benic, D.Blaschke, T.Maruyama, T.Tatsumi Finite-size effects at the hadron-quark transition and heavy hybrid stars
doi: 10.1103/PhysRevC.89.065803
2013CH40 Phys.Rev. C 87, 065502 (2013) M.K.Cheoun, K.S.Choi, K.S.Kim, K.Saito, T.Kajino, K.Tsushima, T.Maruyama Effects of the density-dependent weak form factors on the neutrino reaction via neutral current for the nucleon in nuclear matter and 12C NUCLEAR REACTIONS 12C(ν, ν'), (ν-bar, ν-bar'), E<80 MeV; calculated density-dependent form factors for electron neutrino and electron antineutrino collisions with 12C, σ(E). Large asymmetry in the antineutrino cross sections due to difference in helicities of neutrino and antineutrino. Quark-meson-coupling (QMC) model.
doi: 10.1103/PhysRevC.87.065502
2013MA52 J.Phys.:Conf.Ser. 445, 012023 (2013) G.J.Mathews, M.Meixner, J.P.Olson, I.-S.Suh, T.Kajino, T.Maruyama, J.Hidaka, C.-Y.Ryu, M.-K.Cheoun, N.Q.Lan Updates of the nuclear equation of state for core-collapse supernovae and neutron stars: effects of 3-body forces, QCD, and magnetic fields
doi: 10.1088/1742-6596/445/1/012023
2013OK01 Phys.Rev. C 88, 025801 (2013) M.Okamoto, T.Maruyama, K.Yabana, T.Tatsumi Nuclear "pasta" structures in low-density nuclear matter and properties of the neutron-star crust
doi: 10.1103/PhysRevC.88.025801
2012RY01 Phys.Rev. C 85, 045803 (2012) C.-Y.Ryu, T.Maruyama, T.Kajino, G.J.Mathews, M.-K.Cheoun Spin change of a proto-neutron star by the emission of neutrinos
doi: 10.1103/PhysRevC.85.045803
2011MA83 J.Phys.:Conf.Ser. 312, 042015 (2011) Liquid-gas mixed phase in nuclear matter at finite temperature
doi: 10.1088/1742-6596/312/4/042015
2011RY01 Phys.Rev. C 83, 018802 (2011) C.Y.Ryu, T.Maruyama, T.Kajino, M.-K.Cheoun Properties of a proto-neutron star with smeared trapped neutrinos
doi: 10.1103/PhysRevC.83.018802
2011YA24 J.Phys.:Conf.Ser. 312, 042027 (2011) N.Yasutake, T.Maruyama, T.Tatsumi Pasta Structures of Quark-Hadron Phase Transition in Proto-Neutron Stars
doi: 10.1088/1742-6596/312/4/042027
2010MA46 Nucl.Phys. A834, 561c (2010) T.Maruyama, T.Tatsumi, S.Chiba Liquid-gas phase transition in asymmetric nuclear matter at finite temperature
doi: 10.1016/j.nuclphysa.2010.01.091
2010MU15 Nucl.Phys. A835, 370c (2010) Effects of the Λ(1405) on the Structure of Multi-Antikaonic Nuclei NUCLEAR STRUCTURE 15O; calculated K- hypernucleus density distribution, binding energy.
doi: 10.1016/j.nuclphysa.2010.01.221
2009MA04 Phys.Rev. C 79, 014614 (2009) D.Mancusi, K.Niita, T.Maruyama, L.Sihver Stability of nuclei in peripheral collisions in the JAERI quantum molecular dynamics model NUCLEAR REACTIONS 40Ca(40Ca, 40Ca), E=1 GeV/nucleon; 56Fe(p, xn), E=113 MeV; 208Pb(p, xn), E=3 GeV; Al(56Fe, X), E=1 GeV; calculated σ(θ). R-JAERI quantum molecular dynamics model. Comparisons with JAERI quantum molecular dynamics model and experimental data.
doi: 10.1103/PhysRevC.79.014614
2009MU03 Phys.Rev. C 79, 035207 (2009) Multi-antikaonic nuclei in relativistic mean-field theory NUCLEAR STRUCTURE 15O; calculated density distribution of protons and neutrons, distribution of strangeness density, chiral angle at center of multi-antikaonic nuclei, baryon number density, Coulomb energy, sign-reversed binding energy per strangeness, effective mass of K-, lowest K- energy. Relativistic mean-field theory, chiral symmetry.
doi: 10.1103/PhysRevC.79.035207
2008CH05 Phys.Rev. C 77, 015809 (2008) S.Chiba, H.Koura, T.Hayakawa, T.Maruyama, T.Kawano, T.Kajino Direct and semi-direct capture in low-energy (n, γ) reactions of neutron-rich tin isotopes and its implications for r-process nucleosynthesis NUCLEAR REACTIONS 16O(n, γ), E=0.01-10 MeV; 124,126,128,130,134,136,138Sn(n, γ), E=30 keV; 122Sn(n, γ), E=1 keV-20 MeV; 208Pb(n, γ), E=0-20 MeV; calculated neutron capture cross sections. 132Sn(n, γ), E=1 keV-20 MeV; calculated neutron capture cross sections, reaction rates. 132,133Sn; calculated levels, J, π, compared with experiment.
doi: 10.1103/PhysRevC.77.015809
2006EN01 Prog.Theor.Phys.(Kyoto) 115, 337 (2006) T.Endo, T.Maruyama, S.Chiba, T.Tatsumi Charge Screening Effect in the Hadron-Quark Mixed Phase
doi: 10.1143/PTP.115.337
2006KI09 Phys.Lett. B 639, 429 (2006) T.Kinoshita, H.Yamazaki, H.Fukasawa, K.Hirota, T.Ishikawa, J.Kasagi, A.Kato, T.Katsuyama, K.Kino, F.Miyahara, T.Nakabayashi, K.Nawa, K.Okamura, Y.Saitoh, K.Satou, M.Sengoku, H.Shimizu, K.Suzuki, S.Suzuki, T.Terasawa, H.Kanda, K.Maeda, T.Takahashi, Y.Aruga, T.Fujinoya, A.Iijima, M.Itaya, Y.Ito, T.Iwata, H.Kato, T.Kawamura, T.Michigami, M.Moriya, T.Sasaki, Y.Tajima, S.Takita, T.Noma, M.Yamamoto, H.Y.Yoshida, Y.Yoshida, O.Konno, T.Maruyama, T.Yorita Photoproduction of η-mesons off C and Cu nuclei for photon energies below 1.1 GeV NUCLEAR REACTIONS C, Cu(γ, X), E=600-1100 MeV; measured total η production σ, σ(θ), invariant mass spectra; deduced resonance features. Comparison with other results and model calculations.
doi: 10.1016/j.physletb.2006.05.088
2006MA19 Phys.Rev. C 73, 035802 (2006) T.Maruyama, T.Tatsumi, D.N.Voskresensky, T.Tanigawa, T.Endo, S.Chiba Finite size effects on kaonic "pasta" structures
doi: 10.1103/PhysRevC.73.035802
2006MA40 Phys.Rev. C 74, 014315 (2006) Nuclear electromagnetic current in the relativistic approach with the momentum-dependent self-energies
doi: 10.1103/PhysRevC.74.014315
2006TA29 Nucl.Phys. A774, 827 (2006) T.Tatsumi, T.Maruyama, E.Nakano, K.Nawa Ferromagnetism in quark matter and origin of the magnetic field in compact stars
doi: 10.1016/j.nuclphysa.2006.06.145
2005AK05 Nucl.Phys. A749, 329c (2005) Y.Akimura, T.Maruyama, N.Yoshinaga, S.Chiba Stability and structure of quark matter in a molecular dynamics framework
doi: 10.1016/j.nuclphysa.2004.12.062
2005AK11 Eur.Phys.J. A 25, 405 (2005) Y.Akimura, T.Maruyama, N.Yoshinaga, S.Chiba Molecular dynamics simulation for the baryon-quark phase transition at finite baryon density
doi: 10.1140/epja/i2005-10143-x
2005EN02 Nucl.Phys. A749, 333c (2005) T.Endo, T.Maruyama, S.Chiba, T.Tatsumi Numerical study of the hadron-quark mixed phase
doi: 10.1016/j.nuclphysa.2004.12.063
2005MA12 Prog.Theor.Phys.(Kyoto) 113, 355 (2005) T.Maruyama, H.Kurasawa, T.Suzuki Role of the Landau-Migdal Parameters with the Pseudovector and Tensor Couplings in Relativistic Nuclear Models - The Quenching of the Gamow-Teller Strength -
doi: 10.1143/PTP.113.355
2005MA15 Nucl.Phys. A749, 186c (2005) T.Maruyama, T.Tatsumi, D.N.Voskresensky, T.Tanigawa, S.Chiba Structured mixed phase at charged kaon condensation
doi: 10.1016/j.nuclphysa.2004.12.031
2005MA56 Phys.Rev. C 72, 015802 (2005) T.Maruyama, T.Tatsumi, D.N.Voskresensky, T.Tanigawa, S.Chiba Nuclear "pasta" structures and the charge screening effect
doi: 10.1103/PhysRevC.72.015802
2005MA78 Nucl.Phys. A760, 319 (2005) T.Maruyama, T.Muto, T.Tatsumi, K.Tsushima, A.W.Thomas Kaon condensation and lambda-nucleon loop in the relativistic mean-field approach
doi: 10.1016/j.nuclphysa.2005.06.008
2004MA27 Prog.Theor.Phys.(Kyoto) 111, 229 (2004) In-Medium Effects in Eta Photo-Production through the S11 Resonance in the Relativistic Approach NUCLEAR REACTIONS 1H, 12C(γ, X), E ≈ threshold; calculated η production σ; deduced medium effects.
doi: 10.1143/PTP.111.229
2004MB02 Prog.Theor.Phys.(Kyoto), Suppl. 156, 145 (2004) T.Maruyama, T.Tatsumi, D.N.Voskresensky, T.Tanigawa, S.Chiba, T.Maruyama Structured Mixed Phase in Kaon Condensation
doi: 10.1143/PTPS.156.145
2003MA59 Nucl.Phys. A721, 265c (2003) Ferromagnetism of Nuclear Matter in the Relativistic Approach
doi: 10.1016/S0375-9474(03)01046-7
2003MA64 Nucl.Phys. A721, 697c (2003) The Eta-Photoproduction in the Relativistic Approach NUCLEAR REACTIONS 1H, 12C(γ, X), E=high; calculated η meson production σ, in-medium effects. Relativistic mean field approach.
doi: 10.1016/S0375-9474(03)01155-2
2003PA32 Phys.Rev. C 68, 034606 (2003) M.Papa, A.Bonanno, F.Amorini, A.Bonasera, G.Cardella, A.Di Pietro, P.P.Figuera, T.Maruyama, G.Pappalardo, F.Rizzo, S.Tudisco Coherent and incoherent giant dipole resonance γ-ray emission induced by heavy ion collisions: Study of the 40Ca + 48Ca system by means of the constrained molecular dynamics model NUCLEAR REACTIONS 46Ti, 48Ca(40Ca, X), E=25, 35, 50 MeV/nucleon; calculated coherent and incoherent Eγ, Iγ, fragment yields. Constrained molecular dynamics model.
doi: 10.1103/PhysRevC.68.034606
2002HI14 Nucl.Phys. A707, 193 (2002) Y.Hirata, A.Ohnishi, Y.Nara, T.Kido, T.Maruyama, N.Otuka, K.Niita, H.Takada, S.Chiba Sideward Peak of Intermediate Mass Fragments in High Energy Proton Induced Reactions NUCLEAR REACTIONS 197Au(p, X), E=12 GeV; calculated fragments energy, angle, and mass distributions; deduced intermediate mass fragment formation and sideward enhancement mechanism features. Transport and nonequilibrated percolation models.
doi: 10.1016/S0375-9474(02)00747-9
2002MA42 Eur.Phys.J. A 14, 191 (2002) T.Maruyama, A.Bonasera, M.Papa, S.Chiba Formation and Decay of Super-Heavy Systems NUCLEAR REACTIONS 197Au(197Au, X), E=5-35 MeV/nucleon; calculated large fragments survival probabilities, fission lifetimes, fission mass asymmetry. Possibilities of forming super heavy nuclei discussed, Constrained Molecular Dynamics model.
doi: 10.1140/epja/i2001-10196-9
2002MA76 Prog.Theor.Phys.(Kyoto), Suppl. 146, 587 (2002) T.Maruyama, A.Bonasera, M.Papa, S.Chiba Formation and Decay of Super Heavy Systems NUCLEAR REACTIONS 197Au(197Au, X), E ≈ 8-40 MeV/nucleon; calculated averaged fission time of compound system, fragment mass asymmetry.
doi: 10.1143/PTPS.146.587
2002MA87 J.Nucl.Radiochem.Sci. 3, No 1, 77 (2002) T.Maruyama, A.Bonasera, M.Papa, S.Chiba Lifetime of Heavy Composite Systems Formed by Fusion between Heavy Nuclei NUCLEAR REACTIONS 197Au(197Au, X), E ≈ 5-35 MeV/nucleon; calculated composite system lifetime, fission fragment survival probabilities, mass distributions. Constrained molecular dynamics.
2002PA54 Acta Phys.Hung.N.S. 16, 223 (2002) M.Papa, A.Bonasera, G.Cardella, T.Maruyama Constraint Molecular Dynamics and Results on Isotopic Distributions Produced in Heavy Ion Collision - The Sn + Ni Systems NUCLEAR REACTIONS 64Ni(124Sn, X), 58Ni(112Sn, X), E=35 MeV/nucleon; analyzed fragment charge, mass, and multiplicity distributions; deduced dynamic effects. Constraint molecular dynamics approach.
doi: 10.1556/APH.16.2002.1-4.25
2002SU21 J.Nucl.Sci.Technol.(Tokyo) 39, 816 (2002) E.S.Sukhovitsky, S.Chiba, J.-Y.Lee, Y.-O.Lee, J.Chang, T.Maruyama, O.Iwamoto Nuclear Level Structure, B(E2) Gamma-Transitions and Nucleon Interaction Data for 56Fe by a Unified Soft-Rotator Model and Couple-Channels Framework NUCLEAR STRUCTURE 56Fe; calculated levels, J, π, B(E2). Soft-rotator model, comparison with data. NUCLEAR REACTIONS 56Fe(n, X), E < 160 MeV; calculated total neutron σ. 56Fe(n, n), E=8-75 MeV; 56Fe(n, n'), E=8-26 MeV; 56Fe(p, p), E=7-156 MeV; 56Fe(p, p'), E=7-62 MeV; calculated σ(θ). Coupled-channels approach, comparison with data.
2001CH06 Phys.Rev. C63, 024602 (2001) S.Chikazumi, T.Maruyama, S.Chiba, K.Niita, A.Iwamoto Quantum Molecular Dynamics Simulation of Expanding Nuclear Matter and Nuclear Multifragmentation
doi: 10.1103/PhysRevC.63.024602
2001MA13 Nucl.Phys. A681, 72c (2001) T.Maruyama, T.Hatsuda, S.Chiba Color Molecular Dynamics Simulation of Nuclei and Dense Matter
doi: 10.1016/S0375-9474(00)00483-8
2001MA41 Phys.Rev. C63, 057601 (2001) T.Maruyama, A.Bonasera, S.Chiba Nuclear Fragmentation by Tunneling NUCLEAR STRUCTURE 230U; calculated fragment mass distributions following fragmentation of excited nucleus. Tunneling mechanism, molecular dynamics simulation.
doi: 10.1103/PhysRevC.63.057601
2001MA72 Nucl.Phys. A693, 710 (2001) Ferromagnetism of Nuclear Matter in the Relativistic Approach
doi: 10.1016/S0375-9474(01)00811-9
2001PA30 Phys.Rev. C64, 024612 (2001) M.Papa, T.Maruyama, A.Bonasera Constrained Molecular Dynamics Approach to Fermionic Systems NUCLEAR REACTIONS 40Ca(40Ca, X), E=35 MeV/nucleon; 197Au(197Au, X), E=35 MeV/nucleon; calculated fragments isotopic distributions; deduced reaction mechanism features. Constrained molecular dynamics.
doi: 10.1103/PhysRevC.64.024612
2000CH05 Phys.Lett. 476B, 273 (2000) S.Chikazumi, T.Maruyama, K.Niita, A.Iwamoto QMD Simulation of Expanding Nuclear Matter
doi: 10.1016/S0370-2693(00)00161-1
2000KI10 Nucl.Phys. A663-664, 877c (2000) T.Kido, T.Maruyama, K.Niita, S.Chiba MD Simulation Study for Nuclear Matter
doi: 10.1016/S0375-9474(99)00736-8
2000KO03 Phys.Rev.Lett. 84, 1086 (2000) V.N.Kondratyev, T.Maruyama, S.Chiba Shell Structure of Nuclei in Strong Magnetic Fields in Neutron Star Crusts NUCLEAR STRUCTURE Z=8-42; A=16-90; calculated shell modifications due to strong magnetic fields. Strutinsky approach, astrophysical implications discussed.
doi: 10.1103/PhysRevLett.84.1086
2000MA10 Phys.Rev. C61, 037301 (2000) Isoscalar Giant Quadrupole Resonance State in a Relativistic Approach with the Momentum-Dependent Self-Energies
doi: 10.1103/PhysRevC.61.037301
2000MA40 Phys.Rev. C61, 062201 (2000) Color Molecular Dynamics for High Density Matter
doi: 10.1103/PhysRevC.61.062201
2000YA12 Nucl.Phys. A670, 202c (2000) H.Yamazaki, T.Yorita, T.Kinoshita, T.Okuda, H.Matsui, T.Maruyama, J.Kasagi, T.Suda, K.Itoh, T.Miyakawa, H.Okuno, H.Shimizu, H.Y.Yoshida, T.Kinashi Study of S11 Resonance in Nuclei Through (γ, η) Reactions NUCLEAR REACTIONS C, 27Al, Cu(γ, X), E=680-1000 MeV; measured total η production σ; deduced resonance features.
doi: 10.1016/S0375-9474(00)00099-3
2000YO02 Phys.Lett. 476B, 226 (2000) T.Yorita, H.Yamazaki, T.Kinoshita, T.Okuda, H.Matsui, J.Kasagi, T.Suda, K.Itoh, T.Miyakawa, H.Okuno, H.Shimizu, H.Y.Yoshida, T.Kinashi, T.Maruyama Observation of S11(1535) Resonance in Nuclear Medium via the 12C(γ, η) Reaction NUCLEAR REACTIONS 12C(γ, X), E=0.68-1.0 GeV; measured η meson associated σ, σ(θ); deduced in-medium S11 resonance properties.
doi: 10.1016/S0370-2693(00)00176-3
1999MA90 J.Phys.(London) G25, 2361 (1999) Equation of State of Neutron-Star Matter and the Isovector Nucleon Optical Model Potential
doi: 10.1088/0954-3899/25/12/306
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
1999MB10 Nucl.Phys. (Supplement) A654, 908c (1999) T.Maruyama, K.Niita, K.Oyamatsu, T.Maruyama, S.Chiba, A.Iwamoto Nuclear Matter Structure Studied with Quantum Molecular Dynamics
doi: 10.1016/S0375-9474(00)88570-X
1998MA04 Phys.Rev. C57, 655 (1998) T.Maruyama, K.Niita, K.Oyamatsu, T.Maruyama, S.Chiba, A.Iwamoto Quantum Molecular Dynamics Approach to the Nuclear Matter Below the Saturation Density
doi: 10.1103/PhysRevC.57.655
1997MA52 Prog.Theor.Phys.(Kyoto) 97, 579 (1997) Multifragmentation Through Exotic Shape Nuclei in α(5 GeV/u) + Au Collisions NUCLEAR REACTIONS 197Au(α, X), E=5 GeV/nucleon; calculated light, intermediate fragments σ(θ); deduced annular intermediate shape. Quantum molecular dynamics approach.
doi: 10.1143/PTP.97.579
1997MA71 Prog.Theor.Phys.(Kyoto) 98, 87 (1997) T.Maruyama, K.Niita, T.Maruyama, A.Iwamoto On the IMF Multiplicity in Au + Au Reactions NUCLEAR REACTIONS 197Au(197Au, X), E=100, 250, 400 MeV/nucleon; calculated intermediate mass fragment multiplicity distributions. Quantum molecular dynamics approach, evaporation model. Comparison with data.
doi: 10.1143/PTP.98.87
1996AB02 Phys.Rev.Lett. 76, 587 (1996) K.Abe, T.Akagi, P.L.Anthony, R.Antonov, R.G.Arnold, T.Averett, H.R.Band, J.M.Bauer, H.Borel, P.E.Bosted, V.Breton, J.Button-Shafer, J.P.Chen, T.E.Chupp, J.Clendenin, C.Comptour, K.P.Coulter, G.Court, D.Crabb, M.Daoudi, D.Day, F.S.Dietrich, J.Dunne, H.Dutz, R.Erbacher, J.Fellbaum, A.Feltham, H.Fonvieille, E.Frlez, D.Garvey, R.Gearhart, J.Gomez, P.Grenier, K.A.Griffioen, S.Hoibraten, E.W.Hughes, C.Hyde-Wright, J.R.Johnson, D.Kawall, A.Klein, S.E.Kuhn, M.Kuriki, R.Lindgren, T.J.Liu, R.M.Lombard-Nelsen, J.Marroncle, T.Maruyama, X.K.Maruyama, J.McCarthy, W.Meyer, Z.-E.Meziani, R.Minehart, J.Mitchell, J.Morgenstern, G.G.Petratos, R.Pitthan, D.Pocanic, C.Prescott, R.Prepost, P.Raines, B.Raue, D.Reyna, A.Rijllart, Y.Roblin, L.S.Rochester, S.E.Rock, O.A.Rondon, I.Sick, L.C.Smith, T.B.Smith, M.Spengos, F.Staley, P.Steiner, S.St.Lorant, L.M.Stuart, F.Suekane, Z.M.Szalata, H.Tang, Y.Terrien, T.Usher, D.Walz, J.L.White, K.Witte, C.C.Young, B.Youngman, H.Yuta, G.Zapalac, B.Zihlmann, D.Zimmermann, and the E143 Collaboration Measurements of the Proton and Deuteron Spin Structure Function g2 and Asymmetry A2 NUCLEAR STRUCTURE 1,2H; analyzed data; deduced spin structure function, asymmetry data. Polarized ammonia targets, (polarized e, e') reaction. NUCLEAR REACTIONS 1,2H(polarized e, e'), E=29.1 GeV; measured spin asymmetries. 1,2H deduced spin structure functions. Polarized ammonia targets.
doi: 10.1103/PhysRevLett.76.587
1996CH10 Phys.Rev. C53, 1824 (1996) S.Chiba, M.B.Chadwick, K.Niita, T.Maruyama, T.Maruyama, A.Iwamoto Nucleon-Induced Preequilibrium Reactions in Terms of the Quantum Molecular Dynamics NUCLEAR REACTIONS 58Ni(p, xp), E=120, 200 MeV; 90Zr(p, xp), (p, xn), E=160 MeV; 27Al(p, xp), (p, xn), E=90 MeV; 90Zr(p, xn), E=160 MeV; analyzed σ(θ, E(nucleon)); deduced multiple pre-equilibrium particle emission role. Quantum molecular dynamics approach.
doi: 10.1103/PhysRevC.53.1824
1996CH15 Phys.Rev. C54, 285 (1996) S.Chiba, O.Iwamoto, T.Fukahori, K.Niita, T.Maruyama, T.Maruyama, A.Iwamoto Analysis of Proton-Induced Fragment Production Cross Sections by the Quantum Molecular Dynamics Plus Statistical Decay Model NUCLEAR REACTIONS, ICPND 56Fe(p, n), (p, 3n2p), (p, 3n3p), (p, 5n4p), (p, 3n6p), (p, 4n6p), (p, 5n6p), (p, 6n8p), E=threshold-5 GeV; 27Al(p, n3p), (p, 3n3p), (p, 5n5p), (p, 11n10p), E ≤ 6 GeV; analyzed residuals production σ(E). Quantum molecular dynamics plus statistical decay models.
doi: 10.1103/PhysRevC.54.285
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
1996MA02 Phys.Rev. C53, 297 (1996) T.Maruyama, K.Niita, A.Iwamoto Extension of Quantum Molecular Dynamics and Its Application to Heavy-Ion Collisions NUCLEAR STRUCTURE 12C, 93Nb, 197Au; calculated density distribution, Gaussian widths. NUCLEAR REACTIONS, ICPND 12C(12C, X), E=29 MeV/nucleon; 27Al(40Ar, X), E=44 MeV/nucleon; calculated σ vs fragment mass. 16O(16O, X), E ≤ 200 MeV; calculated fusion σ(E). Extended quantum molecular dynamics method.
doi: 10.1103/PhysRevC.53.297
1995AB02 Phys.Rev.Lett. 74, 346 (1995) K.Abe, T.Akagi, P.L.Anthony, R.Antonov, R.G.Arnold, T.Averett, H.R.Band, J.M.Bauer, H.Borel, P.E.Bosted, V.Breton, J.Button-Shafer, J.P.Chen, T.E.Chupp, J.Clendenin, C.Comptour, K.P.Coulter, G.Court, D.Crabb, M.Daoudi, D.Day, F.S.Dietrich, J.Dunne, H.Dutz, R.Erbacher, J.Fellbaum, A.Feltham, H.Fonvieille, E.Frlez, D.Garvey, R.Gearhart, J.Gomez, P.Grenier, K.A.Griffioen, S.Hoibraten, E.W.Hughes, C.Hyde-Wright, J.R.Johnson, D.Kawall, A.Klein, S.E.Kuhn, M.Kuriki, R.Lindgren, T.J.Liu, R.M.Lombard-Nelsen, J.Marroncle, T.Maruyama, X.K.Maruyama, J.McCarthy, W.Meyer, Z.-E.Meziani, R.Minehart, J.Mitchell, J.Morgenstern, G.G.Petratos, R.Pitthan, D.Pocanic, C.Prescott, R.Prepost, P.Raines, B.Raue, D.Reyna, A.Rijllart, Y.Roblin, L.S.Rochester, S.E.Rock, O.A.Rondon, I.Sick, L.C.Smith, T.B.Smith, M.Spengos, F.Staley, P.Steiner, S.St.Lorant, L.M.Stuart, F.Suekane, Z.M.Szalata, H.Tang, Y.Terrien, T.Usher, D.Walz, J.L.White, K.Witte, C.C.Young, B.Youngman, H.Yuta, G.Zapalac, B.Zihlmann, D.Zimmermann, and the E143 Collaboration Precision Measurement of the Proton Spin Structure Function g1(p) NUCLEAR REACTIONS 1H(polarized e, e'), E=9.7-29.1 GeV; measured asymmetry. 1H deduced spin structure function g1(p). Polarized 15NH3 target.
doi: 10.1103/PhysRevLett.74.346
1995CH49 Phys.Rev. C52, 2800 (1995) M.B.Chadwick, S.Chiba, K.Niita, T.Maruyama, A.Iwamoto Quantum Molecular Dynamics and Multistep-Direct Analyses of Multiple Preequilibrium Emission NUCLEAR REACTIONS 90Zr(p, xp), E=160 MeV; calculated angle-integrated σ for primary, multiple preequilibrium emission. Quantum molecular dynamics, multi-step direct analysis.
doi: 10.1103/PhysRevC.52.2800
1995EN06 Phys.Rev. C52, 3231 (1995) A.Engel, E.I.Tanaka, T.Maruyama, A.Ono, H.Horiuchi Δ Degrees of Freedom in Antisymmetrized Molecular Dynamics and (p, p') Reactions in the Δ Region NUCLEAR REACTIONS 12C(p, p'), E=800 MeV; measured σ(θ) vs momentum. One-step Monte Carlo calculations, antisymmetrized molecular dynamics, Δ degrees of freedom.
doi: 10.1103/PhysRevC.52.3231
1995MA72 Phys.Lett. 358B, 34 (1995) T.Maruyama, T.Maruyama, K.Niita Relativistic Effects in Simulations of the Fragmentation Process with the Microscopic Framework NUCLEAR REACTIONS Ca(Ca, X), E=1.05 GeV/nucleon; calculated p-, α-multiplicities vs impact parameter, fragment production σ vs mass, relativistic effects. Statistical decay model, Lorentz covariant RQMD, noncovariant QMD approaches.
doi: 10.1016/0370-2693(95)00976-R
1995NI12 Phys.Rev. C52, 2620 (1995) K.Niita, S.Chiba, T.Maruyama, T.Maruyama, H.Takada, T.Fukahori, Y.Nakahara, A.Iwamoto Analysis of the (N, xN') Reactions by Quantum Molecular Dynamics Plus Statistical Decay Model NUCLEAR REACTIONS 1n, 1H(p, X), E=0.5-3 GeV; calculated elastic, inelastic, total, pion production σ(E). 27Al(p, xp), (p, xπ-), E=3.17 GeV; 56Fe(p, xn), E=113, 597 MeV; 208Pb(p, xn), E=0.256-3 GeV; calculated σ(θ, E(particle)). Quantum molecular dynamics model.
doi: 10.1103/PhysRevC.52.2620
1995TA14 Phys.Rev. C52, 316 (1995) E.I.Tanaka, A.Ono, H.Horiuchi, T.Maruyama, A.Engel Proton Inelastic Scattering to Continuum Studied with Antisymmetrized Molecular Dynamics NUCLEAR REACTIONS 12C(p, p'X), E=90, 200 MeV; 58Ni(p, p'X), E=120 MeV; calculated σ(θ, E(p')). Anti-symmetrized molecular dynamics model.
doi: 10.1103/PhysRevC.52.316
1994MA31 Nucl.Phys. A573, 653 (1994) T.Maruyama, W.Cassing, U.Mosel, S.Teis, K.Weber Study of High-Energy Heavy-Ion Collisions in a Relativistic BUU Approach with Momentum-Dependent Mean Fields NUCLEAR REACTIONS 197Au(197Au, X), E=0.4, 1 GeV/nucleon; calculated maximum density vs time, directivity distribution. K, Cl(Ar, X), E=800 MeV/nucleon; 197Au(197Au, X), E=150, 400 MeV/nucleon; calculated per nucleon mean transverse momentum vs center-of-mass rapidity. Na, F(Ne, X), 197Au(197Au, X), E=1 GeV/nucleon; calculated inclusive K+ production σ, multiplicity. Relativistic BUU approach, momentum dependent mean fields.
doi: 10.1016/0375-9474(94)90235-6
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
1994TE03 Phys.Rev. C50, 388 (1994) S.Teis, W.Cassing, T.Maruyama, U.Mosel Analysis of Subthreshold Antiproton Production in p-nucleus and Nucleus-Nucleus Collisions in the Relativistic Boltzmann-Uehling-Uhlenbeck Approach NUCLEAR REACTIONS 1H(p, p-barX), E=high; calculated inclusive p-bar production σ. 12C, 63Cu(p, p-bar), E=3.5-5 GeV; calculated invariant differential σ. 197Au(197Au, X), Si(Si, p-bar), E=2.1 GeV/nucleon; Ni(Ni, p-bar), E=1.85 GeV/nucleon; calculated differential p-bar production probability. Relativistic Boltzmann-Uehling-Uhlenbeck approach.
doi: 10.1103/PhysRevC.50.388
1994WI07 Z.Phys. A348, 153 (1994) A.Wierling, B.G.Giraud, F.Mekideche, H.Horiuchi, T.Maruyama, A.Ohnishi, J.C.Lemm, A.Weiguny Antisymmetrization of a Mean Field Calculation of the T-Matrix
doi: 10.1007/BF01291912
1993AN12 Phys.Rev.Lett. 71, 959 (1993) P.L.Anthony, R.G.Arnold, H.R.Band, H.Borel, P.E.Bosted, V.Breton, G.D.Cates, T.E.Chupp, F.S.Dietrich, J.Dunne, R.Erbacher, J.Fellbaum, H.Fonvieille, R.Gearhart, R.Holmes, E.W.Hughes, J.R.Johnson, D.Kawall, C.Keppel, S.E.Kuhn, R.M.Lombard-Nelsen, J.Marroncle, T.Maruyama, W.Meyer, Z.-E.Meziani, H.Middleton, J.Morgenstern, N.R.Newbury, G.G.Petratos, R.Pitthan, R.Prepost, Y.Roblin, S.E.Rock, S.H.Rokni, G.Shapiro, T.Smith, P.A.Souder, M.Spengos, F.Staley, L.M.Stuart, Z.M.Szalata, Y.Terrien, A.K.Thompson, J.L.White, M.Woods, J.Xu, C.C.Young, G.Zapalac, and the E142 Collaboration Determination of the Neutron Spin Structure Function NUCLEAR REACTIONS 3He(polarized e, e'), E=19-26 GeV; measured neutron asymmetry. 1n deduced spin structure function. Polarized target.
doi: 10.1103/PhysRevLett.71.959
1993BO42 Prog.Theor.Phys.(Kyoto) 90, 1155 (1993) Kaon Production in Proton-Nucleus and Deuteron-Nucleus Collisions Near the Kinematical Threshold NUCLEAR REACTIONS 12C(p, K+), E ≈ 840-1000 MeV; 12C(d, K+), E at 0.9, 1.5 GeV/nucleon; calculated kaon yields. Boltzmann type equation, three-nucleon collisions.
doi: 10.1143/ptp/90.5.1155
1993ON01 Phys.Rev. C47, 2652 (1993) A.Ono, H.Horiuchi, T.Maruyama, A.Ohnishi Momentum Distribution of Fragments in Heavy-Ion Reactions: Dependence on the stochastic collision process NUCLEAR REACTIONS 12C(12C, X), E=28.7 MeV/nucleon; analyzed σ(fragment E, θ), other data. Stochastic collision process, many body effects, antisymmetrized molecular dynamics model.
doi: 10.1103/PhysRevC.47.2652
1993ON03 Phys.Rev. C48, 2946 (1993) Nucleon Flow and Fragment Flow in Heavy Ion Reactions NUCLEAR REACTIONS 12C(12C, X), E=84 MeV/nucleon; analyzed σ(θp, Ep). 12C(12C, X), E ≈ 40-160 MeV/nucleon; calculated nucleon, α flow, multiplicities vs E, nucleon emission rate vs time. Asymmetrized version of molecular dynamics, statistical decay.
doi: 10.1103/PhysRevC.48.2946
1993TE06 Phys.Lett. 319B, 47 (1993) S.Teis, W.Cassing, T.Maruyama, U.Mosel Antiproton Production in p-Nucleus and Nucleus-Nucleus Collisions with a Relativistic Transport Approach NUCLEAR REACTIONS 63Cu, 12C(p, p-barX), E=3.5-5 GeV; 28Si(28Si, p-barX), E=2.1 GeV/nucleon; Ni(Ni, p-barX), E=1.85 GeV/nucleon; calculated antiproton production invariant σ. Relativistic BUU approach.
doi: 10.1016/0370-2693(93)90779-H
1992MA13 Phys.Rev. C45, 2355 (1992) T.Maruyama, A.Ohnishi, H.Horiuchi Evolution of Reaction Mechanisms in the Light Heavy-Ion System NUCLEAR REACTIONS 16O(16O, X), E ≤ 200 MeV/nucleon; calculated fragment mass distribution vs E; deduced reaction mechanism evolution. 12C(14N, X), E=35 MeV/nucleon; calculated fragment production σ vs fragment mass. 12C(16O, X), E=25 MeV/nucleon; calculated σ(fragment θ, E) for X=p, d, t; deduced reaction mechanism clarifying conditions.
doi: 10.1103/PhysRevC.45.2355
1992ON01 Phys.Rev.Lett. 68, 2898 (1992) A.Ono, H.Horiuchi, T.Maruyama, A.Ohnishi Fragment Formation Studied with Antisymmetrized Version of Molecular Dynamics with Two-Nucleon Collisions NUCLEAR REACTIONS 12C(12C, X), E=28.7 MeV/nucleon; calculated fragment production σ vs fragment mass=2-14. Antisymmetrized molecular dynamics model, two-nucleon collisions.
doi: 10.1103/PhysRevLett.68.2898
1992ON02 Prog.Theor.Phys.(Kyoto) 87, 1185 (1992) A.Ono, H.Horiuchi, T.Maruyama, A.Ohnishi Antisymmetrized Version of Molecular Dynamics with Two-Nucleon Collision and Its Application to Heavy Ion Reactions NUCLEAR REACTIONS 12C(12C, X), E=28.7 MeV/nucleon; calculated fragment production σ vs mass for H, He, Li, Be, B, C, N isotopes. Molecular dynamics, antisymmetrization.
doi: 10.1143/ptp/87.5.1185
1991LI33 Nucl.Phys. A534, 697 (1991) G.Li, D.T.Khoa, T.Maruyama, S.W.Huang, N.Ohtsuka, A.Faessler, J.Aichelin Subthreshold Pion Production in Nucleus-Nucleus Collisions within the Quantum Molecular Dynamics Approach NUCLEAR REACTIONS 12C(12C, X), Ca(Ca, X), 93Nb(93Nb, X), E=200 MeV/nucleon; 20Ne(20Ne, X), E=183 MeV/nucleon; 64Cu(20Ne, X), E=250 MeV/nucleon; calculated pion production σ(θ, E(π)). Quantum molecular dynamics model.
doi: 10.1016/0375-9474(91)90467-K
1990MA32 Phys.Rev. C42, 386 (1990) T.Maruyama, A.Ohnishi, H.Horiuchi Quantum Molecular Dynamics Study of Fusion and Its Fade Out in the 16O + 16O System NUCLEAR REACTIONS 16O(16O, X), E ≤ 220 MeV; calculated fusion probability, σ(E).
doi: 10.1103/PhysRevC.42.386
1990MA57 Phys.Lett. 245B, 325 (1990) Isoscalar Giant Monopole States of Finite Nuclei in the Relativistic Random Phase Approximation NUCLEAR STRUCTURE A=16-208; calculated isosclar giant monopole resonances. Relativistic RPA.
doi: 10.1016/0370-2693(90)90652-M
1989MA09 Phys.Lett. 219B, 43 (1989) Isoscalar Giant Monopole States of Finite Nuclei in the σ-(Omega) Model NUCLEAR STRUCTURE A=12-208; calculated isoscalar giant monopole states, rms radii, mass parameter, incompressibility. Relativistic constrained Hartree method, σ-(omega) model.
doi: 10.1016/0370-2693(89)90834-4
1989MA61 Prog.Theor.Phys.(Kyoto) 82, 1009 (1989) T.Maruyama, T.-Y.Saito, T.Tsukamoto Skyrme Interaction with Attractive Pairing Property without Density Dependent Force NUCLEAR STRUCTURE 16O, 40Ca; calculated binding energy per nucleon, compressibility, Fermi momentum. Skyrme interaction, pairing, no density dependence.
doi: 10.1143/PTP.82.1009
1988NI08 Nucl.Phys. A485, 515 (1988) S.Nishizaki, T.Maruyama, H.Kurasawa, T.Suzuki Quasielastic Electron Scattering on 12C and 40Ca in the Relativistic Hartree Approximation Relativistic Corrections to the Resopnse Functions NUCLEAR REACTIONS 12C, 40Ca(e, e'), E ≈ 10-200 MeV; calculated longitudinal, transverse response functions, σ(θ(e'), E(e')). Relativistic Hartree approximation.
doi: 10.1016/0375-9474(88)90551-9
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