NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = H.Masui Found 35 matches. 2022MA11 Few-Body Systems 63, 20 (2022) Two-Neutron Halo Structure and Anti-halo Effect in 31F NUCLEAR STRUCTURE 29,31F; calculated the radius and total reaction cross section using a three-body wave function, anti-halo effect that suppresses the halo structure in the ground state.
doi: 10.1007/s00601-021-01715-z
2020MA15 Phys.Rev. C 101, 041303 (2020) Two-neutron halo structure of 31F and a novel pairing antihalo effect NUCLEAR STRUCTURE 31F; calculated S(2n), rms matter radius, valence neutron occupation number of the p3/2 and f7/2 orbits, and radial density distribution using cluster orbital shell model; discussed two-neutron-halo structure, binding mechanism, and the novel antihalo effect. NUCLEAR REACTIONS 1H, 12C(31F, X), (29F, X), E=240, 900 MeV/nucleon; calculated total σ(E) using Glauber theory, and compared with available experimental data.
doi: 10.1103/PhysRevC.101.041303
2019OD01 Phys.Rev. C 99, 034312 (2019) M.Odsuren, Y.Kikuchi, T.Myo, H.Masui, K.Kato Photodisintegration cross sections for resonant states and virtual states NUCLEAR REACTIONS 9Be(γ, n), E=1.6-3 MeV; calculated photodisintegration σ(E) for E1 transitions, E1 matrix elements, level density, E1 strength functions, transition strengths, and pole trajectory of the resonance state using complex-scaled two-body model. Compared experimental photodisintegration σ(E) data with other calculations.
doi: 10.1103/PhysRevC.99.034312
2018OD01 Acta Phys.Pol. B49, 319 (2018) M.Odsuren, T.Myo, G.Khuukhenkhuu, H.Masui, K.Kato Analysis of a Virtual State Using the Complex Scaling Method NUCLEAR STRUCTURE 9Be; calculated levels, J, π and continuum level density considering 9Be as 8Be+n system and using the Complex Scaling Method (CSM).
doi: 10.5506/aphyspolb.49.319
2017OD01 Phys.Rev. C 95, 064305 (2017) M.Odsuren, Y.Kikuchi, T.Myo, G.Khuukhenkhuu, H.Masui, K.Kato Virtual-state character of the two-body system in the complex scaling method NUCLEAR REACTIONS 9Be(γ, n); calculated pole trajectories for 0+, 1-, and second 0+ states, photodisintegration σ(Eγ) for E1, continuum level density, scattering length and phase shifts of the 0+ state. Simple schematic two-body (8Be+n) model with complex scaling method (CSM).
doi: 10.1103/PhysRevC.95.064305
2016NO09 Phys.Rev. C 94, 034909 (2016) T.Nonaka, T.Sugiura, S.Esumi, H.Masui, X.Luo Importance of separated efficiencies between positively and negatively charged particles for cumulant calculations
doi: 10.1103/PhysRevC.94.034909
2016SA40 Nucl.Phys. A956, 850 (2016) H.Sako, H.Harada, T.Sakaguchi, T.Chujo, S.Esumi, T.Gunji, S.Hasegawa, S.H.Hwang, Y.Ichikawa, K.Imai, K.Itakura, M.Kaneta, B.C.Kim, M.Kinsho, M.Kitazawa, Y.Liu, H.Masui, S.Nagamiya, K.Nishio, M.Okamura, K.Oyama, K.Ozawa, P.K.Saha, A.Sakaguchi, S.Sato, K.Shigaki, H.Sugimura, K.Tanida, J.Tamura, H.Tamura, Y.Nara, T.R.Saito, for the J-PARC and Heavy-Ion Collaboration Studies of high density baryon matter with high intensity heavy-ion beams at J-PARC
doi: 10.1016/j.nuclphysa.2016.03.030
2015SU05 Phys.Rev. C 91, 024903 (2015) X.Sun, H.Masui, A.M.Poskanzer, A.Schmah Blast wave fits to elliptic flow data at √ sNN = 7.7-2760 GeV
doi: 10.1103/PhysRevC.91.024903
2014MA20 Phys.Rev. C 89, 044317 (2014) H.Masui, K.Kato, N.Michel, M.Ploszajczak Precise comparison of the Gaussian expansion method and the Gamow shell model NUCLEAR STRUCTURE 6He, 6Be; calculated level energies and poles of ground states and first 2+ unbound states with 4He+2n and 4He+2p systems, density of valence neutrons. Gamow shell model (GSM), and Gaussian expansion method with complex scaling (GEM+CS).
doi: 10.1103/PhysRevC.89.044317
2012IT03 Prog.Theor.Phys.(Kyoto), Suppl. 196, 192 (2012) N.Itagaki, K.Muta, H.Masui, M.Ploszajczak, J.Cseh Simplified Modeling of Cluster-Shell Competition and Appearance of Various Cluster Structures in Light Nuclei NUCLEAR STRUCTURE 20Ne; calculated energy levels, J, π, yrast states. Antisymmetrized Quasi-Cluster approach.
doi: 10.1143/PTPS.196.192
2012MA50 Nucl.Phys. A895, 1 (2012) Expansion of the 16O-core in neutron drip-line nuclei: 23O and 24O NUCLEAR STRUCTURE 16,17,18,19,20,22,23,24,25,26O; calculated neutron binding energy, Q, rms nuclear radii, first excited state energy, nuclear core, matter density distribution using m-scheme of extended COSM (cluster-orbitting shell model) with various parameters, rms radii also with coupled-channel model. Compared with available data.
doi: 10.1016/j.nuclphysa.2012.09.004
2011MA87 J.Phys.:Conf.Ser. 312, 092038 (2011) Properties of drip-line nuclei with an m-scheme cluster-orbital shell model approach NUCLEAR STRUCTURE 18,19,20,21,22,23,24,25,26O; calculated rms radius, mass excess using m-scheme of COSM (cluster-orbital shell model). Compared with available data.
doi: 10.1088/1742-6596/312/9/092038
2011YA15 J.Korean Phys.Soc. 59, 907s (2011) K.Yamamoto, H.Masui, M.Ohta, K.Kato Particle Capture Reaction using Extended Core Plus Valence Nucleon Model NUCLEAR REACTIONS 17O(n, γ), E=0-0.5 MeV; calculated σ using COSM (Cluster Orbital Shell Model). NUCLEAR STRUCTURE 18O; calculated levels, J, π using COSM (Cluster Orbital Shell Model) and CSM (Complex Scaling Method). Comparison with data.
doi: 10.3938/jkps.59.907
2009FI07 Phys.Rev. C 80, 054903 (2009) P.Filip, R.Lednicky, H.Masui, N.Xu Initial eccentricity in deformed 197Au+197Au and 238U+238U collisions at √ sNN=200 GeV at the BNL Relativistic Heavy Ion Collider
doi: 10.1103/PhysRevC.80.054903
2009MA63 Nucl.Phys. A830, 463c (2009) H.Masui, J.-Y.Ollitrault, R.Snellings, A.Tang The centrality dependence of ν2/ϵ: the ideal hydro limit and η/s
doi: 10.1016/j.nuclphysa.2009.10.103
2009MA76 Eur.Phys.J. A 42, 535 (2009) Study of neutron-rich nuclei with an m -scheme cluster-orbital shell model approach NUCLEAR STRUCTURE 16,17,18,19,20,21,22,23,24,25,26O; calculated single-neutron separation energies, radii using cluster-orbital shell model. Comparison with data.
doi: 10.1140/epja/i2009-10839-9
2009YA03 Prog.Theor.Phys.(Kyoto) 121, 375 (2009) K.Yamamoto, H.Masui, J.Kato, T.Wada, M.Ohta Radiative Capture Cross Section for 16O(n, γ)17O and 16O(p, γ)17F below Astrophysical Energies NUCLEAR REACTIONS 16O(n, γ), E(cm) < 10 MeV; calculated cross sections.16O(p, γ), E(cm) < 3 MeV; calculated astrophysical S-factor.
doi: 10.1143/PTP.121.375
2007MA17 Phys.Rev. C 75, 034316 (2007) Comparison between the Gamow shell model and the cluster-orbital shell model for weakly bound systems NUCLEAR STRUCTURE 18,19,20O; calculated levels, J, π, configurations. 5,6,7,8He; calculated ground-state energies. 6,8He; calculated radii. Gamow and cluster-orbital shell models.
doi: 10.1103/PhysRevC.75.034316
2007MA38 Phys.Rev. C 75, 054309 (2007) Simplified modeling of cluster-shell competition in carbon isotopes NUCLEAR STRUCTURE 12,14,16C; calculated level energies and B(E2) by combining a simplied modeling of spin-orbit interaction and AMD triple-S.
doi: 10.1103/PhysRevC.75.054309
2007MA54 Nucl.Phys. A790, 303c (2007) Study of weakly bound nuclei with an extended cluster-orbital shell model NUCLEAR STRUCTURE 16,17,18,19,20O, 17F, 18Ne, 20Mg; calculated radii, binding energies. Extended cluster-orbital shell model.
doi: 10.1016/j.nuclphysa.2007.03.049
2006IT02 Phys.Rev. C 73, 034310 (2006) N.Itagaki, H.Masui, M.Ito, S.Aoyama, K.Ikeda Simplified method to include the tensor contribution in α-cluster model NUCLEAR STRUCTURE 8Be, 12C; calculated 0+ α-cluster states energies, role of tensor interaction, spin-orbit contribution.
doi: 10.1103/PhysRevC.73.034310
2006MA17 Phys.Rev. C 73, 034318 (2006) Study of oxygen isotopes and N=8 isotones with an extended cluster-orbital shell model NUCLEAR STRUCTURE 16,17,18,19,20O, 17F, 18Ne, 20Mg; calculated radii, ground-state energies. Extended cluster-orbital shell model.
doi: 10.1103/PhysRevC.73.034318
2006MA89 Nucl.Phys. A774, 511 (2006) H.Masui, and the PHENIX collaboration Anisotropic Flow in √ sNN = 200 GeV Cu+Cu and Au+Au collisions at PHENIX NUCLEAR REACTIONS Cu(Cu, X), Au(Au, X), E(cm)=200 GeV/nucleon; measured charged-particle invariant mass; deduced charged-pion, proton, anti-proton and inclusive hadron elliptic flow. Comparison with parton cascade model.
doi: 10.1016/j.nuclphysa.2006.06.077
2005IT04 Phys.Rev. C 71, 064307 (2005) N.Itagaki, H.Masui, M.Ito, S.Aoyama Simplified modeling of cluster-shell competition NUCLEAR STRUCTURE 10Be; calculated ground state energy, contribution of the cluster-shell and spin-orbit interactions. 9,10Be, 12C, 20Ne; calculated excited state energies, contribution of the cluster-shell and spin-orbit interactions.
doi: 10.1103/PhysRevC.71.064307
2005MA98 Eur.Phys.J. A 25, Supplement 1, 505 (2005) H.Masui, T.Myo, K.Kato, K.Ikeda Study of drip-line nuclei with a core plus multi-valence nucleon model NUCLEAR STRUCTURE 15N, 16,17,18,19,20,21,22,23,24O, 17F, 18Ne, 19Na, 20Mg; calculated radii. Extended cluster-orbital shell model.
doi: 10.1140/epjad/i2005-06-135-8
2003MA70 Nucl.Phys. A722, 469c (2003) H.Masui, T.Myo, K.Kato, K.Ikeda Coupled-channel study for O-isotopes with the core plus valence neutrons model NUCLEAR STRUCTURE 17,18O; calculated level energies, configurations. Core plus neutron model, complex scaling method, Jost function method.
doi: 10.1016/S0375-9474(03)01410-6
2003MA79 Prog.Theor.Phys.(Kyoto) 110, 233 (2003) Study of Resonance States in a Coupled-Channel System with the Jost Function Method Applying the Orthogonality Condition Model NUCLEAR STRUCTURE 10Li, 20Ne; calculated resonance states energies, J, π, widths in two-body systems. Jost function method. NUCLEAR REACTIONS 9Li(n, X), 16O(α, X), E not given; calculated resonance states energies, J, π, widths in two-body systems. Jost function method.
doi: 10.1143/PTP.110.233
2003MB05 Mod.Phys.Lett. A 18, 186 (2003) H.Masui, T.Myo, K.Kato, K.Ikeda Coupled-channel study for O-isotopes with the core plus valence neutrons model NUCLEAR STRUCTURE 17,18O; calculated level energies, configurations. Coupled-channels and resonating group method approach.
doi: 10.1142/S0217732303010223
2002KU44 Prog.Theor.Phys.(Kyoto), Suppl. 146, 581 (2002) C.Kurokawa, H.Masui, T.Myo, K.Kato Study of the s-Wave Virtual State in 10Li with the Jost Function Method NUCLEAR STRUCTURE 10Li; calculated level energies, widths.
doi: 10.1143/PTPS.146.581
2002MA32 Phys.Rev. C65, 054305 (2002) Resonance States with the Complex Absorbing Potential Method
doi: 10.1103/PhysRevC.65.054305
2002MA77 Prog.Theor.Phys.(Kyoto), Suppl. 146, 589 (2002) H.Masui, S.Aoyama, T.Myo, K.Kato, K.Ikeda Study of the s-Wave Properties for 10Li through the Analysis of the Break-Up Reaction NUCLEAR STRUCTURE 10Li; analyzed break-up reaction data; deduced neutron-core potential features.
doi: 10.1143/PTPS.146.589
2001MA37 Nucl.Phys. A684, 609c (2001) H.Masui, S.Aoyama, T.Myo, K.Kato, K.Ikeda Study of Resonant and Virtual States with the Complex Scaling Method and the Developments NUCLEAR STRUCTURE 5He, 10Li; calculated virtual states energies, related features. Jost function method.
doi: 10.1016/S0375-9474(01)00452-3
2000MA32 Nucl.Phys. A673, 207 (2000) H.Masui, S.Aoyama, T.Myo, K.Kato, K.Ikeda Study of Virtual States in 5He and 10Li with the Jost Function Method NUCLEAR STRUCTURE 5He, 10Li; calculated virtual state features. Jost function method, core-plus-neutron picture.
doi: 10.1016/S0375-9474(00)00148-2
1999MA91 Prog.Theor.Phys.(Kyoto) 102, 1119 (1999) H.Masui, S.Aoyama, T.Myo, K.Kato Partial Decay Widths in Coupled-Channel Systems with the Complex-Scaled Jost Function Method
doi: 10.1143/PTP.102.1119
1998MA92 Prog.Theor.Phys.(Kyoto) 100, 977 (1998) Monte-Carlo Study of Bound States in a Few-Nucleon System - Method of Continued Fractions -
doi: 10.1143/PTP.100.977
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