NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = S.Mizutori Found 28 matches. 2018IN03 Phys.Rev. C 98, 044312 (2018) Rod-shaped rotational states in N=Z even-even nuclei from 12C to 32S NUCLEAR STRUCTURE 12C, 16O, 20Ne, 24Mg, 28Si, 32S; calculated rotational excitation energies of rod-shaped state as function of angular momentum, nucleon density distribution of g.s. and superdeformed state, nucleon localization measure, elongation, and triaxiality of rod-shaped states for N=Z nuclei using cranked Skyrme Hartree-Fock method.
doi: 10.1103/PhysRevC.98.044312
2009OG01 Prog.Theor.Phys.(Kyoto) 121, 357 (2009) H.Ogasawara, K.Yoshida, M.Yamagami, S.Mizutori, K.Matsuyanagi Rotational Frequency Dependence of Octupole Vibrations on Superdeformed States in 40Ca
doi: 10.1143/PTP.121.357
2008OG02 Prog.Theor.Phys.(Kyoto) 120, 1169 (2008) H.Ogasawara, K.Yoshida, M.Yamagami, S.Mizutori, K.Matsuyanagi Triaxiality Dependence of Octupole Excitations on Superdeformed States in 44Ti
doi: 10.1143/PTP.120.1169
2006IN01 Nucl.Phys. A768, 61 (2006) T.Inakura, H.Imagawa, Y.Hashimoto, S.Mizutori, M.Yamagami, K.Matsuyanagi Mixed representation RPA calculation for octupole excitations on superdeformed states in the 40Ca and neutron-rich sulfur regions NUCLEAR STRUCTURE 32,36,48,50S, 36Ar, 40Ca, 44Ti; calculated energy, J, octupole transition strengths for low-frequency negative-parity excitations built on superdeformed states. Self-consistent RPA approach, comparison with other models.
doi: 10.1016/j.nuclphysa.2006.01.008
2005IN02 Eur.Phys.J. A 25, Supplement 1, 545 (2005) T.Inakura, H.Imagawa, Y.Hashimoto, M.Yamagami, S.Mizutori, K.Matsuyanagi Soft octupole vibrations on superdeformed states in nuclei around 40Ca suggested by Skyrme-HF and self-consistent RPA calculations NUCLEAR STRUCTURE 32S, 36Ar, 40Ca, 44Ti; calculated energy, J for low-frequency negative-parity excitations built on superdeformed states. Self-consistent RPA approach.
doi: 10.1140/epjad/i2005-06-111-4
2005YO13 Eur.Phys.J. A 25, Supplement 1, 557 (2005) K.Yoshida, T.Inakura, M.Yamagami, S.Mizutori, K.Matsuyanagi Microscopic structure of negative-parity vibrations built on superdeformed states in sulfur isotopes close to the neutron drip line NUCLEAR STRUCTURE 50S; calculated isoscalar octupole transition strengths, neutron density distributions, superdeformed states features. Woods-Saxon potential, RPA.
doi: 10.1140/epjad/i2005-06-142-9
2004IN01 Int.J.Mod.Phys. E13, 157 (2004) T.Inakura, M.Yamagami, K.Matsuyanagi, S.Mizutori, H.Imagawa, Y.Hashimoto Static and dynamic non-axial octupole deformations suggested by Skyrme-HF and selfconsistent RPA calculations NUCLEAR STRUCTURE 32,34,36,38,40,42,44,46,48,50S, 36Ar, 40Ca, 44Ti, 48Cr; calculated deformation energy curves. 32,36,48,50S; calculated levels, J, π, transition matrix elements. Skyrme-Hartree-Fock and RPA calculations.
doi: 10.1142/S0218301304001886
2003IN03 Nucl.Phys. A728, 52 (2003) T.Inakura, S.Mizutori, M.Yamagami, K.Matsuyanagi Superdeformed bands in neutron-rich sulfur isotopes suggested by cranked Skyrme-Hartree-Fock calculations NUCLEAR STRUCTURE 32,34,36,38,40,42,44,46,48,50S, 38Ar; calculated potential energy vs deformation. 32,36,50S deduced superdeformed configurations. Cranked Skyrme-Hartree-Fock approach.
doi: 10.1016/j.nuclphysa.2003.08.012
2002IN04 Nucl.Phys. A710, 261 (2002) T.Inakura, S.Mizutori, M.Yamagami, K.Matsuyanagi Cranked Skyrme-Hartree-Fock calculation for superdeformed and hyperdeformed rotational bands in N = Z nuclei from 32S to 48Cr NUCLEAR STRUCTURE 32S, 36Ar, 40Ca, 44Ti, 48Cr; calculated rotational bands deformation, related features. 32S, 36Ar, 40Ca, 44Ti; deduced superdeformed bands. 36Ar, 40Ca, 44Ti, 48Cr; deduced hyperdeformed bands. 40Ca deduced octupole softness. Symmetry-unrestricted cranked Skyrme-Hartree-Fock method.
doi: 10.1016/S0375-9474(02)01164-8
2002IN06 Prog.Theor.Phys.(Kyoto), Suppl. 146, 567 (2002) T.Inakura, M.Yamagami, S.Mizutori, K.Matsuyanagi Cranked Skyrme-Hartree-Fock Calculations for Superdeformed and Hyperdeformed Bands in N = Z Nuclei 32S, 36Ar, 40Ca, and in Neutron Rich Nuclei, 14Be, 26Ne, 46S NUCLEAR STRUCTURE 32,46S, 36Ar, 40Ca, 44Ti, 48Cr; calculated superdeformed and hyperdeformed bands energy vs spin. Cranked Skyrme-Hartree-Fock approach.
doi: 10.1143/PTPS.146.567
2001FU11 Nucl.Phys. A690, 243c (2001) Y.Fujita, T.Adachi, G.P.A.Berg, B.A.Brown, H.Ejiri, H.Fujimura, H.Fujita, M.Fujiwara, K.Hara, M.N.Harakeh, K.Hatanaka, F.Hofmann, J.Kamiya, K.Katori, T.Kawabata, S.Mizutori, P.von Neumann-Cosel, T.Noro, B.Reitz, A.Richter, Y.Shimbara, T.Shinada, H.Ueno, M.Yoshifuku, M.Yosoi Decomposition of M1 Transitions into Isoscalar and Isovector, Spin and Orbital Contributions NUCLEAR REACTIONS 24Mg, 28Si, 27Al(3He, t), E=150 MeV; analyzed B(M1), B(GT). 24Mg, 28Si, 27Al deduced orbital contributions to M1 strengths.
doi: 10.1016/S0375-9474(01)00950-2
2001NA31 Acta Phys.Pol. B32, 2349 (2001) W.Nazarewicz, J.Dobaczewski, M.Matev, S.Mizutori, W.Satula Rotational Properties of Neutron Drip-Line Nuclei NUCLEAR STRUCTURE 108Ru; calculated total Routhain surfaces. 208Er, 230Th; calculated quasiparticle Routhians. 30,32,34,36,38Ne, 32,34,36,38,40Mg; calculated deformation, radii vs rotational frequency. Deformed shell model, self-consistent Skyrme-Hartree-Fock theory.
2000DO07 Phys.Rev.Lett. 84, 4317 (2000) P.Donati, T.Dossing, Y.R.Shimizu, S.Mizutori, P.F.Bortignon, R.A.Broglia Effective Nucleon Mass in Deformed Nuclei NUCLEAR STRUCTURE 168Yb; calculated nucleon effective mass vs rotational frequency. 169Yb; calculated quadrupole RPA response functions.
doi: 10.1103/PhysRevLett.84.4317
2000FU13 Phys.Rev. C62, 044314 (2000) Y.Fujita, B.A.Brown, H.Ejiri, K.Katori, S.Mizutori, H.Ueno Separation of Isoscalar, Isovector, Orbital, and Spin Contributions in M1 Transitions in Mirror Nuclei NUCLEAR STRUCTURE 27Al, 27Si; calculated transitions B(M1); deduced isovector, isoscalar, orbital, spin components. Shell model, comparisons with data.
doi: 10.1103/PhysRevC.62.044314
2000MI08 Phys.Rev. C61, 044326 (2000) S.Mizutori, J.Dobaczewski, G.A.Lalazissis, W.Nazarewicz, P.-G.Reinhard Nuclear Skins and Halos in the Mean-Field Theory NUCLEAR STRUCTURE Sn, Ni, Pb; calculated neutron, proton densities, radii, related features. Z=4-124; calculated neutron halo parameters, proton surface thickness. 20,34,38Ne; calculated form factors. Spherical self-consistent mean-field theory.
doi: 10.1103/PhysRevC.61.044326
1997SA36 Phys.Lett. 407B, 103 (1997) W.Satula, D.J.Dean, J.Gary, S.Mizutori, W.Nazarewicz On the Origin of the Wigner Energy NUCLEAR STRUCTURE A=24-64; analyzed Wigner energy coefficient in N=Z nuclei. 24Mg, 48Cr; calculated binding energy displacement; deduced contribution from neutron-proton pairing interactions.
doi: 10.1016/S0370-2693(97)00711-9
1997SK01 Nucl.Phys. A617, 282 (1997) J.Skalski, S.Mizutori, W.Nazarewicz Equilibrium Shapes and High-Spin Properties of Neutron-Rich A ≈ 100 Nuclei NUCLEAR STRUCTURE 100,102,104,106Zr, 100,102,104,106Mo, 104,106,108,110Ru, 96,98,100,102,104Sr; calculated total energy surfaces, equilibrium deformations of yrast, near-yrast bands, potential energy curves, equilibrium deformations for these, other isotopes, kinematic moments of inertia vs rotational frequency for superdeformed bands in some cases. 90,92,94,96,98Se, 92,94,96,98,100,102,104,106,108Kr, 94,96,98,100,102,104,106,108,110Sr, 96,98,100,102,104,106,108,110,112,114Zr, 100,102,104,106,108,110,112,114,116Mo, 104,106,108,110,112,114,116,118,120Ru, 102,104,106,108,110,112,114,116,118,120,122,124Pd, 104,106,108,110,112,114,116,118,120,122,124Cd; calculated ground state, excited minima, quadrupole moments. Macroscopic-microscopic approach, Nilsson-Strutinsky method, cranked Woods-Saxon average potential.
doi: 10.1016/S0375-9474(97)00125-5
1996NA07 Phys.Rev. C53, 2213 (1996) T.Nakatsukasa, K.Matsuyanagi, S.Mizutori, Y.R.Shimizu Microscopic Structure of High-Spin Vibrational Excitations in Superdeformed 190,192,194Hg NUCLEAR STRUCTURE 190,192,194Hg; calculated octupole, (γ) vibrations excitation energy, B(λ), superdeformed bands dynamic moments of inertia. Cranked shell model extended by RPA.
doi: 10.1103/PhysRevC.53.2213
1995AF05 Z.Phys. A353, 267 (1995) Octupole Correlations at Medium Spin in Odd-Proton 153Eu Nucleus NUCLEAR STRUCTURE 153Eu; analyzed data; deduced static octupole deformation plausibility. Cranking calculation with, without deformation.
1995MI20 Phys.Scr. T56, 276 (1995) S.Mizutori, Y.R.Shimizu, K.Matsuyanagi Microscopic Structure of Octupole Correlations at High-Spin in Superdeformed Open-Shell Nuclei NUCLEAR STRUCTURE 146Nd, 148Sm, 150Gd, 152Dy, 154Er; calculated octupole strength function; deduced superdeformed bands octupole softness related features.
doi: 10.1088/0031-8949/1995/T56/048
1995NA03 Phys.Lett. 343B, 19 (1995) T.Nakatsukasa, K.Matsuyanagi, S.Mizutori, W.Nazarewicz Octupole Correlations in Excited Bands of Superdeformed 152Dy NUCLEAR STRUCTURE 152Dy; calculated superdeformed band dynamical moments of inertia; deduced rotation, octupole vibration interplay features. Cranked shell model, RPA.
doi: 10.1016/0370-2693(94)01484-T
1994HA22 Phys.Lett. 324B, 273 (1994) Dynamical Moments of Inertia at Normal Deformation in Neighbouring Odd and Even-Even Nuclei NUCLEAR STRUCTURE 157,159,161,163Ho, 159,161,163,165,167,169Tm, 163,165,167,169,171,173,175Lu, 171,173,175,177,179,181Ta, 177,179,181,183,185Re; calculated dynamical moments of inertia fractional changes. Cranking HFB calculations.
doi: 10.1016/0370-2693(94)90193-7
1993MI10 Nucl.Phys. A557, 125c (1993) S.Mizutori, T.Nakatsukasa, K.Arita, Y.R.Shimizu, K.Matsuyanagi Octupole Correlations in Superdeformed High-Spin States NUCLEAR STRUCTURE 158,156,154,152,150,148,146,144,142Gd, 184,186,188,190,192,194,196,198,200Hg; calculated curvature against octupole deformation, stretched octupole strengths; deduced octupole instability, superdeformed shape relationship.
doi: 10.1016/0375-9474(93)90536-7
1993MI16 Z.Phys. A346, 1 (1993) Level and Width Statistics for a Decaying Chaotic System NUCLEAR STRUCTURE N=2-160; calculated levels, widths, correlations. Decaying chaotic systems.
doi: 10.1007/BF01290775
1993NA16 Prog.Theor.Phys.(Kyoto) 89, 847 (1993) T.Nakatsukasa, S.Mizutori, K.Matsuyanagi Effects of Octupole Vibrations on Quasiparticle Modes of Excitation in Superdeformed 193Hg NUCLEAR STRUCTURE 192Hg; calculated superdeformed states octupole transitions strength distribution. 193Hg; calculated superdeformed rotational bands. Cranked shell model, RPA based particle-vibration coupling.
doi: 10.1143/ptp/89.4.847
1992NA15 Prog.Theor.Phys.(Kyoto) 87, 607 (1992) T.Nakatsukasa, S.Mizutori, K.Matsuyanagi Octupole Vibrations in the Harmonic-Oscillator-Potential Model with Axis Ratio Two to One NUCLEAR STRUCTURE Z=80; N=80; calculated RPA octupole transition strength functions; deduced open shell superdeformed configurations octupole vibrations evidence. Harmonic osillator potential model, axis ratio two to one, RPA solutions.
doi: 10.1143/ptp/87.3.607
1991MI07 Prog.Theor.Phys.(Kyoto) 85, 559 (1991) S.Mizutori, Y.R.Shimizu, K.Matsuyanagi Octupole Vibrations with K = 1 and 2 in Superconducting, Superdeformed Nuclei NUCLEAR STRUCTURE 192Hg, 144Gd; calculated octupole strength functions, superdeformed nuclei. RPA.
doi: 10.1143/ptp/85.3.559
1990MI13 Prog.Theor.Phys.(Kyoto) 83, 666 (1990) S.Mizutori, Y.R.Shimizu, K.Matsuyanagi Octupole Vibrations Built on Superdeformed Rotational Bands NUCLEAR STRUCTURE 152Dy; calculated giant octupole resonance strength functions; deduced resonances built on superdeformed band states. Cranking model based RPA.
doi: 10.1143/PTP.83.666
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