NSR Query Results
Output year order : Descending NSR database version of May 6, 2024. Search: Author = N.Shikazono Found 27 matches. 1994IK01 Phys.Rev. C49, 968 (1994) H.Ikezoe, Y.Nagame, I.Nishinaka, Y.Sugiyama, Y.Tomita, K.Ideno, S.Hamada, N.Shikazono, A.Iwamoto, T.Ohtsuki Prescission and Postscission Charge Particle Emissions from the 19F + 159Tb Reaction NUCLEAR REACTIONS 159Tb(19F, F), E=124.1, 159.1 MeV; measured fission (fragment)p-, (fragment)α-coin, prescission, postscission p-, α-multiplicities; deduced fission fragment temperatures. Statistical model.
doi: 10.1103/PhysRevC.49.968
1992IK01 Phys.Rev. C46, 1922 (1992) H.Ikezoe, N.Shikazono, Y.Nagame, Y.Sugiyama, Y.Tomita, K.Ideno, I.Nishinaka, B.J.Qi, H.J.Kim, A.Iwamoto, T.Ohtsuki Charged Particle Multiplicities in Heavy-Ion-Induced Fission NUCLEAR REACTIONS 197Au(19F, F), E=94-149.3 MeV; 181Ta, 197Au, 208Pb(19F, F), E=92-162.4 MeV; 197Au, 208Pb(28Si, F), E=147.2-194.1 MeV; measured pre-scission, post-scission charged particle multiplicity, fission, (fragment)(light charged particle)(θ); deduced fission dynamics. Statistical model.
doi: 10.1103/PhysRevC.46.1922
1990IK02 Phys.Rev. C42, 342 (1990) H.Ikezoe, N.Shikazono, Y.Nagame, Y.Sugiyama, Y.Tomita, K.Ideno, A.Iwamoto, T.Ohtsuki Pre-Scission 4He Multiplicity in the 19F + 197Au Reaction NUCLEAR REACTIONS 19F(197Au, F), E=92-161 MeV; measured cross section, fission (fragment)α-coin; deduced pre-, post-scission α-multiplicities, emission barrier. Statistical model calculations.
doi: 10.1103/PhysRevC.42.342
1990IK03 Phys.Rev. C42, R1187 (1990) H.Ikezoe, N.Shikazono, Y.Nagame, Y.Sugiyama, Y.Tomita, K.Ideno, A.Iwamoto, T.Ohtsuki Pre-Scission 1H and 4He Emissions in 16O + 197Au Reaction NUCLEAR REACTIONS 197Au(16O, F), E=94-149.3 MeV; measured fission fragment (light particle)-coin; deduced emission barriers, pre-scission p, α multiplicities. Statistical model analysis.
doi: 10.1103/PhysRevC.42.R1187
1988IK01 Z.Phys. A330, 289 (1988) H.Ikezoe, N.Shikazono, Y.Tomita, Y.Sugiyama, K.Ideno, W.Yokota, Y.Nagame, S.M.Lee, M.Ogihara, S.C.Jeong, H.Fujiwara, D.J.Hinde Mass Distribution of Fission Fragments in the 19F + 197Au Reaction NUCLEAR REACTIONS 197Au(19F, F), E=100-160 MeV; measured fission fragment yield vs mass, σ(θ). Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1357. 1987IK01 Nucl.Phys. A462, 150 (1987) H.Ikezoe, N.Shikazono, Y.Tomita, Y.Sugiyama, K.Ideno Coincidence Measurements of Light Particles and Evaporation Residues in the 16O + 27Al Fusion Reaction NUCLEAR REACTIONS 27Al(16O, pX), (16O, αX), E=150 MeV; measured (fragment)p-, (fragment)α-coin, for fragment mass=28-38, α-multiplicity vs θ(α), Eα, p-multiplicity vs θ(p), E(p); deduced α-emission mechanism. Statistical model.
doi: 10.1016/0375-9474(87)90383-6
1986IK03 Nucl.Phys. A456, 298 (1986) H.Ikezoe, N.Shikazono, Y.Tomita, K.Ideno, Y.Sugiyama, E.Takekoshi, T.Tachikawa, T.Nomura Measurements of Evaporation Residues to Investigate Lower Limiting Angular Momenta in Fusion Reactions NUCLEAR REACTIONS, ICPND 12C(16O, X)25Al/26Al/22Na/21Na/23Na/24Na/25Na, E=70-130 MeV; 16O(16O, X)29Si/28Si/27Si/27Al/26Al/28Al/24Mg/25Mg/26Mg/23Mg/22Na/23Na/24Na/25Na/21Ne/20Ne/22Ne, E=70-130 MeV; measured evaporation residues, velocity spectra, σ(θ), residual prodution σ(E); deduced fusion limiting angular momenta. Statistical, TDHF models.
doi: 10.1016/0375-9474(86)90395-7
1986SU09 Phys.Lett. 176B, 302 (1986) Y.Sugiyama, Y.Tomita, H.Ikezoe, K.Ideno, N.Shikazono, N.Kato, H.Fujita, T.Sugimitsu, S.Kubono Transfer Cross Sections for 28Si + 58,62Ni NUCLEAR REACTIONS 58,62Ni(28Si, 29Si), (28Si, 30Si), (28Si, 28Si), (28Si, 28Si'), E=110 MeV; measured σ(θ), σ(E(29Si)), σ(E(30Si)); deduced energy, angle integrated quasielastic reaction σ. Coupled-channels model, DWBA analyses.
doi: 10.1016/0370-2693(86)90168-1
1985IK02 Nucl.Phys. A444, 349 (1985) H.Ikezoe, N.Shikazono, Y.Tomita, K.Ideno, Y.Sugiyama, E.Takekoshi Incomplete Fusion of the 16O + 27Al Reaction NUCLEAR REACTIONS 27Al(16O, X), E=90, 150 MeV; measured evaporation residues, velocity spectra; deduced reaction mechanism. Statistical model calculation.
doi: 10.1016/0375-9474(85)90354-9
1985SU07 Phys.Lett. 159B, 90 (1985) Y.Sugiyama, N.Shikazono, Y.Tomita, H.Ikezoe, T.Tachikawa, E.Takekoshi, S.Kubono, M.Tanaka Magnetic Substate Population in 12C + 12C Inelastic Scattering NUCLEAR REACTIONS 12C(12C, 12C'γ), E(cm)=19-55 MeV; measured γ(θ), γ(φ). 12C level deduced magnetic substate population vs θ. DWBA analysis.
doi: 10.1016/0370-2693(85)90862-7
1985SU16 Z.Phys. A322, 579 (1985) Y.Sugiyama, Y.Tomita, H.Ikezoe, N.Shikazono Particle Line Shape after γ-Ray Emission in Flight NUCLEAR REACTIONS 12C(12C, 12C'), E=60 MeV; measured particle momentum spectra following γ-emission; deduced line shapes.
doi: 10.1007/BF01415137
1979PO16 Nucl.Phys. A330, 173 (1979) E.C.Pollacco, D.M.Parkinson, J.R.Leigh, D.C.Weisser, N.Shikazono, G.S.Foote, D.Branford 12C and 13C Induced Reactions on N = 28 Nuclei at Energies Near the Coulomb Barrier NUCLEAR REACTIONS 48Ca, 50Ti, 52Cr, 54Fe(13C, 13C); 48Ca, 50Ti, 52Cr, 53Cr, 54Fe(12C, 12C); 52Cr, 54Fe(12C, 12C'); 52Cr, 54Fe(13C, 13C'); 48Ca, 50Ti, 52Cr, 54Fe(13C, 12C); 53Cr(12C, 13C); measured σ(E). 52Cr, 54Fe deduced B(E2), β of ion-ion potential. 49Ca, 51Ti, 53Cr, 55Fe levels deduced S. Enriched targets. DWBA analysis.
doi: 10.1016/0375-9474(79)90543-8
1976FO04 Nucl.Phys. A263, 349 (1976) G.S.Foote, D.Branford, D.C.Weisser, N.Shikazono, R.A.I.Bell, F.C.P.Huang Alpha Capture to the Giant Dipole Resonances of 42Ca, 44Ca and 52Cr NUCLEAR REACTIONS 38Ar(α, γ), E=6-15 MeV; 40Ar(α, γ), E=5.5-11.1 MeV; 48Ti(α, γ), E=6-12 MeV; measured σ(E, Eγ, θ). 42,44Ca, 52Cr deduced resonances, J, π, Γ, GDR. Enriched 38Ar, 48Ti targets.
doi: 10.1016/0375-9474(76)90177-9
1976HI14 J.Phys.(London) G2, L143 (1976) G.T.Hickey, G.M.Crawley, D.C.Weisser, N.Shikazono Mass Measurement of 62Fe Using the 64Ni(18O, 20Ne)62Fe Reaction NUCLEAR REACTIONS 64Ni(18O, 20Ne), E=96 MeV; measured σ(20Ne, θ); deduced Q. 62Fe deduced level, mass excess.
doi: 10.1088/0305-4616/2/9/004
1976LE12 J.Phys.(London) G2, L39 (1976) J.R.Leigh, E.C.Pollacco, N.Shikazono, D.C.Weisser, C.Garrett Differences in the Coulomb-Nuclear Interference Patterns Produced with 12C and 13C Ions NUCLEAR REACTIONS 52Cr, 54Fe(12C, 12C), (12C, 12C'), (13C, 13C), (13C, 13C'), E=18-26 MeV; measured σ(E); deduced differences in Coulomb-nuclear interference patterns.
doi: 10.1088/0305-4616/2/3/005
1975SH16 Nucl.Phys. A250, 260 (1975) Analysis of E1 and E2 Radiative α-Capture and Giant Multipole Resonances NUCLEAR REACTIONS 24Mg, 28Si, 36Ar(α, γ), E < 15 MeV; analyzed σ for E1, E2 strength.
doi: 10.1016/0375-9474(75)90258-4
1974FO04 J.Phys.(London) A7, L4 (1974) G.S.Foote, D.Branford, D.C.Weisser, N.Shikazono, F.C.P.Huang Alpha Capture to the Giant Dipole Resonance NUCLEAR REACTIONS 38,40Ar, 48Ti, 56Fe(α, γ); measured σ(Eγ, θ), calculated σ for inverse (γ, α) reaction.
doi: 10.1088/0305-4470/7/1/002
1974FO05 J.Phys.(London) A7, L27 (1974) G.S.Foote, D.Branford, N.Shikazono, D.C.Weisser Alpha Capture to the Giant Quadrupole Resonance NUCLEAR REACTIONS 28Si(α, γ), E=6-12 MeV; measured σ(E, θ). 32S deduced resonance.
doi: 10.1088/0305-4470/7/3/001
1972SH07 Nucl.Phys. A188, 461 (1972) Study of Odd-A Nuclei in the 2s-1d Shell by Means of the (γ, γ') Reaction NUCLEAR REACTIONS 19F, 23Na, 27Al, 31P, 35Cl, 39K(γ, γ'), E(max)=14 MeV(γ from bremsstrahlung); measured Eγ, Iγ. 19F, 23Na, 27Al, 31P deduced levels, level-width. Natural target.
doi: 10.1016/0375-9474(72)90214-X
1970SH08 Phys.Lett. 32B, 473 (1970) Nuclear Photo-Excitation of T = 3/2 States in 23Na and 31P NUCLEAR REACTIONS 23Na, 31P(γ, γ'), E < 14 MeV; measured σ(Eγ'), nuclear resonance fluorescence. 23Na, 31P levels deduced level-width.
doi: 10.1016/0370-2693(70)90388-6
1969SH05 J.Phys.Soc.Japan 26, 1319(1969) Nuclear Resonant Scattering of 6734-keV Lead Capture Gamma Rays from Tin NUCLEAR REACTIONS Sn(γ, γ), E = 6734 keV; measured resonance scattering. Ge(Li) detector.
doi: 10.1143/JPSJ.26.1319
1969SH10 J.Phys.Soc.Japan 27, 273 (1969) The Ground-State Transition Width of the 7368-keV Level of 66Zn NUCLEAR REACTIONS 66Zn(γ, γ), E=7368 keV; measured resonance scattering. 66Zn level deduced level-width. Ge(Li) detector.
doi: 10.1143/JPSJ.27.273
1968SH14 Nucl.Phys. A118, 114 (1968) Nuclear Photoexcitation of the 7368 keV Level of 66Zn by Lead Capture Gamma Rays NUCLEAR REACTIONS 66Zn(γ, γ'), Eγ=7368 keV; measured resonance fluorescence, σ(Eγ', θ). 66Zn deduced levels, J. Natural target, Ge(Li) detector.
doi: 10.1016/0375-9474(68)90190-5
1966SH07 J.Phys.Soc.Japan 21, 829 (1966) N.Shikazono, H.Takekoshi, T.Shoji Mossbauer Effect Studies of the 46.48-keV Level of W183 NUCLEAR STRUCTURE 183W, 182W; measured not abstracted; deduced nuclear properties.
doi: 10.1143/JPSJ.21.829
1965SH04 J.Phys.Soc.Japan 20, 271 (1965) N.Shikazono, H.Takekoshi, T.Shoji Nuclear Hyperfine Structure in W182 NUCLEAR STRUCTURE 182W; measured not abstracted; deduced nuclear properties.
1963SH11 J.Phys.Soc.Japan 18, 925 (1963) Recoil-Free Resonant Absorption of 35.3 keV Gamma Rays of Te125 and Hyperfine Structure of Absorption Spectrum NUCLEAR STRUCTURE 125Te; measured not abstracted; deduced nuclear properties.
doi: 10.1143/JPSJ.18.925
1961TA09 J.Phys.Soc.Japan 16, 1674 (1961) H.Takahashi, N.Shikazono, P.K.Tseng Weak Gamma Rays in the Decay of La140 NUCLEAR STRUCTURE 140La; measured not abstracted; deduced nuclear properties.
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