NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = T.Horiguchi Found 30 matches. 2003II03 Phys.Rev. C 68, 054328 (2003) H.Iimura, M.Koizumi, M.Miyabe, M.Oba, T.Shibata, N.Shinohara, Y.Ishida, T.Horiguchi, H.A.Schuessler Nuclear moments and isotope shifts of 135La, 137La, and 138La by collinear laser spectroscopy NUCLEAR MOMENTS 135,137,138,139La; measured hfs, isotope shifts, μ, quadrupole moments. Collinear laser spectroscopy.
doi: 10.1103/PhysRevC.68.054328
2000OH02 Nucl.Phys. A665, 3 (2000) T.Ohsawa, T.Horiguchi, M.Mitsuhashi Multimodal Analysis of Prompt Neutron Spectra for 238Pu(sf), 240Pu(sf), 242Pu(sf) and 239Pu(nth, f) RADIOACTIVITY 238,240,242Pu(SF); calculated prompt neutron spectra. Multimodal fission model, comparison with data. NUCLEAR REACTIONS 239Pu(n, F), E=thermal; calculated prompt neutron spectra. Multimodal fission model, comparison with data.
doi: 10.1016/S0375-9474(99)00686-7
1999IS02 Phys.Rev. C59, 1794 (1999) Y.Ishida, H.Iimura, S.Ichikawa, T.Horiguchi Mean-Square Nuclear Charge Radius of Radioactive 144Ce by Laser Spectroscopy NUCLEAR MOMENTS 136,138,140,142,144Ce; measured isotope shifts; deduced mean square charge radii, quadrupole deformation. Collinear laser-ion-beam spectroscopy.
doi: 10.1103/PhysRevC.59.1794
1999KU26 J.Phys.Soc.Jpn. 68, 1877 (1999) T.Kuwamoto, I.Endo, A.Fukumi, T.Horiguchi, M.Iinuma, Y.Ishida, T.Kondo, H.Matsuzaki, T.Takahashi Hyperfine Constants and Tensor Polarizabilities of 4f66s6p9G0-6 States in Sm I NUCLEAR MOMENTS 147,149Sm; measured hfs, isotope shifts. Atomic-beam laser spectroscopy.
doi: 10.1143/JPSJ.68.1877
1999OH06 Nucl.Phys. A653, 17 (1999) T.Ohsawa, T.Horiguchi, H.Hayashi Multimodal Analysis of Prompt Neutron Spectra for 237Np(n, f) NUCLEAR REACTIONS 237Np(n, F), E=0.3-5.5 MeV; calculated prompt neutron spectra. Multimodal fission model, comparisons with data.
doi: 10.1016/S0375-9474(99)00156-6
1997IS06 J.Phys.(London) B30, 2569 (1997) Y.Ishida, H.Iimura, S.Ichikawa, T.Horiguchi Isotope Shifts of Optical Transitions in Ce II by Collinear Laser-Ion-Beam Spectroscopy NUCLEAR MOMENTS 136,138,140,142Ce; measured optical isotope shifts; deduced nuclear charge radius differences, atomic level configurations. ATOMIC PHYSICS 136,138,140,142Ce; measured optical isotope shifts; deduced nuclear charge radius differences, atomic level configurations.
doi: 10.1088/0953-4075/30/11/009
1997KO33 Z.Phys. D39, 209 (1997) T.Kobayashi, I.Endo, A.Fukumi, T.Horiguchi, Y.Ishida, T.Kondo, T.Kuwamoto, N.Minamoto, T.Nakamura, T.Takahashi Measurement of Hyperfine Structure Constants, g Values and Tensor Polarizability of Excited States of Sm I NUCLEAR MOMENTS 144,147,148,149,150,152,154Sm; measured hfs, Zeeman spectra; deduced hfs constants.
doi: 10.1007/s004600050130
1996KU30 J.Phys.Soc.Jpn. 65, 3180 (1996) T.Kuwamoto, I.Endo, A.Fukumi, T.Hasegawa, T.Horiguchi, Y.Ishida, T.Kobayashi, T.Kondo, T.Takahashi Systematic Study of Fine and Hyperfine Structures in Pr I by Doppler-Free Atomic-Beam Laser Spectroscopy NUCLEAR MOMENTS 141Pr; measured optical hfs; deduced hyperfine constants. Double-free atomic-beam laser spectroscopy.
doi: 10.1143/JPSJ.65.3180
1996MA72 Radiochim.Acta 72, 39 (1996) M.Magara, N.Shinohara, Y.Hatsukawa, K.Tsukada, H.Iimura, S.Usuda, S.-I.Ichikawa, T.Suzuki, Y.Nagame, Y.Kobayashi, M.Oshima, T.Horiguchi Decay Properties of 245Cf RADIOACTIVITY 244,246Cf(α); 245Cf(α), (EC), (β+); 240,242Cm(α) [from 238U(12C, X), E=81, 87 MeV]; measured Eα, Iα, αγ-, γγ-coin, E X-ray, I X-ray. 245Cf deduced α-decay T1/2, branching ratio. 241Cm deduced levels, J, π, Nilsson assignments. NUCLEAR REACTIONS 238U(12C, X), (12C, 5n), E=81, 87 MeV; measured Eα, Iα, αγ-, γγ-coin, E X-ray, I X-ray. 245Cf deduced α-decay T1/2, branching ratio. 241Cm deduced levels, J, π, Nilsson assignments.
1995LE19 Phys.Rev. C51, 2770 (1995) Y.S.Lee, M.Kobayashi, T.Hukutome, T.Horiguchi, H.Inoue Experimental Search for a 17-keV Neutrino in the Internal Bremsstrahlung Spectrum of 71Ge RADIOACTIVITY 71Ge(EC); measured internal bremsstrahlung spectra; deduced 17 keV ν mixing fraction upper limit, possibility exclusion. Background, impurities, pileup contributions considered carefully, ultra large size hyperpure Ge detector.
doi: 10.1103/PhysRevC.51.2770
1994II01 Phys.Rev. C50, 661 (1994) H.Iimura, Y.Nakahara, S.Ichikawa, M.Kubota, T.Horiguchi Nuclear Moments of 143Pr by Laser Spectroscopy RADIOACTIVITY 143Pr(β-) [from 142Ce(n, γ)143Ce(β-decay)]; measured hfs; deduced μ, quadrupole moment. Collinear fast-beam laser spectroscopy. Interacting boson-fermion model.
doi: 10.1103/PhysRevC.50.661
1994JI08 Phys.Rev. A49, 4398 (1994) W.G.Jin, T.Horiguchi, W.Yang, I.Endo J Dependences of the Isotope Shift and Hyperfine Structure in the Sm I 4f65d6s 9H Term NUCLEAR MOMENTS 144,148,150,152,154,147,149Sm; measured isotope shifts, hfs; deduced hyperfine parameters for 147,149Sm.
doi: 10.1103/PhysRevA.49.4398
1993SU16 Nucl.Phys. A557, 653c (1993) M.Sugawara, H.Kusakari, T.Morikawa, H.Inoue, Y.Yoshizawa, A.Virtanen, M.Piiparinen, T.Horiguchi Octupole Bands of Gd Isotopes NUCLEAR REACTIONS 154Gd(58Ni, 58Ni'), E=228 MeV; 154Gd(48Ti, 48Ti'), E=177.6 MeV; 154,156,158Gd(32S, 32S'), E=118 MeV; 160Gd(58Ni, 58Ni'), E=225 MeV; measured Eγ, Iγ, γγ-coin following Coulomb excitation. 154,156,158,160Gd deduced levels, J, π, B(λ), γ branching, band structure.
doi: 10.1016/0375-9474(93)90577-K
1992JI06 Hyperfine Interactions 74, 310 (1992) W.G.Jin, T.Horiguchi, M.Wakasugi, T.Hasegawa, W.Yang Systematic Study of Isotope Shifts and Hyperfine Structures in YbI by Atomic-Beam Laser Spectroscopy RADIOACTIVITY 171,173Yb; measured hfs, isotope shifts; deduced hyperfine constants. Atomic beam laser spectroscopy, other isotopes studied.
doi: 10.1007/BF02398640
1992KO20 Hyperfine Interactions 74, 181 (1992) M.Koizumi, T.T.Inamura, K.Morita, M.Takami, M.Wakasugi, A.Yoshida, M.Azuma, H.Katsuragawa, T.Horiguchi, T.Ishizuka, I.Nakamura, M.Nakaoka, A.Iivonen, K.Valli, S.Matsuki, T.Murayama, K.Shimomura, T.Shinozuka, I.Sugai, Y.Tagishi Collinear Fast Atomic-Beam Laser Spectroscopy at RIKEN GARIS/IGISOL NUCLEAR REACTIONS 9Be(166Er, xn), E=16.3 MeV/nucleon; measured Iγ; deduced 169Hf yield Hf isotope yield for fusion reaction. Fast atomic-beam collinear laser spectroscopy.
doi: 10.1007/BF02398628
1992NA18 Hyperfine Interactions 74, 312 (1992) Y.Nakahara, H.Iimura, S.Ichikawa, K.Kotani, M.Wakasugi, T.Horiguchi Measurement of Hyperfine Structure in Pr II by Collinear Laser-Ion-Beam Spectroscopy NUCLEAR MOMENTS 141Pr; measured hfs; deduced hyperfine constants. Collinear laser-ion-beam spectroscopy.
doi: 10.1007/BF02398641
1992WA30 Hyperfine Interactions 74, 316 (1992) M.Wakasugi, T.Horiguchi, W.G.Jin, Y.Watanabe, W.Yang Observation of ΔJ = 2 Forbidden Transition and Anomalous Isotope Shift in NdI Induced by Second-Order Hyperfine Perturbation NUCLEAR MOMENTS 142,143,144,145,146Nd; measured hfs, isotope shift anomalies. Atomic-beam laser spectroscopy induced second-order hyperfine perturbation.
doi: 10.1007/BF02398645
1991JI06 J.Phys.Soc.Jpn. 60, 2896 (1991) W.-G.Jin, T.Horiguchi, M.Wakasugi, T.Hasegawa, W.Yang Systematic Study of Isotope Shifts and Hyperfine Structure in Yb I by Atomic-Beam Laser Spectroscopy NUCLEAR MOMENTS 168,170,171,172,173,174,176Yb; measured hfs, isotope shifts; deduced charge radii changes, 171,173Yb hyperfine constants. Atomic-beam laser spectroscopy.
doi: 10.1143/JPSJ.60.2896
1990II02 J.Phys.Soc.Jpn. 59, 4208 (1990) H.Iimura, Y.Nakahara, S.-I.Ichikawa, K.Kotani, M.Wakasugi, T.Horiguchi Measurement of Hyperfine Structure of the 4f35d5G-4f36p5H in PrII by Collinear Laser-Ion-Beam Spectroscopy NUCLEAR MOMENTS 141Pr; measured hfs; deduced hyperfine constants. Collinear laser-ion-beam spectroscopy.
doi: 10.1143/JPSJ.59.4208
1990JI06 Phys.Rev. A42, 1416 (1990) W.G.Jin, H.Sakata, M.Wakasugi, T.Horiguchi, Y.Yoshizawa J Dependences of the Isotope Shift and Hyperfine Structure in Gd I 4f75d6s9D, 4f75d6s6p 9D, and 9F Terms NUCLEAR MOMENTS 152,154,155,156,157,158,160Gd; measured isotope shifts. 155,157Gd deduced electric quadrupole moments, hyperfine constants.
doi: 10.1103/PhysRevA.42.1416
1990JI07 J.Phys.Soc.Jpn. 59, 3148 (1990) W.G.Jin, T.Horiguchi, M.Wakasugi, Y.Yoshizawa Hyperfine Structure and Isotope Shift in Er I by the Atomic-Beam Laser Spectroscopy NUCLEAR MOMENTS 162,164,166,167,168,170Er; measured hfs, isotope shifts; deduced hyperfine parameters. 162,164,166,167,168,170Er deduced rms charge radii, deformation parameter values.
1990WA25 J.Phys.Soc.Jpn. 59, 2700 (1990) M.Wakasugi, T.Horiguchi, W.G.Jin, H.Sakata, Y.Yoshizawa Changes of the Nuclear Charge Distribution of Nd, Sm, Gd and Dy from Optical Isotope Shifts NUCLEAR MOMENTS 142,144,146,148,150,143,145Nd, 144,148,150,152,154,147,149Sm, 152,154,156,158,160,155,157Gd, 156,158,160,162,164,161,163Dy; measured isotope shifts, hfs; deduced rms charge radii changes, nuclear parameter. Atomic beam laser spectroscopy.
doi: 10.1143/JPSJ.59.2700
1986EB01 Z.Phys. A323, 119 (1986) J.Eberz, U.Dinger, T.Horiguchi, G.Huber, H.Lochmann, R.Menges, R.Kirchner, O.Klepper, T.Kuhl, D.Marx, E.Roeckl, D.Schardt, G.Ulm Collinear Laser Spectroscopy on 108g,108mIn using an Ion Source with Bunched Beam Release RADIOACTIVITY 108,108mIn(EC), (β+) [from 97Mo(16O, 4np)]; measured hfs, isotope shifts. 108,108mIn deduced μ, nuclear rms charge radii, quadrupole moment, J. Collinear laser spectroscopy, bunched beam release ion source.
1986SH26 Phys.Rev. C34, 909 (1986) N.Shinohara, S.Usuda, S.Ichikawa, T.Suzuki, M.Magara, H.Okashita, H.Yoshikawa, T.Horiguchi, Y.Iwata, S.Shibata, I.Fujiwara Actinides Produced by 12C + 242Pu and 16O + 238U Reactions NUCLEAR REACTIONS 238U(16O, X)244Cf/245Cf/246Cf/250Fm, E=85-125 MeV; 242Pu(12C, X)244Cf/245Cf/246Cf/250Fm, E=65-95 MeV; 238U(16O, 4n)250Fm, E=92 MeV; 242Pu(12C, 4n)250Fm, E=72 MeV;238U(16O, 4nα)246Cf, E=97 MeV; 238U(16O, 5nα)245Cf, E=105 MeV;242Pu(12C, 4nα)246Cf, E=83 MeV;242Pu(12C, 5nα)245Cf, E=90 MeV;238U(16O, X)242Cm, E=85-125 MeV;242Pu(12C, X)242Am/242Cm/243Cm/244Cm, E = 65-95 MeV; measured residual production σ(E). 254Fm; deduced Coulomb barrier role, α-cluster transfer mechanism. Radiochemical methods. Evaporation code analysis. Comparison with available data. NUCLEAR REACTIONS 238U(16O, F)244Cf/245Cf/246Cf/250Fm/242Cm, E=85-145 MeV; 242Pu(12C, F)244Cf/245Cf/246Cf/250Fm/242Cm, E=60-120 MeV; calculated fission σ(E). ALICE nuclear mode code, comparison with experimental data.
doi: 10.1103/PhysRevC.34.909
1983HO24 Int.J.Appl.Radiat.Isotop. 34, 1531 (1983) T.Horiguchi, H.Kumahora, H.Inoue, Y.Yoshizawa Excitation Functions of Ge(p, xnyp) Reactions and Production of 68Ge NUCLEAR REACTIONS, ICPND Ge(p, xnyp)68Ge, Ge(p, xnp)68Ge/69Ge, Ge(p, xnα)66Ga/67Ga, Ge(p, xnpα)65Zn, E=19-64 MeV; measured residuals production σ(E), 68Ge thick target yield. Activation technique.
doi: 10.1016/0020-708X(83)90288-0
1980HO16 Int.J.Appl.Radiat.Isotop. 31, 141 (1980) T.Horiguchi, H.Noma, Y.Yoshizawa, H.Takemi, H.Hasai, Y.Kiso Excitation Functions of Proton Induced Nuclear Reactions on 85Rb NUCLEAR REACTIONS 85Rb(p, xn), E=14-70 MeV; measured σ(E) for x=3-5; 85Rb(p, xnp), E=14-70 MeV; measured σ(E) for x=1-4; 85Rb(p, 3nα), E=40-70 MeV; measured σ(E); deduced reaction mechanism, 81Rb thick target yields, 81,84Rb isomeric σ ratio.Enriched target, activation method, Ge(Li) detector.
doi: 10.1016/0020-708X(80)90138-6
1980HO28 J.Phys.Soc.Jpn. 49, 1205 (1980) Decay of 81Sr RADIOACTIVITY 81Sr [from 85Rb(p, 5n)]; measured Eγ, Iγ, T1/2; deduced log ft. 81Rb deduced levels, J, π. Low energy photon spectrometer, Ge(Li) detector.
doi: 10.1143/JPSJ.49.1205
1977NO05 J.Inorg.Nucl.Chem. 39, 1973 (1977) H.Noma, T.Horiguchi, Y.Yoshizawa, I.Fujiwara, S.Kume, K.Chida, T.Matsui, S.Amemiya, T.Katoh Cross Sections of the 63Cu(p, 3n)61Zn and the 63Cu(p, p3n)60Cu Reactions NUCLEAR REACTIONS 63Cu(p, 3n), E=30-47 MeV; 63Cu(p, 3np), E ≤ 52 MeV; measured σ(E).
doi: 10.1016/0022-1902(77)80518-6
1976YO05 Nucl.Instrum.Methods 134, 93 (1976) Y.Yoshizawa, H.Noma, T.Horiguchi, T.Katoh, S.Amemiya, M.Itoh, K.Hisatake, M.Sekikawa, K.Chida Isotope Separator on-Line at INS FM Cyclotron NUCLEAR REACTIONS Cu(p, xn), E=52 MeV; measured 60,61,62,63Zn yields.
doi: 10.1016/0029-554X(76)90128-2
1972YA02 Phys.Lett. 39B, 182 (1972) T.Yamaya, T.Horiguchi, S.Morita, K.Miura The l(n)-Dependence of Excitation Functions for the 89Y(d, p)90Y Reaction below the Coulomb Barrier NUCLEAR REACTIONS 89Y(d, p), E=3.0-4.5 MeV; measured σ(E;θ). 90Y levels deduced L(n), J, π.
doi: 10.1016/0370-2693(72)90768-X
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