NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = T.Kuroyanagi Found 40 matches. 1998EL11 Eur.Phys.J. A 3, 133 (1998) A.M.El-Badry, T.Kuroyanagi, S.Mitarai, A.Odahara, Y.Gono, S.Morinobu, K.Ogawa Recoil Distance Half-Life Measurements of the Excited States in 145Sm NUCLEAR REACTIONS 139La(10B, 4n), E=49 MeV; measured Eγ, Iγ, (X-ray)γ-coin, Doppler-shifted spectra. 145Sm deduced levels, J, π, T1/2, configurations. Shell model calculation. Recoil distance technique.
doi: 10.1007/s100500050159
1996OD01 Z.Phys. A354, 231 (1996) A.Odahara, Y.Gono, S.Mitarai, T.Shizuma, E.Ideguchi, J.Mukai, H.Tomura, B.J.Min, S.Suematsu, T.Kuroyanagi, K.Heiguchi, T.Komatsubara, K.Furuno The β-Decay of 88Tc RADIOACTIVITY 88,88mTc(β+) [from 58Ni(32S, np), E=100-105 MeV]; measured Eγ, Iγ, βγ-, γγ-coin, T1/2; deduced Q(EC), Eβ(max). 88Tc levels deduced J, π, decay scheme.
doi: 10.1007/BF02769518
1996SH27 J.Phys.Soc.Jpn. 65, 3172 (1996) M.Shibata, A.Odahara, S.Mitarai, Y.Gono, M.Kidera, K.Miyazaki, T.Kuroyanagi Anomalous Q(EC)-Values of T(z) = 1 Nuclei, 80Y, 84Nb and 88Tc RADIOACTIVITY 80Y(β+) [from 54Fe(28Si, np), E=88 MeV]; 84Nb(β+) [from 58Ni(28Si, np), E=88 MeV]; 88Tc(β+) [from 58Ni(32S, np), E=100 MeV]; measured βγ-coin; deduced Q(EC), anomalies.
doi: 10.1143/JPSJ.65.3172
1995RO06 J.Phys.(London) G21, L1 (1995) H.A.Roth, S.E.Arnell, J.Blomqvist, D.Foltescu, T.Kuroyanagi, S.Mitarai, A.Nilsson, J.Nyberg, O.Skeppstedt First Observation of the Neutron-Deficient Nucleus 93Rh NUCLEAR REACTIONS 58Ni(40Ca, 2n3p), E=187 MeV; measured Eγ, Iγ, (particle)γ-, γγ-coin. 93Rh deduced high-spin levels, J, π. Enriched target, Ge detector array, particle-multiplicity filter.
doi: 10.1088/0954-3899/21/2/001
1995SU27 J.Phys.Soc.Jpn. 64, 329 (1995) M.Sugawara, S.Mitarai, T.Kuroyanagi, J.Mukai, H.Tomura, T.Morikawa, D.Jerrestam, J.Nyberg, G.Sletten, A.Atac, N.Gjorup, A.Virtanen, S.-E.Arnell, O.Skeppstedt, H.A.Roth, D.Foltescu High Spin States in 79Rb NUCLEAR REACTIONS 58Ni(28Si, 3pα), E=128 MeV; measured γγ-coin. 79Rb deduced high-spin levels, J, π, band structure.
doi: 10.1143/JPSJ.64.329
1994AR33 Phys.Rev. C49, 51 (1994) S.E.Arnell, D.Foltescu, H.A.Roth, O.Skeppstedt, J.Blomqvist, A.Nilsson, T.Kuroyanagi, S.Mitarai, J.Nyberg Yrast Level Structure of the Neutron Deficient N = 49 Isotones 92Tc, 93Ru, 94Rh, and 95Pd up to High Angular Momentum NUCLEAR REACTIONS 58Ni(40Ca, X), E=180 MeV; measured γγ-coin, Eγ, Iγ. 92Tc, 93Ru, 94Rh, 95Pd deduced high-spin levels, J, π, band structure, configuration.
doi: 10.1103/PhysRevC.49.51
1994MU02 Nucl.Phys. A568, 202 (1994) J.Mukai, A.Odahara, H.Tomura, S.Suematsu, S.Mitarai, T.Kuroyanagi, D.Jerrestam, J.Nyberg, G.Sletten, A.Atac, S.E.Arnell, H.A.Roth, O.Skeppstedt High-Spin States in the Odd-Odd Nucleus 82Y NUCLEAR REACTIONS 58Ni(28Si, n3p), E=100, 102, 128 MeV; measured Eγ, Iγ, Iγ(θ), (particle)γ-, γγ-coin. 82Y deduced levels, J, π. Enriched target, Ge detector array, particle-multiplicity filter.
doi: 10.1016/0375-9474(94)90010-8
1994RO08 Phys.Rev. C50, 1330 (1994) H.A.Roth, S.E.Arnell, D.Foltescu, O.Skeppstedt, J.Blomqvist, A.Nilsson, T.Kuroyanagi, S.Mitarai, J.Nyberg Gaps in the Yrast Level Structure of the N = 50 Isotones 93Tc, 94Ru, and 95Rh at High Angular Momentum NUCLEAR REACTIONS 58Ni(40Ca, X), E=180 MeV; measured Eγ, Iγ, γ(θ). 93Tc, 94Ru, 95Rh deduced high-spin levels, J, π, T1/2. Multidetector array NORDBALL including particle selection. Shell model comparison.
doi: 10.1103/PhysRevC.50.1330
1994SH07 Z.Phys. A348, 25 (1994) T.Shizuma, M.Kidera, E.Ideguchi, A.Odahara, H.Tomura, S.Suematsu, T.Kuroyanagi, Y.Gono, S.Mitarai, J.Mukai, T.Komatsubara, K.Furuno, K.Heiguchi The β+ Decay of the New Isotope 86Mo and the First Observation of 86mNb RADIOACTIVITY 86Mo(β+) [from 54Fe(35Cl, 2np), E=103 MeV; 58Ni(32S, 2n2p), E=120 MeV]; measured βγ-, γγ-coin, βγ(t), γγ(t), I(X-ray)/Iγ; deduced T1/2, maximum Eβ+. 86Nb deduced levels, possible J, π, ICC.
doi: 10.1007/BF01291648
1993AR07 Nucl.Phys. A557, 477c (1993) S.E.Arnell, D.Foltescu, T.Kuroyanagi, S.Mitarai, A.Nilsson, H.A.Roth, O.Skeppstedt In-Beam Gamma Ray Study of Neutron Deficient Nuclei with A ≈ 90 NUCLEAR REACTIONS 58Ni(40Ca, X), E=147-187 MeV; measured γ spectra. 91Tc, 92Ru deduced levels. Shell model. In-beam study. NUCLEAR STRUCTURE 90Mo, 91Tc, 92Ru; calculated levels. Shell model.
doi: 10.1016/0375-9474(93)90564-E
1993MI07 Z.Phys. A344, 405 (1993) S.Mitarai, T.Kuroyanagi, A.Odahara, J.Mukai, H.Tomura, S.Suematsu, D.Jerrestam, J.Nyberg, G.Sletten, A.Atac, N.Gjorup, J.Jongman, S.E.Arnell, H.A.Roth, O.Skeppstedt A Rotational Band in 82Zr NUCLEAR REACTIONS 58Ni(28Si, 2n2p), E=128 MeV; measured γγ-coin. 82Zr deduced levels, J, π, band structure.
doi: 10.1007/BF01283195
1993MI11 Nucl.Phys. A557, 381c (1993) S.Mitarai, T.Kuroyanagi, A.Odahara, J.Mukai, H.Tomura, S.Suematsu, T.Morikawa, D.Jerrestam, J.Nyberg, G.Sletten, A.Atac, M.Piiparinen, S.E.Arnell, D.Foltescu, H.A.Roth, O.Skeppstedt Band Structures of Nuclei Around N, Z = 40 Selected by Charged Particle Detection NUCLEAR REACTIONS 58Ni(28Si, 4p), E=128 MeV; 58Ni(32S, 4p), E=125 MeV; measured relative yield with respect to 1p, 2p, 3p exit channels. 58Ni(28Si, pα), E=100 MeV; 58Ni(32S, p2α), (32S, pα), E=120, 125 MeV; measured γγ-, pα-coin. 85Nb, 81Y deduced levels, J, π, yrast band dynamic moment of inertia. 58Ni(28Si, 2n2p), E=128 MeV; measured γ(particle)-coin. 82Zr deduced levels, J, π. 58Ni(32S, 2n2p), E=125 MeV; measured γγ-coin. 86Mo deduced possible yrast level transitions.
doi: 10.1016/0375-9474(93)90555-C
1992KU23 Nucl.Instrum.Methods Phys.Res. A316, 289 (1992) T.Kuroyanagi, S.Mitarai, S.Suematsu, B.J.Min, H.Tomura, J.Mukai, T.Maeda, R.Nakatani, G.Sletten, J.Nyberg, D.Jerrestam The Silcon Ball: A 4π Si detector array for reaction channel selection NUCLEAR REACTIONS 58Ni(28Si, X), E=95, 110 MeV; measured charged particle energy spectra, γ(particle)-, γγ-coin. Seventeen charged particle 4π Si detector.
doi: 10.1016/0168-9002(92)90912-N
1992MU12 Z.Phys. A342, 393 (1992) J.Mukai, A.Odahara, R.Nakatani, Y.Haruta, H.Tomura, B.J.Min, K.Heiguchi, S.Suematsu, S.Mitarai, T.Kuroyanagi The β Decay of the New Isotope 79Y NUCLEAR REACTIONS 54Fe(28Si, 2np), E=92 MeV; measured γγ(t), γβ(t), βγ-coin; deduced evidence for 79Y. RADIOACTIVITY 79Y(β+) [from 54Fe(28Si, 2np), E=97 MeV]; measured γγ(t), γβ(t), βγ-coin; deduced T1/2, Q(EC), J, π. 79Sr level deduced possible J, π.
doi: 10.1007/BF01294949
1991HE04 Z.Phys. A338, 7 (1991) K.Heiguchi, T.Hosoda, T.Komatsubara, T.Nomura, K.Furuno, R.Nakatani, S.Mitarai, T.Kuroyanagi Half-Lives and Q(β) Measurements for New Nuclei of 89Tc and 89mTc NUCLEAR REACTIONS 60Ni(32S, 2np), E=95 MeV; 58Ni(35Cl, 2n2p), E=135 MeV; measured βγ-, γ(X-ray)-, γγ-coin. RADIOACTIVITY 89m,89Tc [from 60Ni(32S, 2np), E=95 MeV; 58Ni(35Cl, 2n2p), E=135 MeV]; measured βγ-, γ(X-ray)-, γγ-coin, Eγ, Iγ, T1/2; deduced Q(EC).
doi: 10.1007/BF01279110
1991MI15 Nucl.Phys. A530, 211 (1991) B.J.Min, S.Suematsu, S.Mitarai, T.Kuroyanagi, K.Heiguchi, M.Matsuzaki The Level Structure of 87Nb RADIOACTIVITY 87Mo [from 58Ni(32S, n2p)]; 87,87mNb [from 58Ni(32S, 3p), E=105 MeV]; measured Eγ, Iγ, T1/2, I(ce). 87Nb deduced levels, J, π, ICC, γ-multipolarity. Enriched target, Si(Au) detector, intrinsic, GAMMA-X Ge detectors, plastic scintillator. NUCLEAR REACTIONS 58Ni(32S, 3p), E=103 MeV; measured Eγ, Iγ, Iγ(θ), (particle)γ-, γγ-coin. 87Nb deduced levels, J, π, δ. Enriched target, Ge, Si detectors.
doi: 10.1016/0375-9474(91)90764-W
1989MI08 Nucl.Instrum.Methods Phys.Res. A277, 491 (1989) S.Mitarai, K.Setoguchi, T.Maeda, Y.Haruta, H.Tomura, B.J.Min, K.Heiguchi, S.Suematsu, Y.Ishikawa, T.Kuroyanagi, K.Toyoshima A Charged Particle Multiplicity Filter for Nuclidic Identification of the Specific Gamma Rays NUCLEAR REACTIONS 60Ni(28Si, xnypzα), E=90 MeV; measured γ(charged particle)-coin, Eγ, Iγ, nγ-coin. Charge particle multiplicity filter.
doi: 10.1016/0168-9002(89)90780-8
1988KU14 Nucl.Phys. A484, 264 (1988) T.Kuroyanagi, S.Mitarai, B.J.Min, H.Tomura, Y.Haruta, K.Heiguchi, S.Suematsu, Y.Onizuka New Neutron-Deficient Isotopes 83Nb and 85Nb RADIOACTIVITY 85Nb(β+) [from 58Ni(32S, αp), 60Ni(28Si, p2n)]; 83Nb(β+) [from 58Ni(28Si, p2n)]; measured βγ-coin, T1/2, E(γ), I(γ), Eβ(max), Q(β), masses. 83,85Zr deduced levels, T1/2. Enriched target, Ge, plastic scintillator detectors.
doi: 10.1016/0375-9474(88)90072-3
1988SU15 Nucl.Phys. A485, 304 (1988) S.Suematsu, Y.Haruta, B.J.Min, K.Heiguchi, Y.Ishikawa, S.Mitarai, T.Kuroyanagi, Y.Onizuka The Nuclear Structure of 83Zr NUCLEAR REACTIONS 58Ni(28Si, n2p), E=85-100 MeV; measured E(γ), I(γ)(θ), I(γ)(E), nγγ-, nγ-, (charged-particle)γ-coin. 83Zr deduced levels, J, π. Enriched target, Ge, Ge(Li), NE213, segmented Si surface barrier detectors.
doi: 10.1016/0375-9474(88)90105-4
1987HE21 Nucl.Phys. A474, 484 (1987) K.Heiguchi, S.Mitarai, B.J.Min, T.Kuroyanagi The States of 73Se Populated by the Beta Decay of 73Br NUCLEAR REACTIONS 60Ni(16O, 2np), E=60 MeV; measured Eγ, Iγ, I(ce), γγ-, βγ-, γ(ce)-coin. RADIOACTIVITY 73Br(β+), (EC) [from 60Ni(16O, 2np), E=60 MeV]; measured Eγ, Iγ, I(ce), γγ-, βγ-, γ(ce)-coin; deduced T1/2. 73Se deduced levels, J, π, ICC.
doi: 10.1016/0375-9474(87)90627-0
1983IS07 Nucl.Phys. A403, 396 (1983) Y.Ishikawa, N.Kato, S.Suematsu, T.Kuroyanagi The Level Structure of 75Ge by the 74Ge(d, pγ) Reaction NUCLEAR REACTIONS 74Ge(d, pγ), E=6 MeV; measured Ep, Eγ, Iγ(θ), pγ-coin. 75Ge deduced levels, J, π, γ-mixing, γ-branching. Enriched target, Si-Au, Ge(Li) detectors.
doi: 10.1016/0375-9474(83)90234-8
1982IS07 Nucl.Phys. A380, 438 (1982) Y.Ishikawa, N.Kato, S.Suematsu, T.Kuroyanagi A New 5/2+ Level at 192.5 keV in 75Ge NUCLEAR REACTIONS 74Ge(d, pγ), E=6 MeV; measured Eγ, Iγ, T1/2, pγ-coin. 75Ge deduced level, J, π, ICC, B(M1), B(E2). Enriched target, Ge(Li) detector.
doi: 10.1016/0375-9474(82)90569-3
1975ON01 J.Phys.Soc.Jap. 38, 308 (1975) Y.Onizuka, T.Sugimitsu, N.Kato, T.Kuroyanagi The Level Structure of 71Ge by the 71Ga(p, n)71Ge Reaction NUCLEAR REACTIONS 71Ga(p, n), E=1.5-5.0 MeV; measured σ(E, Eγ), I(ce), γce-coin. 71Ge deduced levels, ICC, λ, γ-mixing.
doi: 10.1143/JPSJ.38.308
1973IS02 J.Phys.Soc.Jap. 35, 341 (1973) A.Isoya, T.Kuroyanagi, Y.Nakajima, T.Maki, T.Nakashima, N.Kato, T.Sugimitsu, K.Kimura, S.Mitarai, S.Uehara The Level Structure of 69Ge NUCLEAR REACTIONS 69Ga(p, nγ), E=3.4-5.0 MeV; measured Eγ, Iγ, σ(E), I(ce). Deduced ICC. 69Ge deduced levels, J, π, γ-branching, γ-multipolarities.
doi: 10.1143/JPSJ.35.341
1969KU07 Nucl.Phys. A133, 554 (1969) Levels in 185W from the Decay of 185mW and 185Ta RADIOACTIVITY 185W[from 186W(γ, n)]; measured Eγ, Iγ, I(ce), ICC. 185Ta[from W(γ, p)]; measured Eγ, Iγ, I(ce), Eβ, ICC, βγ-delay, Xγ-delay. 185W levels deduced J, π, T1/2, γ-mixing, γ-branching.
doi: 10.1016/0375-9474(69)90555-7
1969TA06 Nucl.Instr.Methods 67, 38 (1969) Internal Conversion Electron Measurement by a Si Surface Barrier Detector RADIOACTIVITY 57Co, 196Au, 137mBa, 185mW, 185Ta; measured E(ce). Si surface-barrier detector.
doi: 10.1016/0029-554X(69)90538-2
1965MI02 Nucl.Phys. 61, 25 (1965) K.Miyano, M.Ishihara, Y.Shida, H.Morinaga, T.Kuroyanagi, T.Tamura Gamma Rays Following Intermediate Energy Proton Bombardments and Collective States in Ba130 NUCLEAR REACTIONS 181Ta(p, xnγ), E=55 MeV; measured σ(Eγ). 178W deduced levels, J, π. 133Cs(p, xnγ), E=27-55 MeV; measured σ(E; Eγ). 130Ba deduced levels, J, π.
doi: 10.1016/0029-5582(65)90932-6
1964KU02 Nucl.Phys. 50, 417 (1964) T.Kuroyanagi, T.Tamura, K.Tanaka, H.Morinaga Potassium-47 NUCLEAR STRUCTURE 47K; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(64)90218-4
1964KU11 Prelim.Abstr.1964 Kyoto Meeting, Phys.Soc.Japan, p.74(1964) Measurement of 179m-W and 185m-W by Use of Semiconductor Detectors NUCLEAR STRUCTURE 185W, 179W; measured not abstracted; deduced nuclear properties.
1963AK04 Radiochim.Acta 2, 1 (1963) E.Akatsu, T.Kuroyanagi, T.Ishimori Photoproduction of Uranium-237 NUCLEAR STRUCTURE 237U; measured not abstracted; deduced nuclear properties.
doi: 10.1524/ract.1963.2.1.1
1963KU22 Nucl.Phys. 48, 675 (1963) Nuclear Spectroscopy of Tm173 NUCLEAR STRUCTURE 172Tm, 173Tm; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90232-3
1963MI17 Nucl.Phys. 49, 315 (1963) The New Nucleide Holmium-169 NUCLEAR STRUCTURE 169Ho; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90096-8
1961HO10 J.Phys.Soc.Japan 16, 841 (1961) S.Homma, T.Kuroyanagi, H.Morinaga Decay of Ir195 and Ir197 NUCLEAR STRUCTURE 197Ir, 195Ir; measured not abstracted; deduced nuclear properties.
doi: 10.1143/JPSJ.16.841
1961KU08 J.Phys.Soc.Japan 16, 2363 (1961) Decay of Sr83 NUCLEAR STRUCTURE 83Sr; measured not abstracted; deduced nuclear properties.
doi: 10.1143/JPSJ.16.2363
1961KU09 J.Phys.Soc.Japan 16, 2369 (1961) Decay of As79 NUCLEAR STRUCTURE 79As; measured not abstracted; deduced nuclear properties.
doi: 10.1143/JPSJ.16.2369
1961KU10 J.Phys.Soc.Japan 16, 2393 (1961) T.Kuroyanagi, H.Yuta, K.Takahashi, H.Morinaga New Activities in Rare Earth Region Produced by the (γ, p) Reactions NUCLEAR STRUCTURE 159Eu, 175Tm, 179Lu, 178Lu, 173Tm; measured not abstracted; deduced nuclear properties.
doi: 10.1143/JPSJ.16.2393
1961TA08 J.Phys.Soc.Japan 16, 1664 (1961) K.Takahashi, T.Kuroyanagi, H.Yuta, K.Kotajima, K.Nagatani, H.Morinaga Some New Activities Produced by Fast Neutron Bombardments NUCLEAR STRUCTURE 176Tm, 174Tm, 160Eu, 180Lu, 170Ho, 168Ho, 100Nb, 98Nb, 76Ga; measured not abstracted; deduced nuclear properties.
doi: 10.1143/JPSJ.16.1664
1960KU06 J.Phys.Soc.Japan 15, 2179 (1960) Decays of Photoreaction Products of Selenium NUCLEAR STRUCTURE 73Se, 79As, 81Se; measured not abstracted; deduced nuclear properties.
doi: 10.1143/JPSJ.15.2179
1960MO01 J.Phys.Soc.Japan 15, 213 (1960) H.Morinaga, T.Kuroyanagi, H.Mitsui, K.Shoda Three New Isotopes, Co63, Ga75, and As81 NUCLEAR STRUCTURE 63Co, 75Ga, 81As; measured not abstracted; deduced nuclear properties.
doi: 10.1143/JPSJ.15.213
1960TA25 Phys.Soc.Japan, Annual Meeting p.108 (October 1960) Y.Takahashi, K.Kotajima, H.Morinaga, T.Kuroyanagi, H.Yuta, K.Nagatani NUCLEAR STRUCTURE 98Nb; measured not abstracted; deduced nuclear properties.
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