NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = H.Tomura Found 11 matches. 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
1995SA35 Nucl.Phys. A588, 229c (1995) K.Sato, S.Yamada, H.Ogawa, K.Kawachi, N.Araki, A.Itano, M.Kanazawa, A.Kitagawa, T.Kohno, M.Kumada, T.Murakami, M.Muramatsu, K.Noda, S.Sato, Y.Sato, E.Takada, A.Tanaka, K.Tashiro, M.Torikoshi, J.Yoshizawa, M.Endo, Y.Furusawa, T.Kanai, H.Koyama-Ito, N.Matsufuji, S.Minohara, N.Miyahara, F.Soga, M.Suzuki, H.Tomura, Y.Hirao Performance of HIMAC
doi: 10.1016/0375-9474(95)00144-P
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
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
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
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
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
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