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NSR database version of May 22, 2024.

Search: Author = H.Tomura

Found 11 matches.

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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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