NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = T.Nomura Found 95 matches. 2009HA11 Phys.Lett. B 674, 276 (2009) T.Hashimoto, H.Ishiyama, Y.X.Watanabe, Y.Hirayama, N.Imai, H.Miyatake, S.C.Jeong, M.-H.Tanaka, N.Yoshikawa, T.Nomura, S.Mitsuoka, K.Nishio, T.K.Sato, A.Osa, S.Ichikawa, M.Matsuda, H.Ikezoe, S.K.Das, Y.Mizoi, T.Fukuda, A.Sato, T.Shimoda, K.Otsuki, T.Kajino A new measurement of the astrophysical 8Li(d, t)7Li reaction NUCLEAR REACTIONS 2H(8Li, t), E=0.18, 0.24, 0.30, 0.40, 0.46, 0.60, 0.75 MeV/nucleon; measured charged-particle spectra, σ, σ(θ), σ(E); deduced 7Li excitation energy spectra, astrophysical reaction rate. Comparison with other data.
doi: 10.1016/j.physletb.2009.03.031
2007MA90 Eur.Phys.J. Special Topics 150, 37 (2007) M.Mazzocco, C.Signorini, M.Romoli, R.Bonetti, A.De Francesco, A.De Rosa, M.Di Pietro, L.Fortunato, T.Glodariu, A.Guglielmetti, G.Inglima, T.Ishikawa, H.Ishiyama, R.Kanungo, N.Khai, S.Jeong, M.La Commara, B.Martin, H.Miyatake, T.Motobayashi, T.Nomura, D.Pierroutsakou, M.Sandoli, F.Soramel, L.Stroe, I.Sugai, M.H.Tanaka, E.Vardaci, Y.Watanabe, A.Yoshida, K.Yoshida Elastic scattering for the system 11Be + 209Bi at Coulomb barrier energies NUCLEAR REACTIONS 209Bi(11Be, 11Be), E=38-50 MeV; measured elastic scattering σ(θ). Compared results to model calculations. Deduced reaction and fusion cross sections.
doi: 10.1140/epjst/e2007-00260-2
2007MI38 Prog.Theor.Phys.(Kyoto), Suppl. 168, 90 (2007) F.Miyahara, J.Kasagi, T.Nakabayashi, H.Fukasawa, R.Hashimoto, T.Ishikawa, T.Iwata, H.Kanda, T.Kinoshita, K.Maeda, K.Nawa, T.Nomura, H.Shimizu, T.Shishido, K.Suzuki, Y.Tajima, T.Takahashi, H.Ueno, H.Yamazaki, H.Y.Yoshida Narrow Resonance at Eγ = 1020 MeV in the D(γ, η)pn Reaction NUCLEAR REACTIONS 2H(γ, X), E=0.6-1.15 GeV; measured cross sections and angular distributions.
doi: 10.1143/PTPS.168.90
2006IS02 Nucl.Instrum.Methods Phys.Res. A560, 366 (2006) H.Ishiyama, T.Ishikawa, T.Hashimoto, Y.X.Watanabe, Y.Hirayama, N.Imai, H.Miyatake, M.H.Tanaka, Y.Fuchi, N.Yoshikawa, S.C.Jeong, H.Kawakami, I.Katayama, T.Nomura, S.Mitsuoka, K.Nishio, M.Matsuda, P.K.Saha, H.Ikezoe, S.K.Das, Y.Mizoi, T.Fukuda Production of a low-energy radioactive nuclear beam with high purity using JAERI-RMS NUCLEAR REACTIONS 9Be(7Li, 8Li), E=24 MeV; 2H(11B, 12B), E=40 MeV; 2H(18O, 16N), E=73 MeV; measured particle spectra, yields. Radioactive beam production.
doi: 10.1016/j.nima.2005.12.244
2006IS04 Phys.Lett. B 640, 82 (2006) H.Ishiyama, T.Hashimoto, T.Ishikawa, Y.X.Watanabe, S.K.Das, H.Miyatake, Y.Mizoi, T.Fukuda, M.-H.Tanaka, Y.Fuchi, N.Yoshikawa, Y.Hirayama, S.C.Jeong, T.Nomura, I.Katayama, S.Mitsuoka, K.Nishio, M.Matsuda, P.K.Saha, S.Ichikawa, H.Ikezoe, T.Furukawa, H.Izumi, T.Shimoda, K.Nakai A new measurement of the astrophysical 8Li(α, n)11B reaction NUCLEAR REACTIONS 4He(8Li, n), E(cm)=0.7-2.6 MeV; measured σ(E), particle spectra. Comparison with other results.
doi: 10.1016/j.physletb.2006.07.036
2006MA51 Eur.Phys.J. A 28, 295 (2006) M.Mazzocco, C.Signorini, M.Romoli, A.De Francesco, M.Di Pietro, E.Vardaci, K.Yoshida, A.Yoshida, R.Bonetti, A.De Rosa, T.Glodariu, A.Guglielmetti, G.Inglima, M.La Commara, B.Martin, D.Pierroutsakou, M.Sandoli, F.Soramel, L.Stroe, R.Kanungo, N.Khai, T.Motobayashi, T.Nomura, T.Ishikawa, H.Ishiyama, S.Jeong, H.Miyatake, M.H.Tanaka, I.Sugai, Y.Watanabe Scattering of 11Be halo nucleus from 209Bi at the Coulomb barrier NUCLEAR REACTIONS 209Bi(11Be, 11Be), E=40 MeV; measured quasielastic σ, σ(θ). Discussed halo structure reaction mechanism features. Comparison with optical model, similar systems. EXODET array.
doi: 10.1140/epja/i2006-10058-0
2006NA28 Phys.Rev. C 74, 035202 (2006) T.Nakabayashi, H.Fukasawa, R.Hashimoto, T.Ishikawa, T.Iwata, H.Kanda, J.Kasagi, T.Kinoshita, K.Maeda, F.Miyahara, K.Nawa, T.Nomura, H.Shimizu, T.Shishido, K.Suzuki, Y.Tajima, T.Takahashi, H.Ueno, H.Yamazaki, H.Y.Yoshida Photoproduction of η mesons off protons for Eγ ≤ 1.15 GeV NUCLEAR REACTIONS 1H(γ, X), E=0.70-1.15 MeV; measured η-meson production σ(θ), excitation function. Tagged photons, comparison with previous results and model predictions.
doi: 10.1103/PhysRevC.74.035202
2005PI08 Nucl.Phys. A753, 3 (2005) J.Pinard, H.T.Duong, D.Marescaux, H.H.Stroke, O.Redi, M.Gustafsson, T.Nilsson, S.Matsuki, Y.Kishimoto, K.Kominato, I.Ogawa, M.Shibata, M.Tada, J.R.Persson, Y.Nojiri, S.Momota, T.T.Inamura, M.Wakasugi, P.Juncar, T.Murayama, T.Nomura, M.Koizumi, and the ISOLDE Collaboration Precision hfs of 126Cs(T1/2=1.63 m) by ABMR NUCLEAR MOMENTS 126Cs; measured hfs; deduced μ. Bohr-Weisskopf effect. Atomic beam magnetic resonance.
doi: 10.1016/j.nuclphysa.2005.01.036
2004HA54 Nucl.Phys. A746, 330c (2004) T.Hashimoto, T.Ishikawa, T.Kawamura, K.Nakai, H.Ishiyama, Y.X.Watanabe, H.Miyatake, M.H.Tanaka, N.Yoshikawa, S.C.Jeong, Y.Fuchi, I.Katayama, T.Nomura, S.K.Das, P.K.Saha, T.Fukuda, K.Nishio, S.Mitsuoka, H.Ikezoe, M.Matsuda, S.Ichikawa, T.Furukawa, H.Izumi, T.Shimoda, Y.Mizoi, M.Terasawa Measurement of the 8Li(α, n)11B reaction cross sections of astrophysical interest NUCLEAR REACTIONS 4He(8Li, n), E=14.6 MeV; measured excitation energy spectra. 8Li(α, n), E(cm)=0.5-3 MeV; deduced excitation function. Astrophysical implications discussed.
doi: 10.1016/j.nuclphysa.2004.09.040
2004MI34 Nucl.Phys. A738, 401 (2004) H.Miyatake, H.Ishiyama, M.-H.Tanaka, Y.X.Watanabe, N.Yoshikawa, S.C.Jeong, Y.Matsuyama, Y.Fuchi, T.Nomura, T.Hashimoto, T.Ishikawa, K.Nakai, S.K.Das, P.K.Saha, T.Fukuda, K.Nishio, S.Mitsuoka, H.Ikezoe, S.Ichikawa, M.Matsuda, Y.Mizoi, T.Furukawa, H.Izumi, T.Shimoda, M.Terasawa Exclusive measurement of the astrophysical 8Li(α, n) reaction cross section NUCLEAR REACTIONS 4He(8Li, n), E(cm)=0.9-2.8 MeV; measured σ, excitation energy spectrum. Comparison with previous results.
doi: 10.1016/j.nuclphysa.2004.04.070
2003GU06 Phys.Rev. C 67, 064601 (2003) V.Guimaraes, S.Kubono, F.C.Barker, M.Hosaka, S.C.Jeong, I.Katayama, T.Miyachi, T.Nomura, M.H.Tanaka, Y.Fuchi, H.Kawashima, S.Kato, C.C.Yun, K.Ito, H.Orihara, T.Terakawa, T.Kishida, Y.Pu, S.Hamada, M.Hirai, H.Miyatake Structure of the unbound 11N nucleus by the (3He, 6He) reaction NUCLEAR REACTIONS 14N(3He, 6He), E=73.4 MeV; measured σ(E, θ). 11N deduced levels, J, π, resonance widths. DWBA analysis.
doi: 10.1103/PhysRevC.67.064601
2003GU30 Braz.J.Phys. 33, 263 (2003) V.Guimaraes, S.Kubono, F.C.Barker, M.Hosaka, S.C.Jeong, I.Katayama, T.Miyachi, T.Nomura, M.H.Tanaka, Y.Fuchi, H.Kawashima, S.Kato, T.Kishida, Y.Pu, S.Hamada Spectroscopic Study of the Unbound 11N Nucleus NUCLEAR REACTIONS 14N(3He, 6He), E=73.4 MeV; measured particle spectra, σ(E, θ). 11N deduced resonance energies, J, π, widths. DWBA analysis.
doi: 10.1590/s0103-97332003000200017
2003IS12 Nucl.Phys. A718, 481c (2003) H.Ishiyama, T.Hashimoto, T.Kawamura, T.Ishikawa, H.Miyatake, M.H.Tanaka, Y.Fuchi, N.Yoshikawa, S.C.Jeong, Y.Watanabe, H.Kawakami, I.Katayama, T.Nomura, S.Mitsuoka, K.Nishio, M.Matsuda, S.Ichikawa, H.Ikezoe, T.Furukawa, H.Yano, H.Izumi, Y.Mizoi, M.Terasawa, T.Fukuda, K.Nakai, T.Shimoda Direct measurements of (α, n) and (p, n) reaction cross sections using light neutron-rich radioactive nuclear beams NUCLEAR REACTIONS 2H(7Li, 6He), (11B, 12B), (22Ne, 20F), 4He(7Li, 10Be), 9Be(7Li, 8Li), E not given; 2H(18O, 16N), E=73 MeV; calculated radioactive beam yields. Application to further cross section measurements discussed.
doi: 10.1016/S0375-9474(03)00863-7
2003IS13 Nucl.Phys. A718, 484c (2003) T.Ishikawa, H.Ishiyama, T.Hashimoto, T.Kawamura, H.Miyatake, M.H.Tanaka, Y.Fuchi, N.Yoshikawa, S.C.Jeong, Y.Watanabe, H.Kawakami, I.Katayama, T.Nomura, S.Mitsuoka, K.Nishio, M.Matsuda, S.Ichikawa, H.Ikezoe, T.Furukawa, H.Yano, H.Izumi, Y.Mizoi, M.Terasawa, T.Fukuda, K.Nakai, T.Shimoda Measurement of the 16N(α, n) reaction cross section NUCLEAR REACTIONS 4He(16N, n), E(cm) ≈ 1-4.5 MeV; measured σ.
doi: 10.1016/S0375-9474(03)00864-9
2002IS05 Nucl.Phys. A701, 58c (2002) H.Ishiyama, H.Miyatake, N.Yoshikawa, S.C.Jeong, M.Wada, Y.Ishida, M.H.Tanaka, S.Takaku, Y.Fuchi, H.Kawashima, I.Katayama, T.Nomura, T.Teranishi, M.Michimasa, N.Imai, Y.Yanagisawa, S.Kubono, P.Strasser, S.Kato A Recoil Mass Separator for Nuclear Astrophysics Experiments
doi: 10.1016/S0375-9474(01)01548-2
2002JE08 Nucl.Phys. A701, 461c (2002) S.C.Jeong, H.Ishiyama, H.Kawakami, H.Miyatake, Y.Ishida, E.Tojyo, M.Oyaizu, S.Mizutani, N.Yoshikawa, M.H.Tanaka, H.Kawashima, Y.Fuchi, M.Wada, I.Katayama, T.Nomura Target-Ion-Source System for RNB Facility at KEK Tanashi
doi: 10.1016/S0375-9474(01)01627-X
2002MI25 Nucl.Phys. A701, 62c (2002) H.Miyatake, S.C.Jeong, H.Ishiyama, Y.Ishida, H.Kawakami, N.Yoshikawa, I.Katayama, M.H.Tanaka, E.Tojyo, M.Oyaizu, S.Arai, S.Tomizawa, K.Niki, Y.Arakaki, M.Okada, Y.Takeda, M.Wada, P.Strasser, S.Kubono, T.Nomura Present Status of the Radioactive Nuclear Beam Facility at KEK-Tanashi and the E-Arena in the KEK-JAERI Joint Project
doi: 10.1016/S0375-9474(01)01549-4
1999TA20 Eur.Phys.J. A 5, 123 (1999) Y.Tagaya, S.Hashimoto, K.Morita, Y.H.Pu, T.Ariga, K.Ohta, T.Minemura, I.Hisanaga, T.Motobayashi, T.Nomura The α-Decay Energies and Halflives of 195g, mAt and 199Fr RADIOACTIVITY 191,191mBi, 195,195mAt, 199Fr(α) [from 169Tm(36Ar, X)]; measured Eα, T1/2. NUCLEAR REACTIONS 169Tm(36Ar, 6n), E=215 MeV; measured Eα, αα-coin following residual nucleus decay; deduced evidence for 199Fr.
doi: 10.1007/s100500050266
1998GU10 Phys.Rev. C58, 116 (1998) V.Guimaraes, S.Kubono, N.Ikeda, I.Katayama, T.Nomura, M.H.Tanaka, Y.Fuchi, H.Kawashima, S.Kato, H.Toyokawa, C.C.Yun, T.Niizeki, T.Kubo, M.Ohura, M.Hosaka Nuclear Structure of 17Ne by the Three-Neutron Pickup (3He, 6He) Reaction NUCLEAR REACTIONS 20Ne(3He, 6He), E=70 MeV; measured σ(E, θ). 17Ne deduced levels, J, π, mass excess. Shell model calculations. NUCLEAR STRUCTURE A=17; analyzed T=3/2 quartet analog states; deduced coefficients. Isobaric multiplet mass equation analysis.
doi: 10.1103/PhysRevC.58.116
1997KU05 Nucl.Phys. A616, 11c (1997) S.Kubono, T.Nomura, S.Arai, Y.Arakaki, Y.Hashimoto, A.Imanishi, S.C.Jeong, I.Katayama, T.Katayama, H.Kawakami, H.Masuda, T.Miyachi, K.Niki, M.Okada, M.Oyaizu, Y.Shirakabe, P.Strasser, Y.Takeda, J.Tanaka, M.H.Tanaka, E.Tojyo, N.Tokuda, M.Tomizawa, M.Wada, K.Yoshida, M.Yoshizawa, M.Fujioka, S.Kato, T.Shinozuka, H.Wollnik New ISOL-Based Radioactive Nuclear Beam Facility at INS
doi: 10.1016/S0375-9474(97)00069-9
1997KU19 Nucl.Phys. A621, 195c (1997) S.Kubono, M.Hosaka, P.Strasser, V.Guimaraes, S.C.Jeong, I.Katayama, T.Miyachi, T.Nomura, M.H.Tanaka, Y.Fuchi, H.Kawashima, S.Kato, C.C.Yun, H.Orihara, T.Niizeki, H.Miyatake, T.Shimoda, T.Kajino, S.Wanajo Study of the Early Stage of the Rapid-Proton Process
doi: 10.1016/S0375-9474(97)00237-6
1997PU01 Z.Phys. A357, 1 (1997) Y.H.Pu, K.Morita, M.G.Hies, K.O.Lee, A.Yoshida, T.Nomura, Y.Tagaya, T.Motobayashi, M.Kurokawa, H.Minemura, T.Uchibori, T.Ariga, K.Sueki, S.A.Shin New α-Decaying Neutron-Deficient Isotope 196Rn NUCLEAR REACTIONS 166Er(36Ar, 6n), (36Ar, xnypzα), E=208 MeV; measured Eα, αα-correlations; deduced 196Rn production σ. 196Rn deduced α-decay T1/2. RADIOACTIVITY 197,197m,196Rn(α) [from 166Er(36Ar, xn), E=208 MeV]; 192Po(α) [from 196Rn(α-decay)]; measured Eα, α-correlation. 196Rn deduced T1/2.
doi: 10.1007/s002180050203
1996NO13 Hyperfine Interactions 103, 33 (1996) Possible New Approaches to Superheavy Elements -the (HI, αxn) Reaction and the Neutron-Rich Beam NUCLEAR REACTIONS, ICPND 232Th(40Ar, 3nα), E=5.2 MeV/nucleon; measured αα-energy correlation from product nuclei decay; deduced 256Sg production σ, utility of neutron-rich nuclei beams for production of superheavy elements. Recoil mass separator, other data compared. RADIOACTIVITY 265Sg(α); 261Sg(α); 257No(α); 253Fm(α) [from 232Th(40Ar, 3nα), E=5.2 MeV/nucleon]; measured αα-energy correlation.
doi: 10.1007/BF02317340
1996YO08 Phys.Lett. 389B, 457 (1996) A.Yoshida, C.Signorini, T.Fukuda, Y.Watanabe, N.Aoi, M.Hirai, M.Ishihara, H.Kobinata, Y.Mizoi, L.Mueller, Y.Nagashima, J.Nakano, T.Nomura, Y.H.Pu, F.Scarlassara Fusion and Breakup at the Barrier with 11Be NUCLEAR REACTIONS, ICPND 209Bi(11Be, 4n), (11Be, 5n), (10Be, 4n), (10Be, 3n), E(cm)=35-70 MeV; 209Bi(9Be, 3n), E(cm)=35-55 MeV; measured excitation σ(E), E(α), I(α); deduced 11Be breakup related features.
doi: 10.1016/S0370-2693(96)01327-5
1995GU08 Nucl.Phys. A588, 161c (1995) V.Guimaraes, S.Kubono, M.Hosaka, N.Ikeda, S.C.Jeong, I.Katayama, T.Miyachi, T.Nomura, M.H.Tanaka, Y.Fuchi, H.Kawashima, S.Ohkawa, S.Kato, H.Toyokawa, C.C.Yun, T.Niizeki, K.Ito, T.Kishida, T.Kubo, Y.Pu, M.Ohura, H.Orihara, T.Terakawa, S.Hamada, M.Hirai, H.Miyatake Structure of Light Proton-Rich Nuclei on the Drip-Line NUCLEAR REACTIONS 14N, 20Ne(3He, 6He), E=70.08 MeV; measured 6He energy spectra; deduced isobaric multiplet mass equation. 11N, 17Ne deduced levels, J, π, configuration.
doi: 10.1016/0375-9474(95)00117-J
1995GU17 Z.Phys. A353, 117 (1995) V.Guimaraes, S.Kubono, M.Hosaka, N.Ikeda, M.H.Tanaka, T.Nomura, I.Katayama, Y.Fuchi, H.Kawashima, S.Kato, H.Toyokawa, T.Niizeki, C.C.Yun, T.Kubo, M.Ohura Structure of 17Ne by the Three-Neutron Pick-Up (3He, 6He) Reaction NUCLEAR REACTIONS 20Ne(3He, 6He), E=70 MeV; measured σ(θ), ejectile momentum spectra. 17Ne deduced levels, J, π. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1599. 1995MO14 Z.Phys. A352, 7 (1995) K.Morita, Y.H.Pu, J.Feng, M.G.Hies, K.O.Lee, A.Yoshida, S.C.Jeong, S.Kubono, T.Nomura, Y.Tagaya, M.Wada, M.Kurokawa, T.Motobayashi, H.Ogawa, T.Uchibori, K.Sueki, T.Ishizuka, K.Uchiyama, Y.Fujita, H.Miyatake, T.Shimoda, T.Shinozuka, H.Kudo, Y.Nagai, S.A.Shin New α-Decaying Neutron Deficient Isotopes 197Rn and 200Fr NUCLEAR REACTIONS 166Er(36Ar, 5n), E=186, 200 MeV; 169Tm(36Ar, 5n), E=186 MeV; measured Eα, Iα; deduced evidence for 197,197mRn, 200Fr. Evaporation residues obtained from gas-filled recoil separator, implanted onto position sensitive solid state detector. RADIOACTIVITY 197,197mRn(α) [from 166Er(36Ar, 5n), E=186, 200 MeV]; 200Fr(α) [from 169Tm(36Ar, 5n), E=186 MeV]; 193,193mPo(α) [from 197,197mRn(α-decay)]; 196Rn(α) [from 166Er(36Ar, 6n)]; 192Po(α) [from 196Rn(α-decay)]; 200Fr(α) [from 169Tm(36Ar, 5n), E=186 MeV]; 196At(α) [from 200Fr(α-decay)]; measured Eα, Iα, T1/2, αα-energy correlations. Evaporation residues obtained from gas-filled recoil separator, implanted onto position sensitive solid state detector.
1995YO03 Nucl.Phys. A588, 109c (1995) A.Yoshida, N.Aoi, T.Fukuda, M.Hirai, M.Ishihara, H.Kobinata, Y.Mizoi, L.Mueller, Y.Nagashima, J.Nakano, T.Nomura, Y.H.Pu, F.Scarlassara, C.Signorini, Y.Watanabe Measurement of Fusion Cross Section with Neutron Halo Nuclei NUCLEAR REACTIONS, ICPND 209Bi(11Be, X), (9Be, X), (10Be, X), E(cm) ≤ 80 MeV; measured Eα, Iα; deduced fusion σ(E).
doi: 10.1016/0375-9474(95)00108-D
1994KU06 Z.Phys. A348, 59 (1994) S.Kubono, C.C.Yun, R.N.Boyd, L.R.Buchmann, Y.Fuchi, M.Hosaka, N.Ikeda, C.L.Jiang, I.Katayama, H.Kawashima, H.Miyatake, T.Niizeki, T.Nomura, A.Odahara, M.Ohura, H.Ohnuma, H.Orihara, C.Rolfs, T.Shimoda, Y.Tajima, M.H.Tanaka, H.Toyokawa High Resolution Study of 24Mg(p, d)23Mg for the Ne-E Problem NUCLEAR REACTIONS 24Mg(p, d), E=34-945 MeV; measured deuteron spectra, σ(θ); deduced 22Na(p, γ) reaction rate, astrophysics related Ne-E problem implications. 23Mg deduced level, possible J, π.
doi: 10.1007/BF01291654
1993DU08 Nucl.Instrum.Methods Phys.Res. A325, 465 (1993) H.T.Duong, C.Ekstrom, M.Gustafsson, T.T.Inamura, P.Juncar, P.Lievens, I.Lindgren, S.Matsuki, T.Murayama, R.Neugart, T.Nilsson, T.Nomura, M.Pellarin, S.Penselin, J.Persson, J.Pinard, I.Ragnarsson, O.Redi, H.H.Stroke, J.L.Vialle, and the ISOLDE Collaboration Atomic Beam Magnetic Resonance Apparatus for Systematic Measurement of Hyperfine Structure Anomalies (Bohr-Weisskopf Effect) NUCLEAR MOMENTS 39K, 87,85Rb; measured hfs; deduced g factor. Atomic beam magnetic resonance technique, systematic hyperfine anomalies study.
doi: 10.1016/0168-9002(93)90392-U
1993SH41 Nucl.Instrum.Methods Phys.Res. A337, 11 (1993) Y.Shirakabe, N.Ikeda, S.Ohkawa, T.Nomura, T.Shinozuka Bunching of Radioactive Ion Beam in the Millisecond Region - a Pulsed Gating-Potential Method in an Ion Source for On-Line Isotope Separation NUCLEAR REACTIONS 40Ca(3He, pα), E=70 MeV; measured γ spectra following 38K(β-decay); deduced in-beam bunching magnitude for radioactive residual ion-beam, comparison with on-line 39K, 23Na, 7Li ions bunching efficiencies.
doi: 10.1016/0168-9002(93)91132-7
1992BO16 Nucl.Phys. A542, 97 (1992) R.N.Boyd, S.Kubono, N.Ikeda, M.Y.Tanaka, T.Nomura, Y.Fuchi, H.Kawashima, M.Ohura, H.Orihara, S.Yun, H.Toyokawa, M.Yosoi, H.Ohnuma 9Be(α, p)12B Reaction and Primordial Nucleosynthesis NUCLEAR REACTIONS 9Be(α, p), E=65 MeV; measured σ(θ). 12B deduced levels, J, π, widths, resonance strength. DWBA calculations.
doi: 10.1016/0375-9474(92)90399-5
1992KU02 Nucl.Phys. A537, 153 (1992) S.Kubono, Y.Funatsu, N.Ikeda, M.Yasue, T.Nomura, Y.Fuchi, H.Kawashima, S.Kato, H.Miyatake, H.Orihara, T.Kajino Level Structure of 21Mg and the 20Na(p, γ)21Mg Stellar Reaction Rate NUCLEAR REACTIONS 24Mg(3He, 6He), E=73.71 MeV; measured σ(θ), θ(lab)=6°-28°; deduced stellar reaction rate of 20Na(p, γ)21Mg. 21Mg deduced levels, J, π.
doi: 10.1016/0375-9474(92)90162-D
1992KU07 Phys.Rev. C46, 361 (1992) S.Kubono, N.Ikeda, Y.Funatsu, M.H.Tanaka, T.Nomura, H.Orihara, S.Kato, M.Ohura, T.Kubo, N.Inabe, A.Yoshida, T.Ichihara, M.Ishihara, I.Tanihata, H.Okuno, T.Nakamura, S.Shimoura, H.Toyokawa, C.C.Yun, H.Ohnuma, K.Asahi, A.Chakrabarti, T.Mukhopadhyay, T.Kajino Decay Property of 20Na for the Onset Mechanism of the Rapid-Proton Process RADIOACTIVITY 20Mg(β+) [from 9Be(24Mg, X), E=100 MeV/nucleon]; measured T1/2, βp-coin; deduced log ft, 19Ne(p, γ) reaction rate implications. 20Na deduced levels, possible J, π.
doi: 10.1103/PhysRevC.46.361
1992KU24 Nucl.Instrum.Methods Phys.Res. B70, 583 (1992) S.Kubono, Y.Funatsu, N.Ikekda, M.H.Tanaka, T.Nomura, H.Orihara, S.Kato, M.Ohura, T.Kubo, N.Inabe, T.Ichihara, M.Ishihara, I.Tanihata, H.Okuno, T.Nakamura, S.Shimoura, H.Toyokawa, C.C.Yun, H.Ohnuma, K.Asahi, A.Chakrabarti, T.Mukhopadhyay, T.Kajino Proton Decay Measurement with RIPS for Astrophysical Interest RADIOACTIVITY 20Mg(β+) [from 9Be(24Mg, X), E=100 MeV/nucleon]; measured decay curve. 20Na(β+p), (α); measured β-delayed particle spectra. 20Na deduced 1+ state may not be s-wave resonance.
doi: 10.1016/0168-583X(92)95987-3
1992MA52 Hyperfine Interactions 74, 223 (1992) S.Matsuki, K.Shimomura, I.Ogawa, K.Suzuki, S.Hamada, T.Nakamura, H.Okuno, M.Koizumi, N.Inabe, Y.Fukashiro, H.Sunaoshi, M.Wada, T.Murayama, T.Kohmoto, M.Kitano, T.Kubo, T.Shinozuka, K.Asahi, Y.Kido, T.T.Inamura, T.Nomura, M.Ishihara, M.Fujioka, H.T.Duong, H.Haas, and the ISOLDE Collaboration Radiation-Detected Optical Pumping in Solids NUCLEAR REACTIONS 160Gd(12C, 5np), E=100 MeV; measured residual nucleus polarization. 160Gd(12C, 6n), E=100 MeV; measured nuclear polarization following residual decay. Optical pumping in SrF, crystal. RADIOACTIVITY 164Tm(β+) [from 164Yb-decay following production in 158Gd(12C, 6n), E=100 MeV]; measured β+ asymmetry. On-line polarization, implantation in CaF2 host crystal. 114mIn(IT); measured β+ asymmetry of 114In decay vs exciting laser wavelength. Polarization of 114In in GaAs crystal, Ti-saphire excited laser for optical pumping. 33Si(β-) [from 9Be(Ar, X), E=94 MeV/nucleon]; measured β-asymmetry, NMR vs exciting laser wavelength. Ion implantation in GaAs host crystal.
doi: 10.1007/BF02398632
1992MA53 Hyperfine Interactions 74, 319 (1992) S.Matsuki, K.Shimomura, I.Ogawa, K.Suzuki, T.Kohmoto, M.Kitano, T.Shinozuka, T.Inamura, T.Nomura, M.Fujioka, H.T.Duong, H.Haas Nuclear Polarization and Magnetic Resonance of 114In with β-RADOP in GaAs RADIOACTIVITY 114In(β-), (β+), (EC); measured β-asymmetry vs laser wavelength; deduced polarization, magnetic resonance. Implantation into p-type GaAs.
doi: 10.1007/BF02398648
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
1991JI02 Phys.Lett. 259B, 427 (1991) C.-L.Jiang, S.Kubono, N.Ikeda, M.Tanaka, H.Kawashima, Y.Fuchi, I.Katayama, T.Nomura, S.C.Pieper Strong Mutual Excitation of 148Nd + 20Ne NUCLEAR REACTIONS 148Nd(20Ne, 20Ne'), (20Ne, 20Ne), E=116 MeV; measured σ(θ); deduced target, projectile mutual excitation evidence.
doi: 10.1016/0370-2693(91)91651-B
1991KU04 Phys.Rev. C43, 1821 (1991) S.Kubono, N.Ikeda, T.Nomura, Y.Fuchi, H.Kawashima, S.Kato, H.Miyatake, H.Orihara Spectroscopic Tool for Proton-Rich Nuclei: The (3He, 6He) reaction NUCLEAR REACTIONS 24Mg(3He, 6He), E=73.71 MeV; measured σ(θ); deduced model parameters, L-dependence.
doi: 10.1103/PhysRevC.43.1821
1991KU10 Z.Phys. A338, 459 (1991) S.Kubono, R.Boyd, N.Ikeda, M.H.Tanaka, T.Nomura, Y.Fuchi, H.Kawashima, M.Ohura, H.Orihara, S.Yun, H.Toyokawa, M.Yosoi, H.Ohnuma, I.Tanihata, T.Kajino Key Resonant States in the 8Li(α, n)11B Reaction in the Inhomogeneous Big Bang Models NUCLEAR REACTIONS, ICPND 9Be(α, p), E=64 MeV; measured σ(θ), Ep; deduced increased value for 8Li(α, n) reaction S-factor. 12B deduced levels, J, π, Γ.
doi: 10.1007/BF01295776
1991KU31 Z.Phys. A341, 121 (1991) S.Kubono, N.Ikeda, M.H.Tanaka, T.Nomura, I.Katayama, Y.Fuchi, H.Kawashima, M.Ohura, H.Orihara, C.C.Yun, Y.Tajima, M.Yosoi, H.Ohnuma, H.Toyokawa, H.Miyatake, T.Shimoda, R.N.Boyd, T.Kubo, I.Tanihata, T.Kajino Decay Properties of the Key Resonant States in 8Li(α, n)11B for Primordial Nucleosynthesis NUCLEAR REACTIONS 9Be(α, p), E=50.29 MeV; measured pn-coin, (particle)(particle)-correlation; deduced implications to astrophysical reaction 8Li(α, n). 12B level deduced decay L, branching ratios, Γn/Γ, Γα/Γ.
doi: 10.1007/BF01281284
1991NA01 Phys.Rev. C43, R9 (1991) Y.Nagai, K.Kunihiro, T.Toriyama, S.Harada, Y.Torii, A.Yoshida, T.Nomura, J.Tanaka, T.Shinozuka Branching Ratio for 10C Superallowed Fermi β Decay RADIOACTIVITY 10C(β+); measured Eγ, Iγ; deduced log ft. Conserved vector current hypotheses, standard model. 207mPb [from 206Pb(3He, 2p)]; 205mPo [from 206Pb(3He, xn), E=38 MeV]; measured Eγ, Iγ, γ(θ), γγ-coin. 207Pb, 205Po levels deduced side feeding.
doi: 10.1103/PhysRevC.43.R9
1990KA01 Phys.Rev. C41, 1276 (1990) S.Kato, S.Kubono, M.H.Tanaka, M.Yasue, T.Nomura, Y.Fuchi, Y.Funatsu, S.Ohkawa, T.Miyachi, K.Iwata, T.Suehiro, Y.Yoshida, O.Nitoh Determination of 86Zr and 88Mo Atomic Masses by the (α, 8He) Reactions on 90Zr and 92Mo NUCLEAR REACTIONS 92Mo, 90Zr(α, 8He), E=65 MeV; measured Q. 86Zr, 88Mo deduced atomic mass excesses.
doi: 10.1103/PhysRevC.41.1276
1990KA10 Phys.Rev. C41, 2004 (1990) S.Kato, S.Kubono, T.Nomura, Y.Fuchi, Y.Funatsu, S.Ohkawa, T.Miyachi, T.Suehiro, Y.Yoshida Determination of 200Pb, 204Po, 208Rn, 212Ra, and 216Th Atomic Masses by the 204Pb(α, 8He)200Pb Reaction NUCLEAR REACTIONS 204Pb(α, 8He), E=64.8 MeV; 204,206,208Pb(α, 6He), E=65 MeV; measured particle spectra; deduced Q value for (α, 8He) Reaction. 200Pb, 204Po, 208Rn, 212Ra, 216Th deduced mass excesses. Other data input.
doi: 10.1103/PhysRevC.41.2004
1990KA19 Phys.Rev. C42, 563 (1990) S.Kato, S.Kubono, M.H.Tanaka, T.Nomura, Y.Fuchi, Y.Funatsu, S.Ohkawa, T.Miyachi, T.Suehiro, Y.Yoshida Determination of 181Re and 181Os Atomic Masses from the 185Re(α, 8He)181Re Reaction NUCLEAR REACTIONS 185Re(α, 8He), E=65 MeV; measured Q-value, particle spectra. 181Re, 181Os deduced mass excesses.
doi: 10.1103/PhysRevC.42.563
1989KA04 Phys.Rev. C39, 818 (1989) S.Kato, S.Kubono, M.H.Tanaka, M.Yasue, T.Nomura, Y.Fuchi, S.Ohkawa, T.Miyachi, K.Iwata, T.Suehiro, Y.Yoshida Determination of 193Au and 193Hg Atomic Masses by the 197Au(α, 8He)193Au Reaction NUCLEAR REACTIONS 197Au(α, 8He), E=65.12 MeV; measured σ(E(8He)), Q. 193Au, 193Hg deduced atomic mass excesses.
doi: 10.1103/PhysRevC.39.818
1989KU08 Nucl.Phys. A494, 203 (1989) H.Kudo, T.Nomura, K.Sueki, M.Magara, N.Yoshida Isomeric Transtions of 211mPo and 212mPo and E4 Effective Charge RADIOACTIVITY 211mPo(α) [from 208Pb(α, n)]; 212mPo(α) [from 209Bi(α, p)]; measured Eα, Iα, αγ-coin. 211m,212mPo deduced IT branching ratios, levels, J, π, γ-multipolarity. Natural target.
doi: 10.1016/0375-9474(89)90019-5
1989KU26 Z.Phys. A334, 511 (1989) S.Kubono, Y.Funatsu, N.Ikeda, M.Yasue, T.Nomura, Y.Fuchi, H.Kawashima, S.Kato, H.Orihara, H.Miyatake, T.Kajino The Proton Threshold States in 21Mg Relevant to the rp-Process NUCLEAR REACTIONS 24Mg(3He, 6He), E=73.71 MeV; measured σ(E(6He)), σ(θ); deduced rp-process relevance. 21Mg deduced levels, J, π, L. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1326. 1989MI17 Nucl.Phys. A501, 557 (1989) H.Miyatake, T.Nomura, S.Kubono, J.Tanaka, M.Oyaizu, H.Okawa, N.Ikeda, K.Sueki, H.Kudo, K.Morita, T.Shinozuka Alpha Decays of 221Pa and 218,219Ac NUCLEAR REACTIONS 209Bi(16O, xn), (16O, xnα), E=87-102 MeV; measured α decay yields, Eα from residues. Gas-filled recoil separator. RADIOACTIVITY 221Pa, 218,219Ac [from 205Tl, 209Bi(16O, xnα), E=87-102 MeV]; measured Eα, α-decay yields. 221Pa, 218,219Ac deduced T1/2, Qα. Gas-filled recoil separator.
doi: 10.1016/0375-9474(89)90148-6
1988KU23 Z.Phys. A331, 359 (1988) S.Kubono, N.Ikeda, M.Yasue, T.Nomura, Y.Fuchi, H.Kawashima, S.Kato, H.Orihara, T.Shinozuka, H.Ohnuma, H.Miyatake, T.Shimoda The p + 19Ne s-Wave Resonant State in 20Na at Stellar Energies NUCLEAR REACTIONS 20Ne(3He, t), E=55.33 MeV; measured σ(Et), σ(θ). 20Na deduced level, possible J, π. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1258. 1987SA41 Nucl.Phys. A473, 317 (1987) M.Sakai, Y.Fujita, M.Imamura, K.Omata, K.Miyatake, T.Nomura, S.Ohya, S.Chojnacki Anomalous Electron Intensity Ratio of the E0 Internal Conversion in the Transition of 154Gd RADIOACTIVITY 154Tb(EC) [from 153En(α, 3n)]; measured Iγ, I(ce). 154Gd transitions deduced δ, subshell ICC ratios. Enriched target, iron-free magnetic spectrometer.
doi: 10.1016/0375-9474(87)90147-3
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
1986KU18 Nucl.Instrum.Methods Phys.Res. A251, 74 (1986) S.Kubono, M.H.Tanaka, H.Kawakami, K.Sueki, H.Miyatake, T.Nomura, K.Morita, M.Ishihara, S.Kato, C.Konno, A.Sakaguchi High-Energy Gamma Ray Spectrometer for Heavy-Ion Induced Experiments NUCLEAR REACTIONS 11B, 14N(p, γ), E=6.91 MeV; measured γ spectra. NaI(Tl) spectrometer.
doi: 10.1016/0168-9002(86)91151-4
1984FU11 Nucl.Phys. A429, 193 (1984) T.Fukuda, T.Nomura, T.Shimoda, K.Katori, S.Shimoura, K.Sueki, H.Ogata Linear Momentum Transfer in the Reaction 232Th(14N, light particles) at 208 MeV NUCLEAR REACTIONS 232Th(14N, pF), (14N, dF), (14N, tF), (14N, αF), E=208 MeV; measured fission fragment σ(θ); deduced transferred momentum distributions.
doi: 10.1016/0375-9474(84)90155-6
1983IT01 Nucl.Phys. A410, 156 (1983) Y.Itoh, Y.Gono, T.Kubo, M.Sugawara, T.Nomura Excited States in 216Ra NUCLEAR REACTIONS 208Pb(12C, 4n), (13C, 5n), E=65-95 MeV; measured Eγ, Iγ, γγ-coin, γ(t), Iγ(θ), γ-linear polarization, I(ce). 216Ra deduced level sequences, J, π, T1/2.
doi: 10.1016/0375-9474(83)90408-6
1983UT01 Phys.Rev. C28, 1975 (1983) H.Utsunomiya, S.Kubono, M.H.Tanaka, M.Sugitani, K.Morita, T.Nomura, Y.Hamajima Breakup Fusion of 7Li NUCLEAR REACTIONS 159Tb(7Li, X), (7Li, 2nα), (7Li, 3nα), (7Li, 4nα), (7Li, 5nα), (7Li, 6nα), (7Li, pF), (7Li, αF), (7Li, dF), (7Li, tF), E=77 MeV; measured σ(fragment θ, E), αγ-coin, σ(θp), σ(Ep), σ(θd), σ(Ed), σ(θt), σ(Et), σ(θα), σ(Eα), γγ(θ), γ(φ), fission (fragment)(light particle)-coin; deduced residual nuclei < J > alignment, magnitude, projectile breakup fusion effects.
doi: 10.1103/PhysRevC.28.1975
1982KO17 Phys.Lett. 114B, 107 (1982) S.Kohmoto, M.Ishihara, H.Kamitsubo, T.Nomura, Y.Gono, H.Utsunomiya, T.Sugitate, K.Ieki Final-State Interaction and Time Information in 14N-Induced Reactions Studied by α-α Correlations NUCLEAR REACTIONS 27Al, 93Nb(14N, 2α), E=115 MeV; measured σ(E1, E2, θ1, θ2); deduced final state interaction effects.
doi: 10.1016/0370-2693(82)90125-3
1982SU07 Nucl.Phys. A388, 402 (1982) T.Sugitate, T.Nomura, M.Ishihara, Y.Gono, H.Utsunomiya, K.Ieki, S.Kohmoto Polarization of Preequilibrium Proton Emission in the 93Nb + 14N Reaction NUCLEAR REACTIONS 93Nb(14N, p), E=95 MeV; measured σ(E, θ), spin polarization vs E, θ; deduced reaction mechanism. Double scattering method.
doi: 10.1016/0375-9474(82)90422-5
1981GO06 J.Phys.Soc.Jpn. 50, 377 (1981) Y.Gono, K.Hiruta, T.Nomura, M.Ishihara, H.Utsunomiya, T.Sugitate, K.Ieki In-Beam α- and γ-Ray Spectroscopy for 214Rn NUCLEAR REACTIONS 208Pb(12C, 2nα), E=79 MeV; measured αα, γα-coin, Eα, Iα, Eγ, Iγ, T1/2. 214Rn levels deduced T1/2, B(E2), Qα, α-reduced widths. Shell model.
doi: 10.1143/JPSJ.50.377
1981UT01 Phys.Lett. 105B, 135 (1981) H.Utsunomiya, T.Nomura, M.Ishihara, T.Sugitate, K.Ieki, S.Kohmoto Angular-Momentum Transfer and Alignment following Preequilibrium α-Particle Emission in the Reaction 209Bi + 14N NUCLEAR REACTIONS, Fission 209Bi(14N, αF), E=115 MeV; measured σ(Eα), (fragment)α-coin, σ(fragment θ, θα), σ(fragment φα); deduced reaction mechanism, angular momentum transfer, alignment effects. Preequilibrium α-emission.
doi: 10.1016/0370-2693(81)91006-6
1980MO07 J.Phys.Soc.Jpn. 48, 687 (1980) H.Morinaga, J.Imazato, M.Yanokura, T.Nomura, M.Ishihara Reaction Cross Section Measurement for 40Ca(16O, p)55Co NUCLEAR REACTIONS 40Ca(16O, p), E=39-89 MeV; measured production σ(E) for 55Co, 52Mn, 48,49Cr, 43,44Sc.
doi: 10.1143/JPSJ.48.687
1980UT01 Nucl.Phys. A334, 127 (1980) H.Utsunomiya, T.Nomura, T.Inamura, T.Sugitate, T.Motobayashi Preequilibrium α-Particle Emission in Heavy-Ion Reactions NUCLEAR REACTIONS 159Tb, 169Tm, 181Ta, 197Au, 209Bi(14N, p), (14N, d), (14N, t), (14N, α), E=85-115 MeV; measured σ(E, θ). Si detectors.
doi: 10.1016/0375-9474(80)90144-X
1979IN03 Phys.Lett. 84B, 71 (1979) T.Inamura, T.Kojima, T.Nomura, T.Sugitate, H.Utsunomiya Multiplicity of γ-Rays Following Fast α-Particle Emission in the 95 MeV 14N + 159Tb Reaction NUCLEAR REACTIONS 159Tb(14N, 3nα), (14N, 4nα), (14N, 5nα), E=95 MeV; measured average γ-multiplicity vs Eα; deduced linear relationship between γ-multiplicity, Lα.
doi: 10.1016/0370-2693(79)90651-8
1979NO03 J.Phys.Soc.Jpn. 46, 335 (1979) T.Nomura, H.Utsunomiya, T.Inamura, T.Motobayashi, T.Sugitate Energy Relaxation during the Fusion Process Probed by Preequilibrium α Emission in Heavy-Ion Reactions NUCLEAR REACTIONS 209Bi, 197Au, 181Ta, 169Tm(14N, α), E=85, 95, 115 MeV; measured σ(Eα); deduced local nuclear temperature. Hot spot model, Ericson statistical model.
doi: 10.1143/JPSJ.46.335
1978NO01 Phys.Rev.Lett. 40, 694 (1978) T.Nomura, H.Utsunomiya, T.Motobayashi, T.Inamura, M.Yanokura Statistical Analysis of Preequilibrium α-Particle Spectra and Possible Local Heating NUCLEAR REACTIONS 209Bi(14N, X), (14N, F), E=85, 95 MeV; measured σ(Z, θ), Z ≤ 8, in-beam Eα.
doi: 10.1103/PhysRevLett.40.694
1978NO07 Nucl.Phys. A305, 262 (1978) T.Nomura, J.Delaunay, C.Tosello, N.Bendjaballah Partial Breakdown of the Evaporation Model and Possible Preequilibrium α-Particle Emission in Heavy-Ion Fusion Reactions NUCLEAR REACTIONS 52Cr(12C, X), E=56.0 MeV; 48Ti(16O, X), E=57.7 MeV; measured Eγ, Iγ; deduced product cross sections. Enriched targets. Compared with evaporation model.
doi: 10.1016/0375-9474(78)90177-X
1977BE16 Nucl.Phys. A280, 228 (1977) N.Bendjaballah, B.Delaunay, J.Delaunay, T.Nomura High Spin States in 57Co NUCLEAR REACTIONS 48Ti(12C, 2np), E=26-48 MeV; 54Fe(α, p)E=12-24 MeV; measured σ(E, Eγ, θ), γγ-coin, DSA. 57Co deduced levels, J, T1/2, δ. Enriched targets.
doi: 10.1016/0375-9474(77)90306-2
1977BE27 Nucl.Phys. A284, 513 (1977) N.Bendjaballah, J.Delaunay, A.Jaffrin, T.Nomura, K.Ogawa The Level Structure of 56Fe NUCLEAR REACTIONS 50Cr(12C, 2pα), E=26-58 MeV; 54Fe(α, 2p), E=12-24 MeV; 56Fe(α, α), E=12-24 MeV; measured σ(E, Eγ), γγ-coin, σ(E, Eγ, θ), T1/2 by Doppler methods. 56Fe deduced levels, spins, T1/2, mixing ratios. Enriched targets.
doi: 10.1016/0375-9474(77)90400-6
1977CA28 Nucl.Phys. A293, 125 (1977) S.Cavallaro, J.Delaunay, R.Ballini, T.Nomura, N.Bendjaballah, C.Tosello High Spin Levels in 58Fe: Ground-State and Quasi-γ Bands NUCLEAR REACTIONS 55Mn(α, p), E=12-24 MeV; measured reaction products, Eγ, Iγ, γγ-coin, 58Fe; deduced levels, J, σ(E, Eγ), σ(E, Eγ, θ), T1/2, mixing ratios, B(E2), B(M1). Monoisotopic target. Doppler Shift Attenuation (DSA).
doi: 10.1016/0375-9474(77)90481-X
1976BE26 Phys.Rev.Lett. 36, 1536 (1976) N.Bendjaballah, J.Delaunay, T.Nomura, H.J.Kim Possible Shape Transition in the Yrast Band of 56Fe NUCLEAR REACTIONS 50Cr(12C, 2pαγ), E=26-58 MeV; 54Fe(α, 2pγ), 56Fe(α, α), E=12-24 MeV; measured σ(E, Eγ, θ), γγ-coin. 54Fe(α, 2pγ), E=20, 24 MeV; measured DSA. 56Fe deduced levels, J, π, T1/2, B(λ).
doi: 10.1103/PhysRevLett.36.1536
1975KU17 Phys.Rev. C12, 813 (1975) W.Kutschera, B.A.Brown, H.Ikezoe, G.D.Sprouse, Y.Yamazaki, Y.Yoshida, T.Nomura, H.Ohnuma Lifetimes of the 61+ States in 42Ti and 46Ca and E2 Effective Charges in (1f7/2)±2 Nuclei NUCLEAR REACTIONS 40Ca(3He, nγ), E=12 MeV; 48Ca(α, 2nαγ), E=50 MeV; measured γ(t). 42Ti, 46Ca levels deduced T1/2, B(E2).
doi: 10.1103/PhysRevC.12.813
1975NO09 Phys.Lett. 58B, 273 (1975) T.Nomura, K.Hiruta, M.Yoshie, H.Ikezoe, T.Fukuda, O.Hashimoto In-Beam α- and γ-Ray Spectroscopy for 216Ra RADIOACTIVITY 216Ra; measured Eα, Iα(t); deduced Qα. NUCLEAR REACTIONS 208Pb(12C, 4nγ), 207Pb(12C, 3nγ), E=60-90 MeV; measured Eα, Iα(t), Eγ, Iγ(t). 216Ra deduced levels.
doi: 10.1016/0370-2693(75)90650-4
1974HA06 Nucl.Phys. A218, 180 (1974) O.Hashimoto, A.Sumi, T.Nomura, S.Nagamiya, K.Nakai, T.Yamazaki, K.Miyano Measurement of the g-Factor of the 0.57 ms 7+ State in 202Tl NUCLEAR REACTIONS Hg(p, xn), E=28 MeV; measured γ(θ, H, t). 202Tl level deduced g.
doi: 10.1016/0375-9474(74)90029-3
1974NO02 Phys.Rev. C9, 1168 (1974) T.Nomura, K.Hiruta, M.Yoshie, O.Hashimoto Alpha Decay of 215Fr NUCLEAR REACTIONS 209Bi(12C, xn), (12C, αxn), E=73-80 MeV; measured σ(E), Eα, α(t). 215Fr deduced T1/2, α-width.
doi: 10.1103/PhysRevC.9.1168
1973GI02 J.Phys.Soc.Jap. 34, 874 (1973) C.Gil, K.Nishiyama, T.Nomura, T.Yamazaki, K.Miyano A New Short-Lived Isomer in 114Sb NUCLEAR REACTIONS 116Sn(p, 3nγ), E=17-52 MeV; measured Eγ, Iγ, pγ(t). Deduced ICC. 114Sb deduced levels, transitions, γ-multipolarity, T1/2.
doi: 10.1143/JPSJ.34.874
1973HA36 J.Phys.Soc.Jap. 35, 337 (1973) O.Hashimoto, T.Nomura, T.Yamazaki, K.Miyano, M.Ishihara The g Factor of the 8+ State in 86Sr NUCLEAR REACTIONS 88Sr(p, p2nγ), E=51 MeV; measured γ(θ, H, t). 86Sr level deduced g.
doi: 10.1143/JPSJ.35.337
1973HI06 Phys.Lett. 45B, 244 (1973) K.Hiruta, T.Nomura, T.Inamura, M.Odera Alpha-Particle Decay of 218Th, a New Isotope RADIOACTIVITY 218Th [from 209Bi(14N, 5n), E=65-96 MeV]; measured Eα, T1/2.
doi: 10.1016/0370-2693(73)90194-9
1973NA18 Nucl.Phys. A211, 381 (1973) S.Nagamiya, Y.Yamazaki, O.Hashimoto, T.Nomura, K.Nakai, T.Yamazaki Magnetic Moments of the [πh29/2]8+ States in Po Isotopes and of the [(πh29/2)8+ X νp-11/2]17/2- State in 209Po NUCLEAR REACTIONS 204,206Pb(3He, 3nγ), E=30 MeV; 204Pb(α, 2nγ), E=29 MeV; 208Pb(3He, 3nγ), E=28 MeV; 207Pb(α, 2nγ), E=28 MeV; 208Pb(α, 2nγ), E=25 MeV; measured γ(θ, H, t). 204,206,208,209,210Po levels deduced g, stroboscopic method.
doi: 10.1016/0375-9474(73)90727-6
1973NO02 Nucl.Instrum.Methods 108, 61 (1973) A Method of Measuring Alpha-Decays in the Nanosecond Range RADIOACTIVITY 217Ac [from 207Pb(14N, X)]; measured T1/2, Eα.
doi: 10.1016/0029-554X(73)90635-6
1973NO09 Nucl.Phys. A217, 253 (1973) T.Nomura, K.Hiruta, T.Inamura, M.Odera Ground-State α-Decay of N = 128 Isotones 216Ra, 217Ac and 218Th NUCLEAR REACTIONS 208Pb(12C, xn), E=65-96 MeV; 207,208Pb, 209Bi(14N, xn), E=70-96 MeV; measured σ(E, Eα, Eγ), α(θ), α(t), γ(t). 216Ra, 217Ac, 218Th levels deduced T1/2, Qα, α-branching.
doi: 10.1016/0375-9474(73)90195-4
1973YA06 Phys.Lett. 44B, 440 (1973) Y.Yamazaki, S.Nagamiya, T.Nomura, K.Nakai, T.Yamazaki Magnetic Moment of a Core-Excited Isomeric State in 210Po NUCLEAR REACTIONS 208Pb(α, 2nγ), E=33 MeV; measured Iγ(θ, H). 210Po level deduced g.
doi: 10.1016/0370-2693(73)90328-6
1972NO06 Phys.Lett. 40B, 543 (1972) T.Nomura, K.Hiruta, T.Inamura, M.Odera In-Beam Alpha Spectroscopy of N = 128 Isotones. Lifetimes of 216Ra and A New Isotope 217Ac RADIOACTIVITY 216Ra, 217Ac; measured T1/2. 217Ac; measured Eα; deduced Q.
doi: 10.1016/0370-2693(72)90477-7
1972NO09 J.Phys.Soc.Jap. 33, 286 (1972) T.Nomura, T.Yamazaki, S.Nagamiya, T.Katou Magnetic Moment of the Lowest 6+ State in 42Ca NUCLEAR REACTIONS 40Ca(α, 2pγ), E=25 MeV; measured αγ(θ, H, t). 42Ca level deduced g, T1/2.
doi: 10.1143/JPSJ.33.286
1971NA16 J.Phys.Soc.Japan 31, 319 (1971) S.Nagamiya, T.Katou, T.Nomura, T.Yamazaki Magnetic Moments of the 8+ Isomeric States of 90Zr and 92Mo NUCLEAR REACTIONS 88Sr, 90Zr(α, 2nγ), E=29, 25 MeV; measured αγ(θ, H, t). 90mZr, 92mMo deduced g.
doi: 10.1143/JPSJ.31.319
1971NO06 Phys.Rev.Lett. 27, 523 (1971) T.Nomura, T.Yamazaki, S.Nagamiya, T.Katou Magnetic Moment of the Lowest 6+ State in 42Ca and Effects of the Deformed States NUCLEAR REACTIONS 40Ca(α, 2pγ), E=25 MeV; measured αγ(θ, H, t). 42Ca level deduced g.
doi: 10.1103/PhysRevLett.27.523
1971SA07 J.Phys.Soc.Jap. 30, 1252 (1971) The Lifetime of the Lowest 6+ State in 54Fe and E2 Effective Charge RADIOACTIVITY 54mCo; measured βγ-delay. 54Fe level deduced T1/2, B(E2), E2 effective charge.
doi: 10.1143/JPSJ.30.1252
1970NA11 Nucl.Phys. A159, 653 (1970) S.Nagamiya, T.Nomura, T.Yamazaki Stroboscopic Determination of the Magnetic Moment of the 8+ Isomeric State of 208Po NUCLEAR REACTIONS 206Pb(α, 2nγ), E=29 MeV; measured αγ(θ, H, t). 208Po level deduced μ. Stroboscopic method.
doi: 10.1016/0375-9474(70)90864-X
1970NA13 Phys.Lett. 33B, 574 (1970) S.Nagamiya, T.Katou, T.Nomura, T.Yamazaki Effective Spin and Orbital Magnetism of the Proton Studied from the g-Factors of the 8+ States in 90Zr, and 92Mo NUCLEAR REACTIONS 88Sr, 90Zr(α, 2nγ), E=29, 25 MeV; measured αγ(θ, H, t). 90Zr, 92Mo levels deduced g.
doi: 10.1016/0370-2693(70)90353-9
1970NO04 Phys.Rev.Lett. 25, 1342 (1970) T.Nomura, C.Gil, H.Saito, T.Yamazaki, M.Ishihara E2 Effective Charges of the f7/2 Proton and Neutron Deduced from the Lifetimes of the 6+ States in 50Ti, 54Fe, and 42Ca RADIOACTIVITY 50Sc, 54mCo; measured βγ-delay. 50Ti, 54Fe levels deduced T1/2, E2 effective charges. NUCLEAR REACTIONS 40Ca(α, 2pγ), E=25 MeV; measured αγ-delay. 42Ca level deduced T1/2, E2 effective charge.
doi: 10.1103/PhysRevLett.25.1342
1970YA02 Phys.Rev.Lett. 24, 317 (1970) T.Yamazaki, T.Nomura, U.Kato, T.Inamura, A.Hashizume, Y.Tendow Core Polarization Effect on the Magnetic Moment of the (h9/22) 8+ State of 210Po NUCLEAR REACTIONS 208Pb(α, 2nγ), E=25 MeV; measured αγ(θ, H, t). 210Po level deduced g.
doi: 10.1103/PhysRevLett.24.317
1970YA06 Phys.Rev.Lett. 25, 547 (1970) T.Yamazaki, T.Nomura, S.Nagamiya, T.Katou Anomalous Orbital Magnetism of Proton Deduced from the Magnetic Moment of the 11- State of 210Po NUCLEAR REACTIONS 208Pb(α, 2n), E=30 MeV; measured αγ(θ, H, t). 210Po level deduced g. 1H deduced anomalous orbital magnetism.
doi: 10.1103/PhysRevLett.25.547
1969NO02 Nucl.Phys. A127, 1 (1969) Gamma Rays Following Heavy-Ion Bombardment of Light Nuclei NUCLEAR REACTIONS 12C(10B, Xγ), 12C(12C, Xγ), 10B, 12C, 14N, 16O, 24Mg, 28Si(14N, Xγ), 12C, 16O, 24Mg, 28Si(16O, Xγ), E=20-30 MeV; measured Eγ, γγ-coin; deduced σ. Enriched 10B target, Ge(Li) detector.
doi: 10.1016/0375-9474(69)90762-3
1969YA06 Contrib.Intern.Conf.Properties Nucl.States, Montreal, Canada, p.96 (1969) T.Yamazaki, T.Nomura, U.Kato, T.Inamura, A.Hashizume, Y.Tendow Magnetic Core Polarization in the (h9/22)8+ State of 210Po RADIOACTIVITY 210Po [from 208Pb(α, 2n)]; measured γγ(θ, H, t). 210Po level deduced g.
1968NO06 Z.Physik 215, 91 (1968) Spin Assignment of the 8.555 MeV State in 28Si NUCLEAR STRUCTURE 28Si; measured not abstracted; deduced nuclear properties.
doi: 10.1007/BF01382518
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