NSR Query Results
Output year order : Descending NSR database version of May 8, 2024. Search: Author = M.Adachi Found 46 matches. 1999OG03 Phys.Lett. 451B, 11 (1999) H.Ogawa, K.Asahi, K.Sakai, A.Yoshimi, M.Tsuda, Y.Uchiyama, T.Suzuki, K.Suzuki, N.Kurokawa, M.Adachi, H.Izumi, H.Ueno, T.Shimoda, S.Tanimoto, N.Takahashi, W.-D.Schmidt-Ott, M.Schafer, S.Fukuda, A.Yoshida, M.Notani, T.Kubo, H.Okuno, H.Sato, N.Aoi, K.Yoneda, H.Iwasaki, N.Fukuda, N.Fukunishi, M.Ishihara, H.Miyatake Magnetic Moment and Electric Quadrupole Moment of the 18N Ground State RADIOACTIVITY 18N(β-) [from 22Ne fragmentation]; measured β-NMR. 18Ne deduced μ, quadrupole moment. NUCLEAR REACTIONS 12C(22Ne, X)18N, E=110 MeV/nucleon; measured fragment polarization.
doi: 10.1016/S0370-2693(99)00219-1
1998OG04 J.Phys.(London) G24, 1399 (1998) H.Ogawa, K.Asahi, K.Sakai, A.Yoshimi, M.Tsuda, Y.Uchiyama, T.Suzuki, K.Suzuki, N.Kurokawa, M.Adachi, H.Izumi, H.Ueno, T.Shimoda, S.Tanimoto, N.Takahashi, W.-D.Schmidt-Ott, M.Schafer, S.Fukuda, A.Yoshida, M.Notani, T.Kubo, H.Okuno, H.Sato, N.Aoi, K.Yoneda, H.Iwasaki, N.Fukuda, N.Fukunishi, M.Ishihara Static Moments of the 18N Ground State RADIOACTIVITY 18N(β-) [from 22Ne primary beam fragmentation]; measured Iβ(H, t). 18N deduced ground-state Q, μ. β-NMR technique.
1996IZ01 Phys.Lett. 366B, 51 (1996) H.Izumi, K.Asahi, H.Ueno, H.Okuno, H.Sato, K.Nagata, Y.Hori, M.Adachi, N.Aoi, A.Yoshida, G.Liu, N.Fukunishi, M.Ishihara Electric Quadrupole Moments of Neutron-Rich Nuclei 14B and 15B RADIOACTIVITY 14,15B(β-) [from 93Nb(18O, X), E=64.7 MeV/nucleon]; measured β-NMR, polarized nuclei; deduced electric quadrupole moments. Shell model comparison.
doi: 10.1016/0370-2693(95)01312-1
1996IZ02 Hyperfine Interactions 97/98, 509 (1996) H.Izumi, K.Asahi, H.Ueno, H.Okuno, H.Sato, K.Nagata, Y.Hori, M.Adachi, N.Aoi, A.Yoshida, G.Liu, N.Fukunishi, M.Ishihara Measurement of Electric Quadrupole Moments of Neutron-Rich Nuclei 14B and 15B RADIOACTIVITY 12,14,15B(β-) [from 93Nb(18O, X), E=64.7 MeV/nucleon]; measured β-NMR, polarized sources. 17N, 17,14,15B deduced electric quadrupole moments. Other data input.
doi: 10.1007/BF02150193
1996UE02 Phys.Rev. C53, 2142 (1996) H.Ueno, K.Asahi, H.Izumi, K.Nagata, H.Ogawa, A.Yoshimi, H.Sato, M.Adachi, Y.Hori, K.Mochinaga, H.Okuno, N.Aoi, M.Ishihara, A.Yoshida, G.Liu, T.Kubo, N.Fukunishi, T.Shimoda, H.Miyatake, M.Sasaki, T.Shirakura, N.Takahashi, S.Mitsuoka, W.-D.Schmidt-Ott Magnetic Moments of 17N and 17B RADIOACTIVITY 17N(β-) [from 93Nb(18O, X), E=64.7 MeV/nucleon]; 17B(β-) [from 93Nb(22Ne, X), E=94.4 MeV/nucleon]; measured NMR; deduced μ. Model comparison. NUCLEAR STRUCTURE 17N, 17B, 19F; calculated μ. 16,18O; calculated levels. Model comparison.
doi: 10.1103/PhysRevC.53.2142
1995AS05 Nucl.Phys. A588, 135c (1995) K.Asahi, H.Ueno, H.Izumi, H.Okuno, K.Nagata, H.Ogawa, Y.Hori, H.Sato, K.Mochinaga, M.Adachi, A.Yoshida, G.Liu, N.Aoi, T.Kubo, M.Ishihara, W.-D.Schmidt-Ott, T.Shimoda, H.Miyatake, S.Mitsuoka, N.Takahashi Electromagnetic Moments of Unstable Nuclei Studied with Polarized Projectile Fragments NUCLEAR REACTIONS 197Au(14N, X), E=39.4 MeV/nucleon; 197Au(15N, X), E=68, 109.6 MeV/nucleon; 93Nb(93Nb, X), E=67.3 MeV/nucleon; 27Al(15N, X), E=68 MeV/nucleon; measured ejectile yield, spin polarization spectra vs (p-p0)/p0.
doi: 10.1016/0375-9474(95)00112-E
1995OK04 Phys.Lett. 354B, 41 (1995) H.Okuno, K.Asahi, H.Ueno, H.Izumi, H.Sato, M.Adachi, T.Nakamura, T.Kubo, N.Inabe, A.Yoshida, N.Fukunishi, T.Shimoda, H.Miyatake, N.Takahashi, W.-D.Schmidt-Ott, M.Ishihara Measurement of the Magnetic Moments of 14B and 15B using Projectile Fragmentation Spin Polarization RADIOACTIVITY 12,14,15B(β-) [from 93Nb(18O, X), E=68 MeV/nucleon]; measured β NMR; deduced μ. Polarized nuclei. Model comparison.
doi: 10.1016/0370-2693(95)00630-4
1994OK03 Phys.Lett. 335B, 29 (1994) H.Okuno, K.Asahi, H.Sato, H.Ueno, J.Kura, M.Adachi, T.Nakamura, T.Kubo, N.Inabe, A.Yoshida, T.Ichihara, Y.Kobayashi, Y.Ohkubo, M.Iwamoto, F.Ambe, T.Shimoda, H.Miyatake, N.Takahashi, J.Nakamura, D.Beaumel, D.J.Morrissey, W.-D.Schmidt-Ott, M.Ishihara Systematic Behavior of Ejectile Spin Polarization in the Projectile Fragmentation Reaction NUCLEAR REACTIONS 197Au, 93Nb, 27Al(15N, X), E=70-112 MeV/nucleon; 197Au(14N, X), E=39.4 MeV/nucleon; measured ejectile(12,13B) spin polarization; deduced role of new reaction mechanism.
doi: 10.1016/0370-2693(94)91553-9
1994UE04 Hyperfine Interactions 84, 371 (1994) H.Ueno, H.Okuno, K.Asahi, H.Sato, T.Kubo, T.Nakamura, N.Inabe, A.Yoshida, Y.Ohkubo, M.Adachi, T.Ichihara, M.Ishihara, T.Shimoda, H.Miyatake, N.Takahashi, W.-D.Schmidt-Ott Spin-Polarized Radioactive Beams and β-NMR Experiments RADIOACTIVITY 14,15B, 21F(β-) [from 197Au(14N, X), E=40.6 MeV/nucleon; 197Au(15N, X), E=69.5, 111 MeV/nucleon; 27Al, 93Nb(15N, X), E=69.5 MeV/nucleon]; measured β NMR, polarized sources; deduced μ. Model comparison.
doi: 10.1007/BF02060685
1993OK02 Hyperfine Interactions 78, 97 (1993) H.Okuno, K.Asahi, H.Ueno, H.Sato, M.Adachi, T.Kubo, T.Nakamura, N.Inabe, A.Yoshida, Y.Ohkubo, T.Ichihara, M.Ishihara, T.Shimoda, H.Miyatake, N.Takahashi Polarization in Projectile Fragmentation and g-Factor Measurements for Neutron-Rich Nuclei NUCLEAR REACTIONS 159Tb, 27Al, 93Nb, 197Au(15N, 12B), (15N, 13B), 93Nb(18O, 12B), (18O, 14B), E=70 MeV/nucleon; 197Au(14N, 12B), E=40 MeV/nucleon; 197Au(15N, 12B), (15N, 13B), E=112 MeV/nucleon; measured projectile fragment polarization. RADIOACTIVITY 14,15B(β-n) [from 93Nb(18O, X), E=70 MeV/nucleon]; 21F(β-n) [from 93Nb(22Ne, X), E=70 MeV/nucleon]; measured NMR spectra; deduced g factor.
doi: 10.1007/BF00568122
1992AS01 Hyperfine Interactions 75, 101 (1992) K.Asahi, H.Okuno, H.Ueno, H.Sato, J.Kura, T.Kubo, T.Nakamura, N.Inabe, A.Yoshida, Y.Ohkubo, M.Adachi, T.Ichihara, M.Ishihara, T.Shimoda, H.Miyatake, N.Takahashi, D.Beaumel, D.J.Morrissey, W.-D.Schmidt-Ott Spin-Oriented Projectile Fragments: The first application to g-factor measurements NUCLEAR REACTIONS 197Au(14N, 12B), E=40.6 MeV/nucleon; 27Al(15N, 13B), E=69.5 MeV/nucleon; measured fragment spin polarization, yield. RADIOACTIVITY 14,15B(β-) [from 93Nb(18O, X), E=70 MeV/nucleon]; measured g-factor, preliminary results.
doi: 10.1007/BF02398968
1991FU10 Phys.Lett. 268B, 339 (1991) M.Fukuda, T.Ichihara, N.Inabe, T.Kubo, H.Kumagai, T.Nakagawa, Y.Yano, I.Tanihata, M.Adachi, K.Asahi, M.Kouguchi, M.Ishihara, H.Sagawa, S.Shimoura Neutron Halo in 11Be Studied via Reaction Cross Sections NUCLEAR REACTIONS 12C, 27Al(11Be, X), E=33 MeV/nucleon; measured reaction, fragmentation σ. 11Be deduced neutron halo evidence in density distribution.
doi: 10.1016/0370-2693(91)91587-L
1990AD02 J.Phys.Soc.Jpn. 59, 66 (1990) M.Adachi, A.Tamura, M.Kouguchi, H.Takanashi, H.Taketani g-Factor of the (27/2)+ Isomeric State in 149Tb NUCLEAR REACTIONS 141Pr(12C, 4nγ), E=80 MeV; measured Iγ, Iγ(θ, H), γγ-coin. 149Tb level deduced T1/2, g. Hyperpure Ge, Ge(Li) detectors, natural target.
doi: 10.1143/JPSJ.59.66
1990AS07 Phys.Lett. 251B, 488 (1990) K.Asahi, M.Ishihara, N.Inabe, T.Ichihara, T.Kubo, M.Adachi, H.Takanashi, M.Kouguchi, M.Fukuda, D.Mikolas, D.J.Morrissey, D.Beaumel, T.Shimoda, H.Miyatake, N.Takahashi New Aspect of Intermediate Energy Heavy Ion Reactions. Large Spin Polarization of Fragments NUCLEAR REACTIONS 197Au(14N, 12BX), E=40.6 MeV/nucleon; measured ejectile 12B spin polarization, yield. Projectile fragmentation.
doi: 10.1016/0370-2693(90)90784-4
1989HA01 Phys.Rev. C39, 132 (1989) H.Harada, M.Sugawara, H.Kusakari, H.Shinohara, Y.Ono, K.Furuno, T.Hosoda, M.Adachi, S.Matsuki, N.Kawamura High-Spin States in 114Sn NUCLEAR REACTIONS 100Mo(18O, 4n), E=65 MeV; measured γγ-coin. 114Sn deduced levels, J, π, band structure. Spin projected HFB calculation.
doi: 10.1103/PhysRevC.39.132
1986AD11 J.Phys.Soc.Jpn., Suppl. 55, 1042 (1986) M.Adachi, N.Yamada, M.Taya, T.Kohno, A.Makishima, T.Suzuki, S.Fukuda, M.Fukuda, T.Nagafuchi, H.Taketani Measurement of the atomic polarization and nuclear magnetic moment of the 2+1 state in 22Ne with a tilted-foil method NUCLEAR REACTIONS 19F(α, p), E=8 MeV; measured Eγ, Iγ(θ, H, t). 22Ne level deduced g factor. Tilted-foil method.
1986KO01 Phys.Rev. C33, 392 (1986) T.Kohno, M.Adachi, S.Fukuda, M.Taya, M.Fukuda, H.Taketani, Y.Gono, M.Sugawara, Y.Ishikawa Level Structure and Electromagnetic Properties in 212Ra NUCLEAR REACTIONS 204Pb(12C, 4nγ), E=70-90 MeV; measured Eγ, Iγ, γ(θ), I(ce), γγ-, ce(γ)-coin, γ linear polarization. 212Ra deduced levels, J, π, ICC, T1/2, B(E2), B(E3), g, configurations. Ge(Li) detector, hyperpure Ge-Compton polarimeter, superconducting solenoid with Si(Li) detector.
doi: 10.1103/PhysRevC.33.392
1986MA39 Phys.Rev. C34, 576 (1986) A.Makishima, M.Adachi, H.Taketani, M.Ishii Yrast Bands in 136,138Sm and 132Nd NUCLEAR REACTIONS 107Ag(35Cl, 2n2p), E=155 MeV; 107Ag(32S, 2np), (32S, 2npα), E=160 MeV; measured Eγ, Iγ, γ(θ), γγ-coin. 136,138Sm, 132Nd deduced levels, J, π, T1/2, B(E2), γ-branching. Interacting boson model.
doi: 10.1103/PhysRevC.34.576
1985AD09 Nucl.Phys. A442, 361 (1985) M.Adachi, T.Kohno, A.Makishima, S.Fukuda, M.Fukuda, M.Taya, H.Taketani g-Factors of High-Spin Isomeric States in 216Ra NUCLEAR REACTIONS 208Pb(12C, 4nγ), E=80 MeV; measured Iγ(θ, H, t). 216Ra deduced levels, isomer g, T1/2, J, π, configurations. Pulsed beam, enriched target, Ge(Li) detector.
doi: 10.1016/0375-9474(85)90149-6
1985FU03 Nucl.Phys. A435, 7 (1985) Y.Fujita, S.Morinobu, I.Katayama, M.Fujiwara, T.Yamazaki, H.Ikegami, H.Taketani, M.Adachi, T.Matsuzaki, M.Matoba, N.Koori High-Resolution Study of 49Cr through the (p, d) Reaction NUCLEAR REACTIONS 50Cr(p, d), E=55 MeV; measured σ(Ed), σ(θ). 49Cr deduced levels, L, C2S, J, π. Enriched target.
doi: 10.1016/0375-9474(85)90299-4
1984MA35 Nucl.Phys. A425, 1 (1984); Erratum Nucl.Phys. A433, 743 (1985) A.Makishima, M.Ishii, M.Ohshima, M.Adachi, H.Taketani E0 Transition in 74Se RADIOACTIVITY 74mBr(β+), (EC) [from 46Ti(35Cl, 3n4p), E=155 MeV]; measured Eγ, Iγ, I(ce); deduced T1/2. 74Se deduced levels, ICC, γ-branching, multipole branching ratio, monopole strength. Enriched target, Ge(Li), Si-Li mini-orange electron filter, mechanical lifetime filter.
doi: 10.1016/0375-9474(84)90215-X
1983KO12 Nucl.Phys. A398, 493 (1983) Level Structure of the Doubly Odd Nucleus 112In from the (p, nγ) Reaction NUCLEAR REACTIONS, ICPND 112Cd(p, nγ), E=3.95-4.75 MeV; measured σ(E, Eγ, θγ), Eγ, Iγ, γγ-coin, γ-ray linear polarization, γ yields. 112In deduced levels, J, π, γ-branching, γ-mixing ratio.
doi: 10.1016/0375-9474(83)90298-1
1982TA09 Phys.Lett. 113B, 11 (1982) H.Taketani, M.Adachi, N.Endo, T.Suzuki A Multi-Detector Coincidence Study of the 12C(p, p) Bremsstrahlung Spectrum and the Time Delay NUCLEAR REACTIONS 12C(p, p'γ), E=1700-1835 keV; measured σ(θγ, Eγ, θp'), bremsstrahlung spectra; deduced phase difference, reaction time delay.
doi: 10.1016/0370-2693(82)90098-3
1982TA11 Nucl.Instrum.Methods 196, 283 (1982) H.Taketani, N.Endo, G.Ishikawa, T.Suzuki, M.Adachi, T.Kohno, A.Makishima, T.Ikuta A List-Mode Study of Bremsstrahlung Spectra near the 12C(p, p) Resonance and the Time Delays NUCLEAR REACTIONS 12C(p, p), E=1.5-1.9 MeV; measured σ(E). 12C(p, p'), E=1.7, 1.765, 1.795, 1.835 MeV; measured σ(Ep'), σ(Eγ, θγ, θp'), bremsstrahlung photons; deduced incident, exit channel phase difference, time delay.
doi: 10.1016/0029-554X(82)90656-5
1980AD04 Z.Phys. A295, 251 (1980) M.Adachi, A.Muroi, T.Matsuzaki, H.Taketani Low-Lying States in 112In NUCLEAR REACTIONS 112Cd(p, nγ), E=4 MeV; measured σ(Eγ), γγ-coin, γ(θ), linear polarizations, γ(t); deduced Q. 112In deduced levels, J, π, T1/2, multipolarities, δ.
doi: 10.1007/BF01412205
1980TA04 Phys.Lett. 90B, 214 (1980) H.Taketani, M.Adachi, T.Matsuzaki, M.Matoba, N.Koori, T.Yamazaki, S.Morinobu, I.Katayama, M.Fujiwara, Y.Fujita, H.Ikegami Line Broadening and Coulomb Displacement Energies of the Hole-State Analogs in the A = 111-123 Odd-Mass Sn Isotopes NUCLEAR REACTIONS 112,114,116,118,120,122,124Sn(p, d), E=55 MeV; measured σ(Ed). 111,113,115,117,119,121,123Sn deduced levels, T, J, π, IAR, Coulomb displacement energies, spreading widths. Thick targets.
doi: 10.1016/0370-2693(80)90726-1
1979AD02 Nucl.Phys. A314, 80 (1979) M.Adachi, T.Matsuzaki, H.Taketani Low-Lying Levels in 120Sb Studied with the 120Sn(p, nγ) Reaction NUCLEAR REACTIONS 120Sn(p, nγ), E=3.40-4.10 MeV; measured σ(E, Eγ, θγ), Eγ, Iγ, γγ-coin, γ(t), γ-linear plarization. 120Sb levels deduced J, π, γ-branching, T1/2, δ. Enriched target.
doi: 10.1016/0375-9474(79)90556-6
1979IK04 Nucl.Phys. A329, 84 (1979) H.Ikegami, T.Yamazaki, S.Morinobu, I.Katayama, M.Fujiwara, Y.Fujita, H.Taketani, M.Adachi, T.Matsuzaki, N.Koori, M.Matoba Systematic Observation of Fine Structure of the Hole-State Analogues in Ni Isotopes NUCLEAR REACTIONS 58,62,64Ni(p, d), E=50 MeV; measured σ(Ed, θ). 57,61,63Ni deduced levels, J, π, L, spreading width. Enriched target. Magnetic spectrograph.
doi: 10.1016/0375-9474(79)90282-3
1977MA22 J.Phys.Soc.Jap. 43, 369 (1977) T.Matsuzaki, M.Adachi, H.Taketani Lifetimes of Some Low-Lying l = 1 States in 51Mn NUCLEAR REACTIONS 50Cr(3He, dγ), E=7.98 MeV; measured Eγ(θ), DSA. 51Mn deduced levels, T1/2, J, π, γ-branching, B(λ). Enriched target.
doi: 10.1143/JPSJ.43.369
1976AD04 Nucl.Phys. A263, 173 (1976) M.Adachi, H.Taketani, T.Hattori, T.Matsuzaki, A.Yokoyama, T.Oda Lifetimes of the First and Second Excited 3/2- States in 55Co NUCLEAR REACTIONS 54Fe(3He, dγ), E=8.1 MeV; measured Eγ(θ), Doppler shift. 55Co levels deduced T1/2. Enriched target.
doi: 10.1016/0375-9474(76)90191-3
1976HA57 J.Phys.Soc.Jap. 41, 1830 (1976) T.Hattori, M.Adachi, H.Taketani A Level-Structure Study of 108Ag and 110Ag with the (p, nγ) Reactions NUCLEAR REACTIONS 108Pd(p, nγ), E=2.6-3.95 MeV; 110Pd(p, nγ), E=1.6-3.95 MeV; measured σ(E, Eγ, θ), Eγ, Iγ, γ(θ, H, t). 108,110Ag deduced levels, J, π, T1/2, g, δ.
doi: 10.1143/JPSJ.41.1830
1976TA10 Phys.Lett. 63B, 154 (1976) H.Taketani, M.Adachi, T.Hattori, T.Matsuzaki, H.Nakayama Identification of an Excited Rotational Band in 'Spherical' 151Eu NUCLEAR REACTIONS 152Sm(p, 2nγ), E=18.8 MeV; measured Eγ, Iγ, γ(θ), γγ-coin. 151Eu deduced levels, K, J, π.
doi: 10.1016/0370-2693(76)90637-7
1975AS09 Nucl.Instrum.Methods 130, 221 (1975) K.Ashibe, M.Adachi, H.Taketani A Three Ge(Li) Compton Polarimeter for Nuclear-Reaction Gamma-Rays NUCLEAR REACTIONS 48Ca(p, nγ); measured γγγ-coin, linear polarization. 48Sc level deduced δ, J, π.
doi: 10.1016/0029-554X(75)90177-9
1974AD06 J.Phys.Soc.Jap. 36, 1266 (1974) M.Adachi, T.Hattori, E.Arai, M.Ogawa, H.Sato High Resolution Study of the g9/2 Isobaric Analogue State in 61Cu NUCLEAR REACTIONS 60Ni(p, p), (p, γ), E=3.67-3.95 MeV; measured Eγ, Iγ, γ(θ), IAR, σ(E). 61Cu deduced IAS, levels, J, π, γ-width, B(M1).
doi: 10.1143/JPSJ.36.1266
1974AK01 J.Phys.Soc.Jap. 37, 562 (1974) M.Akiba, T.Hattori, M.Adachi, M.Fujioka, K.Hisatake The Magnetic Moment of the Second Excited State in 26Al NUCLEAR REACTIONS 25Mg(p, γ), E=956 keV; measured γ(θ, H, t). 26Al level deduced T1/2, g.
doi: 10.1143/JPSJ.37.562
1973AD05 J.Phys.Soc.Jap. 35, 317 (1973) Spin-Parity Assignments of the 49Sc Levels from the Gamma-Decay of the 3/2- Isobaric Analogue State in 49Sc NUCLEAR REACTIONS 48Ca(p, γ), (p, nγ), E=1.94-2.00 MeV; measured γ(θ), Eγ, γγ-coin. 48Ca(d, nγ), E=3.0, 3.5 MeV; measured Eγ. 49Sc deduced levels, J, π, γ-mixing, γ-branching.
doi: 10.1143/JPSJ.35.317
1973AD06 J.Phys.Soc.Jap. 35, 325 (1973) The M1 Transition Strength from the 3/2- Isobaric Analogue State in 49Sc NUCLEAR REACTIONS 48Ca(p, γ), (p, nγ), E=1.94-2.00 MeV; measured Eγ, γ(θ), γγ-coin. 49Sc resonances deduced B(M1), γ-hindrance, Γ.
doi: 10.1143/JPSJ.35.325
1973TA07 Nucl.Phys. A204, 385 (1973) H.Taketani, M.Adachi, M.Ogawa, K.Ashibe Level Structure of N = 49 Nuclei up to an Excitation Energy of 13 MeV by the (p, d) Reaction NUCLEAR REACTIONS 89Y(p, d), 90Zr(p, d), E=55 MeV; 88Sr(p, d), 92Mo(p, d), E=52 MeV; measured σ(Ed, θ). 87Sr, 89Zr, 91Mo, 88Y deduced levels, J, π, L(n), T, S. Natural, enriched targets.
doi: 10.1016/0375-9474(73)90280-7
1971TA11 J.Phys.Soc.Jap. 30, 1499 (1971) H.Taketani, M.Adachi, M.Ogawa, K.Ashibe, T.Hattori Spins and Parities of 47K Levels Observed in the 48Ca(p, d)47Ca(IAS) Reaction NUCLEAR REACTIONS 48Ca(p, d), E=52 MeV; measured σ(Ed, θ). 47Ca deduced levels, J, π, isobaric analogs.
doi: 10.1143/JPSJ.30.1499
1971TA16 Phys.Rev.Lett. 27, 520 (1971) H.Taketani, M.Adachi, M.Ogawa, K.Ashibe, T.Hattori 0+ States in Mo Isotopes from (p, t) Reactions and Anomalies in the New Transitional Region NUCLEAR REACTIONS 92,94,96,98,100Mo(p, t), E=52 MeV; measured σ(Et, θ). 90,92,94,96,98Mo deduced 0+ state strengths.
doi: 10.1103/PhysRevLett.27.520
1970TA04 Nucl.Phys. To Be Published (1970) H.Taketani, M.Adachi, M.Ogawa, K.Ashibe, T.Hattori, H.Sanada
1969TA01 J.Phys.Soc.Japan 26, 204 (1969) H.Taketani, M.Adachi, Y.Yoshida, M.Ogawa, K.Ashibe Levels of 88Zr Excited with the Reaction 90Zr(p, t)88Zr NUCLEAR REACTIONS 90Zr(p, t), E=55 MeV; measured σ(Et, θ), Q. 88Zr deduced levels, J, π. Enriched 90Zr target.
doi: 10.1143/JPSJ.26.204
1969TA16 Genshikaku Kenkyu 14, 99 (1969) Extensive Level Structure of Nuclei Excited with (p, d) and (p, t) Reactions NUCLEAR REACTIONS 48Ca, 88Sr, 92Mo, 138Ba, 142Nd(p, d), E not given; 88Sr, 92Mo, 138Ba, 142Nd(p, t), E not given; measured σ(Ed, θ), σ(Et, θ). 47Ca, 86,87Sr, 91,90Mo, 136,137Ba, 140,141Nd deduced levels, J, π, L.
1968AD02 J.Phys.Soc.Japan 24, 227 (1968) M.Adachi, H.Taketani, K.Hisatake Decay of 2-Year 102Rh NUCLEAR STRUCTURE 102Rh; measured not abstracted; deduced nuclear properties.
doi: 10.1143/JPSJ.24.227
1968TA03 Phys.Letters 26B, 660 (1968); Erratum Phys.Lett. 27B, 222 (1968) H.Taketani, M.Adachi, Y.Yoshida, M.Ogawa, K.Ashibe Analog States Excited with the 93Nb(p, d)92Nb Reaction NUCLEAR STRUCTURE 92Nb; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(68)90381-X
1968TA07 Phys.Lett. 27B, 499 (1968) H.Taketani, M.Adachi, Y.Yoshida, M.Ogawa, K.Ashibe Level Structure of 89Zr via the Reaction 90Zr(p, d)89Zr NUCLEAR STRUCTURE 89Zr; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(68)90205-0
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