NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = Y.Aoki Found 76 matches. 2019RO02 Nucl.Phys. A982, 207c (2019) C.Rohrhofer, Y.Aoki, G.Cossu, H.Fukaya, L.Glozman, S.Hashimoto, C.B.Lang, S.Prelovsek Observation of approximate SU(2)CS and SU(2nf) symmetries in high temperature lattice QCD
doi: 10.1016/j.nuclphysa.2018.10.004
2013NA13 Hyperfine Interactions 220, 65 (2013) D.Nagae, T.Niwa, Y.Ishibashi, Y.Abe, S.Fukuoka, R.Nishikiori, S.Okada, Y.Saito, N.Inaba, A.Ozawa, Y.Aoki Development of rotating magnetic field system for the β-NMR method
doi: 10.1007/s10751-012-0721-5
2011OZ01 Phys.Rev. C 84, 064315 (2011) A.Ozawa, Y.Hashizume, Y.Aoki, K.Tanaka, T.Aiba, N.Aoi, H.Baba, B.A.Brown, M.Fukuda, K.Inafuku, N.Iwasa, T.Izumikawa, K.Kobayashi, M.Komuro, Y.Kondo, T.Kubo, M.Kurokawa, T.Matsuyama, S.Michimasa, T.Motobayashi, T.Nakabayashi, S.Nakajima, T.Nakamura, T.Ohtsubo, H.Sakurai, R.Shinoda, M.Shinohara, H.Suzuki, T.Suzuki, M.Takechi, E.Takeshita, S.Takeuchi, Y.Togano, K.Yamada, T.Yamaguchi, T.Yasuno, M.Yoshitake One- and two-neutron removal reactions from 19, 20C with a proton target NUCLEAR REACTIONS 1H(19C, 18C), (20C, 19C), (20C, 18C), [19,20C secondary beams from Ta(40Ar, X), E=63 MeV/nucleon primary reaction], E=40 MeV/nucleon; measured time of flight, energy loss, total energy, fragment longitudinal momentum distributions, inclusive cross section. 18,19C; calculated levels, J, π, cross sections. Continuum-discretized coupled-channel (CDCC) analysis of longitudinal momentum distributions. Riken Projectile Fragment Separator (RIPS). Comparison of inclusive removal cross sections with theoretical calculations using shell model spectroscopic factors and Glauber-model single-particle cross sections.
doi: 10.1103/PhysRevC.84.064315
2009AO05 Nucl.Phys. A830, 805c (2009) Y.Aoki, S.Borsanyi, S.Durr, Z.Fodor, S.D.Katz, S.Krieg, K.K.Szabo QCD transition temperature: approaching the continuum on the lattice
doi: 10.1016/j.nuclphysa.2009.10.141
2007AO01 Phys.Rev. D 75, 014507 (2007) Y.Aoki, C.Dawson, J.Noaki, A.Soni Proton decay matrix elements with domain-wall fermions NUCLEAR STRUCTURE 1H; calculated decay matrix elements.
doi: 10.1103/PhysRevD.75.014507
2007II02 Nucl.Phys. A793, 79 (2007) M.Iijima, Y.Aoki, A.Ozawa, N.Okumura CDCC analysis of 118Sn(d, p) reaction below Coulomb barrier NUCLEAR REACTIONS 118Sn(d, p), E≈2.5-10 MeV; calculated σ, elastic and inelastic σ(θ). DWBA and continuum discretized coupled channels analyses.
doi: 10.1016/j.nuclphysa.2007.06.013
2006YA21 Phys.Rev.C 74, 064606 (2006) M.Yamaguchi, Y.Tagishi, Y.Aoki, T.Iizuka, T.Nagatomo, T.Shinba, N.Yoshimaru, Y.Yamato, T.Katabuchi, M.Tanifuji Analyzing powers of polarized deuterons in low-energy 6Li(d, α)4He and 6Li(d, p0)7Li reactions in a resonance region NUCLEAR REACTIONS 6Li(polarized d, α), (polarized d, p), E=90 keV; measured Ep, Eα, vector and tensor analyzing powers; deduced resonance contributions.
doi: 10.1103/PhysRevC.74.064606
2005AO01 Nucl.Phys. B(Proc.Supp.) S140, 405 (2005) Y.Aoki, and the RBC Collaboration Nucleon Decay Matrix Elements with Nf = 0 and 2 Domain-Wall Quarks NUCLEAR STRUCTURE 1n, 1H; calculated nucleon decay matrix elements. Domain wall fermions.
doi: 10.1016/j.nuclphysbps.2004.11.372
2005YA02 Nucl.Phys. A747, 3 (2005) M.Yamaguchi, Y.Tagishi, Y.Aoki, N.Kawachi, N.Okumura, N.Yoshimaru Measurement of proton polarization in the 208Pb(d, p)209Pb reaction at an incident energy of 20 MeV NUCLEAR REACTIONS 208Pb(d, p), E=20.5 MeV; measured Ep, polarization, iT11(θ). DWBA and continuum discretized coupled channels analyses.
doi: 10.1016/j.nuclphysa.2004.09.001
2004AO02 Nucl.Phys. B(Proc.Supp.) S129/130, 305 (2004) Y.Aoki, and the RBC Collaboration Nucleon Decay with Domain-Wall Fermions NUCLEAR STRUCTURE 1n, 1H; calculated decay matrix elements.
doi: 10.1016/j.nuclphysbps.2003.12.141
2003AO03 Nucl.Phys. B(Proc.Supp.) S119, 380 (2003) Y.Aoki, for the RBC Collaboration Nucleon Decay Matrix Elements for Domain-Wall Fermions NUCLEAR STRUCTURE 1H; calculated decay matrix elements.
doi: 10.1016/S0920-5632(03)01560-3
2003HI01 Nucl.Phys. A714, 3 (2003) S.Hirowatari, Syafarudin, F.Aramaki, A.Nohtomi, G.Wakabayashi, Y.Uozumi, N.Ikeda, M.Matoba, Y.Aoki, K.Hirota, N.Okumura, T.Joh 100Mo(p(pol), d)99Mo reaction at 21 MeV and direct reaction analysis of the low-lying continuum spectrum NUCLEAR REACTIONS 100Mo(polarized p, d), E=21 MeV; measured deuteron spectra, σ(E, θ), Ay(E, θ). 99Mo deduced levels, J, π, spectroscopic factors, continuum features. DWBA analysis.
doi: 10.1016/S0375-9474(02)01353-2
2002OK04 Nucl.Instrum.Methods Phys.Res. A 487, 565 (2002) N.Okumura, Y.Aoki, T.Joh, Y.Honkyu, K.Hirota, K.S.Itoh Measuring system of proton total reaction cross-sections at tandem energy region NUCLEAR REACTIONS 27Al, Si(p, X), E=14-17 MeV; measured products; deduced σ, σ(E). Data were imported from EXFOR entry E2041.
doi: 10.1016/S0168-9002(01)02201-X
2001KA49 Phys.Rev. C64, 047601 (2001) T.Katabuchi, K.Kudo, K.Masuno, T.Iizuka, Y.Aoki, Y.Tagishi Polarization Transfer Coefficient Kyy' in the 2H(d, p)3H Reaction at θ = 0± at Very Low Energies NUCLEAR REACTIONS 2H(polarized d, p), E=90 keV; measured polarization transfer coefficient.
doi: 10.1103/PhysRevC.64.047601
2001TO07 Phys.Rev. C63, 035801 (2001) Y.Tokimoto, H.Utsunomiya, T.Yamagata, M.Ohta, Y.-W.Lui, R.P.Schmitt, S.Typel, Y.Aoki, K.Ieki, K.Katori Coulomb Breakup of 7Li for Nuclear Astrophysics NUCLEAR REACTIONS 27Al, 58Ni, 64Zn, 90Zr, 120Sn, 144Sm, 169Tm, 197Au, 208Pb(7Li, tα), E=42 MeV; measured triton, α spectra, σ(θ) following resonant and nonresonant Coulomb breakup; deduced postacceleration effect. 3H(α, γ), E(cm) ≈ 0.05-0.8 MeV; deduced astrophysical S factors.
doi: 10.1103/PhysRevC.63.035801
2000AO02 Nucl.Phys. A673, 189 (2000) Y.Aoki, N.Okumura, T.Joh, N.Takahashi, Y.Honkyu Coulomb Breakup and Polarizability of the Deuteron NUCLEAR REACTIONS 208Pb(d, d), E=3-7 MeV; analyzed σ(θ), related data; deduced effective deuteron polarizability. Continuum discretized coupled channels analysis.
doi: 10.1016/S0375-9474(00)00136-6
1999UT03 Nucl.Phys. (Supplement) A654, 928c (1999) H.Utsunomiya, Y.Tokimoto, T.Yamagata, M.Ohta, Y.Aoki, K.Hirota, K.Ieki, Y.Iwata, K.Katori, S.Hamada, Y.-W.Lui, R.P.Schmitt, S.Typel, G.Baur Excitation of Continuum States in 7Li and Their Decay by Quantum Tunneling NUCLEAR REACTIONS 27Al, 58Ni, 64Zn, 90Zr, 120Sn, 144Sm, 197Au(7Li, tα), E=42 MeV; measured particle spectra, forward-backward asymmetry; deduced E1, E2, higher-order effects in Coulomb breakup.
doi: 10.1016/S0375-9474(00)88575-9
1998HI05 Nucl.Phys. A628, 547 (1998) K.Hirota, Y.Aoki, N.Okumura, Y.Tagishi Deuteron Elastic Scattering and (d, p) Reactions on 208Pb at E(d) = 22 MeV and j-Dependence of T20 in (d, p) Reaction NUCLEAR REACTIONS 208Pb(polarized d, d), (polarized d, p), E=22 MeV; measured σ(θ), iT11(θ), T20(θ), T21(θ), T22(θ); deduced model independent optical parameters, j-dependence of T20. Continuum discretized coupled channels, DWBA analyses.
doi: 10.1016/S0375-9474(97)00641-6
1998LI39 Phys.Lett. 435B, 13 (1998) X.Liu, S.M.Lee, D.X.Jiang, T.Nakagawa, K.Yoshida, K.Yuasa-Nakagawa, Y.Aoki Reaction Time and Reaction Mechanisms of the Medium-Mass Reaction System 84Kr + 27Al at 8.5 MeV/u NUCLEAR REACTIONS 27Al(84Kr, X), E=8.5 MeV/nucleon; measured fragments charge distributions, Eα, Iα(θ), proton, α multiplicities; deduced reaction time. Diffusion model calculations.
doi: 10.1016/S0370-2693(98)00835-1
1998TA11 Nucl.Instrum.Methods Phys.Res. A402, 436 (1998) Y.Tagishi, T.Katabuchi, K.Mizukoshi, N.Yamada, M.Yamaguchi, N.Kawachi, Y.Aoki Analyzing Powers for 2H(d, p)3H and 2H(d, n)3He Reactions at Very Low Energies NUCLEAR REACTIONS 2H(polarized d, p), (polarized d, n), E=30-100 keV; measured vector, tensor analyzing powers.
doi: 10.1016/S0168-9002(97)00887-5
1998UT01 Phys.Lett. 416B, 43 (1998) H.Utsunomiya, Y.Tokimoto, H.Mabuchi, K.Osada, T.Yamagata, M.Ohta, Y.Aoki, K.Hirota, K.Ieki, Y.Iwata, K.Katori, S.Hamada, Y.-W.Lui, R.P.Schmitt Strongly-Suppressed Post-Coulomb Acceleration in Non-Resonant Breakup of 7Li NUCLEAR REACTIONS 27Al, 58Ni, 90Zr, 120Sn, 144Sm, 197Au(7Li, tα), E=42 MeV; measured tα-coin, σ(θ, Et, Eα); deduced no evidence for fragment post-acceleration. Non-resonant breakup, Coulomb dissociation, astrophysical implications.
doi: 10.1016/S0370-2693(97)01328-2
1998UT03 Nucl.Instrum.Methods Phys.Res. A402, 417 (1998) H.Utsunomiya, Y.Tokimoto, K.Osada, T.Yamagata, M.Ohta, Y.Aoki, K.Hirota, K.Ieki, Y.Iwata, K.Katori, S.Hamada, Y.-W.Lui, R.P.Schmitt Method of Coulomb Breakup Probing Primordial 7Li Synthesis NUCLEAR REACTIONS 90Zr(7Li, tα), E=42 MeV; measured t-, α-spectra, tα-coin; deduced astrophysical S-factors. Comparison with direct capture data.
doi: 10.1016/S0168-9002(97)00883-8
1998UT04 J.Phys.(London) G24, 1637 (1998) H.Utsunomiya, Y.Tokimoto, K.Osada, T.Yamagata, M.Ohta, Y.Aoki, K.Hirota, K.Ieki, Y.Iwata, K.Katori, S.Hamada, Y.-W.Lui, R.P.Schmitt Astrophysical Implications of Non-Resonant Break-Up of 7Li NUCLEAR REACTIONS 90Zr, 197Au(7Li, tα), E not given; analyzed nonresonant breakup data; deduced role of post-Coulomb acceleration.
doi: 10.1088/0954-3899/24/8/044
1997IS11 Physica B237-238, 304 (1997) K.Ishida, H.Mukuda, Y.Kitaoka, K.Asayama, H.Sugawara, Y.Aoki, H.Sato 59Co NQR Study in Superconducting CeCo2 NUCLEAR MOMENTS 59Co; measured NQR; deduced spin-lattice relaxation rate in CeCo2, superconducting properties.
doi: 10.1016/S0921-4526(97)00183-X
1997YU03 J.Phys.Soc.Jpn. 66, 73 (1997) H.Yuki, T.Sato, T.Ohtsuki, T.Yorita, Y.Aoki, H.Yamazaki, J.Kasagi, K.Ishii Measurement of the D(d, p)T Reaction in Ti for 2.5 < E(d) < 6.5 keV and Electron Screening in Metal NUCLEAR REACTIONS, ICPND 2H(d, p), E=2.5-6.5 keV; measured proton spectra, thick target yields, σ; deduced electron screening potential in Ti.
doi: 10.1143/JPSJ.66.73
1997YU04 J.Phys.(London) G23, 1459 (1997) H.Yuki, T.Satoh, T.Ohtsuki, T.Yorita, Y.Aoki, H.Yamazaki, J.Kasagi D + D Reaction in Metal at Bombarding Energies Below 5 keV NUCLEAR REACTIONS, ICPND 2H(d, p), E=2.5-7 keV; measured thick target yields ; deduced electron screening effects. Deuterium gas absorbed in thick Ti, Yb plates.
doi: 10.1088/0954-3899/23/10/036
1996AO01 Nucl.Phys. A599, 417 (1996) Y.Aoki, K.Hirota, H.Kishita, K.Koyama, M.Masaki, K.Miura, Y.Mukouhara, S.Nakagawa, N.Okumura, Y.Tagishi A New Approach to a ' Model-Independent ' Optical Potential and Its Application to Proton Elastic Scattering Near the (p, n) Threshold Energy Region NUCLEAR REACTIONS 40Ca, 28Si(polarized p, p), E=12.5-20.5 MeV; measured σ(θ), analyzing power vs θ. New approach to mode independent optical potential.
doi: 10.1016/0375-9474(95)00479-3
1996GO56 Nucl.Instrum.Methods Phys.Res. B118, 251 (1996) P.Goppelt-Langer, S.Yamamoto, Y.Aoki, H.Takeshita, H.Naramoto Light and Heavy Element Profiling using Heavy Ion Beams
doi: 10.1016/0168-583X(96)00252-2
1994MA18 Nucl.Phys. A573, 1 (1994) M.Masaki, Y.Aoki, K.Katoh, S.Nakagawa, N.Nakamoto, Y.Tagishi CDCC Analysis of 22 MeV Deuteron Elastic Scattering and (d, p) Reactions on 52Cr and 206Pb NUCLEAR REACTIONS 52Cr, 206Pb(polarized d, d), (polarized d, p), E=22 MeV; measured σ(θ), iT11(θ), T20(θ), T21(θ), T22(θ); deduced reaction mechanism. Enriched targets. CDCC analysis.
doi: 10.1016/0375-9474(94)90012-4
1993MI33 Hyperfine Interactions 78, 111 (1993) T.Minamisono, T.Ohtsubo, S.Fukuda, Y.Nakayama, T.Araki, K.Mashitani, K.Matsuda, E.Takahashi, M.Tanigaki, M.Tanaka, H.Shiohara, Y.Someda, Y.Aoki, A.Kitagawa, M.Fukuda, K.Matsuta, Y.Nojiri Precise Measurement of the Magnetic Moment of Doubly Closed Shell+1 Nucleon Nucleus 17F(I(π) = (5/2)+, T1/2 = 64.5s) RADIOACTIVITY 17F(β+); measured β-NMR spectra asymmetry change in NaF; deduced μ.
doi: 10.1007/BF00568124
1992TA19 Phys.Rev. C46, R1155 (1992) Y.Tagishi, N.Nakamoto, K.Katoh, J.Togawa, T.Hisamune, T.Yoshida, Y.Aoki Analyzing Powers for 2H(d, p)3H at Incident Energies of 30, 50, 70, and 90 keV NUCLEAR REACTIONS 2H(polarized d, p), E=30-90 keV; measured σ(θ), vector, tensor analyzing powers vs θ. Legendre polynomials analysis.
doi: 10.1103/PhysRevC.46.R1155
1991IS07 Phys.Lett. 265B, 207 (1991) Y.Iseri, M.Tanifuji, Y.Aoki, M.Kawai Effects of Tensor Interaction in p-n Breakup States on Deuteron Elastic Scattering NUCLEAR REACTIONS 40Ca(polarized d, d), E=56 MeV; analyzed σ(θ), vector, tensor analyzing power vs θ; deduced tensor interaction role in p-n breakup.
doi: 10.1016/0370-2693(91)90042-O
1990TO05 Phys.Rev. C41, 1486 (1990) M.Tomizawa, T.Aoki, Y.Aoki, T.Murayama, T.Sakai, Y.Tagishi, K.Yagi Asymmetry of Spin-Flip of Polarized Protons in the Inelastic Scattering to the First 2+ States of 48Ti and 50Ti NUCLEAR REACTIONS 48,50Ti(polarized p, p'), E=11.18 MeV; measured σ(θ), analyzing power vs θ, spin-flip probability vs θ, spin-flip asymmetry; deduced model parameters. Enriched target. Coupled-channel, DWBA analyses.
doi: 10.1103/PhysRevC.41.1486
1990TO16 J.Phys.(Paris), Colloq.C-6, 419 (1990) M.Tomizawa, T.Aoki, Y.Aoki, T.Murayama, T.Sakai, Y.Tagishi, K.Yagi Spin-Flip Asymmetry in the Proton Inelastic Scattering to the First 2+ States of 48,50Ti NUCLEAR REACTIONS 48,50Ti(polarized p, p'γ), E=11-18 MeV; measured σ(θ), analyzing power, spin-flip probability, asymmetry vs θ; deduced model parameters. DWBA, coupled-channels analyses. Coincidence techniques.
1987HA25 Nucl.Phys. A471, 520 (1987) K.Hashimoto, Y.Aoki, Y.Tagishi, K.Yagi Mechanism of (d, α) Reation: 208Pb(d, α)206Tl and 90Zr(d, α)88Y using vector- and tensor-polarized deuterons NUCLEAR REACTIONS 208Pb(polarized d, α), E=21.5 MeV; 90Zr(polarized d, α), E=22 MeV; measured σ(θ), iT11(θ), T20(θ), T21(θ), T22(θ); deduced mechanism. 206Tl level deduced (d, α) transition matrix element. Two-step processes, S-, D-state components of α-particle.
doi: 10.1016/0375-9474(87)90097-2
1987KU14 Nucl.Phys. A470, 377 (1987) M.Kurokawa, Y.Aoki, Y.Tagishi, K.Yagi One- and Two-Step Processes in Natural- and Unnatural-Parity 208Pb(p(pol), t)206Pb Reaction at E(p) = 22 MeV NUCLEAR REACTIONS 208Pb(polarized p, t), E=22 MeV; measured σ(Et, θ), A(Et, θ); deduced reaction mechansim. 206Pb levels deduced normalization factor. Magnetic spectrograph. First- and second-order DWBA analysis.
doi: 10.1016/0375-9474(87)90008-X
1987NA20 J.Phys.Soc.Jpn. 56, 1974 (1987) K.Nagano, Y.Aoki, T.Kishimoto, Y.Tagishi, K.Yagi Analyzing Powers for (p, t) Transitions to the First-Excited 2+ States of Medium-Mass Nuclei and Nuclear Collective Motion NUCLEAR REACTIONS, MECPD 94,96,98Mo, 100,102,104Ru, 104,106,108,110Pd, 112,114,116Cd, 118Sn, 122,128,130Te, 138Ba(polarized p, t), E=22 MeV; 104,110Pd(polarized p, t), E=52.2 MeV; measured σ(θ), analyzing power vs θ; deduced direct, two-step process interference, model parameters. First-, second-order DWBA.
doi: 10.1143/JPSJ.56.1974
1987TA07 Phys.Rev. C35, 1153 (1987) Y.Tagishi, Y.Aoki, M.Kurokawa, T.Murayama, T.Sakai, M.Takei, M.Tomizawa, K.Yagi Vector and Tensor Analyzing Power for the (d(pol), 6Li) Reactions on 12C and 16O NUCLEAR REACTIONS 12C, 16O(polarized d, 6Li), E=18, 22 MeV; measured σ(θ), iT11, T20, T21, T22 vs θ. DWBA analysis.
doi: 10.1103/PhysRevC.35.1153
1986BU14 Nucl.Phys. A457, 337 (1986) B.L.Burks, R.E.Anderson, T.B.Clegg, E.J.Ludwig, B.C.Karp, Y.Aoki A DWBA Analysis of the 86Sr(d(pol), p)87Sr Reaction and Implications for a 87Rb Solar Neutrino Detector NUCLEAR REACTIONS 86Sr(polarized d, p), (polarized d, d), E=11 MeV; measured σ(θ), vector analyzing power versus θ. 87Sr deduced levels, J, π, S. DWBA, optical model analyses.
doi: 10.1016/0375-9474(86)90382-9
1985YA02 Phys.Rev. C31, 120 (1985) K.Yagi, H.Iida, Y.Aoki, K.Hashimoto, Y.Tagishi Energy Dependence of (p, t) Analyzing Powers arising from Strong, Sequential, Two-Step Processes with j Dependence NUCLEAR REACTIONS 92Zr(polarized p, t), E=17, 18.5, 20.1, 21, 21.5, 22, 22.5, 28.5 MeV; 138Ba(polarized p, t), E=18.5, 20, 21, 22, 28.5 MeV; measured σ(θ), analyzing power vs θ. First-, second-order DWBA calculations, two-step processes.
doi: 10.1103/PhysRevC.31.120
1985YA03 Phys.Rev. C31, 676 (1985) K.Yagi, Y.Aoki, K.Hashimoto, H.Iida, H.Sakamoto, Y.Tagishi, M.Matoba, M.Igarashi, K.-I.Kubo Analyzing Power as a Probe for Clarifying Nuclear Reaction Mechanisms: Study of the two-step unbound channel contribution NUCLEAR REACTIONS 208Pb(polarized p, t), E=22, 35, 50 MeV; measured σ(θ), analyzing power vs θ; deduced two-step unbound channel role. First-, second-order finite range DWBA analysis.
doi: 10.1103/PhysRevC.31.676
1984BU23 Phys.Rev. C30, 742 (1984) B.L.Burks, R.E.Anderson, Y.Aoki, B.C.Karp, E.J.Ludwig, W.J.Thompson, R.L.Varner 81Kr-81Br Ground-State Mass Difference and Implications for Calibration of a 81Br Solar Neutrino Detector NUCLEAR REACTIONS 82Kr(d, t), (d, 3He), E=17 MeV; measured σ(Et), σ(E(3He)); deduced Q-value difference. 81Kr, 81Br deduced mass difference.
doi: 10.1103/PhysRevC.30.742
1984II01 Phys.Rev. C29, 328 (1984) H.Iida, Y.Aoki, K.Hashimoto, K.Nagano, Y.Tagishi, Y.Toba, K.Yagi Drastic Changes of (p, t) Analyzing Powers for the Isotopes 58,60,62,64Ni and Marked Incident-Energy Dependence of the Analyzing Powers as Evidence for Strong, Sequential, Two-Step Processes NUCLEAR REACTIONS 58,60,62,64Ni(polarized p, t), E=18, 20, 22 MeV; measured σ(θ), analyzing power vs θ; deduced optical model parameters, strong sequential, two-step process roles. DWBA analysis.
doi: 10.1103/PhysRevC.29.328
1983AO01 Nucl.Phys. A393, 52 (1983) Y.Aoki, H.Iida, K.Nagano, Y.Toba, K.Yagi Analyzing Powers and Cross Sections for (p, d) Reactions on Nuclei of N = 50-82 NUCLEAR REACTIONS 92Zr, 102Ru, 106,108Pd, 112,114Cd, 118Sn(polarized p, d), E=22 MeV; measured σ(θ, Ed), analyzing power vs θ, Ed. 91Zr, 101Ru, 105,107Pd, 111,113Cd, 117Sn levels deduced S. Adiabatic approximation, D-state effects, two-step processes, angular momentum mismatch, zero-range, finite-range DWBA analysis. Magnetic spectrograph.
doi: 10.1016/0375-9474(83)90064-7
1983AO02 Nucl.Phys. A394, 413 (1983) Y.Aoki, H.Iida, K.Hashimoto, K.Nagano, M.Takei, Y.Toba, K.Yagi Elastic and Inelastic Scattering of Polarized Protons from the Isotopes 104,106,108,110Pd NUCLEAR REACTIONS 104,106,108,110Pd(polarized p, p), (polarized p, p'), E=22 MeV; measured σ(θ), σ(E(p')), A(θ); deduced quadrupole spin-orbit deformation. 104,106,108,110Pd levels deduced β2, β3. Optical model, first-order DWBA, and coupled channel calculations.
doi: 10.1016/0375-9474(83)90115-X
1982AO01 Phys.Rev. C25, 1050 (1982) Y.Aoki, H.Iida, S.Kunori, K.Nagano, Y.Toba, K.Yagi Marked Changes in (p, t) Analyzing Powers for the Isotopes of Zr, Mo, Ru, and Pd and Strong, Sequential, Two-Step Transfer Processes in both (p, t) and (t, p) Reactions NUCLEAR REACTIONS 92Zr, 94,96,98Mo, 100,102,104Ru, 104,106,108,110Pd, 138Ba(polarized p, t), E=22 MeV; measured σ(θ), A(θ); deduced A(θ) dependence on (Q), E, structure effects, one-step, sequential transfer amplitude interference. First-, second-order DWBA.
doi: 10.1103/PhysRevC.25.1050
1982AO05 Nucl.Phys. A382, 269 (1982) Y.Aoki, S.Kunori, K.Nagano, Y.Toba, K.Yagi Importance of the Sequential Two-Step Transfer Process in a ΔS = 1 and ΔT = 1 Inelastic Transition of the 14N(p, p')14N Reaction NUCLEAR REACTIONS 14N(polarized p, p'), (polarized p, d), E=21 MeV; measured σ(θ), vector analyzing power; deduced reaction mechanism. DWBA analysis, knockon exchange, two-step processes. Gas target.
doi: 10.1016/0375-9474(82)90136-1
1981KU01 Phys.Rev.Lett. 46, 810 (1981) S.Kunori, Y.Aoki, H.Iida, K.Nagano, Y.Toba, K.Yagi Direct Experimental Evidence for Strong, Sequential, Two-Step, Transfer Processes in Allowed (p, t) Reactions NUCLEAR REACTIONS 92Zr, 94Mo(polarized p, t), E=22 MeV; 92Zr(polarized p, t), E=20.1 MeV; measured σ(θ), analysing power A(θ); deduced sequential two-step transfer process. DWBA analyses.
doi: 10.1103/PhysRevLett.46.810
1981TO05 Nucl.Phys. A359, 76 (1981) Y.Toba, K.Nagano, Y.Aoki, S.Kunori, K.Yagi Analyzing Powers for (p, d) Reactions on 208Pb and 142,144Nd Exciting Neutron-Hole States at Ep=22.0 MeV NUCLEAR REACTIONS 208Pb, 142,144Nd(polarized p, d), E=22 MeV; measured A(Ed, θ), σ(Ed, θ). 207Pb, 141,143Nd levels deduced S, configuration. 207Pb levels deduced j-dependence of A(θ). DWBA analysis. Enriched targets.
doi: 10.1016/0375-9474(81)90212-8
1981TO06 Phys.Lett. 100B, 232 (1981) Y.Toba, Y.Aoki, H.Iida, S.Kunori, K.Nagano, K.Yagi Strong Sequential Transfer Processes in 0+ → 0+ (p, t) Reactions on Pb Isotopes NUCLEAR REACTIONS 208,206,204Pb(polarized p, t), E=22 MeV; measured σ(θ), A(θ). 206,204,202Pb deduced strong sequential process for 0+ to 0+ ground state transition. First-, second-order DWBA, global potentials, shell model spectroscopic amplitudes.
doi: 10.1016/0370-2693(81)90323-3
1979AO01 Nucl.Phys. A322, 117 (1979) Y.Aoki, J.Sanada, K.Yagi, S.Kunori, Y.Higashi, S.Kato, J.Kawa, K.Okada, T.Izumoto Isospin Non-Conservation in the 14N(d, d')14N Reaction NUCLEAR REACTIONS 14N(d, d), (d, d'), (d, p), E=10.03-17.88 MeV; measured σ(θ, Ed), σ(θ, Ed'), σ(θ, Ep). Natural target. Second-order DWBA, Hauser-Feshbach analysis.
doi: 10.1016/0375-9474(79)90336-1
1979AO02 J.Phys.Soc.Jpn. 47, 329 (1979) Y.Aoki, K.Nagano, S.Kunori, K.Yagi Competition of Two-Step Process with Spin-Dependent Interaction in the 14N(p, p')14N(2.31 MeV) Reaction at E = 21.0 MeV NUCLEAR REACTIONS 14N(p, p'), E=21 MeV; measured σ(θ); deduced reaction mechanism, dependence on residual interaction.
doi: 10.1143/JPSJ.47.329
1979MA28 Nucl.Phys. A325, 389 (1979) M.Matoba, M.Hyakutake, N.Koori, Y.Irie, Y.Aoki Inelastic Proton Scattering on Doubly Even Selenium Isotopes NUCLEAR REACTIONS 76,78,80,82Se(p, p), (p, p'), E=51.9 MeV; measured σ(Ep, θ). 76,78,80,82Se deduced levels, L, β. Enriched target. DWBA, coupled channel analyses.
doi: 10.1016/0375-9474(79)90022-8
1979RA17 Phys.Rev. C20, 397 (1979) C.Rangacharyulu, Y.Aoki, K.Yagi, M.Matoba, M.Hyakutake 119,117Sn(p, t) Reactions at 52 MeV NUCLEAR REACTIONS 119,117Sn(p, t), E=52 MeV; measured σ(θ). 117,115Sn levels deduced J, π, integral σ, L-transfer. Unnormalized DWBA analysis.
doi: 10.1103/PhysRevC.20.397
1979TO14 Phys.Rev. C20, 1204 (1979) Y.Toba, Y.Aoki, S.Kunori, K.Nagano, K.Yagi Analyzing Power for the 208Pb(p, t)206Pb (3+) Reaction and (p, d)(d, t) Sequential Transfer Processes NUCLEAR REACTIONS 208Pb(polarized p, t), E=22 MeV; measured σ(Et, θ), Ay(E(t, θ)); deduced reaction mechanism. First-, second-order DWBA analysis. Enriched target.
doi: 10.1103/PhysRevC.20.1204
1979YA01 Phys.Rev. C19, 285 (1979) K.Yagi, S.Kunori, Y.Aoki, K.Nagano, Y.Tagishi, Y.Toba Systematic Nuclear-Structure Dependence of Analyzing Powers for (p, t) Reactions on Medium-Mass Vibrational Nuclei NUCLEAR REACTIONS 100Ru, 104,110Pd, 116Cd, 118Sn, 122,128Te(polarized p, t), E=22 MeV; measured σ(θ), Ay(θ). Enriched targets.
doi: 10.1103/PhysRevC.19.285
1979YA09 Phys.Rev.Lett. 43, 1087 (1979) K.Yagi, S.Kunori, Y.Aoki, K.Nagano, Y.Toba, K.-I.Kubo Anomalous Analyzing Powers for Strong(pol p, t) Ground-State Transitions and Interference between Direct and (p, d)(d, t) Sequential Process NUCLEAR REACTIONS 100Ru, 104,110Pd, 116Cd, 118Sn, 122,128,130Te, 144Nd(polarized p, t), E=22 MeV; measured σ(θ), A(θ); deduced interference effects between two-step, one-step processes.
doi: 10.1103/PhysRevLett.43.1087
1978YA01 Phys.Rev.Lett. 40, 161 (1978) K.Yagi, S.Kunori, Y.Aoki, Y.Higashi, J.Sanada, Y.Tagishi Difference in Analyzing Powers for (p, t) Reactions Due to a Phase Change of Interference between Direct and Indirect Processes in Two-Nucleon Transfer Reactions NUCLEAR REACTIONS 128Te, 110Pd(polarized p, t), E=22.0 MeV; measured σ(θ), A(θ).
doi: 10.1103/PhysRevLett.40.161
1977YA02 Phys.Rev. C15, 1178 (1977) K.Yagi, Y.Aoki, M.Matoba, M.Hyakutake Destructive Interference between Direct and Indirect Processes in (p, t) Reactions on Spherical Vibrational Nuclei and Strong Resemblance to That in (p, t) Reactions on Well-Deformed Nuclei NUCLEAR REACTIONS 104,108,110Pd(p, t), E=52 MeV; measured σ(Et, θ); deduced reaction mechanism.
doi: 10.1103/PhysRevC.15.1178
1976AO01 Phys.Lett. 61B, 437 (1976) Y.Aoki, S.Kato, J.Kawa, K.Okada, T.Izumoto Study of Isospin Forbidden and Allowed Transitions in 14N(d, d') at E = 10.03 and 11.65 MeV NUCLEAR REACTIONS 14N(d, d'), E=10.03, 11.65 MeV; measured σ(Ed', θ). 14N deduced isospin forbidden, allowed transitions.
doi: 10.1016/0370-2693(76)90722-X
1976MA21 Nucl.Phys. A261, 223 (1976) M.Matoba, M.Hyakutake, K.Yagi, Y.Aoki, C.Rangacharyulu Excitation of 3-, 5- and 7- States in Te Isotopes A = 120, 122, 124, 126, 128 with (p, t) Reactions NUCLEAR REACTIONS 122,124,126,128Te(p, t), E=51.9 MeV; measured σ(Et, θ). 120,122,124,126,128Te deduced levels, J, π, L. Enriched targets.
doi: 10.1016/0375-9474(76)90566-2
1975IZ02 Phys.Lett. 57B, 17 (1975) T.Izumoto, Y.Aoki, C.Rangacharyulu, K.Yagi, M.Matoba, M.Hyakutake One- and Two-Step Processes in (p, t) Transitions to the Quadrupole- and Octupole-Vibrational States in 122,128Te NUCLEAR REACTIONS 124,130Te(p, t), E=51.9 MeV; calculated σ(Et, θ).
doi: 10.1016/0370-2693(75)90232-4
1975MA03 Nucl.Phys. A237, 260 (1975) M.Matoba, M.Hyakutake, K.Yagi, Y.Aoki Elastic and Inelastic Scattering of 51.9 MeV Protons by Doubly Even Tellurium Nuclei NUCLEAR REACTIONS 122,124,126,128,130Te(p, p), (p, p'), E=51.9 MeV; measured σ(Ep, θ). 122,124,126,128,130Te deduced levels, J, π, L, βL. Enriched targets.
doi: 10.1016/0375-9474(75)90424-8
1974MA22 J.Phys.Soc.Jap. 36, 1486 (1974) M.Matoba, M.Hyakutake, K.Yagi, Y.Aoki, C.Rangacharyulu Excitation of Two Quasi-Particle 5- and 7- States in the 124,126,128,130Te(p, t) Reactions NUCLEAR REACTIONS 124,126,128,130Te(p, t), E=51.9 MeV; measured σ(Et, θ). 122,124,126,128Te deduced levels, L, J, π.
doi: 10.1143/JPSJ.36.1486
1974SA12 Phys.Lett. 51B, 51 (1974) M.Sakai, M.Sekiguchi, F.Soga, Y.Hirao, K.Yagi, Y.Aoki Excitation of the Deeply Bound g9/2 Neutron Hole State in 117Sn by a Neutron Pickup Reaction with 81.7 MeV 3He Particles NUCLEAR REACTIONS 92Mo, 118Sn, 140Ce, 208Pb(3He, α), E=81.7 MeV; measured σ(Eα, θ), deduced reaction mechanism.
doi: 10.1016/0370-2693(74)90149-X
1973KA08 J.Phys.Soc.Jap. 34, 1128 (1973) 2He(d, p)4He Reaction Proton Asymmetry with Polarized 3He Beam NUCLEAR REACTIONS 2H(polarized 3He, p), E=9 MeV; measured σ(Ep, θ).
doi: 10.1143/JPSJ.34.1128
1973MA12 Phys.Lett. 44B, 159 (1973) M.Matoba, M.Hyakutake, S.Nakamura, T.Katayama, T.Tonai, K.Yagi, K.Sato, Y.Aoki Splittings of the Octupole Strength in Te Isotopes NUCLEAR REACTIONS 126,128,130Te(p, p'), E=51.91 MeV; measured σ(Ep, θ). 126,128,130Te deduced octupole levels, strengths.
doi: 10.1016/0370-2693(73)90509-1
1973MA29 Phys.Lett. 45B, 463 (1973) M.Matoba, M.Hyakutake, J.Niidome, K.Yagi, Y.Aoki, K.Sato Strong L = 5 Transition in Te(p, p') Reactions NUCLEAR REACTIONS 122,124,126,128,130Te(p, p'), E=51.9 MeV; measured σ(Ep', θ). 122,126,128,130Te deduced levels, J, π, B(EL).
doi: 10.1016/0370-2693(73)90644-8
1973YA07 Phys.Lett. 44B, 447 (1973) K.Yagi, Y.Aoki, C.Rangacharyulu, K.Matoba, M.Hyakutake, J.Nidome Effect of Inelastic Scattering Processes on (p, t) Reactions Exciting the First 2+ States in Te, Sn and Cd Isotopes NUCLEAR REACTIONS 114,116Cd, 116,118Sn, 122,124,126,128,130Te(p, t), E=52 MeV; measured σ(θ).
doi: 10.1016/0370-2693(73)90330-4
1972YA07 Phys.Rev.Lett. 29, 1334 (1972) K.Yagi, K.Sato, Y.Aoki, T.Udagawa, T.Tamura (p, t) Excitations of Removal and Addition Types of Quadrupole-Pairing Vibrational States in Even Nd Isotopes NUCLEAR REACTIONS 142,144,146,148,150Nd(p, t), E=52 MeV; analyzed σ(θ). 2-step coupled-channel Born approximation.
doi: 10.1103/PhysRevLett.29.1334
1972YA09 J.Phys.Soc.Jap. 33, 1482 (1972) One-Proton Coupled L = 0 and 2 Transitions in the 141Pr(p, t) Reaction NUCLEAR REACTIONS 141Pr(p, t), E=52 MeV; measured σ(θ). 139Pr deduced levels, L.
doi: 10.1143/JPSJ.33.1482
1971YA10 Phys.Lett. 37B, 369 (1971) Coupled Particle-Pairing Vibrational Excitations in 141Nd and 143Nd by The (p, t) Reaction NUCLEAR REACTIONS 143,145Nd(p, t), E=52 MeV; measured σ(Et, θ), Q. 142,144Nd(p, t), E=52 MeV; measured σ(Et, θ), Q. 141,143Nd deduced coupled particle-pairing vibrational states, L.
doi: 10.1016/0370-2693(71)90205-X
1971YA11 J.Phys.Soc.Jap. 31, 1838 (1971) The (p, t) and (p, d) Reactions on the Nd Isotopes of A = 142-150 NUCLEAR REACTIONS 142,144,146,148,150Nd(p, d), E=52 MeV; measured σ(Ed).
doi: 10.1143/JPSJ.31.1838
1970YA04 J.Phys.Soc.Jap. 28, 1583 (1970) Pairing Vibrational [f7/2(1, 0)] States in 141Nd Obtained from L = 0 and 2 Transitions in a 143Nd(p, t) Reaction NUCLEAR REACTIONS 143Nd(p, t), E=52 MeV; measured σ(Et, θ). 141Nd deduced levels, L, configurations.
doi: 10.1143/JPSJ.28.1583
1970YA05 Nucl.Phys. A149, 45 (1970) Strong L = 0 and 2 Transitions in (p, t) Reactions on Even-Mass Ce Isotopes NUCLEAR REACTIONS 140,142Ce(p, t), E=52.1 MeV; measured σ(Et, θ); deduced Q. 138,140Ce duduced levels, J, π. Enriched target.
doi: 10.1016/0375-9474(70)90377-5
1969YA07 Phys.Letters 29B, 647 (1969) K.Yagi, Y.Aoki, J.Kawa, K.Sato Strong L=0 and 2 Transitions in (p, t) Reactions in Even-Mass Nd Isotopes NUCLEAR REACTIONS 142,144,146,150Nd(p, t), E=51.7 MeV; measured σ(Et, θ). 140,142,144,146Nd deduced levels, L. Enriched targets.
doi: 10.1016/0370-2693(69)90098-7
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