NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = T.Inoue Found 55 matches. 2020PA12 Eur.Phys.J. A 56, 93 (2020) A.Park, S.H.Lee, T.Inoue, T.Hatsuda Baryon-baryon interactions at short distances: constituent quark model meets lattice QCD
doi: 10.1140/epja/s10050-020-00078-z
2020SA12 Nucl.Phys. A998, 121737 (2020) K.Sasaki, S.Aoki, T.Doi, S.Gongyo, T.Hatsuda, Y.Ikeda, T.Inoue, T.Iritani, N.Ishii, K.Murano, T.Miyamoto, for the HAL QCD Collaboration ΛΛ and NΞ interactions from lattice QCD near the physical point
doi: 10.1016/j.nuclphysa.2020.121737
2018MC02 Phys.Rev. C 97, 021303 (2018) C.Mcilroy, C.Barbieri, T.Inoue, T.Doi, T.Hatsuda Doubly magic nuclei from lattice QCD forces at MPS = 469 MeV/C2 NUCLEAR STRUCTURE 4He, 16O, 40Ca; calculated ground-state energies as functions of harmonic oscillator frequency, model space size and effective box radius, matter and charge radii, single-particle spectral strength distribution of 16O. Self-consistent calculations with HAL469 QCD potentials in the algebraic diagrammatic construction (ADC) approach. Use of Bethe-Goldstone equation (BGE) in ab initio approach. Comparison with experimental data.
doi: 10.1103/PhysRevC.97.021303
2018MI02 Nucl.Phys. A971, 113 (2018) T.Miyamoto, S.Aoki, T.Doi, S.Gongyo, T.Hatsuda, Y.Ikeda, T.Inoue, T.Iritani, N.Ishii, D.Kawai, K.Murano, H.Nemura, K.Sasaki ΛcN interaction from lattice QCD and its application to Λc hypernuclei NUCLEAR STRUCTURE 208Pb; calculated Λc-208Pb hypernuclei folding potentials for different mass of π-meson. 12C, 28Si, 40Ca, 58Ni, 90Zr, 208Pb; calculated expected Λc hypernuclei binding energy, Q.
doi: 10.1016/j.nuclphysa.2018.01.015
2017DO07 Phys.Rev. C 95, 062201 (2017) Fully coupled-channels complex scaling method for the K-pp
doi: 10.1103/PhysRevC.95.062201
2015IN01 Phys.Rev. C 91, 011001 (2015) T.Inoue, S.Aoki, B.Charron, T.Doi, T.Hatsuda, Y.Ikeda, N.Ishii, K.Murano, H.Nemura, K.Sasaki Medium-heavy nuclei from nucleon-nucleon interactions in lattice QCD NUCLEAR STRUCTURE 16O, 40Ca; calculated single-particle levels, total energy, ground-state energy, rms radius, mass number dependence of binding energies, and density distributions. Brueckner-Hartree-Fock method with the nucleon-nucleon forces from lattice QCD simulations.
doi: 10.1103/PhysRevC.91.011001
2014AS03 Physics of Part.and Nuclei 45, 199 (2014) K.Asahi, Y.Ichikawa, M.Chikamori, Y.Ohtomo, E.Hikota, T.Suzuki, T.Inoue, T.Furukawa, A.Yoshimi, K.Suzuki, T.Nanao, H.Miyatake, M.Tsuchiya, N.Yoshida, H.Shirai, T.Ino, H.Ueno, Y.Matsuo, T.Fukuyama Search for electric dipole moment in 129Xe atom using a nuclear spin oscillator ATOMIC PHYSICS 129Xe; analyzed experimental sensitivity for electric dipole moment measurements.
doi: 10.1134/S1063779614010080
2014IT01 Phys.Rev.Lett. 113, 102501 (2014) M.Itoh, S.Ando, T.Aoki, H.Arikawa, S.Ezure, K.Harada, T.Hayamizu, T.Inoue, T.Ishikawa, K.Kato, H.Kawamura, Y.Sakemi, A.Uchiyama Further Improvement of the Upper Limit on the Direct 3α Decay from the Hoyle State in 12C NUCLEAR REACTIONS 12C(12C, 3α)12C, E=110 MeV; measured reaction products, Eα, Iα; deduced yields, Dalitz plots, Hoyle state, branching ratios, J, π. Comparison with available data.
doi: 10.1103/PhysRevLett.113.102501
2013DO06 Nucl.Phys. A912, 66 (2013) Comprehensive application of a coupled-channel complex scaling method to the K(bar) N - π Γ systems
doi: 10.1016/j.nuclphysa.2013.05.003
2013IC02 Hyperfine Interactions 220, 47 (2013) Y.Ichikawa, H.Ueno, Y.Ishii, T.Furukawa, A.Yoshimi, D.Kameda, H.Watanabe, N.Aoi, K.Asahi, D.L.Balabanski, R.Chevrier, J.M.Daugas, N.Fukuda, G.Georgiev, H.Hayashi, H.Iijima, N.Inabe, T.Inoue, M.Ishihara, T.Kubo, T.Nanao, T.Ohnishi, K.Suzuki, M.Tsuchiya, H.Takeda, M.M.Rajabali Novel method for the production of spin-aligned RI beams in projectile fragmentation reaction with the dispersion matching technique NUCLEAR REACTIONS 9Be(48Ca, X)33Al, E=345 MeV/nucleon; Al(33Al, X)32Al, E not given; measured reaction products, Eγ, Iγ; deduced spin-aligned radioactive ion beam.
doi: 10.1007/s10751-012-0682-8
2013IN03 Hyperfine Interactions 220, 59 (2013) T.Inoue, T.Furukawa, A.Yoshimi, Y.Ichikawa, M.Chikamori, Y.Ohtomo, M.Tsuchiya, N.Yoshida, H.Shirai, M.Uchida, K.Suzuki, T.Nanao, H.Miyatake, H.Ueno, Y.Matsuo, T.Fukuyama, K.Asahi Nuclear spin maser and experimental search for 129Xe atomic EDM NUCLEAR MOMENTS 129Xe; measured time-variations of the maser frequency and the cell temperature; deduced sources of systematic errors in electric dipole moment measurements.
doi: 10.1007/s10751-012-0751-z
2013IN04 Phys.Rev.Lett. 111, 112503 (2013) T.Inoue, S.Aoki, T.Doi, T.Hatsuda, Y.Ikeda, N.Ishii, K.Murano, H.Nemura, K.Sasaki, for the HAL QCD Collaboration Equation of State for Nucleonic Matter and its Quark Mass Dependence from the Nuclear Force in Lattice QCD
doi: 10.1103/PhysRevLett.111.112503
2012CH16 Phys.Rev.Lett. 108, 162501 (2012) R.Chevrier, J.M.Daugas, L.Gaudefroy, Y.Ichikawa, H.Ueno, M.Hass, H.Haas, S.Cottenier, N.Aoi, K.Asahi, D.L.Balabanski, N.Fukuda, T.Furukawa, G.Georgiev, H.Hayashi, H.Iijima, N.Inabe, T.Inoue, M.Ishihara, Y.Ishii, D.Kameda, T.Kubo, T.Nanao, G.Neyens, T.Ohnishi, M.M.Rajabali, K.Suzuki, H.Takeda, M.Tsuchiya, N.Vermeulen, H.Watanabe, A.Yoshimi Is the 7/21-1 Isomer State of 43S Spherical? NUCLEAR MOMENTS 43S; measured isomer deexciting Eγ, Iγ; deduced spectroscopic quadrupole moment. Comparison with SDPF-U interaction shell model calculations.
doi: 10.1103/PhysRevLett.108.162501
2012DO03 Prog.Theor.Phys.(Kyoto) 127, 723 (2012) T.Doi, S.Aoki, T.Hatsuda, Y.Ikeda, T.Inoue, N.Ishii, K.Murano, H.Nemura, K.Sasaki, for the HAL QCD Collaboration Exploring Three-Nucleon Forces in Lattice QCD
doi: 10.1143/PTP.127.723
2012IC06 J.Phys.:Conf.Ser. 381, 012090 (2012) Y.Ichikawa, H.Ueno, Y.Ishii, T.Furukawa, A.Yoshimi, D.Kameda, H.Watanabe, N.Aoi, K.Asahi, D.L.Balabanski, R.Chevrier, J.M.Daugas, N.Fukuda, G.Georgiev, H.Hayashi, H.Iijima, N.Inabe, T.Inoue, M.Ishihara, T.Kubo, T.Nanao, T.Ohnishi, K.Suzuki, M.Tsuchiya, H.Takeda, M.M.Rajabali Production of spin-aligned RI beam via two-step fragmentation with dispersion matching
doi: 10.1088/1742-6596/381/1/012090
2012IC07 Nat.Phys. 8, 918 (2012) Y.Ichikawa, H.Ueno, Y.Ishii, T.Furukawa, A.Yoshimi, D.Kameda, H.Watanabe, N.Aoi, K.Asahi, D.L.Balabanski, R.Chevrier, J.-M.Daugas, N.Fukuda, G.Georgiev, H.Hayashi, H.Iijima, N.Inabe, T.Inoue, M.Ishihara, T.Kubo, T.Nanao, T.Ohnishi, K.Suzuki, M.Tsuchiya, H.Takeda, M.M.Rajabali Production of spin-controlled rare isotope beams
doi: 10.1038/nphys2457
2012IN01 Nucl.Phys. A881, 28 (2012) T.Inoue, S.Aoki, T.Doi, T.Hatsuda, Y.Ikeda, N.Ishii, K.Murano, H.Nemura, K.Sasaki, for the HAL QCD Collaboration Two-baryon potentials and H-dibaryon from 3-flavor lattice QCD simulations
doi: 10.1016/j.nuclphysa.2012.02.008
2009AS05 Int.J.Mod.Phys. E18, 2020 (2009) K.Asahi, K.Shimada, K.Kameda, D.Nagae, M.Uchida, K.Suzuki, T.Inoue, N.Hatakeyama, S.Kagami, Y.Hasama, H.Ueno, H.Yoshimi, T.Nagatomo, T.Sugimoto, M.Ishihara, J.Murata, H.Kawamura, K.Narita Study of neutron-rich nuclei through static electromagnetic moments
doi: 10.1142/S0218301309014214
2009NA03 Phys.Rev. C 79, 027301 (2009) D.Nagae, H.Ueno, D.Kameda, M.Takemura, K.Asahi, K.Takase, A.Yoshimi, T.Sugimoto, K.Shimada, T.Nagatomo, M.Uchida, T.Arai, T.Inoue, S.Kagami, N.Hatakeyama, H.Kawamura, K.Narita, J.Murata Ground-state electric quadrupole moment of 31Al NUCLEAR REACTIONS 93Nb(40Ar, X)31Al, E=95 MeV/nucleon; measured ground state electric quadrupole moment for a spin polarized 31Al beam using β-NQR spectroscopy. NUCLEAR MOMENTS 31Al; measured ground state electric quadrupole moments using the β-NQR method.
doi: 10.1103/PhysRevC.79.027301
2008NA28 Nucl.Instrum.Methods Phys.Res. B266, 4612 (2008) D.Nagae, H.Ueno, D.Kameda, M.Takemura, K.Asahi, K.Takase, A.Yoshimi, T.Sugimoto, K.Shimada, T.Nagatomo, M.Uchida, T.Arai, T.Inoue, S.Kagami, N.Hatakeyama, J.Murata, H.Kawamura, K.Narita Electric quadrupole moment of 31Al NUCLEAR REACTIONS 93Nb(40Ar, X)31Al, E=95 MeV/nucleon; measured ground state electric quadrupole moment for a spin polarized 31Al beam using β-NQR spectroscopy using RIPS at RIKEN facility. NUCLEAR MOMENTS 31Al; measured ground state electric quadrupole moments using the β-NQR method.
doi: 10.1016/j.nimb.2008.05.111
2007IN05 Nucl.Phys. A790, 530c (2007) A pentaquark model for Λ(1405)
doi: 10.1016/j.nuclphysa.2007.03.172
2007KA18 Phys.Lett. B 647, 93 (2007) D.Kameda, H.Ueno, K.Asahi, M.Takemura, A.Yoshimi, T.Haseyama, M.Uchida, K.Shimada, D.Nagae, G.Kijima, T.Arai, K.Takase, S.Suda, T.Inoue, J.Murata, H.Kawamura, Y.Kobayashi, H.Watanabe, M.Ishihara Measurement of the electric quadrupole moment of 32Al RADIOACTIVITY 32Al(β-) [from 40Ar fragmentation]; measured β-NMR spectra. 32Al deduced quadrupole moment.
doi: 10.1016/j.physletb.2007.01.063
2007KA68 Hyperfine Interactions 180, 61 (2007) D.Kameda, H.Ueno, K.Asahi, D.Nagae, M.Takemura, K.Shimada, A.Yoshimi, T.Nagatomo, T.Sugimoto, M.Uchida, T.Arai, K.Takase, S.Suda, T.Inoue, J.Murata, H.Kawamura, H.Watanabe, Y.Kobayashi, M.Ishihara Electric quadrupole moments of neutron-rich nuclei 32Al and 31Al NUCLEAR MOMENTS 32,31Al(β-); measured ground state electric quadrupole moments using the β-NQR method.
doi: 10.1007/s10751-008-9685-x
2007SH50 Hyperfine Interactions 180, 43 (2007) K.Shimada, D.Nagae, K.Asahi, T.Inoue, K.Takase, S.Kagami, N.Hatakeyama, Y.Kobayashi, H.Ueno, A.Yoshimi, D.Kameda, T.Nagatomo, T.Sugimoto, S.Kubono, H.Yamaguchi, Y.Wakabayashi, G.Amadio, S.Hayakawa, J.Murata, H.Kawamura Production of spin-polarized 17N beam using inverse-kinematics low-energy transfer reactions
doi: 10.1007/s10751-008-9626-8
2007UE02 Eur.Phys.J. Special Topics 150, 185 (2007) H.Ueno, D.Kameda, D.Nagae, M.Takemura, K.Asahi, K.Shimada, K.Takase, T.Sugimoto, T.Nagatomo, M.Uchida, T.Arai, T.Inoue, A.Yoshimi, T.Kawamura, K.Narita Nuclear moments of neutron-rich aluminum isotopes RADIOACTIVITY 30,31,32Al(β-); measured magnetic dipole and electric quadrupole moments using the β-NMR method.
doi: 10.1140/epjst/e2007-00299-y
2005CH75 Phys.Rev. C 72, 061001 (2005) J.-W.Chen, T.Inoue, X.Ji, Y.Li Fixing two-nucleon weak-axial coupling L1, A from μ-d capture NUCLEAR REACTIONS 2H(μ-, ν), E at rest; calculated capture σ vs outgoing neutrons relative energy; deduced constraints on weak-axial coupling. Pionless effective field theory.
doi: 10.1103/PhysRevC.72.061001
2004IN02 Phys.Rev. C 69, 035207 (2004) T.Inoue, V.E.Lyubovitskij, Th.Gutsche, A.Faessler Updated analysis of meson-nucleon σ terms in the perturbative chiral quark model
doi: 10.1103/PhysRevC.69.035207
2003IN04 Nucl.Phys. A721, 661c (2003) η nucleus optical potential in a chiral unitary approach
doi: 10.1016/S0375-9474(03)01147-3
2003SA28 Nucl.Phys. A726, 349 (2003) The ΛΛ → YN weak transition in double - Λ hypernuclei NUCLEAR STRUCTURE 6He; calculated two-Λ hypernucleus decay rate. Hybrid approach.
doi: 10.1016/j.nuclphysa.2003.07.008
2003SA45 Nucl.Phys. A721, 971c (2003) Nonmesonic decay of Λ and ΛΛ hypernuclei NUCLEAR STRUCTURE 5,6He; calculated hypernucleus nonmesonic decay widths. Comparison with data.
doi: 10.1016/S0375-9474(03)01262-4
2003SA68 Mod.Phys.Lett. A 18, 131 (2003) Nonmesonic decay of Λ and ΛΛ hypernuclei NUCLEAR STRUCTURE 5,6He; calculated nonmesonic decay rates for one- and two-Λ hypernuclei.
doi: 10.1142/S0217732303010107
2002GA46 Phys.Lett. 550B, 47 (2002) C.Garcia-Recio, T.Inoue, J.Nieves, E.Oset η bound states in nuclei NUCLEAR STRUCTURE 12C, 24Mg, 27Al, 28Si, 40Ca, 208Pb; calculated η-meson bound states energies, widths.
doi: 10.1016/S0370-2693(02)02960-X
2002IN01 Phys.Rev. C65, 035204 (2002) T.Inoue, E.Oset, M.J.Vicente Vacas Chiral Unitary Approach to S-Wave Meson Baryon Scattering in the Strangeness S = 0 Sector
doi: 10.1103/PhysRevC.65.035204
2002IN05 Nucl.Phys. A710, 354 (2002) η in the nuclear medium within a chiral unitary approach
doi: 10.1016/S0375-9474(02)01167-3
2002SA35 Nucl.Phys. A707, 477 (2002) Nonmesonic Weak Decay of Light Hypernuclei with Coherent Σ Mixing NUCLEAR STRUCTURE 4H, 4,5He; calculated hypernuclei nonmesonic decay rates. Quark-meson hybrid model.
doi: 10.1016/S0375-9474(02)01006-0
2001IN02 Nucl.Phys. A684, 478c (2001) Study of pn → pΛ Weak Scattering in a Quark Model NUCLEAR REACTIONS 1H(n, X), E at 900-1200 MeV/c; calculated Λ hyperon production σ. Quark cluster approach.
doi: 10.1016/S0375-9474(01)00511-5
2001SA59 Nucl.Phys. A691, 201c (2001) Non-Mesonic Weak Decay of Light Hypernuclei NUCLEAR STRUCTURE 4H, 4,5He; calculated nonmesonic hypernucleus decay widths. Quark-meson hybrid model.
doi: 10.1016/S0375-9474(01)01031-4
2000IN03 Nucl.Phys. A670, 301c (2000) Weak Hyperon Nucleon Interaction in a Quark Model NUCLEAR REACTIONS 1n(p, X), E=900-1200 MeV; calculated hyperon production σ; deduced reaction mechanism features.
doi: 10.1016/S0375-9474(00)00118-4
2000IN06 Prog.Theor.Phys.(Kyoto), Suppl. 137, 147 (2000) T.Inoue, K.Sasaki, S.Takeuchi, M.Oka Weak Hyperon-Nucleon Interaction in a Quark Model and Application to the pn → Λp Scattering NUCLEAR REACTIONS 1H(n, X), E=900-1200 MeV; calculated hyperon production σ; deduced role of direct quark mechanism, other reaction mechanism features.
doi: 10.1143/PTPS.137.147
2000SA17 Nucl.Phys. A669, 331 (2000); Erratum Nucl.Phys. A678, 455 (2000) Weak Decay of Λ in Nuclei: Quarks versus mesons
doi: 10.1016/S0375-9474(99)90427-X
1999TA10 J.Radioanal.Nucl.Chem. 239, 117 (1999) K.Takamiya, T.Inoue, K.Nakanishi, A.Yokoyama, N.Takahashi, T.Saito, H.Baba, Y.Nakagome Fission Fragment Configurations at the Scission Point of 233U, 235U and 239Pu(nth, f) NUCLEAR REACTIONS 233,235U, 239Pu(n, F), E=thermal; measured fission fragments kinetic energy, mass distributions, deformation; deduced multi-mode fission mechanism.
doi: 10.1007/BF02349541
1999YO03 J.Radioanal.Nucl.Chem. 239, 143 (1999) A.Yokoyama, S.Morimoto, T.Inoue, J.Sanada, H.Araki, T.Saito, H.Baba, S.Shibata, A.Shinohara, T.Muroyama, Y.Ohkubo Reaction Mechanism for Target-Like Products from 197Au Target Bombarded with 12C Ions of Energies Above 100 MeV/u NUCLEAR REACTIONS 197Au(12C, X), E=180, 230, 400 MeV/nucleon; measured Z=77-79 products production σ; deduced reaction mechanism features. Activation technique.
doi: 10.1007/BF02349546
1998IN01 Nucl.Phys. A633, 312 (1998) T.Inoue, M.Oka, T.Motoba, K.Itonaga Non-Mesonic Weak Decays of Light Hypernuclei in the Direct Quark and the One-Pion Exchange Mechanisms NUCLEAR STRUCTURE 4H, 4,5He; calculated hypernuclei non-mesonic decay rates; deduced contributions from one pion exchange, direct quark mechanisms. Comparison with data.
doi: 10.1016/S0375-9474(98)00005-0
1996IN01 Nucl.Phys. A597, 563 (1996) Direct Quark Transition Potential for ΛN → NN Decay
doi: 10.1016/0375-9474(95)00441-6
1994IN02 Nucl.Phys. A577, 281c (1994) Nonleptonic Weak Decays of Hyperon and Hypernuclei
doi: 10.1016/0375-9474(94)90868-0
1987KI26 Phys.Lett. 199B, 331 (1987) K.Kimura, K.Anai, Y.Funatsu, Y.Ikeda, H.Inoue, T.Inoue, M.Izumi, N.Kato, Y.Nakajima, T.Okamoto, T.Sugimitsu, T.Tachikawa, Y.Yamaguchi, H.Fujita Excitation of J(π) = 2+ Resonances in 24Mg by the 23Na(p, 12C)12C Reaction NUCLEAR REACTIONS, MECPD 23Na(p, 12C), E=8-18 MeV; measured σ(θ) vs E. ΔE-E telescope. S-matrix analyses. 24Mg deduced resonances, J, π, Γ, reduced width ratios.
doi: 10.1016/0370-2693(87)90928-2
1986AR15 Nucl.Phys. A459, 286 (1986) A.Arima, N.Onishi, T.Inoue, Y.Akiyama, T.Suzuki Three-Body Forces and the Structure of the sd-Shell NUCLEAR STRUCTURE 16O, 40Ca; calculated total energies. 17O, 17F; calculated total energies, single particle states. A=16-22; calculated rms radii, binding energy, incompressibility vs mass number. A=34-40; calculated rms radii, binding energy, incompressibility vs mass number. 20Ne, 36Ar; calculated levels, quadrupole moments, B(E2). Three-body forces effective interaction.
doi: 10.1016/0375-9474(86)90136-3
1986IW01 Radiat.Eff. 92, 191 (1986) S.Iwasaki, H.Tamura, T.Inoue, T.Tamura, J.Koyama, K.Sugiyama Measurement and Analysis of Neutron Emission Spectra for Pb(n, xn) Reaction between 14 and 20 MeV NUCLEAR REACTIONS Pb(n, xn), E=14-20 MeV; measured σ(E); deduced (n, 2n), (n, 3n) reaction σ(E).
doi: 10.1080/00337578608208319
1984IN04 J.Phys.Soc.Jpn. 53, 4158 (1984) Fluctuations in the Reaction 19F(p, α)16O in the Range E(p) = 7.6-13.0 MeV NUCLEAR REACTIONS 19F(p, α), E=4.15-13 MeV; measured σ(Eα), σ(θ). 20Ne deduced coherence width. Statistical model, DWBA analyses.
doi: 10.1143/JPSJ.53.4158
1984TA08 Phys.Lett. 139B, 267 (1984) T.Tachikawa, N.Kato, H.Fujita, K.Kimura, T.Sugimitsu, K.Morita, K.Anai, T.Inoue, H.Inoue, Y.Nakajima, M.H.Tanaka, S.Kubono The Phase Anomaly for Elastic and Inelastic Scattering of the 19F + 12C System NUCLEAR REACTIONS 19F(12C, 12C), (12C, 12C'), E=30-60 MeV; measured σ(E(12C)), σ(θ). 12C(19F, 19F), (19F, 19F'), E=63.8 MeV; measured σ(E(19F)); deduced optical model parameters, phase anomaly characteristics. DWBA, coupled-channels analyses.
doi: 10.1016/0370-2693(84)91077-3
1976IN04 J.Inorg.Nucl.Chem. 38, 1425 (1976) Production of 7Be from Proton Bombardment of Light Elements NUCLEAR REACTIONS Be, B, N, O(p, 7Be), E ≤ 52 MeV; measured σ(E, E(7Be)).
doi: 10.1016/0022-1902(76)90001-4
1969RA10 AFCRL-69-0071 (MITNE-85) (1969) N.C.Rasmussen, Y.Hukai, T.Inouye, V.J.Orphan Thermal Neutron Capture Gamma-Ray Spectra of the Elements NUCLEAR REACTIONS Li, Be, B, C, N, F, Na, Mg, Al, Si, P, S, Cl, K, Ca, Sc, Ti, V, Cr, Mn, Fe, Co, Ni, Cu, Zn, Ga, Ge, As, Se, Br, Rb, Sr, Y, Zr, Nb, Mo, Ru, Rh, Pd, Ag, Sn, Sb, Te, I, Cs, Ba, La, Ce, Pr, Nd, Sm, Eu, Gd, Tb, Dy, Ho, Er, Tm, Yb, Lu, Hf, Ta, W, Re, Os, Ir, Pt, Au, Hg, Tl, Pb, Bi(n, γ), E=thermal; measured Eγ, Iγ. Ge(Li) detector, natural targets.
1967IN03 Nucl.Phys. A99, 305 (1967) T.Inoue, T.Sebe, K.K.Huang, A.Arima The Structure of the sd-Shell Nuclei (III). Effect of Non-Central Interactions
doi: 10.1016/0375-9474(67)90343-0
1966IN01 Nucl.Phys. 85, 184 (1966) T.Inoue, T.Sebe, H.Hagiwara, A.Arima The Structure of the sd-shell Nuclei (II). Spectroscopic Factor of One-Nucleon Transfer Reaction NUCLEAR STRUCTURE 20Ne; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(66)90141-6
1964IN03 Nucl.Phys. 59, 1 (1964) T.Inoue, T.Sebe, H.Hagiwara, A.Arima The Structure of the sd-shell Nuclei (I). C18, F18, O19, F19 and Ne20 NUCLEAR STRUCTURE 19F, 18F, 19O, 20Ne, 18C; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(64)90110-5
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