NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = Y.Abe Found 100 matches. 2023IW01 J.Nucl.Sci.Technol.(Tokyo) 60, 1 (2023) O.Iwamoto, N.Iwamoto, S.Kunieda, F.Minato, S.Nakayama, Y.Abe, K.Tsubakihara, S.Okumura, C.Ishizuka, T.Yoshida, S.Chiba, N.Otuka, J.-C.Sublet, H.Iwamoto, K.Yamamoto, Y.Nagaya, K.Tada, C.Konno, N.Matsuda, K.Yokoyama, H.Taninaka, A.Oizumi, M.Fukushima, S.Okita, G.Chiba, S.Sato, M.Ohta, S.Kwon Japanese evaluated nuclear data library version 5: JENDL-5 NUCLEAR REACTIONS 233,235,238U, 237Np, 238,239,240,242Pu, 241,243Am, 243,244,245,246Cm(n, F), (n, γ), E<20 MeV; analyzed available data; deduced σ, average energies of prompt fission neutrons, prompt neutron multiplicities. Neutron sublibrary for all of stable and unstable isotopes with the half-lives longer than 1 day for Z<101 except 257Es. Comparison with JENDL-4.0, ENDF/B-VIII.0 and EXFOR libraries.
doi: 10.1080/00223131.2022.2141903
2023TS06 Phys.Rev.Lett. 131, 092502 (2023) K.Tsukada, Y.Abe, A.Enokizono, T.Goke, M.Hara, Y.Honda, T.Hori, S.Ichikawa, Y.Ito, K.Kurita, C.Legris, Y.Maehara, T.Ohnishi, R.Ogawara, T.Suda, T.Tamae, M.Wakasugi, M.Watanabe, H.Wauke First Observation of Electron Scattering from Online-Produced Radioactive Target NUCLEAR REACTIONS 137Cs(e-, e-), E=149.3 MeV; measured reaction products; deduced σ(θ). Comparison with calculations. Self-confining RI ion target (SCRIT), 150-MeV electron microtron.
doi: 10.1103/PhysRevLett.131.092502
2023YO01 Eur.Phys.J. A 59, 191 (2023) A.Yogo, Y.Arikawa, Y.Abe, S.R.Mirfayzi, T.Hayakawa, K.Mima, R.Kodama Advances in laser-driven neutron sources and applications
doi: 10.1140/epja/s10050-023-01083-8
2022LI20 Phys.Rev.Lett. 128, 152701 (2022) H.F.Li, S.Naimi, T.M.Sprouse, M.R.Mumpower, Y.Abe, Y.Yamaguchi, D.Nagae, F.Suzaki, M.Wakasugi, H.Arakawa, W.B.Dou, D.Hamakawa, S.Hosoi, Y.Inada, D.Kajiki, T.Kobayashi, M.Sakaue, Y.Yokoda, T.Yamaguchi, R.Kagesawa, D.Kamioka, T.Moriguchi, M.Mukai, A.Ozawa, S.Ota, N.Kitamura, S.Masuoka, S.Michimasa, H.Baba, N.Fukuda, Y.Shimizu, H.Suzuki, H.Takeda, D.S.Ahn, M.Wang, C.Y.Fu, Q.Wang, S.Suzuki, Z.Ge, Y.A.Litvinov, G.Lorusso, P.M.Walker, Z.Podolyak, T.Uesaka First Application of Mass Measurements with the Rare-RI Ring Reveals the Solar r-Process Abundance Trend at A=122 and A=123 ATOMIC MASSES 123Pd, 125Cd, 126In; measured frequencies; deduced mass excess values with low uncertainties. Comparison with calculations. Radioactive Isotope Beam Factory (RIBF) in RIKEN.
doi: 10.1103/PhysRevLett.128.152701
2022MO16 J.Phys.(London) G49, 065103 (2022) T.Mori, A.Yogo, T.Hayakawa, S.R.Mirfayzi, Z.Lan, T.Wei, Y.Abe, Y.Arikawa, M.Nakai, K.Mima, H.Nishimura, S.Fujioka, R.Kodama Thermal neutron fluence measurement using a cadmium differential method at the laser-driven neutron source NUCLEAR REACTIONS 197Au, 59Co, 55Mn(n, γ), (n, 2n), 180Hf(n, γ), (n, n'), 176Hf(n, 2n), E thermal; measured reaction products, Eγ, Iγ; deduced γ-ray energies, thermal neutron fluence. The LFEX laser at the ILE in Osaka U niversity.
doi: 10.1088/1361-6471/ac6272
2021AB02 Prog.Theor.Exp.Phys. 2021, 021D01 (2021) Y.Abe, D.Boilley, Q.Hourdille, C.Shen A dynamical study of fusion hindrance with the Nakajima-Zwanzig projection method
doi: 10.1093/ptep/ptab005
2021MO19 Phys.Rev. C 104, 015808 (2021) T.Mori, A.Yogo, T.Hayakawa, S.R.Mirfayzi, Z.Lan, Y.Abe, Y.Arikawa, D.Golovin, T.Wei, Y.Honoki, M.Nakai, K.Mima, H.Nishimura, S.Fujioka, R.Kodama Direct evaluation of high neutron density environment using (n, 2n) reaction induced by laser-driven neutron source NUCLEAR REACTIONS 55Mn, 59Co, Hf, 197Au(n, 2n), (n, γ)54Mn/56Mn/56Co/58Co/175Hf/180mHf/181Hf/196Au/198Au, E=8-20 MeV neutrons from 9Be(p, n), E=30 MeV and 9Be(d, n), E=20 MeV reactions and laser-driven neutron source (LDNS) at the fast ignition experiment (LFEX) laser system at the ILE, Osaka University; measured Eγ, Iγ; deduced production reaction rates for isotopes and isomer, σ(E) for (n, 2n) reaction; evaluated neutron fluxes from (n, 2n) reaction using the activation method and the TOF. 196,198Au; measured half-lives of decays of ground states from γ-decay curves. Relevance to evaluation of high-density neutrons in stellar environments and nucleosynthesis by r-process.
doi: 10.1103/PhysRevC.104.015808
2020MO05 Nucl.Phys. A994, 121663 (2020) T.Moriguchi, M.Amano, A.Ozawa, W.Horiuchi, Y.Abe, T.Fujii, R.Kagesawa, D.Kamioka, A.Kitagawa, M.Mukai, D.Nagae, M.Sakaue, S.Sato, S.Suzuki, T.Suzuki, T.Yamaguchi, K.Yokota Energy dependence of total reaction cross sections for 17Ne on a proton target
doi: 10.1016/j.nuclphysa.2019.121663
2017SA16 Nucl.Phys. A961, 142 (2017) K.Sawahata, A.Ozawa, Y.Saito, Y.Abe, Y.Ichikawa, N.Inaba, Y.Ishibashi, A.Kitagawa, S.Matsunaga, T.Moriguchi, D.Nagae, S.Okada, S.Sato, S.Suzuki, T.Suzuki, Y.Takeuchi, T.Yamaguchi, J.Zenihiro Investigations of charge-changing processes for light proton-rich nuclei on carbon and solid-hydrogen targets NUCLEAR REACTIONS 1H, 12C(25Si, x), (26Si, x), (27Si, x), (28Si, x), (33Cl, x), (34Ar, x), (35Ar, x), (36Ar, x), E≈300 MeV/nucleon; measured charge-changing reaction products; deduced total charge-changing σ, partial charge-changing σ; calculated total charge-changing σ, partial charge-changing σ. 1H, 25,26,27Si, 33Cl; calculated, estimated nuclear proton RMS radii using total charge-changing σ and Glauber model with correction factor. 33Cl; calculated, estimated proton skin thickness.
doi: 10.1016/j.nuclphysa.2017.02.012
2016AB02 Phys.Rev. C 93, 054608 (2016) Y.Abe, for the Double Chooz Collaboration Muon capture on light isotopes measured with the Double Chooz detector NUCLEAR REACTIONS 12C(μ-, xnypzαν)6He/8B/8Li/11Be/12B/8He/9Li, E at rest; 13C(μ-, xnypzαν)8Li/9Li/11Li/12Be/12B/13B, E at rest; 14N(μ-, 5nν)9C, E at rest; 16O(μ-, xnypzαν)14B/9C/15C/12N, E at rest; measured Eγ, Iγ, yields, neutrons, β decays in Double Chooz reactor neutrino detector.
doi: 10.1103/PhysRevC.93.054608
2016KU11 Phys.Rev. C 93, 054313 (2016) A.Kusoglu, G.Georgiev, C.Sotty, D.L.Balabanski, A.Goasduff, Y.Ishii, Y.Abe, K.Asahi, M.Bostan, R.Chevrier, M.Chikamori, J.M.Daugas, T.Furukawa, H.Nishibata, Y.Ichikawa, Y.Ishibashi, R.Lozeva, H.Miyatake, D.Nagae, T.Nanao, M.Niikura, T.Niwa, S.Okada, A.Ozawa, Y.Saito, H.Shirai, H.Ueno, D.T.Yordanov, N.Yoshida Magnetic moment of the 13/2+ isomeric state in 69Cu: Spin alignment in the one-nucleon removal reaction NUCLEAR MOMENTS 69Cu; measured Eγ, Iγ, γγ-, (particle)γ-coin, γ-ray yields, γ(θ), Larmor precession under external magnetic field, time-dependent perturbed angular distribution (TDPAD) method; deduced isomer half-life, magnetic moment, multipolarity, spin alignment in one-nucleon removal reaction at RIKEN facility. 69Cu beam from 9Be(70Zn, X), E=63.13 MeV/nucleon reaction using RIPS separator at RIKEN. NUCLEAR REACTIONS 9Be(70Zn, X)69Cu, E=63.13 MeV/nucleon; measured Eγ, Iγ, γγ-coin, γ(θ), isomer half-life by γ(t) using RIPS separator at RIKEN. 69Cu; deduced levels, multipolarity, g factor of a level in 69Cu, configurations. Comparison with shell-model calculations using JUN45 and jj4b interactions.
doi: 10.1103/PhysRevC.93.054313
2016LU08 Phys.Rev. C 94, 034616 (2016) H.Lu, D.Boilley, Y.Abe, C.Shen Synthesis of superheavy elements: Uncertainty analysis to improve the predictive power of reaction models NUCLEAR REACTIONS 208Pb(58Fe, n)265Hs, E not given; calculated distribution of the empirical formation probability. Z=102-114; calculated cross sections for evaporation residues (ER) for one-neutron evaporation from compound nuclei with Z=102-114, formation and survival probabilities using uncertainty analysis for experimental data and theoretical parameters to constrain fusion models.
doi: 10.1103/PhysRevC.94.034616
2014MC08 Nucl.Data Sheets 120, 88 (2014) E.Mcneice, K.Setoodehnia, B.Singh, Y.Abe, D.N.Binh, A.A.Chen, J.Chen, S.Cherubini, S.Fukuoka, T.Hashimoto, T.Hayakawa, Y.Ishibashi, Y.Ito, D.Kahl, T.Komatsubara, S.Kubono, T.Moriguchi, D.Nagae, R.Nishikiori, T.Niwa, A.Ozawa, T.Shizuma, H.Suzuki, H.Yamaguchi, T.Yuasa In-beam γ-ray Spectroscopy of 30P via the 28Si(3He, pγ)30P Reaction NUCLEAR REACTIONS 28Si(3He, p), E=9 MeV; measured reaction products, Eγ, Iγ, γ-γ-coin.; deduced level structure, J, π, resonance states, γ-γ directional correlation of oriented nuclei. Comparison with available data.
doi: 10.1016/j.nds.2014.07.014
2014MO19 Nucl.Phys. A929, 83 (2014) T.Moriguchi, A.Ozawa, S.Ishimoto, Y.Abe, M.Fukuda, I.Hachiuma, Y.Ishibashi, Y.Ito, T.Kuboki, M.Lantz, D.Nagae, K.Namihira, D.Nishimura, T.Ohtsubo, H.Ooishi, T.Suda, H.Suzuki, T.Suzuki, M.Takechi, K.Tanaka, T.YamaguchI Density distribution of 14Be from reaction cross-section measurements NUCLEAR REACTIONS 1H, 12C(14Be, x), E=46, 79 MeV/nucleon; measured reaction products; deduced reaction σ. 14Be deduced using also data at other energies, mass density distribution, radius; calculated σ.
doi: 10.1016/j.nuclphysa.2014.06.003
2013AB09 Phys.Lett. B 723, 66 (2013) Y.Abe, for the Double Chooz Collaboration First measurement of Θ13 from delayed neutron capture on hydrogen in the Double Chooz experiment
doi: 10.1016/j.physletb.2013.04.050
2013IS07 Hyperfine Interactions 220, 71 (2013) Y.Ishibashi, D.Nagae, Y.Abe, T.Nagatomo, A.Ozawa, H.Suzuki, S.Fukuoka, R.Nishikiori, T.Niwa, K.Matsuta, Y.Tagishi Production of nuclear polarization of unstable nuclei via polarization transfer reactions NUCLEAR REACTIONS 19F(polarized d, p)20F, E=7 MeV; 24Mg(polarized p, n)24Al, E=20 MeV; 29Si(polarized p, n)29P, E=12 MeV; 28Si(polarized d, n)29P, E=4 MeV; 40Ca(polarized d, n)41Sc, E=7 MeV; measured reaction products; deduced yields, polarization. Comparison with available data.
doi: 10.1007/s10751-012-0750-0
2013MI10 Hyperfine Interactions 220, 83 (2013) M.Mihara, K.Matsuta, D.Nishimura, M.Fukuda, M.Yaguchi, K.Iwamoto, M.Wakabayashi, Y.Kamisho, J.Ohno, Y.Morita, T.Izumikawa, T.Ohtsubo, S.Suzuki, M.Nagashima, K.Abe, T.Sakai, S.Momota, A.Ozawa, D.Nagae, Y.Ishibashi, Y.Abe, T.Niwa, T.Nagatomo, T.Minamisono, M.K.Kubo, A.Kitagawa, M.Torikoshi, M.Kanazawa, S.Sato Production of spin polarized 12N through heavy ion reactions NUCLEAR REACTIONS Be(14N, X)12N, E=70, 100 MeV/nucleon; 1H(12C, n)12N, E=70 MeV/nucleon; measured reaction products; deduced spin polarization and production yields. Comparison with available data.
doi: 10.1007/s10751-013-0869-7
2013MO21 Phys.Rev. C 88, 024610 (2013) T.Moriguchi, A.Ozawa, S.Ishimoto, Y.Abe, M.Fukuda, I.Hachiuma, Y.Ishibashi, Y.Ito, T.Kuboki, M.Lantz, D.Nagae, K.Namihira, D.Nishimura, T.Ohtsubo, H.Ooishi, T.Suda, H.Suzuki, T.Suzuki, M.Takechi, K.Tanaka, T.Yamaguchi Density distributions of 11Li deduced from reaction cross-section measurements NUCLEAR REACTIONS 1H, 12C(11Li, X), E=31, 41 MeV/nucleon; measured particle spectra, time-of-flight, reaction σ(E) using RIPS at RIKEN facility. 11Li; deduced neutron, proton, and matter density distributions, root-mean-square (rms) radii. Glauber model calculations based on the optical limit approximation. Comparison with previous data for 6,7,8,9,11Li. Discussed disappearance of N=8 shell gap.
doi: 10.1103/PhysRevC.88.024610
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
2013SE08 Phys.Rev. C 87, 065801 (2013) K.Setoodehnia, A.A.Chen, D.Kahl, T.Komatsubara, J.Jose, R.Longland, Y.Abe, D.N.Binh, J.Chen, S.Cherubini, J.A.Clark, C.M.Deibel, S.Fukuoka, T.Hashimoto, T.Hayakawa, J.Hendriks, Y.Ishibashi, Y.Ito, S.Kubono, W.N.Lennard, T.Moriguchi, D.Nagae, R.Nishikiori, T.Niwa, A.Ozawa, P.D.Parker, D.Seiler, T.Shizuma, H.Suzuki, C.Wrede, H.Yamaguchi, T.Yuasa Nuclear structure of 30S and its implications for nucleosynthesis in classical novae NUCLEAR REACTIONS 32S(p, t), E=34.5 MeV; measured triton spectra, σ(θ) using Enge split-pole magnetic spectrograph at WNSL, Yale facility. 28Si(3He, n), E=9 MeV; measured Eγ, Iγ, γγ-coin, γ(θ), γγ(θ)(DCO) at UTTAC facility. 30S; deduced levels, resonances, J, π, multipolarity, σ/J, mixing ratio, branching ratios, proton and gamma widths, resonance strengths. DWBA and coupled reaction channel analyses of σ(θ) data in (p, t). 29P(p, γ)30S, at T=0.01-1.5 GK; deduced astrophysical reaction rates, nova isotopic abundances of Si to Ca mass region isotopes using 1D hydrodynamic model.
doi: 10.1103/PhysRevC.87.065801
2012UE02 Prog.Theor.Phys.(Kyoto) 127, 831 (2012) Resonances in 28Si + 28Si. I - Dinuclear Molecular Model with Axial Asymmetry - NUCLEAR REACTIONS 28Si(28Si, X), E not given; calculated rotational properties, moment of inertia, energy levels, J, π. Dinuclear molecular model, comparison with available data.
doi: 10.1143/PTP.127.831
2012UE03 Prog.Theor.Phys.(Kyoto) 127, 877 (2012) Resonances in 28Si + 28Si. II - Analyses for the Angular Distributions and Angular Correlations - NUCLEAR REACTIONS 28Si(28Si, X), E(cm)=55.8 MeV; calculated rotational properties, moment of inertia, energy levels, J, π, resonance widths, σ(θ). Dinuclear molecular model, comparison with available data.
doi: 10.1143/PTP.127.877
2011BO27 Phys.Rev. C 84, 054608 (2011) D.Boilley, H.Lu, C.Shen, Y.Abe, B.G.Giraud Fusion hindrance of heavy ions: Role of the neck NUCLEAR REACTIONS 100Mo(100Mo, X), 110Pd(110Pd, X), E not given; calculated liquid drop model potential energy, neck distribution, LDM potential contour plots, fusion probability.
doi: 10.1103/PhysRevC.84.054608
2011OC01 J.Korean Phys.Soc. 59, 1953s (2011) K.Ochiai, K.Kondo, S.Ohnishi, K.Takakura, S.Sato, Y.Abe, C.Konno, C.Suzuki, T.Yagi DT Neutronics Benchmark Experiment on Lead at JAEA-FNS NUCLEAR REACTIONS 27Al(n, α), 90Zr(n, 2n), 93Nb(n, 2n)93mNb, 115In(n, n'), E≈14.5 MeV; measured reaction rates, neutron flux; calculated reaction rates, neutron flux using FENDL-2.1, JENDL-3.3, ENDF/B-VII.0, JEFF-3.1.
doi: 10.3938/jkps.59.1953
2011SH19 Phys.Rev. C 83, 054620 (2011) C.Shen, D.Boilley, Q.Li, J.Shen, Y.Abe Fusion hindrance in reactions with very heavy ions: Border between normal and hindered fusion NUCLEAR REACTIONS 208Pb(86Kr, X), 110Pd(110Pd, X), 100Mo(100Mo, X), 90Zr(90Zr, X), E not given; calculated LDM potential, fusion hindrance. Two-center liquid drop model.
doi: 10.1103/PhysRevC.83.054620
2010AB19 Nucl.Phys. A834, 349c (2010) Y.Abe, C.Shen, D.Boilley, B.G.Giraud, G.Kosenko Mechanism of Fusion Hindrance and Predictions of SHE Production NUCLEAR REACTIONS 249Bk, 249Cf(48Ca, xn), E*=20-55 MeV; calculated σ, reaction mechanism features.
doi: 10.1016/j.nuclphysa.2010.01.037
2010UE02 Nucl.Phys. A834, 796c (2010) Resonances of nuclear molecule 28Si-28Si NUCLEAR REACTIONS 28Si(28Si, 28Si), (28Si, 28Si'), E not given; calculated σ(θ), angular correlations for mutual 2+ excitations assuming di-nuclear molecular state responsible for 55.8 MeV resonance.
doi: 10.1016/j.nuclphysa.2010.01.149
2009AB28 Int.J.Mod.Phys. E18, 2169 (2009) Y.Abe, C.Shen, D.Boilley, B.G.Giraud From di-nucleus to mono-nucleus: Neck evolution in fusion of massive systems NUCLEAR REACTIONS 100Mo(100Mo, X), E not given; calculated the neck degree of freedom during fusioning process between heavy ions, average trajectory, over-passing probability and the current at the top of the barrier.
doi: 10.1142/S0218301309014494
2008AB26 Int.J.Mod.Phys. E17, 2214 (2008) Y.Abe, C.Shen, G.Kosenko, D.Boilley, B.G.Giraud Di-nucleus dynamics toward fusion of heavy nuclei
doi: 10.1142/S0218301308011367
2008BO34 Int.J.Mod.Phys. E17, 1681 (2008) D.Boilley, A.Marchix, D.Wilgenbus, Y.Lallouet, F.Gimbert, Y.Abe What can we learn from the fission time of the super-heavy elements?
doi: 10.1142/S0218301308010696
2008SH26 Int.J.Mod.Phys. E17, Supplement 1, 66 (2008) C.W.Shen, Y.Abe, D.Boilley, G.Kosenko, E.Zhao Isospin dependence of reactions 48Ca+243-251Bk NUCLEAR REACTIONS 243,244,245,246,247,248,249,250,251Bk(48Ca, X), E(cm)=203.3 MeV; calculated fusion σ. Two-step model, KEWPIE code.
doi: 10.1142/S0218301308011768
2008UE02 Int.J.Mod.Phys. E17, 2034 (2008) Molecular resonances in the 28Si + 28Si system NUCLEAR REACTIONS 28Si(28Si, X), E(cm)=55.8 MeV; analyzed resonances for medium light heavy-ion collisions; deduced di-nuclear molecular model, σ(θ), energy levels. Comparison with experiment.
doi: 10.1142/S0218301308011045
2007AB08 Int.J.Mod.Phys. E16, 491 (2007) Y.Abe, A.Marchix, C.Shen, B.Yilmaz, G.Kosenko, D.Boilley, B.G.Giraud Dynamics of massive systems and synthesis of superheavy elements NUCLEAR REACTIONS 208Pb(58Fe, n), E(cm)=210-235 MeV; 132Sn, 160Gd(132Sn, n), (132Sn, 2n), (132Sn, 3n), (132Sn, 4n), E(cm)=265-295 MeV; calculated fusion and evaporation residue σ.
doi: 10.1142/S0218301307005922
2007SA30 J.Nucl.Sci.Technol.(Tokyo) 44, 657 (2007) S.Sato, Y.Verzilov, K.Ochiai, M.Wada, C.Kutsukake, S.Tanaka, Y.Abe, M.Seki, Y.Oginuma, M.Kawabe, T.Nishitani, C.Konno Neutronics Experimental Study on Tritium Production in Solid Breeder Blanket Mockup with Neutron Reflector
doi: 10.1080/18811248.2007.9711854
2006AB33 Phys.Atomic Nuclei 69, 1101 (2006) Y.Abe, G.I.Kosenko, C.W.Shen, B.Bouriquet, A.Marchix, D.Boilley, B.Giraud Fusion Hindrance and Synthesis of Superheavy Elements NUCLEAR REACTIONS 208Pb(58Ni, X), (64Ni, X), (70Zn, X), (71Ga, X), (76Ge, X), E(cm) ≈ 210-310 MeV; 209Bi(70Zn, X), E(cm) ≈ 260-300 MeV; 160Gd(132Sn, X), E(cm) ≈ 325-350 MeV; calculated fusion excitation functions. 208Pb(58Fe, n), (64Ni, n), (70Zn, n), (71Ga, n), (76Ge, n), E(cm) ≈ 215-285 MeV; 209Bi(64Ni, n), (70Zn, n), E(cm) ≈ 235-275 MeV; 160Gd(132Sn, γ), (132Sn, n), (132Sn, 2n), (132Sn, 3n), E(cm) ≈ 325-350 MeV; calculated σ. Fusion hindrance mechanism discussed.
doi: 10.1134/S1063778806070027
2004AB07 Nucl.Phys. A734, 168 (2004) Y.Abe, B.Bouriquet, G.Kosenko, C.Shen Theoretical Predictions of Residue Cross Sections for Superheavy Elements NUCLEAR REACTIONS 208Pb(64Ni, n), (70Zn, n), (71Ga, n), (76Ge, n), E(cm) ≈ 230-290 MeV; 209Bi(64Ni, n), (70Zn, n), E(cm) ≈ 230-270 MeV; calculated excitation functions. Two-step model, comparison with data.
doi: 10.1016/j.nuclphysa.2004.01.026
2004AB25 Acta Phys.Hung.N.S. 19, 77 (2004) Y.Abe, D.Boilley, B.Giraud, G.Kosenko, C.Shen Fusion Theory for Synthesis of the Superheavy Elements NUCLEAR REACTIONS 238U, 244Pu, 248Cm, 252Cf(48Ca, X), E(cm) ≈ 180-250 MeV; calculated fusion excitation functions. Fluctuation-dissipation dynamics, comparison with data.
doi: 10.1556/APH.19.2004.1-2.11
2004BO11 Comput.Phys.Commun. 159, 1 (2004) KEWPIE: A dynamical cascade code for decaying exited compound nuclei NUCLEAR REACTIONS 246Cm(12C, xn), 242Pu(16O, xn), 236U(22Ne, xn), 232Th(26Mg, xn), E* ≈ 30-70 MeV; calculated evaporation residue σ. 208Pb(48Ca, xn), E*=5-50 MeV; calculated fusion and evaporation residue σ. Dynamical cascade code, comparisons with data.
doi: 10.1016/j.cpc.2003.10.002
2004BO31 Prog.Theor.Phys.(Kyoto), Suppl. 154, 425 (2004) Theoretical Predictions of Cross-Sections of the Super-Heavy Elements NUCLEAR REACTIONS 208Pb, 209Bi(64Ni, n), (70Zn, n), 208Pb(58Fe, n), (71Ga, n), (76Ge, n), E(cm) ≈ 200-290 MeV; calculated σ. Two-step model, comparisons with data.
doi: 10.1143/PTPS.154.425
2004BO40 Eur.Phys.J. A 22, 9 (2004) Predictions of the residue cross-sections for the elements Z = 113 and Z = 114 NUCLEAR REACTIONS 208Pb(58Fe, X), (64Ni, X), (70Zn, X), (71Ga, X), (76Ge, X), 209Bi(70Zn, X), E(cm) ≈ 200-320 MeV; calculated fusion σ. 208Pb(58Fe, n), (71Ga, n), (76Ge, n), 208Pb, 209Bi(64Ni, n), (70Zn, n), E(cm) ≈ 220-290 MeV; calculated evaporation residue σ. Two-step model, comparisons with data.
doi: 10.1140/epja/i2004-10058-0
2003AB17 Yad.Fiz. 66, 1093 (2003); Phys.Atomic Nuclei 66, 1057 (2003) Y.Abe, C.W.Shen, G.I.Kosenko, D.Boilley Theory of Fusion for Superheavy Elements NUCLEAR REACTIONS 238U, 244Pu, 248Cm, 252Cf(48Ca, X), E(cm) ≈ 180-240 MeV; calculated fusion σ, maximum evaporation residue σ. Two-step model, comparison with data.
doi: 10.1134/1.1586418
2003AB29 Nucl.Phys. A722, 241c (2003); Erratum Nucl.Phys. A733, 351 (2004) Y.Abe, B.Bouriquet, C.Shen, G.Kosenko Theory of fusion hindrance and synthesis of the superheavy elements NUCLEAR REACTIONS 238U, 244Pu, 248Cm, 252Cf(48Ca, X), E(cm)=180-250 MeV; calculated fusion excitation functions. 238U, 244Pu, 248Cm, 252Cf(48Ca, 2n), (48Ca, 3n), (48Ca, 4n), E* ≈ 20-50 MeV; calculated evaporation residue σ. Two-step model, comparisons with data.
doi: 10.1016/S0375-9474(03)01372-1
2003AB33 Acta Phys.Pol. B34, 2091 (2003) Y.Abe, D.Boilley, G.Kosenko, C.Shen Reaction mechanisms for synthesis of superheavy elements NUCLEAR REACTIONS 238U, 244Pu, 248Cm, 252Cf(48Ca, X), E(cm)=180-250 MeV; calculated fusion σ. Two-step mechanism, shape evolution. Comparison with data.
2003AB34 Acta Phys.Pol. B34, 1927 (2003) On theoretical problems in synthesis of superheavy elements NUCLEAR REACTIONS 238U, 244Pu, 248Cm(48Ca, X), E(cm)=180-250 MeV; calculated fusion excitation functions. 208Pb, 244Pu(48Ca, n), (48Ca, 2n), (48Ca, 3n), (48Ca, 4n), E* ≈ 5-50 MeV; calculated fusion, evaporation residue σ. Comparisons with data.
2003BO42 Eur.Phys.J. A 18, 627 (2003) Inverse Kramers formula and fusion dynamics of heavy ions
doi: 10.1140/epja/i2003-10088-0
2003UE05 Acta Phys.Hung.N.S. 18, 289 (2003) Angular Correlations in 28Si + 28Si Resonances NUCLEAR REACTIONS 28Si(28Si, 28Si), (28Si, 28Si'), E(cm)=55.8 MeV; analyzed σ(E, θ), (particle)γ-coin, angular correlations; deduced triaxial deformation, molecular resonance spin alignment features.
doi: 10.1556/APH.18.2003.2-4.29
2002AB06 Eur.Phys.J. A 13, 143 (2002) Reaction Dynamics of Synthesis of Superheavy Elements
doi: 10.1007/s10050-002-8733-1
2002AB28 Prog.Theor.Phys.(Kyoto), Suppl. 146, 104 (2002) Y.Abe, D.Boilley, G.Kosenko, J.D.Bao, C.W.Shen, B.Giraud, T.Wada Fusion Dynamics of Massive Heavy-Ion Systems NUCLEAR REACTIONS 244Pu(48Ca, X), E ≈ threshold; calculated fusion probability, related features. Two-step model.
doi: 10.1143/PTPS.146.104
2002KO71 J.Nucl.Radiochem.Sci. 3, No 1, 19 (2002) A Dynamical Approach to Heavy-ion Fusion: 48Ca + 244Pu NUCLEAR REACTIONS 244Pu(48Ca, X), (48Ca, 2n), (48Ca, 3n), (48Ca, 4n), (48Ca, 5n), E* ≈ 30-70 MeV; calculated fusion, evaporation residue σ.
2002SH38 Phys.Rev. C 66, 061602 (2002) Two-step model of fusion for the synthesis of superheavy elements NUCLEAR REACTIONS 238U, 244Pu, 248Cm, 252Cf(48Ca, X), E(cm) ≈ 190-250 MeV; calculated fusion σ. 244Pu, 248Cm, 252Cf(48Ca, 3n), (48Ca, 4n), E* ≈ 30 MeV; calculated residue production σ. Two-step model, comparison with data.
doi: 10.1103/PhysRevC.66.061602
2001AB13 Nucl.Instrum.Methods Phys.Res. A459, 256 (2001) Ultracold and Cold Neutron Cross-Sections of Liquid Helium at Low Temperatures Down to 0.1 K NUCLEAR REACTIONS 4He(n, n'), E=low; calculated σ(E, θ). Ultracold neutrons.
doi: 10.1016/S0168-9002(00)01009-3
2001AY02 Phys.Rev. C64, 024609 (2001) Stochastic One-Body Transport and Coupling to Mean-Field Fluctuations
doi: 10.1103/PhysRevC.64.024609
1999AR04 Phys.Rev. C59, 796 (1999) Y.Aritomo, T.Wada, M.Ohta, Y.Abe Fluctuation-Dissipation Model for Synthesis of Superheavy Elements NUCLEAR STRUCTURE 268No, 276Rf, 282Sg, 286Hs, 292Ds, 294Cn, 298Fl, 302Lv; calculated fission potential energy curves, evaporation residue cross sections vs excitation energy, fission barrier height. Fluctuation-dissipation model.
doi: 10.1103/PhysRevC.59.796
1999NO06 Phys.Rev. C60, 041303 (1999) R.Nouicer, C.Beck, R.M.Freeman, F.Haas, N.Aissaoui, T.Bellot, G.de France, D.Disdier, G.Duchene, A.Elanique, A.Hachem, F.Hoellinger, D.Mahboub, V.Rauch, S.J.Sanders, A.Dummer, F.W.Prosser, A.Szanto de Toledo, Sl.Cavallaro, E.Uegaki, Y.Abe Vanishing Spin Alignment: Experimental indication of a triaxial 28Si + 28Si Nuclear Molecule NUCLEAR REACTIONS 28Si(28Si, 28Si), (28Si, 28Si'), E=111.6 MeV; measured (fragment)γ-, (fragment)(fragment)-coin, σ(E, θ); deduced fragment spin correlations, molecular configuration.
doi: 10.1103/PhysRevC.60.041303
1999OH10 Acta Phys.Hung.N.S. 10, 253 (1999) M.Ohta, K.Okazaki, T.Wada, Y.Aritomo, Y.Abe Favorable Combination for the Synthesis of Superheavy Elements NUCLEAR REACTIONS 223At(75Cu, X), 231Ra(67Fe, X), 238Pa(60V, X), 246Pu(52Ca, X), 253Bk(45Cl, X), 217At(73Cu, X), 224Ra(66Fe, X), 232Pa(58V, X), 239Pu(51Ca, X), 247Bk(43Cl, X), E*=25-50 MeV; calculated compound nucleus formation probability, evaporation residue σ.
1999WA28 Nucl.Phys. (Supplement) A654, 888c (1999) T.Wada, Y.Aritomo, T.Tokuda, K.Okazaki, M.Ohta, Y.Abe Multi-Dimensional Fluctuation-Dissipation Dynamics of the Synthesis of Superheavy Elements NUCLEAR REACTIONS 149La(149La, X), E*=10-50 MeV; calculated evaporation residue excitation function. Fluctuation-dissipation dynamics, mass asymmetric channels also discussed.
doi: 10.1016/S0375-9474(00)88566-8
1998YU03 Phys.Lett. 420B, 25 (1998) K.Yuasa-Nakagawa, T.Nakagawa, K.Furutaka, K.Matsuda, Y.Futami, K.Yoshida, J.Kasagi, S.M.Lee, T.Suomijarvi, W.Q.Shen, T.Wada, S.Yamaji, Y.Abe Angular Momentum Dependence of the Prescission Time of Medium Mass Hot Nuclei NUCLEAR REACTIONS 56Fe(58Ni, X), E=10 MeV/nucleon; measured Ep, Eα, multiplicity distributions; deduced angular momentum dependence of prescission time.
doi: 10.1016/S0370-2693(97)01522-0
1997AB33 Phys.Rev. C56, 2557 (1997) Y.Abe, B.G.Giraud, Y.Hahn, H.Inamori, J.LeTourneux Adiabatic Models of the Efimov Effect
doi: 10.1103/PhysRevC.56.2557
1997AB38 J.Phys.(London) G23, 1275 (1997) Y.Abe, Y.Aritomo, T.Wada, M.Ohta A New Mechanism for Synthesis of Superheavy Elements NUCLEAR STRUCTURE 298Fl; calculated potential vs collective degree of freedom, time, shell-correction energy vs temperature, other superheavy residue production related features.
doi: 10.1088/0954-3899/23/10/015
1997AR06 Phys.Rev. C55, R1011 (1997) Y.Aritomo, T.Wada, M.Ohta, Y.Abe Diffusion Mechanism for Synthesis of Superheavy Elements NUCLEAR REACTIONS 149La(149La, X), E not given; calculated evaporation residue σ vs excitation. Smoluchowski equation, finite-range droplet model potential; temperature dependent shell correction energy, superheavy elements.
doi: 10.1103/PhysRevC.55.R1011
1997KA16 Phys.Rev. C55, 1928 (1997) Resonance States in the 12C - 12C Morse Potential NUCLEAR REACTIONS 12C(12C, X), E not given; analyzed resonance staates, explanation associated Morse potential; deduced potential inadequency to provide comprehensive explanation.
doi: 10.1103/PhysRevC.55.1928
1997WA08 Nucl.Phys. A616, 446c (1997) T.Wada, Y.Aritomo, T.Tokuda, M.Ohta, Y.Abe Dynamics of the Superheavy Element Synthesis with a Diffusion Model NUCLEAR REACTIONS 145La(145La, X), 147La(147La, X), 148La(148La, X), 149La(149La, X), E not given; calculated evaporation residue σ vs initial excitation energy for 290114, 294114, 296114, 298114 compound nuclei, formation, survival probabilities; deduced isotope dependence, superheavy element synthesis dynamics related features. Diffusion model.
doi: 10.1016/S0375-9474(97)00116-4
1996AB40 Phys.Rep. 275, 49 (1996) Y.Abe, S.Ayik, P.-G.Reinhard, E.Suraud On Stochastic Approaches of Nuclear Dynamics
doi: 10.1016/0370-1573(96)00003-8
1995BE07 Nucl.Phys. A583, 269c (1995) C.Beck, Y.Abe, N.Aissaoui, B.Djerroud, F.Haas Dynamics of the Di-Nucleus Binary Decay: Role of the number of open channels NUCLEAR REACTIONS, ICPND 12C(35Cl, X), E(cm) ≈ 150-300 MeV; calculated fusion-fission σ(E). 12C(12C, X), 16O(16O, X), 20Ne(20Ne, X), 32S(32S, X), 28Si(28Si, X), 24Mg(24Mg, X), 30Si(30Si, X), 32S(32S, X), E not given; calculated open channel number vs L(grazing); deduced di-nucleus binary decay features. Statistical model.
doi: 10.1016/0375-9474(94)00671-9
1995HI21 Phys.Rev.Lett. 74, 4141 (1995) Y.Hirabayashi, Y.Sakuragi, Y.Abe 3α + 3α and 3α + 12C Configurations in 24Mg NUCLEAR REACTIONS 12C(12C, 12C'), E(cm)=29.5-33 MeV; analyzed σ(θ). 24Mg deduced resonance three α-particle character. Band crossing model.
doi: 10.1103/PhysRevLett.74.4141
1995TA03 Nucl.Phys. A583, 291c (1995) Potential Resonance Affected by Non-Adibatic Transition in Nuclear Heavy-Ion Collisions
doi: 10.1016/0375-9474(94)00675-D
1994BE08 Phys.Rev. C49, 2618 (1994) C.Beck, Y.Abe, N.Aissaoui, B.Djerroud, F.Haas Role of the Number of Open Channels in the Dynamics of the Dincleus Binary Decay NUCLEAR REACTIONS 12C(12C, X), 14C, 15N, 16O(16O, X), 20Ne(20Ne, X), 24Mg(24Mg, X), 28Si(28Si, X), 30Si(30Si, X), 32S(32S, X), 31P, 40Ar, 40Ca, 32S(16O, X), 19F, 24Mg, 28Si, 35Cl, 40,36Ar, 40Ca(12C, X), 18O, 10B(10B, X), 23Na, 24Mg(24Mg, X), 28Si(14N, X), 27Al(20Ne, X), E not given; calculated open channels number vs grazing angular momenta; deduced fusion-fission mechanism, dinucleus binary decay dynamics.
doi: 10.1103/PhysRevC.49.2618
1994BO37 Z.Phys. A349, 119 (1994) D.Boilley, Y.Abe, S.Ayik, E.Suraud A Bohr-Mottelson Model of Nuclei at Finite Temperature
doi: 10.1007/BF01291169
1994UE03 Phys.Lett. 340B, 143 (1994) Di-Nuclear Molecular States in Oblate-Oblate System NUCLEAR REACTIONS 28Si(28Si, X), E not given; calculated effective potential energy, dinuclear spectrum. Molecular model.
doi: 10.1016/0370-2693(94)01308-X
1993BO19 Nucl.Phys. A556, 67 (1993) D.Boilley, E.Suraud, Y.Abe, S.Ayik Nuclear Fission with a Langevin Equation NUCLEAR REACTIONS 205At, 248Cf(n, F), E=thermal; calculated fission rate vs temperature, time. Langevin equation.
doi: 10.1016/0375-9474(93)90238-S
1993WA10 Phys.Rev.Lett. 70, 3538 (1993) One-Body Dissipation in Agreement with Prescission Neutrons and Fragment Kinetic Energies NUCLEAR REACTIONS 181Ta(19F, F), 184W(16O, X), E not given; calculated fission width, emitted neutron, proton, α-particle numbers, time dependence, fusion-fission σ(E). 200Pb deduced fission dynamics. Two-dimensional Langevin equation.
doi: 10.1103/PhysRevLett.70.3538
1992BE34 Z.Phys. A343, 309 (1992) C.Beck, B.Djerroud, F.Hass, R.M.Freeman, A.Hachem, B.Heusch, A.Morsad, M.Youlal, Y.Abe, R.Dayras, J.P.Wieleczko, T.Matsuse, S.M.Lee Competition between the Fusion-Fission and Deep-Inelastic Orbiting Mechanisms in the 35Cl + 12C Reaction NUCLEAR REACTIONS 12C(35Cl, X), E=180, 200 MeV; measured evaporation residue σ(θ), fission like yields charge distributions, σ(θ), fragment spectra, (fragment)(fragment)-coin damped yields σ(E) for X=B-Mg; deduced fusion-fission rather than orbiting process evidence.
doi: 10.1007/BF01291530
1991TA11 Prog.Theor.Phys.(Kyoto) 85, 567 (1991) Quantum-Mechanical Study of the Landau-Zener Resonances in Nuclear Heavy-Ion Collisions NUCLEAR REACTIONS, ICPND 17O(12C, 12C'), E(cm)=10-20 MeV; calculated σ(E). 57Ni(40Ca, X), E(cm)=70-80 MeV; calculated transition probabilities vs E. Two-state Landau-Zener model.
doi: 10.1143/ptp/85.3.567
1990TA01 Phys.Rev. C41, R17 (1990) Resonances Due to the Landau-Zener Transition NUCLEAR REACTIONS 17O(12C, 12C'), E(cm)=10-20 MeV; calculated σ(E). T-matrix, analytic treatment, Landau-Zener transition role.
doi: 10.1103/PhysRevC.41.R17
1989UE02 Phys.Lett. 231B, 28 (1989) On Resonances of the 24Mg + 24Mg System NUCLEAR REACTIONS 24Mg(24Mg, X), E not given; calculated di-nuclear potential energy surfaces. Molecular model. NUCLEAR STRUCTURE 48Cr; calculated di-nuclear potential energy surfaces. Molecular model, 24Mg clusters.
doi: 10.1016/0370-2693(89)90107-X
1986DE09 Z.Phys. A323, 437 (1986) H.Delagrange, C.Gregoire, F.Scheuter, Y.Abe Dynamical Decay of Nuclei at High Temperature: Competition between particle emission and fission decay NUCLEAR STRUCTURE 194Hg, 170Yb; calculated fission width vs neutron multiplicity, p, n, α-multiplicity vs temperature following decay. 248Cf; calculated fission width vs neutron multiplicity.
1985KA28 Prog.Theor.Phys.(Kyoto) 74, 1053 (1985) Structure of 12C + 16O Molecular Bands NUCLEAR STRUCTURE 28Si; calculated cluster levels, B(λ). Semi-microscopic cluster model. NUCLEAR REACTIONS 16O(12C, 12C), E(cm) ≈ 10-25 MeV; calculated phase shifts. 28Si deduced molecular resonances, parameters. Semi-microscopic cluster model.
doi: 10.1143/PTP.74.1053
1984OH02 Phys.Rev. C29, 1948 (1984) M.Ohta, K.Hatogai, S.Okai, Y.Abe Limitation on Heavy Ion Fusion and Nuclear Level Density at High Excitation Energies NUCLEAR STRUCTURE 56Fe, 46Ti; calculated state, level density vs excitation. Partition function method, shell model saddle point equation solution. NUCLEAR REACTIONS, ICPND 26Mg(20Ne, X), E(cm) ≈ 30-100 MeV; calculated fusion σ(E), critical angular momentum, temperature. Compound nuclear level density, finite single particle space.
doi: 10.1103/PhysRevC.29.1948
1984OK05 Phys.Lett. 106A, 435 (1984) 93Nb and 35Cl Nuclear Quadrupole Resonance in the Low Temperature Modification of Niobium Pentachloride NUCLEAR MOMENTS 93Nb, 35Cl; measured NQR vs temperature. 93Nb deduced nuclear coupling constants. Niobium pentachloride sample.
doi: 10.1016/0375-9601(84)90988-5
1983AB08 Phys.Rev. C28, 2316 (1983) Evidence for Nuclear Landau-Zener Effect: New resonance mechanism in heavy-ion reactions NUCLEAR REACTIONS 13C(17O, 17O'), E(cm)=15-25 MeV; analyzed γ-yield vs E; deduced nuclear Landau-Zener effect. Molecular single particle effects.
doi: 10.1103/PhysRevC.28.2316
1983TA07 Phys.Lett. 125B, 30 (1983) Molecular Resonances and Spin Alignment in 12C + 16O Inelastic Scattering NUCLEAR REACTIONS, ICPND 12C(16O, 16O'), E(cm)=19-23 MeV; calculated σ(E), projectile level spin alignment. Coupled-channels approach, band crossing model, molecular viewpoint.
doi: 10.1016/0370-2693(83)91228-5
1982KA35 Prog.Theor.Phys.(Kyoto) 68, 1794 (1982) A Justification of the Band Crossing Model NUCLEAR REACTIONS 16O(12C, 12C), (12C, X), E not given; calculated molecular resonance elastic, aligned subchannel decay probabilities.
doi: 10.1143/PTP.68.1794
1981HA18 Phys.Rev.Lett. 46, 1667 (1981) Surface Transparency and Resonant Behavior in Some Lighter-Heavy-Ion Reactions NUCLEAR REACTIONS 12C(12C, X), E(cm)=15-45 MeV; 12C(14C, X), E(cm)=18-26 MeV; 12C(16O, X), E(cm)=17-18 MeV; 12C(18O, X), E(cm)=10-23.6 MeV; 16O(16O, X), E(cm)=12-40 MeV; 14C(16O, X), E(cm)=16-34 MeV; calculated integrated γ-yield vs grazing angular momentum, available open channel number; deduced surface transparency. Semiclassical method.
doi: 10.1103/PhysRevLett.46.1667
1980KO21 Prog.Theor.Phys.(Kyoto) 63, 722 (1980) Evidence for Molecular Resonances in the 16O+16O System NUCLEAR REACTIONS 16O(16O, 16O), (16O, X), E=15-35 MeV; 16O(16O, 16O'), E=12-40 MeV; calculated σ(E), fusion σ(E); deduced molecular resonances. Band crossing model.
doi: 10.1143/PTP.63.722
1980KO24 Phys.Rev. C22, 1068 (1980) Application of a Band-Crossing Model for Resonances in 16O+16O Scattering NUCLEAR REACTIONS 16O(16O, 16O), (16O, 16O'), E(cm)=10-41 MeV; calculated σ(E), fusion σ(E). Resonance mechanism, band crossing model.
doi: 10.1103/PhysRevC.22.1068
1979AB02 Phys.Rev. C19, 1365 (1979) Intermediate Structure in 12C + 12C Elastic Scattering NUCLEAR REACTIONS 12C(12C, 12C), E(cm)=6-30 MeV; calculated σ(E); deduced resonance mechanism for HI reactions, band crossing, model with smooth cutoff of absorption effect.
doi: 10.1103/PhysRevC.19.1365
1979KO11 Phys.Rev. C19, 1356 (1979) Application of a Band Crossing Model for Resonances in High Energy 12C-12C Scattering NUCLEAR REACTIONS 12C(12C, 12C), 12C(12C, 12C'), E(cm)=10-40 MeV; calculated σ(E); deduced resonance mechanism for HI reactions populating 2+, 3- excited states of 12C. Band crossing model.
doi: 10.1103/PhysRevC.19.1356
1979OK02 Prog.Theor.Phys. 61, 1049 (1979) The Structure of 9Be by a Molecular Model. II NUCLEAR STRUCTURE 9Be; calculated energy levels, charge form factors, rms radii, quadrupole moment of the ground state. Generator coordinator method, effective nucleon-nucleon force from α+n, α+α systems.
doi: 10.1143/PTP.61.1049
1979UE03 Prog.Theor.Phys.(Kyoto) 62, 1621 (1979) E.Uegaki, Y.Abe, S.Okabe, H.Tanaka Structure of the Excited States in 12C. II NUCLEAR STRUCTURE 12C; calculated Γα, charge form factors, B(E2), rms charge radii. Generator coordinate calculation, microscopic α-particle model.
doi: 10.1143/PTP.62.1621
1978KO14 Prog.Theor.Phys. 59, 465 (1978) A Study of Resonances in the Sub-Coulomb 12C-12C Reaction from the Viewpoint of Nuclear Molecule NUCLEAR REACTIONS 12C(12C, X); analyzed sub-Coulomb resonances.
doi: 10.1143/PTP.59.465
1978MA28 Prog.Theor.Phys. 59, 1037 (1978) Molecular Resonances in 12C(16O, 16O)12C* (2+, 4.44 MeV) Inelastic Scattering by a Band Crossing Model NUCLEAR REACTIONS 12C(16O, 16O); calculated σ, molecular resonances.
doi: 10.1143/PTP.59.1037
1978MA50 Prog.Theor.Phys. 59, 1904 (1978) A Band Crossing Model of Resonances in Heavy Ion Reactions. I. Resonances in 12C-16O Scattering NUCLEAR REACTIONS 12C(16O, 16O), (16O, 16O'), E(cm)=15-30 MeV; calculated σ(E, θ). Band crossing model of resonances, coupled-channels calculation, inelastic excitation of 12C, 16O.
doi: 10.1143/PTP.59.1904
1978OK01 Progr.Theor.Phys. 59, 315 (1978) Particle Decay Widths and Charge Form Factors of 9Be by the Molecular Model NUCLEAR STRUCTURE 9Be; calculated Γα, Γn, charge form factors. Molecular model calculations.
doi: 10.1143/PTP.59.315
1978UE02 Prog.Theor.Phys. 59, 1031 (1978) E.Uegaki, Y.Abe, S.Okabe, H.Tanaka On the Positive-Parity States with Anomalous α-Decay Properties in 12C NUCLEAR STRUCTURE 12C; calculated Γα.
doi: 10.1143/PTP.59.1031
1977OK01 Progr.Theor.Phys. 57, 866 (1977) The Structure of 9Be Nucleus by a Molecular Model. I NUCLEAR STRUCTURE 9Be; calculated levels, level properties. Molecular model.
doi: 10.1143/PTP.57.866
1977UE01 Progr.Theor.Phys. 57, 1262 (1977) E.Uegaki, S.Okabe, Y.Abe, H.Tanaka Structure of the Excited States in 12C. I NUCLEAR STRUCTURE 12C; calculated levels, level properties. Microscopic 3α-model.
doi: 10.1143/PTP.57.1262
1976NO10 Progr.Theor.Phys. 55, 1432 (1976) H.Noto, Y.Abe, J.Hiura, H.Tanaka An Octupole Deformation in 20Ne NUCLEAR STRUCTURE 20Ne; calculated octupole deformation, B(E3).
doi: 10.1143/PTP.55.1432
1974NO14 Progr.Theor.Phys. 52, 339 (1974) H.Noto, Y.Abe, J.Hiura, H.Tanaka An Octupole Deformation in 20Ne NUCLEAR STRUCTURE 20Ne; calculated levels.
doi: 10.1143/PTP.52.339
1972AB19 Progr.Theor.Phys.Suppl. 52, 228 (1972) Alpha-Like Four-Body Correlations and Molecular Aspects in Nuclei. Chapter V. Stability and Persistency of Alpha-Cluster Structures NUCLEAR STRUCTURE 9,8Be, 12C; calculated α-cluster structures.
doi: 10.1143/PTPS.52.228
1971AB07 Progr.Theor.Phys. 46, 352 (1971) On the Stability of α-Cluster Structures in 8Be and 12C Nuclei NUCLEAR STRUCTURE 8Be, 12C; calculated binding energy, density distribution. α-cluster model.
doi: 10.1143/PTP.46.352
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