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NSR database version of May 10, 2024.

Search: Author = Y.Abe

Found 100 matches.

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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
Citations: PlumX Metrics


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
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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
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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
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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
Citations: PlumX Metrics


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
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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
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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2669.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2531.


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
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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
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Data from this article have been entered in the XUNDL database. For more information, click here.


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
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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
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Data from this article have been entered in the XUNDL database. For more information, click here.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2474. Data from this article have been entered in the XUNDL database. For more information, click here.


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
Citations: PlumX Metrics


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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2437. Data from this article have been entered in the XUNDL database. For more information, click here.


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2040. Data from this article have been entered in the XUNDL database. For more information, click here.


2012UE02      Prog.Theor.Phys.(Kyoto) 127, 831 (2012)

E.Uegaki, Y.Abe

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
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2012UE03      Prog.Theor.Phys.(Kyoto) 127, 877 (2012)

E.Uegaki, Y.Abe

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
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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
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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
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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
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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
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2010UE02      Nucl.Phys. A834, 796c (2010)

E.Uegaki, Y.Abe

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
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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
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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
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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
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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
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2008UE02      Int.J.Mod.Phys. E17, 2034 (2008)

E.Uegaki, Y.Abe

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
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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
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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
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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
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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
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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
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2004BO11      Comput.Phys.Commun. 159, 1 (2004)

B.Bouriquet, Y.Abe, D.Boilley

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
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2004BO31      Prog.Theor.Phys.(Kyoto), Suppl. 154, 425 (2004)

B.Bouriquet, G.Kosenko, Y.Abe

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
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2004BO40      Eur.Phys.J. A 22, 9 (2004)

B.Bouriquet, Y.Abe, G.Kosenko

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
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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
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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
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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)

Y.Abe, B.Bouriquet

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)

D.Boilley, Y.Abe, J.-D.Bao

Inverse Kramers formula and fusion dynamics of heavy ions

doi: 10.1140/epja/i2003-10088-0
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2003UE05      Acta Phys.Hung.N.S. 18, 289 (2003)

E.Uegaki, Y.Abe

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
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2002AB06      Eur.Phys.J. A 13, 143 (2002)

Y.Abe

Reaction Dynamics of Synthesis of Superheavy Elements

doi: 10.1007/s10050-002-8733-1
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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
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2002KO71      J.Nucl.Radiochem.Sci. 3, No 1, 19 (2002)

G.I.Kosenko, C.Shen, Y.Abe

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)

C.Shen, G.Kosenko, Y.Abe

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
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2001AB13      Nucl.Instrum.Methods Phys.Res. A459, 256 (2001)

Y.Abe, N.Morishima

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
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2001AY02      Phys.Rev. C64, 024609 (2001)

S.Ayik, Y.Abe

Stochastic One-Body Transport and Coupling to Mean-Field Fluctuations

doi: 10.1103/PhysRevC.64.024609
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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
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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
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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
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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
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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
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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
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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
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1997KA16      Phys.Rev. C55, 1928 (1997)

K.Kato, Y.Abe

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
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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
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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
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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
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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
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1995TA03      Nucl.Phys. A583, 291c (1995)

T.Tazawa, N.Takigawa, Y.Abe

Potential Resonance Affected by Non-Adibatic Transition in Nuclear Heavy-Ion Collisions

doi: 10.1016/0375-9474(94)00675-D
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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
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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
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1994UE03      Phys.Lett. 340B, 143 (1994)

E.Uegaki, Y.Abe

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
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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
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1993WA10      Phys.Rev.Lett. 70, 3538 (1993)

T.Wada, Y.Abe, N.Carjan

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
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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
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1991TA11      Prog.Theor.Phys.(Kyoto) 85, 567 (1991)

T.Tazawa, Y.Abe

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
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1990TA01      Phys.Rev. C41, R17 (1990)

T.Tazawa, Y.Abe

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
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1989UE02      Phys.Lett. 231B, 28 (1989)

E.Uegaki, Y.Abe

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
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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)

K.Kato, S.Okabe, Y.Abe

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
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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
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1984OK05      Phys.Lett. 106A, 435 (1984)

N.Okubo, Y.Abe

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
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1983AB08      Phys.Rev. C28, 2316 (1983)

Y.Abe, J.Y.Park

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
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1983TA07      Phys.Lett. 125B, 30 (1983)

T.Tazawa, J.Y.Park, Y.Abe

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
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1982KA35      Prog.Theor.Phys.(Kyoto) 68, 1794 (1982)

K.Kato, S.Okabe, Y.Abe

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
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1981HA18      Phys.Rev.Lett. 46, 1667 (1981)

F.Haas, Y.Abe

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
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1980KO21      Prog.Theor.Phys.(Kyoto) 63, 722 (1980)

Y.Kondo, D.A.Bromley, Y.Abe

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
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1980KO24      Phys.Rev. C22, 1068 (1980)

Y.Kondo, D.A.Bromley, Y.Abe

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
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1979AB02      Phys.Rev. C19, 1365 (1979)

Y.Abe, T.Matsuse, Y.Kondo

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
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1979KO11      Phys.Rev. C19, 1356 (1979)

Y.Kondo, Y.Abe, T.Matsuse

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
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1979OK02      Prog.Theor.Phys. 61, 1049 (1979)

S.Okabe, Y.Abe

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
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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
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1978KO14      Prog.Theor.Phys. 59, 465 (1978)

Y.Kondo, T.Matsuse, Y.Abe

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
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1978MA28      Prog.Theor.Phys. 59, 1037 (1978)

T.Matsuse, Y.Abe, Y.Kondo

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
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1978MA50      Prog.Theor.Phys. 59, 1904 (1978)

T.Matsuse, Y.Abe, Y.Kondo

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
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1978OK01      Progr.Theor.Phys. 59, 315 (1978)

S.Okabe, Y.Abe

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
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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
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1977OK01      Progr.Theor.Phys. 57, 866 (1977)

S.Okabe, Y.Abe, H.Tanaka

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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1972AB19      Progr.Theor.Phys.Suppl. 52, 228 (1972)

Y.Abe, N.Takigawa

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
Citations: PlumX Metrics


1971AB07      Progr.Theor.Phys. 46, 352 (1971)

Y.Abe, J.Hiura, H.Tanaka

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
Citations: PlumX Metrics


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