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NSR database version of April 11, 2024.

Search: Author = T.Ohsawa

Found 45 matches.

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2016CA03      Nucl.Data Sheets 131, 1 (2016)

R.Capote, Y.-J.Chen, F.-J.Hambsch, N.V.Kornilov, J.P.Lestone, O.Litaize, B.Morillon, D.Neudecker, S.Oberstedt, T.Ohsawa, N.Otuka, V.G.Pronyaev, A.Saxena, O.Serot, O.A.Shcherbakov, N.-C.Shu, D.L.Smith, P.Talou, A.Trkov, A.C.Tudora, R.Vogt, A.S.Vorobyev

Prompt Fission Neutron Spectra of Actinides

NUCLEAR REACTIONS ²³²Th, ^{233,234,235,238}U, ²³⁷Np, ²³⁹Pu(n, F), E<30 MeV; calculated prompt fission En, In; Comparison with available data.

doi: 10.1016/j.nds.2015.12.002
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset33084.

2011OH03      J.Korean Phys.Soc. 59, 887s (2011)

T.Ohsawa, A.Matsumoto

Multimodal Analysis of Prompt and Delayed Neutron Emission in Fission

NUCLEAR REACTIONS ²³⁵U(n, f), E=low; calculated prompt dσ(En), scission dσ(En), σ(En, θ), delayed neutron yield. Comparison to data, ENDF/B-VII, JEF-2.2, JENDL-3.2, JENDL-3.3.

doi: 10.3938/jkps.59.887
Citations: PlumX Metrics

2011SH01      J.Nucl.Sci.Technol.(Tokyo) 48, 1 (2011)

K.Shibata, O.Iwamoto, T.Nakagawa, N.Iwamoto, A.Ichihara, s.Kunieda, S.Chiba, K.Furutaka, N.Otuka, T.Ohsawa, T.Murata, H.Matsunobu, A.Zukeran, S.Kamada, J.-i.Katakura

JENDL-4.0: A New Library for Nuclear Science and Engineering

doi: 10.3327/jnst.48.1
Citations: PlumX Metrics

2009IW02      J.Nucl.Sci.Technol.(Tokyo) 46, 510 (2009)

O.Iwamoto, T.Nakagawa, N.Otuka, S.Chiba, K.Okumura, G.Chiba, T.Ohsawa, K.Furutaka

JENDL Actinoid File 2008

doi: 10.3327/jnst.46.510
Citations: PlumX Metrics

2006NI09      Phys.Atomic Nuclei 69, 1399 (2006)

K.Nishio, H.Ikezoe, M.Asai, K.Tsukada, S.Mitsuoka, K.Tsuruta, K.Satou, C.J.Lin, T.Ohsawa

Evidence of Complete Fusion in the Subbarrier ¹⁶O + ²³⁸U Reaction

NUCLEAR REACTIONS ²³⁸U(¹⁶O, 4n), (¹⁶O, 5n), (¹⁶O, 6n), E(cm)=70-95 MeV; measured evaporation residue σ; deduced reaction mechanism features. Comparison with statistical model predictions.

RADIOACTIVITY ^248,249,250Fm(α) [from ²³⁸U(¹⁶O, xn)]; measured Eα, T_1/2.

doi: 10.1134/S1063778806080187
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1916.

2004NI10      Phys.Rev.Lett. 93, 162701 (2004)

K.Nishio, H.Ikezoe, Y.Nagame, M.Asai, K.Tsukada, S.Mitsuoka, K.Tsuruta, K.Satou, C.J.Lin, T.Ohsawa

Evidence of Complete Fusion in the Sub-Barrier ¹⁶O + ²³⁸U Reaction

NUCLEAR REACTIONS ²³⁸U(¹⁶O, 4n), (¹⁶O, 5n), (¹⁶O, 6n), E(cm) ≈ 70-105 MeV; measured evaporation residue σ; deduced complete fusion at sub-barrier energies, role of orientation and deformation. Comparison with statistical model predictions.

doi: 10.1103/PhysRevLett.93.162701
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1916.

2004OH08      Nucl.Sci.Eng. 148, 50 (2004)

T.Ohsawa, F.-J.Hambsch

An Interpretation of Energy Dependence of Delayed Neutron Yields in the Resonance Region for ²³⁵U and ²³⁹Pu

NUCLEAR REACTIONS ²³⁵U, ²³⁹Pu(n, F), E < 100 eV; analyzed fission fragment mass distributions; deduced delayed neutron yields, resonance effects.

doi: 10.13182/NSE04-A2440
Citations: PlumX Metrics

2003NI01      Phys.Rev. C 67, 014604 (2003)

K.Nishio, H.Ikezoe, Y.Nagame, S.Mitsuoka, I.Nishinaka, L.Duan, K.Satou, S.Goto, M.Asai, H.Haba, K.Tsukada, N.Shinohara, S.Ichikawa, T.Ohsawa

Fragment mass distribution of the ²³⁹Pu(d, pf) reaction via the superdeformed β-vibrational resonance

NUCLEAR REACTIONS ²³⁹Pu(d, pF), E=13.5 MeV; measured Ep, (fragment)p-coin, fission fragment mass yields; deduced mass distribution for fission from superdeformed resonance. ²⁴⁰Pu deduced fission mechanism features.

doi: 10.1103/PhysRevC.67.014604
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1813.

2002OH05      Prog.Nucl.Energy 41, 109 (2002)

T.Ohsawa, T.Oyama

Possible Fluctuations in the Delayed Neutron Yields in the Resonance Region of U-235

NUCLEAR REACTIONS ²³⁵U(n, F), E ≈ 0-14 MeV; analyzed delayed neutron yields, resonance effects. Multimodal interpretation.

2002OH07      J.Nucl.Radiochem.Sci. 3, No 1, 93 (2002)

T.Ohsawa

Evaluation of Prompt Neutron Spectra from Fission of Americium Isotopes

NUCLEAR REACTIONS ^241,242m,243Am(n, F), E=thermal-5 MeV; calculated prompt neutron spectra. Comparison with data.

2002SH40      J.Nucl.Sci.Technol.(Tokyo) 39, 1125 (2002)

K.Shibata, T.Kawano, T.Nakagawa, O.Iwamoto, J.Katakura, T.Fukahori, S.Chiba, A.Hasegawa, T.Murata, H.Matsunobu, T.Ohsawa, Y.Nakajima, T.Yoshida, A.Zukeran, M.Kawai, M.Baba, M.Ishikawa, T.Asami, T.Watanabe, Y.Watanabe, M.Igashira, N.Yamamuro, H.Kitazawa, N.Yamano, H.Takano

Japanese Evaluated Nuclear Data Library Version 3 Revision-3: JENDL-3.3

doi: 10.1080/18811248.2002.9715303
Citations: PlumX Metrics

2001KA07      Phys.Rev. C63, 034601 (2001)

T.Kawano, T.Ohsawa, M.Baba, T.Nakagawa

Effect of the Preequilibrium Process Upon Fast Neutron Fission Spectra from ²³⁸U

NUCLEAR REACTIONS ²³⁸U(n, F), E=14, 18 MeV; calculated neutron spectra, angular distributions; deduced role of preequilibrium processes. Comparisons with data.

doi: 10.1103/PhysRevC.63.034601
Citations: PlumX Metrics

2000KA20      J.Nucl.Sci.Technol.(Tokyo) 37, 327 (2000)

T.Kawano, H.Matsunobu, T.Murata, A.Zukeran, Y.Nakajima, M.Kawai, O.Iwamoto, K.Shibata, T.Nakagawa, T.Ohsawa, M.Baba, T.Yoshida

Simultaneous Evaluation of Fission Cross Sections of Uranium and Plutonium Isotopes for JENDL-3.3

NUCLEAR REACTIONS ^233,235,238U, ^239,240,241Pu(n, F), E < 20 MeV; analyzed fission σ. Simultaneous evaluation.

doi: 10.1080/18811248.2000.9714902
Citations: PlumX Metrics

2000OH02      Nucl.Phys. A665, 3 (2000)

T.Ohsawa, T.Horiguchi, M.Mitsuhashi

Multimodal Analysis of Prompt Neutron Spectra for ²³⁸Pu(sf), ²⁴⁰Pu(sf), ²⁴²Pu(sf) and ²³⁹Pu(n_th, f)

RADIOACTIVITY ^238,240,242Pu(SF); calculated prompt neutron spectra. Multimodal fission model, comparison with data.

NUCLEAR REACTIONS ²³⁹Pu(n, F), E=thermal; calculated prompt neutron spectra. Multimodal fission model, comparison with data.

doi: 10.1016/S0375-9474(99)00686-7
Citations: PlumX Metrics

1999OH06      Nucl.Phys. A653, 17 (1999)

T.Ohsawa, T.Horiguchi, H.Hayashi

Multimodal Analysis of Prompt Neutron Spectra for ²³⁷Np(n, f)

NUCLEAR REACTIONS ²³⁷Np(n, F), E=0.3-5.5 MeV; calculated prompt neutron spectra. Multimodal fission model, comparisons with data.

doi: 10.1016/S0375-9474(99)00156-6
Citations: PlumX Metrics

1989FU12      Few-Body Systems 7, 119 (1989)

K.Fukunaga, S.Kakigi, T.Ohsawa, A.Okihana, T.Sekioka, H.Nakamura-Yokota, T.Murayama, T.Hayashi

Break-Up of Deuteron by Vector-Polarized Deuterons at 60 MeV

NUCLEAR REACTIONS ²H(polarized d, pd), E=60 MeV; measured σ(θp, θd, Ep), analyzing power vs Ep. Vector polarized beam. Three-body scattering theory.

doi: 10.1007/BF01087391
Citations: PlumX Metrics

1989KO24      Nucl.Instrum.Methods Phys.Res. A278, 737 (1989)

N.Koori, M.Hyakutake, M.Matoba, H.Ijiri, Y.Fujita, Y.Uozumi, S.Shirato, T.Motobayashi, T.Ohsawa, K.Sagara

High Resolution Measurement of Protons Emitted from Medium-Energy Neutron Induced Reactions by Means of a Magnetic Spectrograph

NUCLEAR REACTIONS ²H(n, p), E=63 MeV; measured proton spectra; deduced finite geometry role. Magnetic spectrograph, high resolution.

doi: 10.1016/0168-9002(89)91197-2
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22165.

1989WA26      Nucl.Phys. A503, 161 (1989)

R.E.Warner, A.Okihana, M.Fujiwara, N.Matsuoka, K.Tamura, M.Tosaki, T.Ohsawa, K.Fukunaga, S.Kakigi, J.Kasagi, N.Koori

Joint Momentum Distribution of p + n in ⁶Li

NUCLEAR REACTIONS ⁶Li(α, 2α), E=118 MeV; measured σ(θ₁, θ₂, E₁, E₂); deduced p+n joint momentum distribution in ⁶Li. Enriched target. PWIA analysis.

doi: 10.1016/0375-9474(89)90259-5
Citations: PlumX Metrics

1988OK02      Bull.Inst.Chem.Res., Kyoto Univ. 66, 22 (1988)

A.Okihana, K.Fukunaga, S.Kakigi, T.Ohsawa, T.Sekioka, H.Yokota, R.Takashima

Continuum Spectra of Deuterons for the p + ³He Reaction at 65 MeV

NUCLEAR REACTIONS, MECPD ³He(polarized p, d), E=65 MeV; measured σ(Ed).

1988WA29      Phys.Rev. C38, 2945 (1988)

R.E.Warner, A.Okihana, M.Fujiwara, N.Matsuoka, K.Tamura, M.Tosaki, T.Ohsawa, K.Fukunaga, P.A.Kimoto, N.Koori

Spectral Function of the p_3/2 Nucleons in ⁶Li

NUCLEAR REACTIONS ⁶Li(α, 2α), E=118 MeV; measured (p+n) spectral function. Plane wave impulse approximation. Enriched target.

doi: 10.1103/PhysRevC.38.2945
Citations: PlumX Metrics

1987FU10      J.Phys.Soc.Jpn. 56, 2357 (1987)

K.Fukunaga, S.Kakigi, T.Ohsawa, A.Okihana, T.Sekioka

Three-Body Breakup Reaction in FSI Region

NUCLEAR REACTIONS ^4,3He(p, p'), E=65 MeV; analyzed σ(θ), analyzing power data. Three-body breakup.

doi: 10.1143/JPSJ.56.2357
Citations: PlumX Metrics

1987KA41      Nucl.Phys. A473, 31 (1987)

S.Kakigi, K.Fukunaga, T.Ohsawa, A.Okihana, T.Sekioka, H.Nakamura-Yokota, S.Tanaka, S.Kato

Multiple Scattering Effect for Quasifree Scattering in the ³He(p, pp)²H Reaction at 64.8 MeV

NUCLEAR REACTIONS, MECPD ³He(p, 2p), E=64.8 MeV; measured σ(E₁, θ₁, θ₂). PWIA analysis, double-scattering effect.

doi: 10.1016/0375-9474(87)90153-9
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1133.

1987OK01      Nucl.Phys. A463, 423c (1987)

A.Okihana, K.Fukunaga, S.Kakigi, T.Ohsawa, T.Sekioka, H.Yokota, R.Takashima

³He Breakup Reaction by 65 MeV Protons in the FSI Region

NUCLEAR REACTIONS ³He(polarized p, p), (polarized p, pd), E=65 MeV; measured σ(θ), σ(θ₁, θ₂), analyzing powers. ΔE-E telescopes, gas target. Theoretical calculations.

doi: 10.1016/0375-9474(87)90685-3
Citations: PlumX Metrics

1986FU05      Nucl.Phys. A456, 48 (1986)

K.Fukunaga, S.Kakigi, T.Ohsawa, A.Okihana, T.Sekioka, H.Nakamura-Yokota, S.Tanaka

Breakup of ⁴He with Polarized Protons at 65 MeV

NUCLEAR REACTIONS ⁴He(polarized p, p'), (polarized p, pt), E=65.05; measured σ(E(p), θ(p)), A(E(p), θ(p)), σ(E(p), E(t), θ(p), θ(t)), A(E(p), E(t), θ(p), θ(t)). Three-body model analysis.

doi: 10.1016/0375-9474(86)90365-9
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1203.

1986OH06      Radiat.Eff. 95, 187 (1986)

T.Ohsawa, K.Fujino, M.Ohta, K.Kudo

A Method of Analysis of Neutron Inelastic Scattering by Heavy Nuclei and Its Application to Cross Section Evaluation for Th-232

NUCLEAR REACTIONS ²³²Th(n, n'), E=threshold-2.5 MeV; calculated, evaluated σ(E). Coupled-channels, Hauser-Feshbach models.

doi: 10.1080/00337578608208692
Citations: PlumX Metrics

1985KO01      Phys.Rev. C31, 246 (1985)

N.Koori, T.Ohsawa, S.Seki, H.Yokota, T.Yanabu, Y.Deschamps, E.Hourani, H.Langevin-Joliot, F.Reide, M.Roy-Stephan

Two-Spectator Quasifree Scattering Process in the ²H(d, pn)pn Reaction at 108 MeV

NUCLEAR REACTIONS ²H(d, np), E=108 MeV; measured breakup σ(Ep, θp, θn); deduced (d, pn), (d, 2p) reaction ratio. Two-spectator quasifree scattering, Sloan four-body theory.

doi: 10.1103/PhysRevC.31.246
Citations: PlumX Metrics

1984OH09      J.Nucl.Sci.Technol.(Tokyo) 21, 887 (1984)

T.Ohsawa, Y.Shigemitsu, M.Ohta, K.Kudo

Systematic Analysis of Fission Cross Sections of Actinides by Means of Double-Humped Barrier Model

NUCLEAR REACTIONS ²³¹Pa, ^{232,234,235,236,238}U, ²³⁷Np, ^{238,239,240,241,242,244}Pu, ^241,242,243Am, ^{243,244,245,246,247,248}Cm, ²⁴⁹Bk, ²⁵²Cf(n, F), E ≈ 0.5-6 MeV; calculated σ(E); deduced optical model parameters. ²³²Pa, ^{233,235,236,237,239}U, ²³⁸Np, ^{239,240,241,242,243,245}Pu, ^242,243,244Am, ^{244,245,246,247,248,249}Cm, ²⁵⁰Bk, ²⁵³Cf deduced fission barriers. Double-humped barrier model.

doi: 10.1080/18811248.1984.9731132
Citations: PlumX Metrics

1983FU08      J.Phys.Soc.Jpn. 52, 69 (1983)

K.Fukunaga, S.Kakigi, T.Ohsawa, A.Okihana

Multiple Scattering Correction on Quasi-Free Scattering

NUCLEAR REACTIONS ²H(p, np), E=65 MeV; calculated quasifree scattering σ normalization factor. Spectator model, impulse approximation, rescattering effects.

doi: 10.1143/JPSJ.52.69
Citations: PlumX Metrics

1983FU18      J.Nucl.Sci.Technol.(Tokyo) 20, 983 (1983)

Y.Fujita, T.Ohsawa, R.M.Brugger, D.M.Alger, W.H.Miller

Measurement of Nuclear Inelastic Scattering Cross Section of Thorium-232 for 144 keV Si-Filtered Neutrons

NUCLEAR REACTIONS ²³²Th(n, n), (n, n'), E=144 keV; measured σ(θ).

doi: 10.1080/18811248.1983.9733500
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12858.

1983MA59      Phys.Rev.Lett. 51, 1741 (1983)

S.Matsuki, T.Higo, T.Ohsawa, T.Shiba, T.Yanabu, K.Ogino, Y.Kadota, K.Haga, N.Sakamoto, K.Kume, M.Matoba

Inelastic Scattering of Polarized Protons and a Possible Hexadecapole-Shape Transition between the Light ^74,76,78Se and the Heavy ^80,82Se Isotopes

NUCLEAR REACTIONS ^{74,76,78,80,82}Se(polarized p, p'), E=65 MeV; measured σ(θ), analyzing power vs θ. ^{74,76,78,80,82}Se deduced β₄, hexadecapole shape transition. Coupled-channels analysis.

doi: 10.1103/PhysRevLett.51.1741
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE0822.

1983YA01      Nucl.Phys. A394, 29 (1983)

M.Yasue, T.Tanabe, F.Soga, J.Kokame, F.Shimokoshi, J.Kasagi, Y.Toba, Y.Kadota, T.Ohsawa, K.Furuno

Deformation Parameter of ¹²C via ¹²C(α, α') and ¹²C(α, α'α) Reactions

NUCLEAR REACTIONS ¹²C(α, α'), (α, 2α), E=65 MeV; measured σ(Eα, θ), in-plane α'α(θ). ¹²C deduced quadrupole, hexadecapole deformation parameter sign. Coupled channel analyses.

doi: 10.1016/0375-9474(83)90159-8
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1191.

1982FU10      Nucl.Phys. A390, 19 (1982)

K.Fukunaga, T.Ohsawa, S.Kakigi, A.Okihana, S.Tanaka, T.Sekioka, H.Nakamura-Yokota

Energy Spectra of Deuterons and Protons for the d + d Reaction at 60 MeV

NUCLEAR REACTIONS ²H(d, d), (d, p), E=59.9 MeV; measured σ(Ed, θd), σ(Ep, θp). Four-body model analysis.

doi: 10.1016/0375-9474(82)90603-0
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE0802.

1982FU12      Bull.Inst.Chem.Res., Kyoto Univ. 60, 156 (1982)

K.Fukunaga, S.Kakigi, T.Ohsawa, A.Okihana

Four Particle Model for Three Body Breakup Reaction

NUCLEAR REACTIONS ²H(d, pd), E=60 MeV; calculated σ(θp, θd, Ep). Four particle model, three-body breakup.

1981FU11      Nucl.Phys. A369, 289 (1981)

K.Fukunaga, S.Kakigi, T.Ohsawa, A.Okihana, S.Tanaka, T.Sekioka, H.Nakamura-Yokota, S.Kato

Deuteron Breakup with ³He at 89.4 and 118.9 MeV

NUCLEAR REACTIONS ²H(³He, ³Hep), (³He, tp), (³He, 2d), E=89.4, 118.9; measured σ(E₁, E₂, θ₁, θ₂). Three-body, four-body model analysis.

doi: 10.1016/0375-9474(81)90021-X
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE0883.

1980KA20      J.Phys.Soc.Jpn. 48, 1797 (1980)

S.Kakigi, K.Fukunaga, T.Ohsawa, S.Tanaka, A.Okihana, H.Nakamura-Yokota, T.Sekioka, N.Fujiwara

Excited States of ⁴He Observed in the ⁴He(α, αd)²H Reaction at 119 MeV

NUCLEAR REACTIONS ⁴He(α, α'), (α, αd), E=119 MeV; measured Eα, σ(Eα, θα, θd). ⁴He deduced levels, J, π. Kinematically complete experiment.

doi: 10.1143/JPSJ.48.1797
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2569.

1980TA11      Nucl.Phys. A341, 199 (1980)

S.Tanaka, N.Fujiwara, K.Fukunaga, T.Higo, T.Ohsawa, A.Okihana, T.Sekioka, T.Miyanaga, T.Yanabu

Continuum Energy Spectra of ³He Scattered by ³He at 120 MeV

NUCLEAR REACTIONS ³He(³He, ³He'), E=120 MeV; measured σ(E(³He), θ); deduced reaction mechanism. ³He deduced no excited states.

doi: 10.1016/0375-9474(80)90308-5
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE0200.

1979OK01      J.Phys.Soc.Jpn. 46, 707 (1979)

A.Okihana, N.Fujiwara, H.Nakamura-Yokota, T.Yanabu, K.Fukunaga, T.Ohsawa, S.Tanaka

The D(d, d)D, D(d, p)T and D(d, ³He)n Reactions at 13.2 MeV

NUCLEAR REACTIONS ²H(d, d), (d, p), (d, t), (d, ³He), E=13.2 MeV; measured σ(θ); deduced σ(θ) for ²H(d, n). Optical model. DWBA analysis.

doi: 10.1143/JPSJ.46.707
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1145.

1978FU03      J.Phys.Soc.Jpn. 44, 1413 (1978)

K.Fukunaga, T.Ohsawa, N.Fujiwara, S.Tanaka, A.Okihana, T.Yanabu

Excited States of ⁴He Observed in the ⁶Li + d Reaction

NUCLEAR REACTIONS ⁶Li(d, α), (d, dα), E=13.6 MeV; measured σ(Eα, θ), σ(Ed, Eα, θ). ⁴He level deduced Γ, J, π.

doi: 10.1143/JPSJ.44.1413
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1503.

1978FU08      J.Phys.Soc.Jpn. 45, 1783 (1978)

K.Fukunaga, N.Fujiwara, S.Kakigi, T.Ohsawa, H.Nakamura-Yokota, S.Tanaka, A.Okihana, T.Sekioka, T.Higo, T.Miyanaga

Breakup Reaction of ³He by ³He at 120 MeV

NUCLEAR REACTIONS ³He(³He, ³Hep), (³He, ³Hed), E=120 MeV; measured ³He-p, ³He-d coin spectra. ³He level deduced no evidence. Quasi-free, final state interaction analysis.

doi: 10.1143/JPSJ.45.1783
Citations: PlumX Metrics

1978TA12      J.Phys.Soc.Jpn. 45, 733 (1978)

S.Tanaka, K.Fukunaga, S.Kakigi, T.Ohsawa, N.Fujiwara, T.Yanabu

Elastic and Inelastic Scattering of Deuterons by ⁹Be in the Energy Range of 12.17 MeV to 14.43 MeV

NUCLEAR REACTIONS ⁹Be(d, d), (d, d'), E=12.17-14.43 MeV; measured σ(E, θ). ⁹Be deduced β₂. Optical model, DWBA, coupled-channel analyses.

doi: 10.1143/JPSJ.45.733
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE0029.

1977FU09      J.Phys.Soc.Jap. 42, 725 (1977)

K.Fukunaga, T.Ohsawa, S.Kakigi, S.Tanaka, N.Fujiwara

Continuous Energy Spectra of Alpha-Particles from ¹¹B(p, α)⁸Be Reaction

NUCLEAR REACTIONS ¹¹B(p, α), E=6.5-7.3 MeV; measured σ(E;Eα, θ).

doi: 10.1143/JPSJ.42.725
Citations: PlumX Metrics

1973MI29      Mem.Fac.Eng., Kyushu Univ. 33, No.2, 47 (1973)

K.Miyamoto, M.Ohta, T.Ohsawa

Calculation of Neutron Inelastic Scattering Cross Sections for ²³³Pa and ²³⁹Np

NUCLEAR REACTIONS ²³³Pa, ²³⁹Np(n, n'), E=.03-11 MeV; calculated σ(En', θ).

1972NA31      Annu.Rep.Res.Reactor Inst., Kyoto Univ. 5, 59 (1972)

Y.Nakagome, T.Ohsawa, I.Kimura, T.Shibata

Measurements of Fragment Mass Distributions for ²³³U and ²³⁵U Thermal-Neutron Fission

NUCLEAR REACTIONS, Fission ^233,235U(n, F), E=thermal; measured fragment mass distribution.

1972YA06      J.Phys.Soc.Jap. 33, 265 (1972)

M.Yasue, T.Ohsawa, N.Fujiwara, S.Kakigi, D.C.Nguyen, S.Yamashita

Excited States of ¹⁰B Near 10 MeV Studied by Proton Induced Reactions on ⁹Be

NUCLEAR REACTIONS ⁹Be(p, p), (p, p'), E=4-6 MeV; measured σ(E;θ). ¹⁰B deduced resonances, level-width.

doi: 10.1143/JPSJ.33.265
Citations: PlumX Metrics
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1969AB02      J.Phys.Soc.Japan 26, 577(1969)

K.Abe, N.Kawamura, H.Nihei, T.Ohsawa, N.Mutsuro

Photoproton Spectrum from ⁵¹V

NUCLEAR REACTIONS ⁵¹V(γ, p), E=26.6 MeV; measured σ(Ep).

doi: 10.1143/JPSJ.26.577
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