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NSR database version of May 24, 2024.

Search: Author = T.Wada

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2023OK02      Phys.Rev. C 107, 034608 (2023)

K.Okada, T.Wada, R.Capote, N.Carjan

Cassini-oval description of the multidimensional potential energy surface for 236U: Role of octupole deformation and calculation of the most probable fission path

NUCLEAR STRUCTURE 236U; calculated potential energy surfaces, static fission path, influence of octupole deformation parameter, total deformation energy. Calculations in the frame of the microscopic-macroscopic model with a Cassini-oval description of the nuclear shapes. Established existence of a triple-humped barrier with a shallow third minimum.

doi: 10.1103/PhysRevC.107.034608
Citations: PlumX Metrics


2022TA12      Phys.Rev. C 106, 014617 (2022)

M.Tanaka, M.Takechi, A.Homma, A.Prochazka, M.Fukuda, D.Nishimura, T.Suzuki, T.Moriguchi, D.S.Ahn, A.Aimaganbetov, M.Amano, H.Arakawa, S.Bagchi, K.-H.Behr, N.Burtebayev, K.Chikaato, H.Du, T.Fujii, N.Fukuda, H.Geissel, T.Hori, S.Hoshino, R.Igosawa, A.Ikeda, N.Inabe, K.Inomata, K.Itahashi, T.Izumikawa, D.Kamioka, N.Kanda, I.Kato, I.Kenzhina, Z.Korkulu, Y.Kuk, K.Kusaka, K.Matsuta, M.Mihara, E.Miyata, D.Nagae, S.Nakamura, M.Nassurlla, K.Nishimuro, K.Nishizuka, K.Ohnishi, M.Ohtake, T.Ohtsubo, S.Omika, H.J.Ong, A.Ozawa, H.Sakurai, C.Scheidenberger, Y.Shimizu, T.Sugihara, T.Sumikama, H.Suzuki, S.Suzuki, H.Takeda, Y.Tanaka, Y.K.Tanaka, I.Tanihata, T.Wada, K.Wakayama, S.Yagi, T.Yamaguchi, R.Yanagihara, Y.Yanagisawa, K.Yoshida, T.K.Zholdybayev

Charge-changing cross sections for 42-51Ca and effect of charged-particle evaporation induced by neutron-removal reactions

NUCLEAR REACTIONS 12C(42Ca, X), (43Ca, X), (44Ca, X), (45Ca, X), (46Ca, X), (47Ca, X), (48Ca, X), (49Ca, X), (50Ca, X), (51Ca, X), E=280 MeV/nucleon; measured reaction products; deduced charge-exchange σ. Comparison to Glauber-like model calculations. Observed significant decrease of charge-exchange cross-section with increase of point-proton radius and attributed this effect to attributed to the charged-particle evaporation induced by the neutron-removal reaction. Used the conclusions of the present work to re-analyze charge-exchange σ for Be, B, C, N, O, F, Si, Ti, Ca, Fe isotopes. BigRIPS fragment separator at RI Beam Factory (RIBF).

doi: 10.1103/PhysRevC.106.014617
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2733.


2020TA05      Phys.Rev.Lett. 124, 102501 (2020)

M.Tanaka, M.Takechi, A.Homma, M.Fukuda, D.Nishimura, T.Suzuki, Y.Tanaka, T.Moriguchi, D.S.Ahn, A.Aimaganbetov, M.Amano, H.Arakawa, S.Bagchi, K.-H.Behr, N.Burtebayev, K.Chikaato, H.Du, S.Ebata, T.Fujii, N.Fukuda, H.Geissel, T.Hori, W.Horiuchi, S.Hoshino, R.Igosawa, A.Ikeda, N.Inabe, K.Inomata, K.Itahashi, T.Izumikawa, D.Kamioka, N.Kanda, I.Kato, I.Kenzhina, Z.Korkulu, Y.Kuk, K.Kusaka, K.Matsuta, M.Mihara, E.Miyata, D.Nagae, S.Nakamura, M.Nassurlla, K.Nishimuro, K.Nishizuka, K.Ohnishi, M.Ohtake, T.Ohtsubo, S.Omika, H.J.Ong, A.Ozawa, A.Prochazka, H.Sakurai, C.Scheidenberger, Y.Shimizu, T.Sugihara, T.Sumikama, H.Suzuki, S.Suzuki, H.Takeda, Y.K.Tanaka, I.Tanihata, T.Wada, K.Wakayama, S.Yagi, T.Yamaguchi, R.Yanagihara, Y.Yanagisawa, K.Yoshida, T.K.Zholdybayev

Swelling of Doubly Magic 48Ca Core in Ca Isotopes beyond N=28

NUCLEAR REACTIONS C(42Ca, X), (43Ca, X), (44Ca, X), (45Ca, X), (46Ca, X), (47Ca, X), (48Ca, X), (49Ca, X), (50Ca, X), (51Ca, X), E=280 MeV/nucleon; measured reaction products. 42,43,44,45,46,47,48,49,50,51Ca; deduced neutron number dependence in root-mean-square matter radii, novel growth in neutron skin thickness. Comparison with mean field calculations.

doi: 10.1103/PhysRevLett.124.102501
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2656.


2010YA08      Prog.Theor.Phys.(Kyoto) 123, 1029 (2010)

K.Yamamoto, K.Kato, T.Wada, M.Ohta

Effect of Uncertainties in Nuclear Reaction Rate on Nucleosynthesis Paths

NUCLEAR REACTIONS 17O(n, γ), E<1 MeV; analyzed network calculations; deduced reaction rates, σ, stellar abundances and nucleosynthesis path.

doi: 10.1143/PTP.123.1029
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2009YA03      Prog.Theor.Phys.(Kyoto) 121, 375 (2009)

K.Yamamoto, H.Masui, J.Kato, T.Wada, M.Ohta

Radiative Capture Cross Section for 16O(n, γ)17O and 16O(p, γ)17F below Astrophysical Energies

NUCLEAR REACTIONS 16O(n, γ), E(cm) < 10 MeV; calculated cross sections.16O(p, γ), E(cm) < 3 MeV; calculated astrophysical S-factor.

doi: 10.1143/PTP.121.375
Citations: PlumX Metrics


2006NA06      Int.J.Mod.Phys. E15, 311 (2006)

A.K.Nasirov, Y.Aritomo, A.Fukushima, M.Ohta, T.Wada, G.Giardina, G.Mandaglio, A.Muminov, R.K.Utamuratov

Role of the nuclear shell structure and orientation angles of deformed reactants in complete fusion

NUCLEAR REACTIONS 238U(16O, X), E=80-160 MeV; 154Sm(60Ni, X), E=240-330 MeV; calculated fusion and evaporation residue σ; deduced shell structure and orientation effects. Dinuclear system concept, Langevin calculations, comparison with data.

doi: 10.1142/S0218301306004144
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2004AS07      Prog.Theor.Phys.(Kyoto), Suppl. 154, 457 (2004)

T.Asano, T.Wada, M.Ohta, T.Ichikawa, S.Yamaji, H.Nakahara

Dynamical Calculation of Multi-Modal Nuclear Fission of Fermium Isotopes

NUCLEAR STRUCTURE 256Fm; calculated fission fragment total kinetic energy and mass distributions, excitation energy dependence. Dynamical calculation.

doi: 10.1143/PTPS.154.457
Citations: PlumX Metrics


2004AS14      J.Nucl.Radiochem.Sci. 5, No 1, 1 (2004)

T.Asano, T.Wada, M.Ohta, T.Ichikawa, S.Yamaji, H.Nakahara

Dynamical Calculation of Multi-Modal Nuclear Fission of Fermium Nuclei

NUCLEAR STRUCTURE 256,258,264Fm; calculated fission fragments kinetic energy and mass distributions. Multi-modal fission model.


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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2002IC03      J.Nucl.Radiochem.Sci. 3, No 1, 67 (2002)

T.Ichikawa, T.Asano, T.Wada, M.Ohta

Dynamics of Fission Modes Studied with the 3-dimensional Langevin Equation

NUCLEAR STRUCTURE 270Sg; calculated fission modes deformations, shell correction energy, fragments kinetic energy and mass distributions.


2001IC02      Prog.Theor.Phys.(Kyoto) 105, 915 (2001)

T.Ichikawa, T.Wada, M.Ohta

Fission Width of Compound Nuclei Calculated Using the Mean First Passage Time Method

NUCLEAR STRUCTURE 238U; calculated fission width vs angular momentum. Mean first passage time method.

NUCLEAR REACTIONS 100Mo, 110Pd(100Mo, X), 110Pd(110Pd, X), E(cm)=170-290 MeV; calculated fission barrier, evaporation residue σ. Mean first passage time method.

doi: 10.1143/PTP.105.915
Citations: PlumX Metrics


2001OK01      J.Phys.(London) G27, 855 (2001)

K.Okei, T.Wada, Y.Yamashita, K.Kuga, M.Nakagawa, I.Yamamoto, N.Takahashi, K.Iwata, M.Aglietta, C.Castagnoli, O.Saavedra

Search for Nuclearites using the TL Stack Detector

doi: 10.1088/0954-3899/27/4/310
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2000WA39      Prog.Theor.Phys.(Kyoto), Suppl. 140, 1 (2000)

T.Wada

Dynamics of the Synthesis of Superheavy Elements

NUCLEAR REACTIONS 258Fm(32Si, X), 244Pu(48Ca, X), 238U(52Ti, X), 234Th(56Cr, X), E*=20-50 MeV; calculated evaporation residue σ. Fluctuation-dissipation dynamics.

doi: 10.1143/PTPS.140.1
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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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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.


1999TO12      Prog.Theor.Phys.(Kyoto) 101, 607 (1999)

T.Tokuda, T.Wada, M.Ohta

Fusion Cross Section of Massive Nuclei by Fluctuation-Dissipation Dynamics

NUCLEAR REACTIONS 100Mo, 110Pd(100Mo, X), 110Pd(110Pd, X), E(cm)=200-280 MeV; calculated fusion σ; deduced fusion hindrance features. Fluctuation-dissipation dynamics.

doi: 10.1143/PTP.101.607
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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
Citations: PlumX Metrics


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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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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1993AI03      Nucl.Phys. A562, 101 (1993)

S.Ait-Tahar, R.S.Mackintosh, S.G.Cooper, T.Wada

Energy Dependence of a Local Equivalent Potential for RGM Phase Shifts for 16O + 16O

NUCLEAR REACTIONS 16O(16O, 16O), E=30-500 MeV; calculated σ(θ). Local equivalent potential for resonating group method phase shifts.

doi: 10.1016/0375-9474(93)90034-U
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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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1990WA01      Phys.Rev. C41, 160 (1990)

T.Wada, S.Yamaguchi, H.Horiuchi

Strength of the Attraction of the Skyrme-Type Forces Used in the Heavy-Ion Reaction Problems

NUCLEAR REACTIONS 16O, 12C(12C, 12C), 16O(α, α), (16O, 16O), E ≈ 10-100 MeV/nucleon; calculated internucleus potentials. Canonical moving wave packet method, Skyrme type forces.

doi: 10.1103/PhysRevC.41.160
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1988WA23      Phys.Rev. C38, 2063 (1988)

T.Wada, H.Horiuchi

Resonating-Group-Method Study of α + 40Ca Elastic Scattering and 44Ti Structure

NUCLEAR REACTIONS 40Ca(α, α), E=29-61 MeV; calculated σ(θ), equivalent local potential. Resonating group method.

NUCLEAR STRUCTURE 44Ti; calculated levels, B(E2), band structure, rms radius. Resonating group method.

doi: 10.1103/PhysRevC.38.2063
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1988WA31      Prog.Theor.Phys.(Kyoto) 80, 488 (1988)

T.Wada, H.Horiuchi

Study of 16O - 16O Potential by the Resonating Group Method. I

NUCLEAR REACTIONS 16O(16O, 16O), E=10 MeV/nucleon; calculated potential parameters dependences. Resonating group method.

doi: 10.1143/PTP.80.488
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1988WA32      Prog.Theor.Phys.(Kyoto) 80, 502 (1988)

T.Wada, H.Horiuchi

Study of 16O - 16O Potential by the Resonating Group Method. II - Analyses of Constituent Components of the Exchange Potential between Heavy-Ion Nuclei -

NUCLEAR REACTIONS 16O(16O, 16O), E not given; calculated potential components, parameter dependences. Resonating group method.

doi: 10.1143/PTP.80.502
Citations: PlumX Metrics


1988YA02      Prog.Theor.Phys.(Kyoto) 79, 19 (1988)

K.Yabana, T.Wada, H.Horiuchi

Microscopic Derivation of the Nucleus-Nucleus Potential by the Use of the Density-Dependent Effective Interaction

NUCLEAR REACTIONS 4He(α, α), E=20, 60 MeV; calculated potential parameters. Microscopic model, density dependent interactions.

doi: 10.1143/PTP.79.19
Citations: PlumX Metrics


1986HO33      Prog.Theor.Phys.(Kyoto) 76, 837 (1986)

H.Horiuchi, T.Wada, K.Yabana

Cranked Cluster Wave Function for Molecular States

NUCLEAR REACTIONS 16O, 4He(α, α), 16O(16O, 16O), E not given; calculated potential energy vs ion-ion distance, critical angular momenta. Cranked cluster wave functions.

NUCLEAR STRUCTURE 8Be, 32S, 20Ne; calculated rotational spectra. Cranked cluster wave function.

doi: 10.1143/PTP.76.837
Citations: PlumX Metrics


1986WA08      Prog.Theor.Phys.(Kyoto) 75, 458 (1986)

T.Wada

Study of 16O + 40Ca Potential by the Resonating Group Method

NUCLEAR REACTIONS 40Ca(16O, 16O), E=2.5, 10, 25 MeV/nucleon; calculated equivalent local potential. Resonating group method, nonlocal potential input, WKB approach.

doi: 10.1143/PTP.75.458
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1986WA09      Prog.Theor.Phys.(Kyoto) 75, 198 (1986)

T.Wada

Study of the Difference between the Spin-Orbit Potentials of 3He and t by the Resonanting Group Method

NUCLEAR REACTIONS 16O, 40Ca(3He, 3He), (t, t), E=5-20 MeV/nucleon; calculated spin-orbit potential projectile dependences. Resonanting group method.

doi: 10.1143/PTP.75.198
Citations: PlumX Metrics


1986WA12      Prog.Theor.Phys.(Kyoto) 75, 619 (1986)

T.Wada, Y.Takahashi, H.Horiuchi

Microscopic Derivation of the Spin-Orbit Potential of Mass-Three Nucleus

NUCLEAR REACTIONS 40Ca, 16O(3He, 3He), E=5, 10, 15 MeV/nucleon; calculated spin-orbit potential parameters. Resonating group method.

doi: 10.1143/PTP.75.619
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1981FU12      J.Phys.Soc.Jpn. 50, 3198 (1981)

T.Fujisawa, N.Kishida, T.Kubo, T.Wada, Y.Toba, T.Hasegawa, M.Sekiguchi, N.Ueda, M.Yasue, F.Soga, H.Kamitsubo, M.Nakamura, K.Hatanaka, Y.Wakuta, T.Tanaka, A.Nagao

Analyzing Power-Polarization Inequality in the Inelastic Scattering of Protons on 12C for Incident Energies from 22.0 to 29.0 MeV

NUCLEAR REACTIONS 12C(polarized p, p'), E=22-29 MeV; measured P(θ), analyzing power vs θ. Proton-gamma coincidence technique.

doi: 10.1143/JPSJ.50.3198
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1406.


1981KO23      Phys.Rev. C24, 1611 (1981)

M.Koike, K.Komura, H.Kawakami, M.Kanbe, H.Yamada, G.Madueme, S.Shibata, T.Fujisawa, T.Wada

Electric Monopole Transitions between 0+ States in 102Ru

RADIOACTIVITY 102Rh [from 102Ru(p, n)]; measured Eγ, Iγ, I(ce). 102Ru levels deduced B(E0)/B(E2), electric monopole moment.

doi: 10.1103/PhysRevC.24.1611
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1980OH08      Phys.Lett. B97, 192 (1980)

H.Ohnuma, T.Kubo, N.Kishida, T.Hasegawa, N.Ueda, T.Fujisawa, T.Wada, K.Iwatani, T.Suehiro

Vector Analyzing Power and Polarization Measurements for the 116Sn(d, p)117Sn Reaction and Deuteron D-State Effects

NUCLEAR REACTIONS 116Sn(polarized d, p), E=22 MeV; measured σ(θ), polarization, analyzing power vs θ; deduced spin-orbit distortion, deuteron D-state effects. Exact finite-range DWBA. Enriched target.

doi: 10.1016/0370-2693(80)90579-1
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE0121.


1980YA05      J.Nucl.Sci.Technol.(Tokyo) 17, 582 (1980)

N.Yamamuro, K.Saito, T.Emoto, T.Wada, Y.Fujita, K.Kobayashi

Neutron Capture Cross Section Measurements of Nb-93, I-127, Ho-165, Ta-181 and U-238 between 3.2 and 80 keV

NUCLEAR REACTIONS 93Nb, 165Ho, 181Ta, 238U(n, γ), E=3.2-80 keV; measured σ. Tof, C6F6, C6D6 scintillators.

doi: 10.1080/18811248.1980.9732628
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset21466.


1978SO10      Phys.Rev. C18, 2457 (1978)

F.Soga, J.Schimizu, H.Kamitsubo, N.Takahashi, K.Takimoto, R.Wada, T.Fujisawa, T.Wada

Intermediate Structures in 12C + 16O System Through Alpha-Induced Reactions on 24Mg

NUCLEAR REACTIONS 24Mg(α, 12C), (α, α), (α, α'), 22 MeV ≤ E ≤ 26 MeV; measured σ(Eα, θ), σ(θ). 28Si deduced intermediate resonances, J, π.

doi: 10.1103/PhysRevC.18.2457
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1388.


1978WA11      Nucl.Phys. A307, 425 (1978)

T.Wada

Elastic and Inelastic Deuteron Scattering from Even-Mass Isotopes of Molybdenum

NUCLEAR REACTIONS 92,94,96,98,100Mo(d, d'), E=21.5 MeV; measured σ(θ). 92,94,96,98,100Mo levels deduced deformation parameter β. Enriched targets. Optical model, coupled-channel analyses. RPA, folding model calculations.

doi: 10.1016/0375-9474(78)90458-X
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE0030.


1975KO12      Nucl.Phys. A248, 237 (1975)

M.Koike, T.Suehiro, K.Pingel, K.Komura, I.Nonaka, T.Wada, T.Fujisawa, H.Kamitsubo, T.Nojiri

Elastic and Inelastic Scattering of 52 MeV Protons from 106Pd, 108Pd and 110Pd

NUCLEAR REACTIONS 106,108,110Pd(p, p), (p, p'), E=51.93 MeV; measured σ(Ep, θ), σ(Ep', θ). 106,108,110Pd deduced levels, deformation parameters β. Enriched targets. DWBA, coupled-channel calculations.

doi: 10.1016/0375-9474(75)90164-5
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1399.


1972AW03      J.Phys.Soc.Jap. 33, 881 (1972)

Y.Awaya, K.Matsuda, T.Wada, N.Nakanishi, S.Takeda, S.Yamaji

Inelastic Scattering of Protons from 100Mo and 98Mo

NUCLEAR REACTIONS 98,100Mo(p, p), (p, p'), E=14.7 MeV; measured σ(θ); deduced optical model parameters. 98,100Mo deduced levels, L, J, π, β.

doi: 10.1143/JPSJ.33.881
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1407.


1970KO15      J.Phys.Soc.Jap. 29, 1 (1970)

S.Kobayashi, S.Motonaga, Y.Chiba, K.Katori, A.Stricker, T.Fujisawa, T.Wada

Spin Flip in the Inelastic Scattering of Protons from 12C at Energies Around 13.1 MeV Resonance

NUCLEAR REACTIONS 12C(p, p'), E=12-14 MeV; measured σ(E;θ), spin-flip probability(θ). 12C(p, p), E=12-14 MeV; measured σ(E;θ).

doi: 10.1143/JPSJ.29.1
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1414.


1969AW01      J.Phys.Soc.Japan 27, 1087 (1969)

Y.Awaya, K.Matsuda, N.Nakanishi, S.Takeda, T.Wada

The 91Zr(p, p') Reaction at 14.52 MeV

NUCLEAR REACTIONS 91Zr(p, p), (p, p'), E = 14.52 MeV; measured σ(E;θ); deduced optical model parameters. 91Zr deduced levels, L, J, π, β(L).

doi: 10.1143/JPSJ.27.1087
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2275.


1969FU04      J.Phys.Soc.Japan 27, 278 (1969)

T.Fujisawa, H.Kamitsubo, T.Wada, M.Igarashi

Optical-Model Analysis of Elastic Scattering of 3He Particles from 58Ni at 24.15, 27.64 and 34.14 MeV

NUCLEAR REACTIONS 58Ni(3He, 3He), E = 24, 28, 34 MeV; measured Q, σ(E;θ); deduced optical model parameters.

doi: 10.1143/JPSJ.27.278
Citations: PlumX Metrics


1969KA01      Phys.Letters 28B, 408(1969)

H.Kamitsubo, T.Wada, T.Fujisawa, M.Igarashi

Large-Angle Scattering of 3He Particles by 58Ni

NUCLEAR REACTIONS 58Ni(3He, 3He), E=24, 27, 34 MeV; measured σ(E; θ); deduced optical model parameters.

doi: 10.1016/0370-2693(69)90334-7
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1495.


1969KO01      Nucl.Phys. A125, 161 (1969)

M.Koike, I.Nonaka, J.Kokame, H.Kamitsubo, Y.Awaya, T.Wada, H.Nakamura

Collective States of 110Cd, 114Cd and 116Cd Excited in Inelastic Scattering of 55 MeV Protons

NUCLEAR REACTIONS 110,114,116Cd(p, p'), Ep=55 MeV; measured σ(Ep', θ); deduced optical model parameters. 110,114,116Cd deduced levels, β(L). Enriched targets.

doi: 10.1016/0375-9474(69)90835-5
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1968KO03      Phys.Letters 26B, 288 (1968)

M.Koike, I.Nonaka, J.Kokame, H.Kamitsubo, Y.Awaya, T.Wada, H.Nakamura

Collective States of 114Cd Excited by Inelastic Scattering of 55 MeV Protons

NUCLEAR STRUCTURE 114Cd; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0370-2693(68)90562-5
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1968KO19      J.Phys.Soc.Japan 25, 626 (1968)

M.Koike, I.Nonaka, H.Nakamura, H.Taketani, Y.Awaya, T.Wada, K.Matsuda

Collective States of 116Sn Excited by Inelastic Scattering of 14.695 MeV Protons

NUCLEAR REACTIONS 116Sn(p, p'), E = 14.695 MeV; measured σ(Ep', θ). 116Sn deduced levels, L, deformation parameters β(λ). Magnetic spectrometer.

doi: 10.1143/JPSJ.25.626
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1968MA46      J.Phys.Soc.Japan 25, 1207(1968)

K.Matsuda, N.Nakanishi, S.Takeda, T.Wada

Cross Sections of the 12C(3He, p)14N Reaction

NUCLEAR REACTIONS 12C(3He, p), E = 25.3 MeV; measured σ(Ep, θ). 14N deduced levels.

doi: 10.1143/JPSJ.25.1207
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1477.


1967MA14      J.Phys.Soc.Jpn. 22, 1311 (1967)

K.Matsuda, H.Nakamura, I.Nonaka, H.Taketani, T.Wada, Y.Awaya, M.Koike

Inelastic Proton Scattering from 90Zr and 92Zr

NUCLEAR STRUCTURE 90Zr, 92Zr; measured not abstracted; deduced nuclear properties.

doi: 10.1143/JPSJ.22.1311
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0372.


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