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NSR database version of April 11, 2024.

Search: Author = T.Tsukamoto

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2004UE01      J.Phys.Soc.Jpn. 73, 875 (2004)

H.Ueno, H.Taneichi, Y.Takahashi, T.Suzuki, K.Shoda, T.Saito, T.Tsukamoto

Cross Sections and Angular Distributions for the ¹⁰B(e, p) and ¹⁰B(e, d) Reactions in the Giant Resonance Region

NUCLEAR REACTIONS ¹⁰Be(e, p), (e, d), E=18.5-27.0 MeV; measured deuteron and proton spectra, σ(θ). ¹⁰Be(γ, p), E^* ≈ 12-29 MeV; deduced σ. ¹⁰Be deduced resonance features.

doi: 10.1143/JPSJ.73.875
Citations: PlumX Metrics

1993OH02      Phys.Rev. D47, 4840 (1993)

T.Ohshima, H.Sakamoto, T.Sato, J.Shirai, T.Tsukamoto, Y.Sugaya, K.Takahashi, T.Suzuki, C.Rosenfeld, S.Wilson, K.Ueno, Y.Yonezawa, H.Kawakami, S.Kato, S.Shibata, K.Ukai

No 17 keV Neutrino: Admixture < 0.073% (95% C.L.)

RADIOACTIVITY ⁶³Ni(β^-); measured β-spectra; deduced 17 keV ν admixing with ν(e) upper limit. High confidence limit, magnetic spectrometer.

doi: 10.1103/PhysRevD.47.4840
Citations: PlumX Metrics

1992KA29      Phys.Lett. 287B, 45 (1992)

H.Kawakami, S.Kato, T.Ohshima, C.Rosenfeld, H.Sakamoto, T.Sato, S.Shibata, J.Shirai, Y.Sugaya, T.Suzuki, K.Takahashi, T.Tsukamoto, K.Ueno, K.Ukai, S.Wilson, Y.Yonezawa

High Sensitivity Search for a 17 keV Neutrino. Negative Indication with an Upper Limit of 0.095%

RADIOACTIVITY ⁶³Ni(β^-); measured β-spectrum near 17 keV ν-threshold; deduced no 17 keV ν indication, admixture upper limit.

doi: 10.1016/0370-2693(92)91874-9
Citations: PlumX Metrics

1989MA61      Prog.Theor.Phys.(Kyoto) 82, 1009 (1989)

T.Maruyama, T.-Y.Saito, T.Tsukamoto

Skyrme Interaction with Attractive Pairing Property without Density Dependent Force

NUCLEAR STRUCTURE ¹⁶O, ⁴⁰Ca; calculated binding energy per nucleon, compressibility, Fermi momentum. Skyrme interaction, pairing, no density dependence.

doi: 10.1143/PTP.82.1009
Citations: PlumX Metrics

1987MI32      Phys.Rev. C36, 1792 (1987)

H.Miyase, H.Tsubota, Y.Kawazoe, T.Tsukamoto

⁸⁹Y(γ, p₀) Cross Section Deduced from the ⁸⁹Y(e, p₀) Reaction

NUCLEAR REACTIONS ⁸⁹Y(e, p), E=13-31 MeV; measured σ(E(e'), E(p'), θ); deduced photonuclear σ(E). ⁸⁹Y deduced E1, E2 transition strength distribution. Resonance model analysis. Direct-semidirect model calculation.

doi: 10.1103/PhysRevC.36.1792
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0462.

1987TS06      J.Phys.Soc.Jpn. 56, 1916 (1987)

T.Tsukamoto, Y.Kawazoe, H.Miyase, H.Tsubota

Surprisal Analysis of the ^63,65Cu(e, p₀) Reactions

NUCLEAR REACTIONS ^63,65Cu(e, p), E not given; analyzed data; deduced ^63,65Cu(γ, p) reaction σ(E). Surprisal analysis, Hauser-Feshbach model.

doi: 10.1143/JPSJ.56.1916
Citations: PlumX Metrics

1986KA01      Phys.Rev. C33, 275 (1986)

Y.Kawazoe, T.Tsukamoto

Estimate of the Pionic Contribution to very forward Electron Scattering from ³He by Surprisal Analysis

NUCLEAR REACTIONS ³He(e, e'), E=2.81, 7.26, 14.69 GeV; analyzed σ(E(e'), θ); deduced pion number contribution. Surprisal analysis.

doi: 10.1103/PhysRevC.33.275
Citations: PlumX Metrics

1986MI19      Nucl.Phys. A457, 109 (1986)

H.Miyase, H.Tsubota, Y.Kawazoe, T.Tsukamoto

The ^63,65Cu(e, p₀) Reactions in the Giant Resonance Region

NUCLEAR REACTIONS ^63,65Cu(e, p), E=11-28 MeV; measured σ(E(e), E(p), θ); deduced photonuclear σ(E). ^63,65Cu deduced E1, E2 transition strength distribution. Resonance model analysis. Statistical, direct-semidirect model calculations. Enriched target.

doi: 10.1016/0375-9474(86)90522-1
Citations: PlumX Metrics

1986TA06      Nucl.Phys. A448, 315 (1986)

H.Taneichi, H.Ueno, K.Shoda, Y.Kawazoe, T.Tsukamoto

The E2 Strength Distribution in ⁶Li Studied by the (e, d₀) Reaction

NUCLEAR REACTIONS ⁶Li(e, d), E=10-28 MeV; measured σ(E, θ). ⁶Li deduced E1, E2 transition strength distributions. Enriched target.

doi: 10.1016/0375-9474(86)90094-1
Citations: PlumX Metrics

1986TS03      Prog.Theor.Phys.(Kyoto) 76, 645 (1986)

T.Tsukamoto

Spin Cutoff Parameter for the Exciton Model

NUCLEAR STRUCTURE A=40-60; calculated spin cutoff parameters, total angular momentum. Harmonic oscillator shell model, restricted population approximation.

doi: 10.1143/PTP.76.645
Citations: PlumX Metrics

1983MI02      Phys.Rev.Lett. 50, 821 (1983)

H.Miyase, H.Tsubota, Y.Kawazoe, T.Tsukamoto

Identification of E2 Strength Distribution in ⁶⁵Cu by the (e, p₀) Reaction

NUCLEAR REACTIONS ⁶⁵Cu(e, p), E=13-28 MeV; measured σ(θp); deduced σ(γ, p₀) vs E. ⁶⁵Cu deduced giant resonance parameters, GDR, GQR, E2 strength distribution. Resonance model analysis.

doi: 10.1103/PhysRevLett.50.821
Citations: PlumX Metrics

1982TS01      Phys.Rev. C25, 1272 (1982)

T.Tsukamoto, Y.Kawazoe

Surprisal Analysis of Inclusive Reactions

NUCLEAR REACTIONS ¹⁸¹Ta(e, e'), E=500 MeV; calculated σ(θ, E(e')). Inclusive reactions, surprisal analysis.

doi: 10.1103/PhysRevC.25.1272
Citations: PlumX Metrics

1982TS02      Prog.Theor.Phys.(Kyoto) 67, 222 (1982)

T.Tsukamoto, T.Honda, C.Ishii, H.Matsuzaki

Two-Dimensional Random Walk Process in Heavy Ion Collisions

NUCLEAR REACTIONS ²⁷Al(¹⁶O, X), E=88 MeV; calculated total kinetic energy loss, variance vs fragment mass; ²³²Th(⁴⁰Ar, X), E=388 MeV; calculated total kinetic energy loss, variance vs fragment mass, Z. Two-dimensional random walk model.

doi: 10.1143/PTP.67.222
Citations: PlumX Metrics

1981KA12      Phys.Rev. C23, 2364 (1981)

Y.Kawazoe, T.Tsukamoto

Splitting of Isovector Giant Quadrupole Resonance

NUCLEAR STRUCTURE ⁴He, ¹⁶O, ^40,48Ca, ⁹⁰Zr, ¹⁵²Sm, ²⁰⁸Pb, ²³⁸U; calculated T=1, GQR fragmentation. Schematic model.

doi: 10.1103/PhysRevC.23.2364
Citations: PlumX Metrics

1980TA15      Nucl.Phys. A350, 157 (1980)

H.Taneichi, H.Ueno, K.Shoda, Y.Kawazoe, T.Tsukamoto

The ¹⁴N(e, d₀) Reaction in the Giant Resonance Region

NUCLEAR REACTIONS ¹⁴N(e, d), E=18-29 MeV; measured σ(Ed, θd). ¹⁴N deduced giant resonances. Cluster model analysis. Natural BN target.

doi: 10.1016/0375-9474(80)90394-2
Citations: PlumX Metrics

1976KA07      Phys.Rev. C13, 1759 (1976)

Y.Kawazoe, T.Tsukamoto

Calculation of Electroexcitation Cross Sections in ¹²C by a Continuum Shell Model

NUCLEAR REACTIONS ¹²C(e, e'), E=15-40 MeV; calculated σ. New method for solving coupled-channel wave functions, orthogonalized wave functions.

doi: 10.1103/PhysRevC.13.1759
Citations: PlumX Metrics

1974KA23      Progr.Theor.Phys. 51, 428 (1974)

Y.Kawazoe, T.Tsukamoto, H.Matsuzaki

Three-Alpha Particle Model for ¹²C Ground State

NUCLEAR STRUCTURE ¹²C; calculated form factor. 3-alpha model.

doi: 10.1143/PTP.51.428
Citations: PlumX Metrics

1963MO23      Suppl.Progr.Theoret.Phys. No.26, 64 (1963)

M.Morita, R.Morita, T.Tsukamoto, M.Yamada

Clebsch-Gordan Coefficients for j₂ = 5/2, 3 and 7/2