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NSR database version of April 11, 2024.

Search: Author = Y.Kawazoe

Found 25 matches.

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2006BA06      Phys.Rev. B 73, 045111 (2006)

M.S.Bahramy, M.H.F.Sluiter, Y.Kawazoe

First-principles calculations of hyperfine parameters with the all-electron mixed-basis method

NUCLEAR MOMENTS 7Li, 23Na, 25Mg, 39K, 43Ca, 63Cu, 87Sr, 107Ag; calculated hyperfine parameters. Density functional theory, mixed-basis method.

doi: 10.1103/PhysRevB.73.045111
Citations: PlumX Metrics

1997PA46      Phys.Rev.Lett. 78, 4063 (1997)

K.Parlinski, Z.Q.Li, Y.Kawazoe

First-Principles Determination of the Soft Mode in Cubic ZrO2

doi: 10.1103/physrevlett.78.4063
Citations: PlumX Metrics

1988KA31      J.Phys.Soc.Jpn. 57, 2869 (1988)

Y.Kawazoe, H.Miyase, H.Tsubota, K.Namai, A.Nomura, H.Kawahara, A.Tanaka, T.Tamae, M.Sugawara

Out-of-Plane Measurement of the 65Cu(e, e'p0) Reaction in the Giant Resonance Region

NUCLEAR REACTIONS 65Cu(e, e'p), E=129 MeV; measured σ(Ep, θ(e'), θp). 65Cu deduced E2 component in GDR region.

doi: 10.1143/JPSJ.57.2869
Citations: PlumX Metrics

1988TA24      Nucl.Phys. A489, 381 (1988)

A.Tanaka, T.Hino, H.Kawahara, M.Nomura, T.Tamae, M.Sugawara, H.Tsubota, H.Miyase, Y.Kawazoe

The 40Ca(e, e'p0)39K Coincidence Cross Section in the Giant Dipole Resonance Region

NUCLEAR REACTIONS 40Ca(e, e'p), E=129 MeV; measured σ(θ, E(e'), θ(p), φ(p)); deduced longitudinal-transverse interference term. Coincidence techniques.

doi: 10.1016/0375-9474(88)90001-2
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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0462.

1987NI04      Z.Phys. A326, 435 (1987)

W.Nitsche, G.J.Wagner, K.T.Knopfle, P.Grabmayr, Y.Kawazoe

Nature of Continua in Inelastic α- and 6Li-Scattering at 26 MeV/A

NUCLEAR REACTIONS 28Si(α, α'γ), E=104 MeV; 28Si, 27Al(6Li, 6Li'γ), E=156 MeV; measured σ(θα', θγ), σ(Eγ, θγ, θα'), σ(Eγ, θγ, θ(6Li)), σ(Eα', θα', θγ), (particle)γ-coin, γ-multiplicity; deduced reaction mechanism. Ge(Li) detectors, telescopes.

1987TA25      Phys.Rev.Lett. 59, 2919 (1987)

T.Tamae, H.Kawahara, A.Tanaka, M.Nomura, K.Namai, M.Sugawara, Y.Kawazoe, H.Tsubota, H.Miyase

Out-of-Plane Measurement of the D(e, e'p) Coincidence Cross Section

NUCLEAR REACTIONS 2H(e, e'p), E=129 MeV; measured σ(E(e'), θ(e'), θp); deduced longitudinal-transverse, transverse-transverse interference term, longitudinal plus transverse σ.

doi: 10.1103/PhysRevLett.59.2919
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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
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1986KA15      Phys.Rev. C33, 1917 (1986)

Y.Kawazoe, H.Miyase, H.Tsubota, J.Yokokawa, M.Oyamada, Y.Torizuka

Electroexcitation of Giant Multipole Resonances in 63Cu

NUCLEAR REACTIONS 63Cu(e, e'), E=100, 140, 220 MeV; measured σ(E(e'), θ). 63Cu deduced levels, E2 resonance, parameters. Enriched target.

doi: 10.1103/PhysRevC.33.1917
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
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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
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1984KL10      Phys.Lett. 145B, 25 (1984)

R.Klein, Y.Kawazoe, P.Grabmayr, G.J.Wagner, J.Friedrich, N.Voegler

Electroexcitation of Giant Resonances in 58Ni

NUCLEAR REACTIONS 58Ni(e, e'), E=124, 180, 300 MeV; measured σ(E(e')), σ(θ) vs effective momentum transfer; deduced response functions. 58Ni deduced giant resonance excitation, B(λ), GDR, GQR strength distribution.

doi: 10.1016/0370-2693(84)90940-7
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1984OG01      Phys.Rev. C30, 1159 (1984)

S.Oguro, Y.Mizuno, T.Terasawa, Y.Torizuka, Y.Kawazoe, K.Arita

180° Electroexcitation of Isobaric Analog States in 40Ca

NUCLEAR REACTIONS 40Ca(e, e'), E=120 MeV; measured σ(E(e'), θ=180°). 40Ca deduced IAS level transverse form factors.

doi: 10.1103/PhysRevC.30.1159
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1983KL09      Nuovo Cim. 76A, 369 (1983)

R.Klein, P.Grabmayr, Y.Kawazoe, G.J.Wagner, J.Friedrich, N.Voegler

Distribution of Electric Multipole Strengths in 58Ni

NUCLEAR REACTIONS 58Ni(e, e'), E=124, 180 MeV; measured σ(E(e')), σ(θ). 58Ni levels deduced B(λ), EWSR strength. DWBA form factors, Tassie transition densities.

doi: 10.1007/BF02833733
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
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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
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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
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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
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1979ZI01      Phys.Rev. C19, 279 (1979)

P.D.Zimmerman, C.F.Williamson, Y.Kawazoe

Test of a Scaling Law for Quasi-Elastic Electron Scattering

NUCLEAR REACTIONS 40Ca(e, e'), E=200-500 MeV; measured σ(quasi-elastic); deduced momentum distribution, scaling law.

doi: 10.1103/PhysRevC.19.279
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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
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1975KA40      Progr.Theor.Phys. 54, 1394 (1975)

Y.Kawazoe, G.Takeda, H.Matsuzaki

Quasielastic Electron Scattering from Nuclei

NUCLEAR REACTIONS 12C, 40Ca(e, e'p), E=500 MeV; calculated σ.

doi: 10.1143/PTP.54.1394
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1975TO02      Phys.Rev. C11, 1174 (1975)

Y.Torizuka, K.Itoh, Y.M.Shin, Y.Kawazoe, H.Matsuzaki, G.Takeda

Electroexcitation of Giant Multipole Resonances in 40Ca

NUCLEAR REACTIONS 40Ca(e, e'), E=300 MeV; measured σ(Ee', θ). 40Ca resonances deduced form factors.

doi: 10.1103/PhysRevC.11.1174
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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
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1973HO05      Phys.Rev.Lett. 30, 388 (1973)

K.Hosoyama, Y.Torizuka, Y.Kawazoe, H.Ui

Transition Charge Densities of the 21+ and 22+ States in 106Pd and 114Cd

NUCLEAR REACTIONS 106Pd, 114Cd(e, e'), E=183, 250 MeV; measured σ(θ). 106Pd, 114Cd deduced B(E2), quadrupole moment.

doi: 10.1103/PhysRevLett.30.388
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