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NSR database version of April 11, 2024.

Search: Author = Y.Kawazoe

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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
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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
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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
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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
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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.

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
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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
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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
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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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