NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = Y.Kawazoe Found 25 matches. 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
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
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
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
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
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
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
1986KA01 Phys.Rev. C33, 275 (1986) 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
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
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
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
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
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
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
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
1982TS01 Phys.Rev. C25, 1272 (1982) 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
1981KA12 Phys.Rev. C23, 2364 (1981) 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
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
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
1976KA07 Phys.Rev. C13, 1759 (1976) 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
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
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
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
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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