NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = S.Yoshida Found 86 matches. 2023KO15 Nature(London) 620, 965 (2023) Y.Kondo, N.L.Achouri, H.Al Falou, L.Atar, T.Aumann, H.Baba, K.Boretzky, C.Caesar, D.Calvet, H.Chae, N.Chiga, A.Corsi, F.Delaunay, A.Delbart, Q.Deshayes, Zs.Dombradi, C.A.Douma, A.Ekstrom, Z.Elekes, C.Forssen, I.Gasparic, J.-M.Gheller, J.Gibelin, A.Gillibert, G.Hagen, M.N.Harakeh, A.Hirayama, C.R.Hoffman, M.Holl, A.Horvat, A.Horvath, J.W.Hwang, T.Isobe, W.G.Jiang, J.Kahlbow, N.Kalantar-Nayestanaki, S.Kawase, S.Kim, K.Kisamori, T.Kobayashi, D.Korper, S.Koyama, I.Kuti, V.Lapoux, S.Lindberg, F.M.Marques, S.Masuoka, J.Mayer, K.Miki, T.Murakami, M.Najafi, T.Nakamura, K.Nakano, N.Nakatsuka, T.Nilsson, A.Obertelli, K.Ogata, F.de Oliveira Santos, N.A.Orr, H.Otsu, T.Otsuka, T.Ozaki, V.Panin, T.Papenbrock, S.Paschalis, A.Revel, D.Rossi, A.T.Saito, T.Y.Saito, M.Sasano, H.Sato, Y.Satou, H.Scheit, F.Schindler, P.Schrock, M.Shikata, N.Shimizu, Y.Shimizu, H.Simon, D.Sohler, O.Sorlin, L.Stuhl, Z.H.Sun, S.Takeuchi, M.Tanaka, M.Thoennessen, H.Tornqvist, Y.Togano, T.Tomai, J.Tscheuschner, J.Tsubota, N.Tsunoda, T.Uesaka, Y.Utsuno, I.Vernon, H.Wang, Z.Yang, M.Yasuda, K.Yoneda, S.Yoshida First observation of 28O NUCLEAR REACTIONS H(29F, X)27O/28O, E=235 MeV/nucleon; measured reaction products; deduced yields. The hydrogen target was surrounded by the MINOS Time Projection Chamber, SAMURAI spectrometer, RIKEN RI Beam Factory. RADIOACTIVITY 28O(4n), 27O(3n); measured decay products, En, In; deduced decay energy spectra and schemes from the measured momenta using the invariant-mass technique, resonance parameters. Comparison with the large-scale shell-model calculations using the new chiral effective field theory (EEdf3) interaction.
doi: 10.1038/s41586-023-06352-6
2023YO03 Phys.Rev. C 108, 044303 (2023) IMSRG-Net: A machine-learning-based solver for the in-medium similarity renormalization group method
doi: 10.1103/PhysRevC.108.044303
2022SA22 Phys.Lett. B 829, 137072 (2022) H.Sagawa, S.Yoshida, T.Naito, T.Uesaka, J.Zenihiro, J.Tanaka, T.Suzuki Isovector density and isospin impurity in 40Ca NUCLEAR STRUCTURE 40Ca; calculated proton and neutron densities with modified occupation probabilities of orbits around the Fermi energy, isospin impurity; deduced isoscalar (IS) and isovector (IV) densities. Comparison with theoretical densities calculated by Skyrme Hatree-Fock (HF) models.
doi: 10.1016/j.physletb.2022.137072
2022TR03 Phys.Rev. C 106, 064314 (2022) V.Tripathi, S.Bhattacharya, E.Rubino, C.Benetti, J.F.Perello, S.L.Tabor, S.N.Liddick, P.C.Bender, M.P.Carpenter, J.J.Carroll, A.Chester, C.J.Chiara, K.Childers, B.R.Clark, B.P.Crider, J.T.Harke, B.Longfellow, R.S.Lubna, S.Luitel, T.H.Ogunbeku, A.L.Richard, S.Saha, N.Shimizu, O.A.Shehu, Y.Utsuno, R.Unz, Y.Xiao, S.Yoshida, Y.Zhu β- decay of exotic P and S isotopes with neutron number near 28 RADIOACTIVITY 42,43,44P, 44,46S(β-), (β-n) [from Be(48Ca, X), E=140 MeV/nucleon)]; 41S(β-) [from 42P(β-n]; measured Iβ, Eγ, Iγ, βγ-coin, (implant)γ-coin; deduced T1/2, logft, delayed neutron emission probabilities. 42P; deduced J, π of the ground state. 42,41S, 41Cl; deduced levels, J, π, transition intensities. The half-lives were extracted from the fitting of decay curves. Comparison to calculations performed with shell-model using SDPFSDG-MU interaction. Beta Counting System (BCS) - 40x40 DSSD as the implant and β detector, surrounded by a γ-array of 16 Clover detectors in close geometry (NSCL).
doi: 10.1103/PhysRevC.106.064314
2022YO06 Prog.Theor.Exp.Phys. 2022, 053D02 (2022) Constructing approximate shell-model wavefunctions by eigenvector continuation NUCLEAR STRUCTURE 24,25Mg, 28Si, 26Al, 46V, 47,48Ti; calculated level energies, J, π, yrast states, magnetic dipole moments with shell-model using a method called eigenvector continuation (EC).
doi: 10.1093/ptep/ptac057
2021II01 Nucl.Instrum.Methods Phys.Res. A986, 164727 (2021) T.Iida, K.Mizukoshi, T.Ohata, T.Uehara, T.Batpurev, K.Fushimi, R.Hazama, M.Ishikawa, H.Kakubata, K.Kanagawa, S.Katagiri, B.T.Khai, T.Kishimoto, X.Li, T.Maeda, K.Matsuoka, K.Morishita, M.Moser, K.Nakajima, M.Nomachi, I.Ogawa, M.Shokati, K.Suzuki, Y.Takemoto, Y.Takihira, Y.Tamagawa, K.Tetsuno, M.Tozawa, V.T.T.Trang, S.Umehara, S.Yoshida The energy calibration system for CANDLES using (n, γ) reaction NUCLEAR REACTIONS 28Si, 56Fe, 58Ni(n, γ), E<2.1 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies and intensities, calibration procedures.
doi: 10.1016/j.nima.2020.164727
2020TS03 Nature(London) 587, 66 (2020) N.Tsunoda, T.Otsuka, K.Takayanagi, N.Shimizu, T.Suzuki, Y.Utsuno, S.Yoshida, H.Ueno The impact of nuclear shape on the emergence of the neutron dripline NUCLEAR STRUCTURE 22,24,26,28,30,32,34,36Ne, 24,26,28,30,32,34,36,38,40,42Mg, 23,25,27,29,31,33,35,37Na, 19,21,23,25,27,29F; analyzed available data; calculated 2+ and 4+ energies using configuration interaction, ground-state energies, dripline, magic numbers, J, π and energy levels using nucleon-nucleon interactions, nuclear shapes. Comparison with ENSDF library, available data; deduced mechanism for the formation of the neutron dripline.
doi: 10.1038/s41586-020-2848-x
2020YO02 Phys.Rev. C 102, 024305 (2020) Nonparametric Bayesian approach to extrapolation problems in configuration interaction methods NUCLEAR STRUCTURE 6Li; calculated ground-state energies using an extrapolation method to very large model space for configuration interaction (CI)-type approach with constrained Gaussian processes.
doi: 10.1103/PhysRevC.102.024305
2020YO05 Phys.Rev. C 102, 064307 (2020) S.Yoshida, H.Sagawa, J.Zenihiro, T.Uesaka Trajectory in 2D plot of isoscalar and isovector densities of 48Ca and 208Pb, and symmetry energy NUCLEAR STRUCTURE 48Ca, 208Pb; calculated nuclear matter incompressibility, volume, slope, and second derivative terms of symmetry energy, proton and neutron rms radii, neutron skin thickness, proton and neutron densities, 2D plot of experimental isoscalar (IS) and isovector (IV) densities, asymmetric isospin term in the nuclear incompressibility. Skyrme and RMF mean-field models with several modern relativistic and nonrelativistic energy density functionals (EDFs). Comparison with experimental data.
doi: 10.1103/PhysRevC.102.064307
2019AB06 Phys.Rev. C 100, 014323 (2019) B.Abromeit, V.Tripathi, H.L.Crawford, S.N.Liddick, S.Yoshida, Y.Utsuno, P.C.Bender, B.P.Crider, R.Dungan, P.Fallon, K.Kravvaris, N.Larson, R.S.Lubna, T.Otsuka, C.J.Prokop, A.L.Richard, N.Shimizu, S.L.Tabor, A.Volya Β- decay of Tz = +11/2 isotopes 37Al and 39Si: Understanding Gamow-Teller strength distribution in neutron-rich nuclei RADIOACTIVITY 37Al, 37,39,40Si, 37,39P(β-)[from 9Be(48Ca, X), E=140 MeV/nucleon, followed by fragment separation using A1900 separator at NSCL-MSU]; 37Al, 39Si(β-n); measured β, Eγ, Iγ, βγ-coin, half-lives of decays of 37Al, 37Si and 39Si, %β-n for decays of 37Al and 39Si using β-counting system (BCS) at NSCL-MSU which consisted of silicon PIN detectors, segmented planar Ge double-sided strip detector (GeDSSD) for implants and β- detection, and an array of 16 segmented Ge detectors for γ rays. 36Si, 37Si, 37,39,40P, 37,39S; deduced levels, J, π, β feedings, logft, %β-n. Systematics of low-lying positive π states in 35,37,39P, and T1/2 in N=20-28 Si isotopes. Comparison with shell model calculations. NUCLEAR STRUCTURE 35,37,39P, 37,39S, 37Si; calculated levels, J, π, logft values. Shell model calculations using the SDPFSDG-MU interaction. Comparison with experimental data from the present experiment, and the evaluated data in the ENSDF database at NNDC.
doi: 10.1103/PhysRevC.100.014323
2019GA11 Phys.Rev.Lett. 122, 192501 (2019) A.Gando, Y.Gando, T.Hachiya, M.Ha Minh, S.Hayashida, Y.Honda, K.Hosokawa, H.Ikeda, K.Inoue, K.Ishidoshiro, Y.Kamei, K.Kamizawa, T.Kinoshita, M.Koga, S.Matsuda, T.Mitsui, K.Nakamura, A.Ono, N.Ota, S.Otsuka, H.Ozaki, Y.Shibukawa, I.Shimizu, Y.Shirahata, J.Shirai, T.Sato, K.Soma, A.Suzuki, A.Takeuchi, K.Tamae, K.Ueshima, H.Watanabe, D.Chernyak, A.Kozlov, S.Obara, S.Yoshida, Y.Takemoto, S.Umehara, K.Fushimi, S.Hirata, B.E.Berger, B.K.Fujikawa, J.G.Learned, J.Maricic, L.A.Winslow, Y.Efremenko, H.J.Karwowski, D.M.Markoff, W.Tornow, T.O'Donnell, J.A.Detwiler, S.Enomoto, M.P.Decowski, J.Menendez, R.Dvornicky, F.Simkovic Precision Analysis of the 136Xe Two-Neutrino ββ Spectrum in KamLAND-Zen and Its Impact on the Quenching of Nuclear Matrix Elements RADIOACTIVITY 136Xe(2β-); measured decay products, Eβ, Iβ; deduced nuclear matrix elements.
doi: 10.1103/PhysRevLett.122.192501
2018AD01 Phys.Rev. C 97, 014601 (2018) S.Adachi, T.Kawabata, K.Minomo, T.Kadoya, N.Yokota, H.Akimune, T.Baba, H.Fujimura, M.Fujiwara, Y.Funaki, T.Furuno, T.Hashimoto, K.Hatanaka, K.Inaba, Y.Ishii, M.Itoh, C.Iwamoto, K.Kawase, Y.Maeda, H.Matsubara, Y.Matsuda, H.Matsuno, T.Morimoto, H.Morita, M.Murata, T.Nanamura, I.Ou, S.Sakaguchi, Y.Sasamoto, R.Sawada, Y.Shimizu, K.Suda, A.Tamii, Y.Tameshige, M.Tsumura, M.Uchida, T.Uesaka, H.P.Yoshida, S.Yoshida Systematic analysis of inelastic α scattering off self-conjugate A=4n nuclei NUCLEAR REACTIONS 12C, 16O, 20Ne, 24Mg, 28Si, 40Ca(α, α), (α, α'), E=130, 386 MeV; measured Eα, Iα, elastic and inelastic σ(θ, E) using Grand Raiden (GR) magnetic spectrometer with two multiwire drift chambers and two plastic scintillation counters at the AVF cyclotron of Research Center of Nuclear Physics (RCNP), Osaka University. 12C, 16O, 20Ne, 24Mg, 28Si, 40Ca; deduced levels, J, π, L transfers, EWSR strengths of the isoscalar dipole transitions. DWBA and coupled-channel (CC) analysis of σ(θ) distributions with the density-independent (DI) and density-dependent (DD) α-nucleus interactions.
doi: 10.1103/PhysRevC.97.014601
2018DI12 Phys.Rev. A 98, 042505 (2018) R.Ding, J.D.Whalen, S.K.Kanungo, T.C.Killian, F.B.Dunning, S.Yoshida, J.Burgdorfer Spectroscopy of 87Sr triplet Rydberg states ATOMIC PHYSICS 87Sr; measured frequencies; deduced level energies, quantum defects. Comparison with theoretical calculations.
doi: 10.1103/PhysRevA.98.042505
2018YO06 Phys.Rev. C 97, 054321 (2018); Erratum Phys.Rev. C 109, 029904 (2024) S.Yoshida, Y.Utsuno, N.Shimizu, T.Otsuka Systematic shell-model study of β-decay properties and Gamow-Teller strength distributions in A ≈ 40 neutron-rich nuclei RADIOACTIVITY 39,40S, 40P, 41Cl(β-); calculated logft values and compared with experimental data. 35,36,37,38,39,40,41,42,43,44,45,46,47Al, 36,37,38,39,40,41,42,43,44,45,46,47,48Si, 37,38,39,40,41,42,43,44,45,46,47,48,49P, 38,39,40,41,42,43,44,45,46,47,48,49,50S, 39,40,41,42,43,44,45,46,47,48,49,50,51Cl, 40,41,42,43,44,45,46,47,48,49,50,51,52Ar(β-)(β-n); calculated β-decay T1/2, β-delayed neutron emission probabilities (Pn), Gamow-Teller (GT) strength distributions, and location of the Gamow-Teller giant resonances using large-scale shell-model with and without first-forbidden (FF) transitions included. Comparison with experimental values from the ENSDF database, and with other theoretical predictions.
doi: 10.1103/PhysRevC.97.054321
2018YO13 Phys.Rev. C 98, 061301 (2018) S.Yoshida, N.Shimizu, T.Togashi, T.Otsuka Uncertainty quantification in the nuclear shell model NUCLEAR STRUCTURE 12,14C; calculated levels, J, π, isotopic spin using shell model and 0p-shell space on top of the 4He core as the model space. Proposed a new method to quantify uncertainties in theoretical values using Laplace approximation (LA) in shell-model calculations. Comparison with experimental values taken from the ENSDF database.
doi: 10.1103/PhysRevC.98.061301
2017GU24 Radiat.Phys.Chem. 140, 493 (2017) L.A.Gurgi, P.H.Regan, P.-A.Soderstrom, H.Watanabe, P.M.Walker, Zs.Podolyak, S.Nishimura, T.A.Berry, P.Doornenbal, G.Lorusso, T.Isobe, H.Baba, Z.Y.Xu, H.Sakurai, T.Sumikama, W.N.Catford, A.M.Bruce, F.Browne, G.J.Lane, F.G.Kondev, A.Odahara, J.Wu, H.L.Liu, F.R.Xu, Z.Korkulu, P.Lee, J.J.Liu, V.H.Phong, A.Yag, G.X.Zhang, T.Alharbi, R.J.Carroll, K.Y.Chae, Zs.Dombradi, A.Estrade, N.Fukuda, C.Griffin, E.Ideguchi, N.Inabe, H.Kanaoka, I.Kojouharov, T.Kubo, S.Kubono, N.Kurz, I.Kuti, S.Lalkovski, E.J.Lee, C.S.Lee, G.Lotay, C.-B.Moon, I.Nishizuka, C.R.Nita, Z.Patel, O.J.Roberts, H.Schaffner, C.M.Shand, H.Suzuki, H.Takeda, S.Terashima, Zs.Vajta, S.Yoshida, J.J.Valiente-Dobon Isomer spectroscopy of neutron-rich 168Tb103 NUCLEAR REACTIONS 9Be(238U, X)168Tb, E=350 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced γ-ray energies, J, π, isomeric state T1/2. Comparison with blocked BCS pairing Nilsson calculations for a well-deformed prolate shape, available data.
doi: 10.1016/j.radphyschem.2016.12.011
2017KA06 Phys.Rev.Lett. 118, 052701 (2017) T.Kawabata, Y.Fujikawa, T.Furuno, T.Goto, T.Hashimoto, M.Ichikawa, M.Itoh, N.Iwasa, Y.Kanada-Enyo, A.Koshikawa, S.Kubono, E.Miyawaki, M.Mizuno, K.Mizutani, T.Morimoto, M.Murata, T.Nanamura, S.Nishimura, S.Okamoto, Y.Sakaguchi, I.Sakata, A.Sakaue, R.Sawada, Y.Shikata, Y.Takahashi, D.Takechi, T.Takeda, C.Takimoto, M.Tsumura, K.Watanabe, S.Yoshida Time-Reversal Measurement of the p -Wave Cross Sections of the 7Be(n, α)4Fe Reaction for the Cosmological Li Problem NUCLEAR REACTIONS 4He(α, n), E=39.15, 38.76 MeV; measured reaction products, En, In, Eγ, Iγ; deduced σ(θ), σ. Comparison with available data.
doi: 10.1103/PhysRevLett.118.052701
2017TR02 Phys.Rev. C 95, 024308 (2017) V.Tripathi, R.S.Lubna, B.Abromeit, H.L.Crawford, S.N.Liddick, Y.Utsuno, P.C.Bender, B.P.Crider, R.Dungan, P.Fallon, K.Kravvaris, N.Larson, A.O.Macchiavelli, T.Otsuka, C.J.Prokop, A.L.Richard, N.Shimizu, S.L.Tabor, A.Volya, S.Yoshida β decay of 38, 40Si (Tz =+5, +6) to low-lying core excited states in odd-odd 38-40P isotopes RADIOACTIVITY 38,40Si(β-), (β-n)[from 9Be(48Ca, X), E=140 MeV/nucleon using A1900 separator at NSCL-MSU facility]; measured Eγ, Iγ, Eβ, γγ-coin, β-correlated γ spectra, half-lives and delayed-neutron probabilities (Pn) of decays of 38Si and 40Si using planar germanium double-sided strip detector (GeDSSD) and SeGA array. 38,40P; deduced levels, J, π, β feedings log ft values. Comparison with known experimental level schemes of 34 and 36P, and with shell model calculations using SDPF-MU interaction. 36,38,40Si(β-); calculated half-lives and log ft values of decays of Si isotopes, beta-delayed neutron probabilities (Pn) using shell model, and compared with experimental values. NUCLEAR STRUCTURE 34,36,38,40P; calculated levels, J, π, proton and neutron occupancies for the ground state and the three excited 1+ states, Gamow-Teller matrix elements for the 1+ states. Shell model calculations with SDPF-MU interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.95.024308
2017WU04 Phys.Rev.Lett. 118, 072701 (2017) J.Wu, S.Nishimura, G.Lorusso, P.Moller, E.Ideguchi, P.-H.Regan, G.S.Simpson, P.-A.Soderstrom, P.M.Walker, H.Watanabe, Z.Y.Xu, H.Baba, F.Browne, R.Daido, P.Doornenbal, Y.F.Fang, G.Gey, T.Isobe, P.S.Lee, J.J.Liu, Z.Li, Z.Korkulu, Z.Patel, V.Phong, S.Rice, H.Sakurai, L.Sinclair, T.Sumikama, M.Tanaka, A.Yagi, Y.L.Ye, R.Yokoyama, G.X.Zhang, T.Alharbi, N.Aoi, F.L.Bello Garrote, G.Benzoni, A.M.Bruce, R.J.Carroll, K.Y.Chae, Z.Dombradi, A.Estrade, A.Gottardo, C.J.Griffin, H.Kanaoka, I.Kojouharov, F.G.Kondev, S.Kubono, N.Kurz, I.Kuti, S.Lalkovski, G.J.Lane, E.J.Lee, T.Lokotko, G.Lotay, C.-B.Moon, H.Nishibata, I.Nishizuka, C.R.Nita, A.Odahara, Zs.Podolyak, O.J.Roberts, H.Schaffner, C.Shand, J.Taprogge, S.Terashima, Z.Vajta, S.Yoshida 94 β-Decay Half-Lives of Neutron-Rich 55Cs to 67Ho: Experimental Feedback and Evaluation of the r-Process Rare-Earth Peak Formation RADIOACTIVITY 144,145,146,147,148,149,150,151Cs, 146,147,148,149,150,151,152,153,154Ba, 148,149,150,151,152,153,154,155,156La, 150,151,152,153,154,155,156,157,158Ce, 153,154,155,156,157,158,159,160Pr, 156,157,158,159,160,161,162Nd, 159,160,161,162,163Pm, 160,161,162,163,164,165,166Sm, 161,162,163,164,165,166,167,168Eu, 165,166,167,168,169,170Gd, 166,167,168,169,170,171,172Tb, 169,170,171,172,172m,173Dy, 172,173,174,175Ho, 174mEr(β-)[from Be(238U, X), E=345 MeV/nucleon]; measured and analyzed reaction products using BigRIPS separator and ZeroDegree Spectrometer (ZDS), γ rays, half-lives by (implant)β correlations using WAS3ABi and EURICA detection systems at RIBF-RIKEN facility; deduced Gamow-Teller strength functions, r-process abundance pattern in the solar system. Comparison with previous experimental half-lives, and with three theoretical calculations using FRDM+QRPA, KTUY+GT2, and RHB+pn-RQRPA models. Numerical values of half-lives listed in supplementary file.
doi: 10.1103/PhysRevLett.118.072701
2016AS01 Nucl.Phys. A946, 171 (2016) K.Asakura, A.Gando, Y.Gando, T.Hachiya, S.Hayashida, H.Ikeda, K.Inoue, K.Ishidoshiro, T.Ishikawa, S.Ishio, M.Koga, S.Matsuda, T.Mitsui, D.Motoki, K.Nakamura, S.Obara, M.Otani, T.Oura, I.Shimizu, Y.Shirahata, J.Shirai, A.Suzuki, H.Tachibana, K.Tamae, K.Ueshima, H.Watanabe, B.D.Xu, H.Yoshida, A.Kozlov, Y.Takemoto, S.Yoshida, K.Fushimi, T.I.Banks, B.E.Berger, B.K.Fujikawa, T.O'Donnell, L.A.Winslow, Y.Efremenko, H.J.Karwowski, D.M.Markoff, W.Tornow, J.A.Detwiler, S.Enomoto, M.P.Decowski Search for double-beta decay of 136Xe to excited states of 136Ba with the KamLAND-Zen experiment
doi: 10.1016/j.nuclphysa.2015.11.011
2016GA30 Phys.Rev.Lett. 117, 082503 (2016) A.Gando, Y.Gando, T.Hachiya, A.Hayashi, S.Hayashida, H.Iked a, K.Inoue, K.Ishidoshiro, Y.Karino, M.Koga, S.Matsuda, T.Mitsui, K.Nakamura, S.Obara, T.Oura, H.Ozaki, I.Shimizu, Y.Shirahata, J.Shirai, A.Suzuki, T.Takai, K.Tamae, Y.Teraoka, K.Ueshima, H.Watanabe, A.Kozlov, Y.Takemoto, S.Yoshida, K.Fushimi, T.I.Banks, B.E.Berger, B.K.Fujikawa, T.O'Donnell, L.A.Winslow, Y.Efremenko, H.J.Karwowski, D.M.Markoff, W.Tornow, J.A.Detwiler, S.Enomoto, M.P.Decowski Search for Majorana Neutrinos Near the Inverted Mass Hierarchy Region with KamLAND-Zen RADIOACTIVITY 136Xe(2β-); measured decay products, Eγ, Iγ, Eβ, Iβ; deduced neutrinoless decay T1/2 limit. Comparison with available data.
doi: 10.1103/PhysRevLett.117.082503
2012MO01 Phys.Rev.Lett. 108, 052501 (2012) P.Moller, W.D.Myers, H.Sagawa, S.Yoshida New Finite-Range Droplet Mass Model and Equation-of-State Parameters NUCLEAR STRUCTURE Z=1-120, A=1-160; calculated masses, symmetry parameters, using finite-range droplet model (FRDM); deduced more accurate FRDM-2011 parameters and constants. Comparison with atomic mass evaluation 2003.
doi: 10.1103/PhysRevLett.108.052501
2012OG07 J.Phys.:Conf.Ser. 375, 042018 (2012) I.Ogawa, T.Kishimoto, S.Umehara, G.Ito, K.Yasuda, H.Kakubata, M.Miyashita, K.Takubo, K.Matsuoka, M.Nomachi, M.Saka, K.Seki, K.Fushimi, R.Hazama, H.Ohsumi, K.Okada, Y.Tamagawa, T.Jinno, N.Fujiwara, S.Yoshida, for the CANDLES Collaboration Study of 48Ca double beta decay by CANDLES
doi: 10.1088/1742-6596/375/1/042018
2009MU11 Nucl.Technology 168, 373 (2009) I.Murata, H.Miyamaru, I.Kato, S.Yoshida, Y.Mori A New Low-Energy Neutron Spectrometer Based on Position-Sensitive Proportional Counter for Accelerator-Based Neutron Source
doi: 10.13182/NT09-A9212
2008UM05 Phys.Rev. C 78, 058501 (2008) S.Umehara, T.Kishimoto, I.Ogawa, R.Hazama, H.Miyawaki, S.Yoshida, K.Matsuoka, K.Kishimoto, A.Katsuki, H.Sakai, D.Yokoyama, K.Mukaida, S.Tomii, Y.Tatewaki, T.Kobayashi, A.Yanagisawa Neutrino-less double-β decay of 48Ca studied by CaF2(Eu) scintillators RADIOACTIVITY 48Ca(2β); measured half-life for neutrinoless double-beta decay.
doi: 10.1103/PhysRevC.78.058501
2008YO03 Phys.Rev. C 77, 054308 (2008) Pairing correlations and effective mass NUCLEAR STRUCTURE 124,136Sn; calculated dependence of average neutron pairing gap energy on effective mass, surface and volume pairing potentials. Skyrme interactions and relativistic Lagrangians used in calculations.
doi: 10.1103/PhysRevC.77.054308
2007GR20 Nucl.Phys. A788, 337c (2007) M.Grasso, S.Yoshida, N.Sandulescu, N.Van Giai Giant halo and anti-halo in the non-relativistic mean field approach NUCLEAR STRUCTURE Zr; calculated radii, two-neutron separation energies, halo features. Non-relativistic mean field approach.
doi: 10.1016/j.nuclphysa.2007.01.063
2007SA40 Phys.Rev. C 76, 024301 (2007) H.Sagawa, S.Yoshida, X.-R.Zhou, K.Yako, H.Sakai Charge exchange spin-dipole excitations in 90Zr and 208Pb and the neutron matter equation of state NUCLEAR REACTIONS 90Zr(n, p), 90Zr, 208Pb(p, n), E*<70 MeV; calculated spin dipole strength distributions using Skyrme Hartree Fock plus random phase approximation.
doi: 10.1103/PhysRevC.76.024301
2007SA46 Phys.Rev. C 76, 034327 (2007); Erratum Phys.Rev. C 77, 049902 (2008) H.Sagawa, S.Yoshida, G.-M.Zeng, J.-Z.Gu, X.-Z.Zhang Isospin dependence of incompressibility in relativistic and nonrelativistic mean field calculations NUCLEAR STRUCTURE 112,114,116,118,120,122,124Sn, 208Pb; calculated isoscalar giant monopole resonance strength distributions using Skyrme-HF and relativistic mean field models.
doi: 10.1103/PhysRevC.76.034327
2007SA65 Eur.Phys.J. Special Topics 150, 215 (2007) Isoscalar and isovector nuclear matter properties and neutron skin thickness
doi: 10.1140/epjst/e2007-00307-4
2007YA12 Nucl.Phys. A788, 273c (2007) K.Yako, H.Sakai, S.Yoshida, H.Sagawa Charge Exchange Spin-Dipole Excitations of 90Zr and the Neutron Skin Thickness NUCLEAR REACTIONS 90Zr(p, n), (n, p), E=300 MeV; analyzed excitation energy spectra; deduced spin dipole strength distributions using multipole decomposition analysis. 90Zr deduced radii.
doi: 10.1016/j.nuclphysa.2007.01.013
2007YO03 Phys.Atomic Nuclei 70, 1357 (2007) Neutron skin thickness and nuclear matter properties
doi: 10.1134/S1063778807080066
2006GR27 Phys.Rev.C 74, 064317 (2006) M.Grasso, S.Yoshida, N.Sandulescu, N.Van Giai Giant neutron halos in the non-relativistic mean field approach NUCLEAR STRUCTURE 56,58,60,62,64,66,68,70,72Ca, 116,118,120,122,124,126,128,130,132,134,136,138,140Zr; calculated radii, two-neutron separation energies, halo features. Non-relativistic mean field approach.
doi: 10.1103/PhysRevC.74.064317
2006YO04 Phys.Rev. C 73, 044320 (2006) Isovector nuclear matter properties and neutron skin thickness NUCLEAR STRUCTURE 208Pb; analyzed neutron skin thickness, relation to neutron equation of state. Correlations between nuclear matter properties discussed.
doi: 10.1103/PhysRevC.73.044320
2005NO02 Nucl.Phys. B(Proc.Supp.) S138, 221 (2005) M.Nomachi, P.Doe, H.Ejiri, S.R.Elliott, J.Engel, M.Finger, J.A.Formaggio, K.Fushimi, V.Gehman, A.Gorin, M.Greenfield, R.Hazama, K.Ichihara, Y.Ikegami, H.Ishii, T.Itahashi, P.Kavitov, V.Kekelidze, K.Kuroda, V.Kutsalo, I.Manouilov, K.Matsuoka, H.Nakamura, T.Ogama, A.Para, K.Rielage, A.Rjazantsev, R.G.H.Robertson, Y.Shichijo, T.Shima, Y.Shimada, G.Shirkov, A.Sissakian, Y.Sugaya, A.Titov, V.Vatulin, O.E.Vilches, V.Voronov, J.F.Wilkerson, D.I.Will, S.Yoshida MOON (Mo Observatory Of Neutrinos) for double beta decay
doi: 10.1016/j.nuclphysbps.2004.11.053
2005YO01 Nucl.Phys. B(Proc.Supp.) S138, 214 (2005) S.Yoshida, T.Kishimoto, I.Ogawa, R.Hazama, S.Umehara, K.Matsuoka, D.Yokoyama, K.Mukaida, K.Ichihara, Y.Tatewaki CANDLES project for double beta decay of 48Ca
doi: 10.1016/j.nuclphysbps.2004.11.051
2004KU04 Phys.Rev. C 69, 015802 (2004) N.Kudomi, M.Komori, K.Takahisa, S.Yoshida, K.Kume, H.Ohsumi, T.Itahashi Precise measurement of the cross section of 3He(3He, 2p)4He by using 3He doubly charged beam NUCLEAR REACTIONS 3He(3He, 2p), E(cm)=30-50 keV; measured particle spectra, σ; deduced astrophysical S-factor. 2H(3He, p), E=90 keV; measured particle spectra.
doi: 10.1103/PhysRevC.69.015802
2004YO01 Phys.Rev. C 69, 024318 (2004) Neutron skin thickness and equation of state in asymmetric nuclear matter NUCLEAR STRUCTURE 100,132Sn, 182,208Pb; calculated relative binding energies, neutron skin thicknesses, dependence on equation of state. Skyrme Hartree-Fock and relativistic mean-field models.
doi: 10.1103/PhysRevC.69.024318
2003DO13 Nucl.Phys. A721, 517c (2003) P.Doe, H.Ejiri, S.R.Elliott, J.Engel, M.Finger, K.Fushimi, V.Gehman, A.Gorine, M.Greenfield, R.Hazama, K.Ichihara, T.Itahashi, P.Kavitov, V.Kekelidze, K.Kuroda, V.Kutsalo, K.Matsuoka, I.Manouilov, M.Nomachi, A.Para, A.Rjazantsev, R.G.H.Robertson, Y.Shichijo, L.C.Stonehill, T.Shima, G.Shirkov, A.Sissakian, Y.Sugaya, A.Titov, V.Vatulin, V.Voronov, O.E.Vilches, J.F.Wilkerson, D.I.Will, S.Yoshida Neutrino Studies in 100Mo and MOON - Mo Observatory of Neutrinos -
doi: 10.1016/S0375-9474(03)01113-8
2003IT04 Nucl.Phys. A718, 466c (2003) T.Itahashi, M.Komori, N.Kudomi, K.Kume, Y.Nagai, M.Ohsumi, K.Takahisa, H.Toki, H.Ejiri, H.Ueda, S.Yoshida Cross section of 3He(3He, 2p)4He measured near the Gamow energy NUCLEAR REACTIONS 3He(3He, 2p), E(cm)=31.2-45.3 keV; measured σ; deduced astrophysical S-factors.
doi: 10.1016/S0375-9474(03)00853-4
2003IT08 Nucl.Phys. A721, 1015c (2003) T.Itahashi, N.Kudomi, S.Yoshida, K.Kume, M.Komori, H.Ohsumi Cross section of 3He(3He, 2p)4He measured near the Gamow peak NUCLEAR REACTIONS 3He(3He, 2p), E(cm)=30-50 keV; measured reaction rate; deduced astrophysical S-factor.
doi: 10.1016/S0375-9474(03)01274-0
2003OG05 Nucl.Phys. A721, 525c (2003) I.Ogawa, R.Hazama, S.Ajimura, K.Matsuoka, N.Kudomi, K.Kume, H.Ohsumi, K.Fushimi, N.Suzuki, T.Nitta, H.miyawaki, S.Shiomi, Y.Tanaka, Y.Ishikawa, M.Itamura, K.Kishimoto, A.Katsuki, H.Sakai, D.Yokoyama, S.Umehara, S.Tomii, K.Mukaida, S.Yoshida, H.Ejiri, T.Kishimoto Double beta decay study of 48Ca by CaF2 scintillator RADIOACTIVITY 48Ca(2β-); measured 0ν-accompanied 2β decay T1/2 lower limit.
doi: 10.1016/S0375-9474(03)01115-1
2003YO09 Nucl.Phys. A721, 1056c (2003) S.Yoshida, H.Ejiri, K.Fushimi, K.Hayashi, T.Kishimoto, N.Kudomi, K.Kume, H.Kuramoto, K.Matsuoka, H.Ohsumi, K.Takahisa, Y.Tsujimoto, S.Umehara Search for WIMPs with NaI(Tl) Detectors at Oto Cosmo Observatory
doi: 10.1016/S0375-9474(03)01284-3
2002EJ05 Nucl.Phys. B(Proc.Supp.) S110, 375 (2002) H.Ejiri, J.Engel, K.Fushimi, K.Hayashi, R.Hazama, T.Kishimoto, P.Krastev, N.Kudomi, K.Kume, H.Kuramoto, K.Matsuoka, R.G.H.Robertson, K.Takahisa, S.Yoshida Double Beta Decays of 100Mo and Molybdenum Observatory of Neutrinos RADIOACTIVITY 100Mo(2β-); measured β-spectra, 2ν-accompanied 2β-decay T1/2, 0ν-accompanied 2β-decay T1/2 lower limit.
doi: 10.1016/S0920-5632(02)01514-1
2002FU05 Phys.Lett. 531B, 190 (2002) K.Fushimi, N.Kudomi, S.Yoshida, H.Ejiri, K.Hayashi, T.Kishimoto, K.Kume, H.Kuramoto, K.Matsuoka, H.Ohsumi, K.Takahisa Limits on Majoron Emitting Neutrinoless Double-Beta Decay of 100Mo RADIOACTIVITY 100Mo(2β-); measured 0ν-accompanied 2β-decay T1/2 lower limit; deduced coupling constant.
doi: 10.1016/S0370-2693(02)01484-3
2001EJ03 Phys.Rev. C63, 065501 (2001) H.Ejiri, K.Fushimi, K.Hayashi, T.Kishimoto, N.Kudomi, K.Kume, H.Kuramoto, K.Matsuoka, H.Ohsumi, K.Takahisa, S.Yoshida Limits on the Majorana Neutrino Mass and Right-Handed Weak Currents by Neutrinoless Double β Decay of 100Mo RADIOACTIVITY 100Mo(2β-); measured neutrinoless 2β decay T1/2 lower limits; deduced neutrino mass limits.
doi: 10.1103/PhysRevC.63.065501
2001KA43 Phys.Rev. C64, 024603 (2001) Interference Effect in the Scattering Amplitudes for Nucleon-Induced Two-Step Direct Process using the Sudden Approximation NUCLEAR REACTIONS 208Pb(p, p'), E=30 MeV; calculated σ(E, θ) for two-step direct process. Sudden approximation.
doi: 10.1103/PhysRevC.64.024603
2001SA22 Nucl.Phys. A688, 755 (2001) New Spin-Orbit Parameters of Skyrme Interactions NUCLEAR STRUCTURE 16O, 208Pb; calculated single-particle energies. 16O, 40,48Ca, 208Pb; calculated radii. 48Sc, 90Nb, 208Bi; calculated Gamow-Teller states energies. 188,190,192,194,196,198,200,202,204,206,208,210,212,214,216Pb; calculated isotope shifts. Spin-orbit potentials of Skyrme interactions. Comparisons with data.
doi: 10.1016/S0375-9474(00)00594-7
2000KU21 Nucl.Phys. B(Proc.Supp.) S87, 301 (2000) N.Kudomi, H.Ejiri, K.Fushimi, K.Hayashi, R.Hazama, T.Kishimoto, K.Kume, H.Kuramoto, T.Matsuoka, H.Ohsumi, K.Takahisa, Y.Tsujimoto, S.Yoshida Double Beta Decay of 100Mo by ELEGANT V at Oto Cosmo Observatory RADIOACTIVITY 100Mo(2β-); measured 0ν-accompanied 2β-decay T1/2 lower limit; deduced neutrino mass limits.
doi: 10.1016/S0920-5632(00)00686-1
1999YO06 Nucl.Phys. A658, 3 (1999) Spin-Orbit Interactions in Mean Field Theories NUCLEAR STRUCTURE 72Kr; calculated spin-orbit potential, single-particle levels. Comparison of Skyrme Hartree-Fock, relativistic mean field models.
doi: 10.1016/S0375-9474(99)00336-X
1998YO10 Phys.Rev. C58, 2796 (1998) S.Yoshida, H.Sagawa, N.Takigawa Incompressibility and Density Distributions in Asymmetric Nuclear Systems NUCLEAR STRUCTURE 100,104,108,112,116,120,124,128,132,136,140,150,160Sn; calculated neutron, charge, matter radii, density distributions; deduced correlation between surface diffuseness, incompressibility.
doi: 10.1103/PhysRevC.58.2796
1997YO04 Phys.Rev. C55, 1255 (1997) Shape Dependence of Pairing Gap Energies and the Structure of Hg and Pb Isotopes NUCLEAR STRUCTURE 194Hg; calculated energy surface, neutron, proton gap parameters, proton single particle levels. 180,182,184,186,188Hg; calculated charge radius isotope dependence, oblate, prolate states intrinsic energies. 190,192,194,196,198Hg; calculated charge radius isotope dependence. 190,192,194,196,198,200,202,204,206,208,210,212,214Pb; calculated scaled isotope shifts. Deformed relativistic mean field theory with pairing interactions in BCS theory.
doi: 10.1103/PhysRevC.55.1255
1996TA01 Phys.Rev. C53, 1038 (1996) N.Takigawa, S.Yoshida, K.Hagino, S.K.Patra, C.R.Praharaj Reply to ' Comment on ' Shape and Superdeformed Structure in Hg Isotopes in Relativistic Mean Field Model ' and ' Structure of Neutron-Deficient Pt, Hg, and Pb Isotopes ' ' NUCLEAR STRUCTURE 176,178,180,182,184,186,188,190,192,194,196,198,200Hg; analyzed predicted binding energy per particle, rms charge radii. 170,172,174Hg, 192,194,196,198,200,202,204,206,208Pb; analyzed predicted rms charge radii; deduced sensitivity to model parameters. Relativistic mean field theory.
doi: 10.1103/PhysRevC.53.1038
1996YO11 Prog.Theor.Phys.(Kyoto), Suppl. 124, 131 (1996) S.Yoshida, S.K.Patra, N.Takigawa Multi-Neutron and Proton Transfer Reactions in Deep Inelastic Heavy-Ion Collisions NUCLEAR REACTIONS 165Ho(56Fe, X), E=465 MeV; calculated projectile-like-fragment mass to charge ratio vs energy loss, multinucleon transfer related features. Comparison with data. Fokker-Planck equation.
doi: 10.1143/PTPS.124.131
1995AB15 Phys.Rev. C52, 837 (1995) Imaginary Part of the Optical Potential for Finite Temperature and for Preequilibrium Processes NUCLEAR REACTIONS 208Pb(n, n), E not given; calculated imaginary potential, temperature dependence. Many-particle, many-hole states.
doi: 10.1103/PhysRevC.52.837
1995PA06 Phys.Rev. C51, 2248 (1995) S.K.Patra, S.Yoshida, N.Takigawa, C.R.Praharaj, A.K.Rath Hexadecapole Shape Change in Ytterbium Isotopes NUCLEAR STRUCTURE 160,162,164,166,168,170,172,174,176,178,180,182,184,186,188,190Yb; calculated binding energy, quadrupole deformation parameter, hexadecapole moments. Relativistic mean field model. 158,160,162,164,166,168,170,172,174,176,178,180,182,184Yb; calculated Hartree-Fock energy, quadrupole, hexadecapole moments. Hartree-Fock calculations, nonrelativistic, relativistic models.
doi: 10.1103/PhysRevC.51.2248
1995SA13 Phys.Lett. 341B, 257 (1995) Spreading Widths of Nucleons in the Semiclassical Approximation NUCLEAR STRUCTURE 208Pb; calculated nucleon spreading widths. Semi-classical approximation.
doi: 10.1016/0370-2693(94)01373-K
1995TA15 Nucl.Phys. A588, 91c (1995) N.Takigawa, S.Yoshida, K.Hagino, S.K.Patra Multi-Nucleon Transfer Reactions and Fusion with Unstable Nuclei NUCLEAR REACTIONS 58Ni(118Cs, X), (133Cs, X), (148Cs, X), E not given; calculated transferred nucleon number vs energy loss due to relative motion. 11Li(9Li, X), E(cm)=0.5-2.5 MeV; calculated fusion σ(E). Transport theory plus friction model. NUCLEAR STRUCTURE 113,133,148,181Cs, 53,58,63,68Ni; calculated neutron, proton separation energies. Mass formula.
doi: 10.1016/0375-9474(95)00105-A
1995YO01 Phys.Rev. C52, 157 (1995) S.Yoshida, S.K.Patra, N.Takigawa, C.R.Praharaj Surface Properties of Cs Isotopes NUCLEAR STRUCTURE 133,148,181Cs; calculated neutron, proton density distributions. Other aspects, other isotopes studies. 40,48Ca, 58,64Ni, 90Zr, 116Sn, 140Ce, 208Pb; calculated neutron, proton distributions rms radii. Deformed relativistic mean field, spherical nonrelativistic Hartree-Fock theories.
doi: 10.1103/PhysRevC.52.157
1994PA29 Phys.Rev. C50, 1924 (1994) S.K.Patra, S.Yoshida, N.Takigawa, C.R.Praharaj Shape and Superdeformed Structure in Hg Isotopes in Relativistic Mean Field Model NUCLEAR STRUCTURE 170,172,174,176,178,180,182,184,186,188,190,192,194,196,198,200Hg; calculated binding energy, quadrupole deformation parameter, hexadecupole moment, charge, rms radii. Relativistic mean field theory.
doi: 10.1103/PhysRevC.50.1924
1994SA05 Phys.Rev. C49, 1099 (1994) Imaginary Part of the Optical Potential for Preequilibrium Processes NUCLEAR STRUCTURE 93Nb; calculated particle, hole, particle-hole state densities. 40Ca, 208Pb, 93Nb; calculated preequilibrium reaction related optical potential imaginary part. Semi-classical approximation, delta function interaction, microscopic approach.
doi: 10.1103/PhysRevC.49.1099
1994YO05 Phys.Rev. C50, 1398 (1994) S.Yoshida, S.K.Patra, N.Takigawa, C.R.Praharaj Structure of Neutron-Deficient Pt, Hg, and Pb Isotopes NUCLEAR STRUCTURE 176,178,180Pt, 180,182,184Hg, 178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208Pb; calculated binding energy, quadrupole deformation parameter, hexadecapole moment, single particle spectra in some cases. Relativistic mean field formalism.
doi: 10.1103/PhysRevC.50.1398
1991SA13 Z.Phys. A339, 129 (1991) K.Sato, Y.Takahashi, S.Yoshida Exciton Level Densities with Spin and Parity Based on Random Matrix Model NUCLEAR STRUCTURE 40Ca, 208Pb; calculated level densities, exciton number. Random matrix model, Woods-Saxon potential.
doi: 10.1007/BF01282942
1989SA12 Z.Phys. A333, 141 (1989) Average Partial Level Density Based on the Random Matrix Model Inclusion of Realistic One-Body Spectrum and Effect of Particle Escape NUCLEAR STRUCTURE 208Pb; calculated partial level densities. Random matrix model.
1988SA22 Z.Phys. A330, 265 (1988) Studies of Nuclear Second Moments for Pre-Equilibrium Nuclear Reaction Theories - Extension to Finite-Range Residual Interaction NUCLEAR STRUCTURE 208Pb, 40Ca; calculated second moments, level densities.
1987AD01 Nucl.Phys. A462, 61 (1987) Widths of the Isobaric Analog State of 208Pb NUCLEAR STRUCTURE 208Pb; calculated IAR escape, spreading widths. Skyrme interaction.
doi: 10.1016/0375-9474(87)90379-4
1987SA30 Z.Phys. A327, 421 (1987) Studies of Nuclear Second Moments for Pre-Equilibrium Nuclear Reaction Theories NUCLEAR STRUCTURE 40Ca, 208Pb; calculated single particle orbits, binding energies, moment matrix elements, eigen values, level densities. Preequilibrium theories.
1986NI11 Ann.Phys.(New York) 172, 67 (1986) H.Nishioka, J.J.M.Verbaarschot, H.A.Weidenmuller, S.Yoshida Statistical Theory of Precompound Reactions: The Multistep Compound Process
doi: 10.1016/0003-4916(86)90020-5
1986YO07 Nucl.Phys. A457, 84 (1986) Test of the Q-Space Approximation in Nuclear Response Theory NUCLEAR STRUCTURE 40Ca, 208Pb; calculated electric monopole state, response function. TDA, Q-space approximation.
doi: 10.1016/0375-9474(86)90520-8
1982YO05 Z.Phys. A308, 133 (1982) Pre-Equilibrium Effect in Heavy Ion Induced Fusion NUCLEAR REACTIONS, ICPND 58Ni(40Ca, xnypzα)93Tc/94Ru/95Rh/96Pd/97Ag, E=50-70 MeV; calculated residuals excitation energy, residual yields, exciton number distribution time evolution. Multi-nucleon emission after fusion.
doi: 10.1007/BF01413003
1981IW03 Z.Phys. A302, 149 (1981) A.Iwamoto, K.Harada, S.Yamaji, S.Yoshida Microscopic Calculation of Friction Coefficients for use in Heavy-Ion Reaction NUCLEAR REACTIONS 196Pt(40Ar, X), E not given; calculated friction coefficient. Deep inelastic collision, linear response theory, two-center shell model.
doi: 10.1007/BF01413045
1981YA09 Phys.Lett. 106B, 433 (1981) S.Yamaji, A.Iwamoto, K.Harada, S.Yoshida Microscopic Calculation of the Mass Diffusion Coefficient using Linear Response Theory NUCLEAR REACTIONS 27Al(20Ne, X), E=120 MeV; 197Au(63Cu, X), E=365, 443 MeV; 209Bi(136Xe, X), E=1130 MeV; 165Ho, 209Bi(84Kr, X), E=714 MeV; 58Ni(16O, X), E=92 MeV; 50Ti(32S, X), E=131, 166 MeV; 197Au, 109Ag(40Ar, X), E=288 MeV; 197Au(40Ar, X), E=340 MeV; 232Th(40Ar, X), E=279, 388 MeV; 197Au(86Kr, X), E=620 MeV; calculated mass diffusion coefficient. Linear response theory.
doi: 10.1016/0370-2693(81)90250-1
1979SA10 Z.Phys. A290, 149 (1979) K.Sato, S.Yamaji, K.Harada, S.Yoshida A Numerical Analysis of the Heavy-Ion Reaction Based on the Linear Response Theory NUCLEAR REACTIONS 28Si(20Ne, X), E=120 MeV; calculated σ(θ). Linear response theory with collective variables, deformation δ, relative distance R, two-dimensional coupled equations of motion.
doi: 10.1007/BF01408109
1978AD02 Nucl.Phys. A306, 53 (1978) Calculation of Widths of Giant Monopole Resonances in 16O and 40Ca NUCLEAR STRUCTURE 16O, 40Ca; calculated monopole resonances.
doi: 10.1016/0375-9474(78)90311-1
1974AR04 Nucl.Phys. A219, 475 (1974) Analysis of α-Decay Widths of Light 4n Nuclei NUCLEAR STRUCTURE 12C, 16O, 20Ne; calculated α-widths.
doi: 10.1016/0375-9474(74)90113-4
1974BO28 Nucl.Phys. A228, 253 (1974) R.N.Boyd, R.Arking, J.C.Lombardi, A.B.Robbins, S.Yoshida, D.C.Slater, H.T.King, R.Avida Decay of the 7/2- Isobaric Analogue Resonance in 125Sb NUCLEAR REACTIONS 124Sn(p, p'), (polarized p, p'), E=10.0-10.9 MeV; measured σ(Ep', θ), A(Ep', θ). 125Sb deduced isobaric analog resonance, p-width.
doi: 10.1016/0375-9474(74)90431-X
1973SA25 Nucl.Phys. A211, 509 (1973) Charge Asymmetry in the Mass-13 Isobar NUCLEAR STRUCTURE 13C; calculated B(M1), log ft, charge asymmetry. 13N, 13C, 13B, 13O calculated binding energies.
doi: 10.1016/0375-9474(73)90440-5
1972AR12 Phys.Lett. 40B, 15 (1972) Alpha-Decay Widths of 20Ne NUCLEAR STRUCTURE 20Ne; calculated α-widths. Su(3) shell model wave functions in α-cluster form.
doi: 10.1016/0370-2693(72)90269-9
1972CO22 Phys.Rev.Lett. 29, 442 (1972) J.R.Comfort, W.J.Braithwaite, J.R.Duray, S.Yoshida Anomalous Two-Phonon (p, t) Transitions in Cadmium NUCLEAR REACTIONS 112,114,116Cd(p, t), E=27.9 MeV; measured σ(θ); deduced multistep mechanism, DWBA normalization factors. 110,112,114Cd transitions deduced L.
doi: 10.1103/PhysRevLett.29.442
1971AR03 Nucl.Phys. A161, 492 (1971) Charge Asymmetry of Nucleon Widths of the Lowest T = 3/2 States of 13N And 13C NUCLEAR STRUCTURE 13C, 13N; calculated isospin-forbidden nucleon widths. First-order perturbation theory, isospin mixing.
doi: 10.1016/0375-9474(71)90383-6
1971AR29 Phys.Rev.Lett. 27, 1396 (1971) R.Arking, R.N.Boyd, J.C.Lombardi, A.B.Robbins, S.Yoshida Inelastic Decay of Analog Resonances with Direct Reaction Background NUCLEAR REACTIONS 124Sn(p, p'), E=10, 10.65 MeV; measured σ(θ), analyzing power(θ). 125Sb deduced isobaric analog resonance, level-width.
doi: 10.1103/PhysRevLett.27.1396
1970ON01 Phys.Rev. C2, 1304 (1970) N.Onishi, R.K.Sheline, S.Yoshida Rotational Spectra of the Ground-State Bands of Even Nuclei by the Generator-Coordinate Method NUCLEAR STRUCTURE A=120-238; calculated rotational energy of ground-state band. Generator-coordinate method.
doi: 10.1103/PhysRevC.2.1304
1970YA11 Progr.Theoret.Phys. 44, 125 (1970) Calculation of the Heavy Particle Stripping Process in the Reaction 11B(d, n)12C NUCLEAR REACTIONS 11B(d, n), E=65 MeV; calculated σ(θ). Microscopic DWBA.
doi: 10.1143/PTP.44.125
1970YU02 Phys.Lett. 33B, 334 (1970) An Alpha-Cluster Model Calculation of 12C NUCLEAR STRUCTURE 12C; calculated levels. Sigma-cluster model.
doi: 10.1016/0370-2693(70)90246-7
1967KE14 Nucl.Phys. A104, 642 (1967) J.Kern, O.Mikoshiba, R.K.Sheline, T.Udagawa, S.Yoshida Gamma-Vibrational States of Deformed Even Nuclei Populated in the (d, p) Reaction
doi: 10.1016/0375-9474(67)90479-4
1964SA01 Nucl.Phys. 50, 497 (1964) Effect of Pairing Correlations on Allowed Beta Transitions of G-T Type
doi: 10.1016/0029-5582(64)90224-X
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