NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = M.Sotona Found 39 matches. 2012BY02 Nucl.Phys. A881, 199 (2012) P.Bydzovsky, M.Sotona, T.Motoba, K.Itonaga, K.Ogawa, O.Hashimoto Electromagnetic production of medium-mass Λ-hypernuclei NUCLEAR REACTIONS 1H(γ, K+)Λ, E=0.9-2.2 GeV;1H(γ, K+)Λ, E(cm)=0.9-2.5 GeV; measured reaction products; deduced σ(θ); calculated σ(θ) using different models. 28Si(γ, K+)28λAl, E=1.3 GeV;40Ca(γ, K+)40ΛK, E=1.3 GeV;52Cr(γ, K+)52Λ, E=1.3 GeV; measured reaction products; deduced DDHF hypernucleus levels, J, π, configuration, σ(θ), spectroscopic factor; calculated levels, J, π, configuration, σ(θ), spectroscopic factor using DWIA, PWIA, other models.
doi: 10.1016/j.nuclphysa.2012.01.023
2010BY02 Nucl.Phys. A835, 246c (2010) Strangeness Electromagnetic Production on Nucleons and Nuclei NUCLEAR REACTIONS 1H(γ, K+), E=1.3, 2.2 GeV; analyzed σ(θ). Compared many models. 2H(γ, K+), (γ, K0), E=0.9-1.2 GeV; calculated Λ production σ(θ) using Saclay-Lyon and Kaon-MAID models. 12C(e, e'K+), E=2.2 GeV; calculated hypernucleus 12B null s(E, θ) using DWIA with Saclay-Lyon model.
doi: 10.1016/j.nuclphysa.2010.01.199
2010CU02 Nucl.Phys. A835, 129c (2010) F.Cusanno, A.Acha, P.Bydzovsky, C.C.Chang, E.Cisbani, C.W.De Jager, R.De Leo, S.Frullani, F.Garibaldi, D.W.Higinbotham, M.Iodice, J.J.LeRose, P.Markowitz, S.Marrone, M.Sotona, G.M.Urciuoli, and the JLab Hall A Collaboration Update of High Resolution (e, e'K+) Hypernuclear Spectroscopy at Jefferson Lab's Hall A NUCLEAR REACTIONS 9Be, 12C, 16O(e, eK+), E not given; calculated hypernuclei σ(θ, E) using DWIA with Saclay-Lyon interaction. Comparison with data.
doi: 10.1016/j.nuclphysa.2010.01.185
2010GA29 Int.J.Mod.Phys. E19, 2487 (2010) F.Garibaldi, E.Cisbani, F.Cusanno, S.Frullani, M.Iodice, G.M.Urciuoli, R.De Leo, L.Lagamba, S.Marrone, J.J.LeRose, C.W.de Jager, R.J.Feuerbach, D.W.Higinbotham, B.Reitz, A.Acha, P.Markowitz, P.Bydzovsky, M.Sotona, C.C.Chang, J.Millener High-resolution hypernuclear spectroscopy electron scattering at JLab, HALL A NUCLEAR REACTIONS 9B, 12C, 16O(E, EK+)9Li/12B/16N, E=4 GeV; measured reaction products; deduced σ(θ, E), hypernuclear levels and relative strengths. Comparison with theoretical calculations.
doi: 10.1142/S0218301310016995
2010MO25 Prog.Theor.Phys.(Kyoto), Suppl. 185, 224 (2010) T.Motoba, P.Bydzovsky, M.Sotona, K.Itonaga Spectroscopy of Electro- and Photo-Productions of Hypernuclei NUCLEAR REACTIONS 9Be, 10B, 12C, 19F, 28Si, 40Ca(π+, K+), (π-, K-), (γ, K+), E<2.5 GeV; calculated hypernucleus production σ(θ), s(θ, E), hyperon recoil, excitation energy. Comparison with experimental data.
doi: 10.1143/PTPS.185.224
2010MO34 Int.J.Mod.Phys. E19, 2470 (2010) T.Motoba, P.Bydzovsky, M.Sotona, K.Itonaga, K.Ogawa, O.Hashimoto Spectroscopy of Medium-mass hypernuclear production NUCLEAR REACTIONS 12C, 28Si, 40Ca(γ, K+)12B/28Al/40K, E=1.3 GeV; calculated excitation spectra, photoproduction differential σ, hyperon recoil momentum.
doi: 10.1142/S0218301310016971
2008LE08 Nucl.Phys. A804, 116 (2008) J.J.LeRose, C.W.de Jager, R.J.Feuerbach, D.W.Higinbotham, B.Reitz, A.Acha, P.Markowitz, P.Bydzovsky, M.Sotona, C.C.Chang, E.Cisbani, F.Cusanno, S.Frullani, F.Garibaldi, R.De Leo, L.Lagamba, S.Marrone, M.Iodice, G.M.Urciuoli, for the Hall A Collaboration Hypernuclear spectroscopy via (e, e' K+) in JLab's Hall A NUCLEAR REACTIONS 9Be, 12C, 16O(e, e'K+), E=3.66 GeV; measured hypernuclei production excitation spectra, σ(E), missing mass spectra. 12B, 16N deduced hypernuclei levels, J, π.
doi: 10.1016/j.nuclphysa.2008.01.011
2008TS04 Phys.Rev. C 78, 014001 (2008); Erratum Phys.Rev. C 83, 039904 (2011) K.Tsukada, T.Takahashi, T.Watanabe, Y.Fujii, K.Futatsukawa, O.Hashimoto, K.Hirose, K.Ito, S.Kameoka, H.Kanda, K.Maeda, A.Matsumura, Y.Miura, H.Miyase, S.N.Nakamura, H.Nomura, K.Nonaka, T.Osaka, Y.Okayasu, H.Tamura, H.Tsubota, M.Ukai, H.Yamauchi, M.Wakamatsu, T.Ishikawa, T.Kinoshita, F.Miyahara, T.Nakabayashi, H.Shimizu, T.Tamae, H.Yamazaki, A.Sasaki, O.Konno, P.Bydzovsky, M.Sotona Photoproduction of neutral kaons on a liquid deuterium target in the threshold region NUCLEAR REACTIONS 2H(γ, K0), E=0.8-1.1 GeV; measured mass spectra, momentum distributions, σ.
doi: 10.1103/PhysRevC.78.014001
2007WA31 Phys.Lett. B 651, 269 (2007) T.Watanabe, P.Bydzovsky, K.Dobashi, S.Endo, Y.Fujii, O.Hashimoto, T.Ishikawa, K.Itoh, H.Kanda, M.Katoh, T.Kinoshita, O.Konno, K.Maeda, A.Matsumura, F.Miyahara, H.Miyase, T.Miyoshi, K.Mizunuma, Y.Miura, S.N.Nakamura, H.Nomura, Y.Okayasu, T.Osaka, M.Oyamada, A.Sasaki, T.Satoh, H.Shimizu, M.Sotona, T.Takahashi, T.Tamae, H.Tamura, T.Terasawa, H.Tsubota, K.Tsukada, M.Ukai, M.Wakamatsu, H.Yamauchi, H.Yamazaki Photo-production of neutral kaons on 12C in the threshold region
doi: 10.1016/j.physletb.2007.06.033
2005BY01 Nucl.Phys. A754, 243c (2005) Kaon electromagnetic production: constraints set by new data NUCLEAR REACTIONS 1H(γ, K+X), E ≈ 1-2.5 GeV; analyzed hyperon production associated σ(θ); deduced resonance contributions.
doi: 10.1016/j.nuclphysa.2005.02.076
2001UR03 Nucl.Phys. A691, 43c (2001) G.M.Urciuoli, P.Brindza, P.Bydzovsky, C.C.Chang, E.Cisbani, F.Cusanno, R.De Leo, S.Frullani, F.Garibaldi, M.Iodice, L.Lagamba, S.Lassiter, J.J.Le Rose, P.Markowitz, M.Sotona Electroproduction of Hypernuclei: An experimental challenge
doi: 10.1016/S0375-9474(01)01005-3
1997CI08 Nucl.Phys. A623, 304c (1997) E.Cisbani, S.Frullani, F.Garibaldi, M.Iodice, G.M.Urciuoli, R.De Leo, R.Perrino, M.Sotona Hypernuclear Physics at TJNAF NUCLEAR REACTIONS 2H(e, e'X), E=4.5 GeV; analyzed hyperon production σ. 12C(π+, K+), E at 1.06 GeV/c; 12C(e, e'X), E not given; analyzed hyperon production σ related data.
doi: 10.1016/S0375-9474(97)00449-1
1994IT01 Phys.Rev. C49, 1045 (1994) K.Itonaga, T.Motoba, O.Richter, M.Sotona Hypernuclear and (Lambda)-Spin Polarizations Produced in the (π+, K+) Reaction NUCLEAR REACTIONS 13,12C, 16O, 10,11B, 14N(π+, K+), E at 1.04 GeV/c; calculated σ(θ), polarization vs excitation energy. DWIA, configuration-mixed wave functions.
doi: 10.1103/PhysRevC.49.1045
1994IT07 Prog.Theor.Phys.(Kyoto), Suppl. 117, 17 (1994) The (K-, π-) and (π+, K+) Reaction and Λ-Hypernuclear Polarization NUCLEAR REACTIONS 1n(π+, X), (K-, X), E at 1-2.4 GeV/c; calculated Λ production σ(θ) vs E. 12C(K-, π-), E at 0.8, 1.1 GeV/c; 12C(π+, K+), E at 1.04, 1.06 GeV/c; 13C(K-, π-), E at 0.8 GeV/c; 13C(π+, K+), E at 1.04, 1.1 GeV/c; 16O(π+, K+), E at 1.04 GeV/c; 16O(K-, π-), E at 1.1 GeV/c; 10B(π+, K+), E at 1.04 GeV/c; calculated σ(θ), Λ hypernuclei production. DWBA, elementary spin-nonflip, spin-flip amplitudes, polarization studies included. NUCLEAR STRUCTURE A=11; A=12; calculated hypernuclei levels.
doi: 10.1143/PTPS.117.17
1994MO49 Prog.Theor.Phys.(Kyoto), Suppl. 117, 123 (1994) Photoproduction of Polarized Hypernuclei NUCLEAR REACTIONS 1H(γ, X), E=1-2 GeV; calculated Λ production σ(θ), polarization vs E. 10B, 12C, 16O(γ, K+), E at 1.2 GeV/c; 16O(π+, K+), E at 1.04 GeV/c; calculated σ(θ), polarization for hypernuclei production. Phenomenological elementary process parametrization.
doi: 10.1143/PTPS.117.123
1994SO30 Prog.Theor.Phys.(Kyoto), Suppl. 117, 151 (1994) Electroproduction of Strangeness and Spectroscopy of Light Hypernuclei NUCLEAR REACTIONS 1H(e, e'X), E not given; 1H(γ, K+), E=0.9-1.3 GeV; analyzed hypernuclei production data. 9Be, 7Li, 12C, 16O(e, e'X), E=3 GeV; calculated σ(E(e'), θ(e'), θ(K+)) for hypernuclei production. One photon exchange approximation, Feynman diagrams approach.
doi: 10.1143/PTPS.117.151
1992AD09 Czech.J.Phys. B42, 1167 (1992) J.Adam, Jr., J.Mares, O.Richter, M.Sotona, S.Frullani Electroproduction of Strangeness NUCLEAR REACTIONS 1H(γ, K+X), E ≤ 2 GeV; calculated strange particle production σ(θ) vs E, polarization. 12C, 4He(e, e'K+), E=3 GeV; calculated σ(E(e'), θ(e'), θ(Ke)). 12C(K-, π-), E at 600 MeV/c; 12C(π+, K+), E at 1050 MeV/c; analyzed σ(θ). Feynman diagrams, one photon exchange approximation. Feynman diagrams, one photon exchange approximation.
doi: 10.1007/BF01591400
1992IT02 Nucl.Phys. A547, 57c (1992) K.Itonaga, T.Motoba, O.Richter, M.Sotona Hypernuclear and (Lambda)-Spin Polarizations in the (π+, K+) and (K-, π-) Reactions NUCLEAR REACTIONS 12C(π+, K+), E at 1.04 GeV/c; 12C(K-, π-), E at 1.1 GeV/c; calculated σ(θ), hypernuclei, lambda-spin polarizations, proton asymmetry.
doi: 10.1016/0375-9474(92)90709-S
1992SO23 Nucl.Phys. A547, 63c (1992) M.Sotona, K.Itonaga, T.Motoba, O.Richter, J.Zofka Production of Polarized Hypernuclei - Photoproduction versus (π, K) and (K, π) Reactions - NUCLEAR REACTIONS 16O(π+, K+), E at 0.72-1.2 GeV/c; calculated σ(θ), hypernuclear, lambda-spin polarizations. 12C, 16O(γ, K+), E at 1.2 GeV/c; calculated σ(θ), hypernuclear polarization.
doi: 10.1016/0375-9474(92)90710-2
1991RI05 Phys.Rev. C43, 2753 (1991) Realistic A = 7 Hypernuclear Productions NUCLEAR REACTIONS 1n(K-, π-), E at < 2 GeV/c; 7Li(K-, π-), E at > 800 MeV/c; 7Li(π+, K+), E at 1.05 GeV/c; 7Li(γ, K+), E at 1050-1200 MeV/c; 1H(γ, K+), E at < 2 GeV/c; calculated σ(θ), polarization. Large basis hypernuclear wave functions.
doi: 10.1103/PhysRevC.43.2753
1990SO07 Czech.J.Phys. B40, 1091 (1990) Polarization in Hypernuclear Photoproduction NUCLEAR REACTIONS 12C(γ, K+), E at 1.2 GeV/c; 12C(π+, K+), E at 1.05 GeV/c; 12C(K-, π-), E at 0.8 GeV/c; calculated hypernuclear polarization. 16O(γ, K+), E not given; calculated hypernuclear photoproduction.
doi: 10.1007/BF01597969
1989BA06 Phys.Rev. C39, 587 (1989) H.Bando, T.Motoba, M.Sotona, J.Zofka Polarization of Hypernuclei in the (π+, K+) Reaction NUCLEAR REACTIONS 12C, 16O, 28Si, 56Fe(π+, K+), E at 1.04 GeV/c; calculated σ(θ), hypernuclear state polarization.
doi: 10.1103/PhysRevC.39.587
1989SO05 Prog.Theor.Phys.(Kyoto) 81, 160 (1989) Elementary Amplitudes of Process π-p → K0(Lambda) NUCLEAR REACTIONS 1H(π-, K0X), E at 0.94-2.4 GeV/c; calculated partial wave amplitudes, Lambda production.
doi: 10.1143/PTP.81.160
1989SO12 Czech.J.Phys. B39, 1273 (1989) M.Sotona, J.Zofka, V.N.Fetisov, H.Bando Hypernuclear Production with a Strong Spin-Flip NUCLEAR REACTIONS 12C(π+, K+), E at 0.95-1.9 GeV/c; calculated σ(θ).
doi: 10.1007/BF01605328
1984ZO02 Nucl.Phys. A431, 603 (1984) J.Zofka, M.Sotona, V.N.Fetisov Fermi Motion in Hypernuclear Production NUCLEAR REACTIONS 12C(K-, π-), E at rest; calculated σ; deduced Fermi motion induced many-body transition matrix renormalization.
doi: 10.1016/0375-9474(84)90271-9
1982SO07 Czech.J.Phys. B32, 283 (1982) Variational Calculation in Light Nuclei with the Jastrow-Type Correlation Function NUCLEAR STRUCTURE 3H, 4He; calculated form factors, rms radii, binding energy. Jastrow type correlation function, three-body clustering.
doi: 10.1007/BF01602069
1980MA21 Phys.Lett. 92B, 256 (1980) L.Majling, M.Sotona, J.Zofka, V.N.Fetisov, R.A.Eramzhyan Supermultiplet Structure and Decay Properties of Hypernuclear 1+ Resonances in 6Li NUCLEAR REACTIONS 6Li(K-, π-), E at 790 MeV/c; calculated σ(E(λ particle), E); deduced λ particle resonance decay properties.
doi: 10.1016/0370-2693(80)90258-0
1978SO11 Czech.J.Phys. B28, 593 (1978) Monopole Vibrations of Nuclei and Effective Interactions NUCLEAR STRUCTURE 16O, 208Pb; calculated ground state characteristics. Effective Gaussian interaction derived from collective-model monopole excitations.
doi: 10.1007/BF01596039
1977SO11 Czech.J.Phys. 27B, 516 (1977) Reaction Matrix for Nonlocal Potentials. II. Effective Interaction for A = 18 Nuclei NUCLEAR STRUCTURE 18O, 18F; calculated levels.
doi: 10.1007/BF01587129
1977SO12 Czech.J.Phys. 27B, 386 (1977) Reaction Matrix for Nonlocal Potentials. I. Magic Nuclei NUCLEAR STRUCTURE 4He, 16O, 40Ca; calculated binding energies.
doi: 10.1007/BF01596730
1976SO04 Nucl.Phys. A262, 400 (1976) Radiative Capture of Negative Pions in Deuterium NUCLEAR REACTIONS 2H(π-, γ); calculated transition rate.
doi: 10.1016/0375-9474(76)90506-6
1975SO07 Phys.Lett. 57B, 27 (1975) Simple Microscopic Foundation of the Breathing Mode NUCLEAR STRUCTURE 4He, 12C, 16O, 40Ca, 56Ni, 90Zr, 120Sn, 208Pb; calculated binding energies, transition radii.
doi: 10.1016/0370-2693(75)90235-X
1974SO08 Nucl.Phys. A229, 471 (1974) Muon Capture in Deuterium with Realistic Potentials NUCLEAR REACTIONS 2H(μ-, γ); calculated transition rates.
doi: 10.1016/0375-9474(74)90665-4
1974SO13 Phys.Rev. C10, 2646 (1974) Nuclear Charge Form Factor with Intrinsic Hyperspherical-Coordinate Wave Functions NUCLEAR STRUCTURE 4He, 16O; calculated intrinsic charge form factor. Lowest-order hyperspherical-coordinate wave functions; comparison with experiment.
doi: 10.1103/PhysRevC.10.2646
1974ZO04 Czech.J.Phys. 24B, 1250 (1974) Inelastic Formfactor and Three-Body Forces in the Hyperspherical Description of 4He NUCLEAR REACTIONS 4He(e, e'); calculated form factor.
doi: 10.1007/BF01587211
1970GM02 Phys.Rev. C2, 356 (1970) Brueckner Reaction Matrix and Separable Potentials NUCLEAR STRUCTURE 4He, 16O; calculated binding energy. Reaction matrix elements of Tabakin potential.
doi: 10.1103/PhysRevC.2.356
1970TR07 Czech.J.Phys. 20B, 865 (1970) Realistic Forces and Deformed State Admixtures in 18O NUCLEAR STRUCTURE 18O; calculated levels, B(E2). Realistic forces, deformed state admixtures.
doi: 10.1007/BF01691079
1969SO11 Phys.Rev. 185, 1448 (1969) M.Sotona, M.Gmitro, Z.Pluhar, L.Trlifaj A = 21 Nuclei in the SU3 NUCLEAR STRUCTURE 21Ne, 21Na; calculated levels. SU(3) model.
doi: 10.1103/PhysRev.185.1448
1966TR02 Nucl.Phys. 86, 681 (1966) Level Structure of Oxygen Isotopes in the SU3 Scheme NUCLEAR STRUCTURE 20O, 18O; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(66)90507-4
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