NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.Zofka Found 36 matches. 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
1991FE06 Z.Phys. A339, 399 (1991) V.N.Fetisov, L.Majling, J.Zofka, R.A.Eramzhyan Effective Lambda N-Interaction and Spectroscopy of Low-Lying States of 1p-Shell Hypernuclei NUCLEAR STRUCTURE A=7-16; analyzed hypernuclei data; deduced model parameters. Shell model, effective Lambda-nucleon potential.
doi: 10.1007/BF01560643
1991MA55 Czech.J.Phys. B41, 1083 (1991) L.Majling, J.Zofka, R.A.Eramzhyan, V.N.Fetisov On the Configurational Splitting of Strangeness Analog State NUCLEAR STRUCTURE A=10; calculated hypernuclear levels, γ-decay; deduced s-1s(lambda) configuration decay features.
doi: 10.1007/BF01598983
1991MO19 Nucl.Phys. A534, 597 (1991) T.Motoba, H.Bando, T.Fukuda, J.Zofka Continuum Pion Spectra in the Weak Decays of 4H(Lambda), 5He(Lambda) and 6He(Lambda)(Lambda) NUCLEAR STRUCTURE A=4, 5, 6; calculated pionic decay strength function. Kapur-Peierls treatment of continuum, decay rates.
doi: 10.1016/0375-9474(91)90463-G
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
1991ZO01 Fiz.Elem.Chastits At.Yadra 22, 1292 (1991); Sov.J.Part.Nucl. 22, 628 (1991) J.Zofka, L.Majling, V.N.Fetisov, R.A.Eramzhyan Decay Properties of 1p-Shell Hypernuclei. I. Excited Bound States NUCLEAR STRUCTURE A=7-16; calculated hypernuclear spectra, decay characteristics. Shell model.
1990MA69 Z.Phys. A337, 337 (1990) L.Majling, J.Zofka, V.N.Fetisov, P.N.Lebedev, R.A.Eramzhyan A Note on the Origin of Secondary Hypernuclear γ-Quanta from 10B(Lambda)
1990MA73 Phys.Lett. 249B, 181 (1990) Hypernuclear Magnetic Moments NUCLEAR STRUCTURE 13C, 17O, 21Ne, 41Ca, 91Zr, 209Pb; calculated hypernuclei μ; deduced relativistic effects contribution. Mean field model.
doi: 10.1016/0370-2693(90)91239-8
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
1989BA27 Phys.Rev. C40, 875 (1989) Formation of Deeply Bound π- States from Hypernuclear Decay ATOMIC PHYSICS, Mesic-Atoms 28Si, 90Zr, 208Pb; calculated pion decay rates, atomic orbits, optical potentials. Hypernuclear weak decay, negative pions. NUCLEAR STRUCTURE 28Si, 90Zr, 208Pb; calculated pion decay rates, atomic orbits, optical potentials. Hypernuclear weak decay, negative pions.
doi: 10.1103/PhysRevC.40.875
1989BA93 Nucl.Phys. A501, 900 (1989) H.Bando, M.Sano, J.Zofka, M.Wakai Production of Hypernuclei in Relativistic Ion Beams
doi: 10.1016/0375-9474(89)90168-1
1989MA30 Z.Phys. A333, 209 (1989) On (Lambda)-Hyperon(s) in the Nuclear Medium NUCLEAR STRUCTURE A=12-90; analyzed (π+, K+) spectra; deduced multi-hypernuclei radii, densities. Relativistic mean field theory.
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
1989ZO02 Nuovo Cim. 102A, 327 (1989) On Some (Lambda)- and Σ-Hypernuclear States, Productions and Their Properties NUCLEAR REACTIONS 12C, 1n(π+, K+), E at 1-2.4 GeV/c; 56Fe(π+, K+), E at 1040 MeV/c; calculated σ(θ), polarization vs θ. ATOMIC PHYSICS, Mesic-Atoms 28Si, 90Zr, 208Pb; calculated pionic decay rate relative to strong interaction width.
doi: 10.1007/BF02735116
1989ZO03 Czech.J.Phys. 39B, 925 (1989) Hypernuclear Physics
doi: 10.1007/BF01599205
1988BA24 Z.Phys. A330, 203 (1988) Σ-Hypernuclear (π-, K+) Production NUCLEAR REACTIONS 56Fe, 28Si(π-, K+), E at 1-2 GeV/c; calculated σ(θ).
1988MA58 Z.Phys. A331, 89 (1988) R.Mach, J.Zofka, K.Itonaga, T.Motoba, H.Bando Pions in Nuclear Interior - Sensitive Test by Hypernuclear Decay
1988MO23 Phys.Rev. C38, 1322 (1988) T.Motoba, H.Bando, R.Wunsch, J.Zofka Hypernuclear Production by the (π+, K+) Reaction NUCLEAR REACTIONS 12C, 16O, 28Si, 40Ca, 56Fe, 90Zr, 208Pb(π+, K+), E at 1040 MeV/c; calculated σ(θ), strength function; deduced effects of resonance and quasifree processes. Kapur-Peierls method, continuum shell model, DWIA analyses.
doi: 10.1103/PhysRevC.38.1322
1987MA08 Phys.Lett. 183B, 263 (1987) L.Majling, J.Zofka, V.N.Fetisov, R.A.Eramzhyan On the Spectroscopy of the 13C(Lambda) Hypernucleus ATOMIC PHYSICS, Mesic-Atoms 13C(K-, π-), E not given; calculated hypernuclear levels, baryonic, γ-decays, excitation, daughter spectra. Many-body bound shell model.
doi: 10.1016/0370-2693(87)90960-9
1987WU05 Phys.Lett. 193B, 7 (1987) Resonant and Quasi-Free Mechanisms of Sigma Production on Nuclei NUCLEAR REACTIONS 12C, 16O(K-, π+), E=450 MeV/c; calculated effective nucleon number vs hypernuclear binding energy. Continuum shell model.
doi: 10.1016/0370-2693(87)90447-3
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
1983FE07 Z.Phys. A314, 239 (1983) V.N.Fetisov, L.Majling, J.Zofka, R.A.Eramzhyan Excitation and Structure of Hypernuclear Resonances in (K+, π-), (K+, π0)-Reactions on 1p-Shell Nuclei NUCLEAR REACTIONS 7,6Li, 10,11B, 9Be, 12,13C, 16O, 14,15N(K-, π-), E not given; analyzed data; deduced Lambda-hyperon nuclear subsystem coupling, 1p-, 1s-state single particle energies. Shell model.
doi: 10.1007/BF01879883
1983MA63 Phys.Lett. 130B, 235 (1983) L.Majling, J.Zofka, V.N.Fetisov, R.A.Eramzhyan On Nucleon Decays of Hypernuclear Resonances - Population of Bound Hypernuclear Levels NUCLEAR REACTIONS 14C, 14N(K-, π-), (K-, π0), E=0-25 MeV; calculated hypernuclear resonance production, nucleon decay characteristics.
doi: 10.1016/0370-2693(83)91132-2
1982ZO01 Czech.J.Phys. B32, 321 (1982) Nuclear Core in Hypernuclear Structure NUCLEAR REACTIONS 6Li(K-, π-), E not given; calculated σ(θ).
doi: 10.1007/BF01602079
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
1977BE29 Radiochem.Radioanal.Lett. 29, 311 (1977) J.Benada, Z.Randa, V.Bouska, V.Hnatowicz, J.Zofka, M.Vobecky On Possible Natural Sources of Superheavy Elements RADIOACTIVITY A > 200; measured X-ray spectra of some metamict minerals; deduced no evidence for superheavy elements.
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
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
1974ZO03 Czech.J.Phys. 24B, 32 (1974) Zero-Range Density Dependence in Effective Interaction NUCLEAR STRUCTURE 20Ne, 16O, 24Mg, 36Ar, 40Ca; calculated binding energy, Q; 32S studied shape transition.
doi: 10.1007/BF01596441
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
1972ZO01 Phys.Lett. 40B, 319 (1972) Spurious Center-of-Mass Effect in the Local Density Approximation NUCLEAR STRUCTURE 12C, 16O, 20Ne, 24Mg, 28Si, 32S, 36Ar, 40Ca; calculated binding energy, rms radius; analyzed spurious center-of-mass effect in local density approximation.
doi: 10.1016/0370-2693(72)90809-X
1971ZO01 Phys.Lett. 34B, 10 (1971) Deformations of Light Nuclei in the Local Density Approximation NUCLEAR STRUCTURE 12C, 16O, 20Ne, 24Mg, 28Si, 32S, 36Ar, 40Ca; calculated levels. Hartree-Fock theory, density-dependent effective interaction.
doi: 10.1016/0370-2693(71)90491-6
1971ZO03 Nucl.Phys. A168, 65 (1971) Hartree-Fock Calculations of Light Deformed Nuclei Using Density-Dependent Effective Interactions NUCLEAR STRUCTURE 12C, 16O, 20Ne, 24Mg, 28Si, 32S, 36Ar, 40Ca; calculated levels, quadrupole moment, binding energy, radii. Hartree-Fock method, density-dependent effective interactions.
doi: 10.1016/0375-9474(71)90652-X
Back to query form |