NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = L.D.Skouras Found 51 matches. 2005HA45 Phys.Rev. C 72, 024303 (2005) S.Harissopulos, J.Doring, M.La Commara, K.Schmidt, C.Mazzocchi, R.Borcea, S.Galanopoulos, M.Gorska, H.Grawe, M.Hellstrom, Z.Janas, R.Kirchner, E.Roeckl, I.P.Johnstone, R.Schwengner, L.D.Skouras β decay of 95Ag RADIOACTIVITY 95Ag(EC) [from 58Ni(40Ca, 2np)]; measured β-delayed Eγ, Iγ, γγ-, βγ-coin. 95Pd deduced levels, J, π. Mass separator. Comparison with shell-model predictions.
doi: 10.1103/PhysRevC.72.024303
2003BA39 Nucl.Phys. A720, 245 (2003) L.Batist, J.Doring, I.Mukha, C.Plettner, C.R.Bingham, R.Borcea, M.Gierlik, H.Grawe, K.Hauschild, Z.Janas, I.P.Johnstone, M.Karny, M.Kavatsyuk, R.Kirchner, M.La Commara, C.Mazzocchi, F.Moroz, J.Pavan, A.Plochocki, E.Roeckl, B.Salvachua, K.Schmidt, R.Schwengner, L.D.Skouras, S.L.Tabor, M.Wiedeking Isomerism in 96Ag and non-yrast levels in 96Pd and 95Rh, studied in β decay RADIOACTIVITY 96mAg(EC), (β+), (β+p) [from 60Ni(40Ca, 3np)]; measured Eγ, Iγ, Ep, βγ-, γγ-, pγ-coin, T1/2, Q(EC), Gamow-Teller strengths. 96Ag deduced isomeric states J, π. 96Pd, 95Rh deduced levels, J, π, feeding intensities. Comparison with shell-model predictions.
doi: 10.1016/S0375-9474(03)01093-5
2003MA24 Phys.Rev. C 67, 061301 (2003) N.Marginean, D.Bucurescu, C.Rossi Alvarez, C.A.Ur, L.D.Skouras, I.P.Johnstone, D.Bazzacco, S.Lunardi, G.de Angelis, M.Axiotis, E.Farnea, A.Gadea, M.Ionescu-Bujor, A.Iordachescu, W.Krolas, Th.Kroll, S.M.Lenzi, T.Martinez, R.Marginean, R.Menegazzo, D.R.Napoli, P.Pavan, M.De Poli, B.Quintana, C.Rusu, P.Spolaore, J.Wrzesinski Yrast isomers in 95Ag, 95Pd, and 94Pd NUCLEAR REACTIONS 58Ni(40Ca, 2n2p), (40Ca, n2p), (40Ca, 2np), E=135 MeV; measured Eγ, Iγ, γγ-, (neutron)γ-, (charged particle)γ-coin. 94,95Pd, 95Ag deduced levels, J, π, configurations, yrast isomers. GASP, ISIS arrays, comparison with shell model calculations.
doi: 10.1103/PhysRevC.67.061301
2002DI14 Nucl.Phys. A703, 409 (2002) P.C.Divari, J.D.Vergados, T.S.Kosmas, L.D.Skouras The Exotic Double-Charge Exchange μ- → e+ Conversion in Nuclei NUCLEAR REACTIONS 27Al(μ-, e+), E not given; calculated transition matrix elements for neutrinoless conversion; deduced reaction mechanism features.
doi: 10.1016/S0375-9474(01)01533-0
2001DI21 Part. and Nucl., Lett. 104, 53 (2001) P.C.Divari, J.D.Vergados, T.S.Kosmas, L.D.Skouras Exotic Muon-to-Positron Conversion in Nuclei: Partial transition sum evaluation by using shell model NUCLEAR REACTIONS 27Al(μ-, e+), E not given; calculated matrix elements, strength distribution, total rate. Intermediate neutrino mixing model.
2001JO23 Eur.Phys.J. A 11, 125 (2001) Charge-Independent Effective Interactions for Shell-Model Studies in the Og9/2-1p1/2 Space NUCLEAR STRUCTURE 91,92Mo, 89,90,91Tc, 92Ru, 92Rh; calculated levels, J, π, binding energies, potential matrix elements. Comparison with data.
doi: 10.1007/s100500170077
2000DI12 Phys.Rev. C61, 054612 (2000) P.C.Divari, T.S.Kosmas, J.D.Vergados, L.D.Skouras Shell Model Calculations for Light Supersymmetric Particle Scattering Off Light Nuclei NUCLEAR STRUCTURE 19F, 23Na, 29Si; calculated wave functions, matrix elements, form factors for elastic scattering of light supersymmetric particles. Shell model. Application to cold dark matter search discussed.
doi: 10.1103/PhysRevC.61.054612
1997AM08 Nucl.Phys. A625, 633 (1997) K.Amir-Azimi-Nili, J.M.Udias, H.Muther, L.D.Skouras, A.Polls Correlations and the Cross Section of Exclusive (e, e'p) Reactions for 16O NUCLEAR REACTIONS 16O(e, e'p), E not given; calculated reduced σ vs missing momentum; deduced long-range correlations role. DWIA analysis. Comparison with data.
doi: 10.1016/S0375-9474(97)00595-2
1997JO04 Phys.Rev. C55, 1227 (1997) Particle-Hole Excitations in N = 50 Nuclei NUCLEAR STRUCTURE 93Tc, 94Ru, 91Nb, 95Rh, 92Mo, 96Pd; calculated levels. Shell model approach.
doi: 10.1103/PhysRevC.55.1227
1997SC30 Nucl.Phys. A624, 185 (1997) K.Schmidt, P.C.Divari, Th.W.Elze, R.Grzywacz, Z.Janas, I.P.Johnstone, M.Karny, H.Keller, R.Kirchner, O.Klepper, A.Plochocki, E.Roeckl, K.Rykaczewski, L.D.Skouras, J.Szerypo, J.Zylicz Decay Properties of Very Neutron-Deficient Isotopes of Silver and Cadmium RADIOACTIVITY 95Ag(β+), (EC) [from 58Ni(40Ca, 2np), E=4-4.5 MeV/nucleon]; 96Ag(β+), (EC) [from 60Ni(40Ca, 3np), E=4.1 MeV/nucleon]; 97Ag(β+), (EC) [from 60Ni(40Ca, 2np), E=4.1 MeV/nucleon]; 97Cd(β+), (EC) [from 60Ni(40Ca, 3n), E=4.2 MeV/nucleon]; measured Eγ, Iγ, γγ-, Xγ-coin, beta delayed Ep, Ip, pγ-coin; deduced log ft. 95,96,97Pd deduced levels, J, π. On-line mass separation, Ge, Si(Li) detectors. NUCLEAR STRUCTURE 95,96,97Pd, 97Ag; calculated levels, Gamow-Teller transition strength. Shell model.
doi: 10.1016/S0375-9474(97)81834-9
1997SU02 Phys.Rev. C55, 714 (1997) J.Suhonen, P.C.Divari, L.D.Skouras, I.P.Johnstone Double Beta Decay of 92Mo: Comparison of the shell model and the quasiparticle random-phase approximation RADIOACTIVITY 92Mo(2β); calculated 2ν-accompanied 2β-decay double Gamow-Teller matrix elements, T1/2. Quasiparticle RPA.
doi: 10.1103/PhysRevC.55.714
1996AM05 Nucl.Phys. A604, 245 (1996) K.Amir-Azimi-Nili, H.Muther, L.D.Skouras, A.Polls Long-Range Correlations and the Momentum Distribution in Nuclei NUCLEAR STRUCTURE 16O; calculated binding energy per nucleon, nucleon distribution radius, particle number. Green's function approach, long-range correlations.
doi: 10.1016/0375-9474(96)00142-X
1996JO06 Phys.Rev. C53, 3150 (1996); Erratum Phys.Rev. C55, 2739 (1997) Isomers in 94Rh RADIOACTIVITY 94Rh(β+); calculated log ft, other β-decay properties; deduced isomers related features.
doi: 10.1103/PhysRevC.53.3150
1995JO14 Phys.Rev. C51, 2817 (1995) Binding Energies of Proton-Rich Nuclei in the Vicinity of 100Sn NUCLEAR STRUCTURE 90,91,92Zr, 91,92,93Nb, 92,93,94Mo, 93,94,95Tc, 94,95,96Ru, 95,96,97Rh, 96,97,98Pd, 97,98,99Ag, 98,99,100Cd, 99,100,101In, 100,101,102Sn; calculated binding energies; deduced relevance to β-decay, β-delayed proton emission.
doi: 10.1103/PhysRevC.51.2817
1995JO15 J.Phys.(London) G21, L63 (1995) The Spectrum and Decay of 100Sn NUCLEAR STRUCTURE 100Sn, 100In; calculated levels; deduced β+-decay characteristics.
doi: 10.1088/0954-3899/21/8/001
1995MU02 Nucl.Phys. A581, 247 (1995) Long-Range Correlations in Closed-Shell Nuclei NUCLEAR STRUCTURE 16O, 40Ca; calculated binding energy/nucleon. Large model space, long range correlations.
doi: 10.1016/0375-9474(94)00438-S
1994SC35 Z.Phys. A350, 99 (1994) K.Schmidt, T.W.Elze, R.Grzywacz, Z.Janas, R.Kirchner, O.Klepper, A.Plochocki, E.Roeckl, K.Rykaczewski, L.D.Skouras, J.Szerypo Decay Properties of the New Isotopes 94Ag and 95Ag RADIOACTIVITY 94,95Ag(β+p) [from 58Ni(40Ca, xnp), E=5 MeV/nucleon]; measured β-delayed proton energy, time spectra, T1/2. Model comparison.
doi: 10.1007/BF01290677
1993MU04 Nucl.Phys. A555, 541 (1993) Low-Energy Excitations and Occupation Probabilities NUCLEAR STRUCTURE 16O; calculated single particle strength distribution; deduced fragmentation. Green function, shell model approaches comparison, realistic nucleon-nucleon interaction.
doi: 10.1016/0375-9474(93)90487-I
1993MU07 Phys.Lett. 306B, 201 (1993) Correlations in Nuclei. Self-Consistent Treatment and the BAGEL Approach NUCLEAR STRUCTURE 16O; calculated single particle energies, occupation probabilities, strengths. Self-consistent treatment.
doi: 10.1016/0370-2693(93)90068-S
1993SK03 J.Phys.(London) G19, 731 (1993) Shell-Model Calculation of the β+ Decay of 98Cd, 96Pd and 94Ru RADIOACTIVITY 94Ru, 96Pd, 98Cd(β+); calculated Gamow-Teller transition hindrance factors, β+ strength distribution. 94Tc, 96Rh, 98Ag levels deduced Gamow-Teller transition strength distribution. Shell model.
doi: 10.1088/0954-3899/19/5/007
1993SK05 Nucl.Phys. A561, 157 (1993) L.D.Skouras, H.Muther, M.A.Nagarajan Determination of Dipole Polarization Effects in 7Li and 11Li NUCLEAR STRUCTURE 6,7Li; calculated μ, quadrupole moment, rms radii, B(λ). 11Li; calculated μ, quadrupole moment, rms radii. Shell model.
doi: 10.1016/0375-9474(93)90148-Q
1992PL01 Z.Phys. A342, 43 (1992) A.Plochocki, K.Rykaczewski, T.Batsch, J.Szerypo, J.Zylicz, R.Barden, O.Klepper, E.Roeckl, D.Schardt, H.Gabelmann, P.Hill, H.Ravn, T.Thorsteinsen, I.S.Grant, H.Grawe, P.Manakos, L.D.Skouras, and the ISOLDE Collaboration Gamow-Teller Beta Decay of the Very Neutron-Deficient N = 50 Nuclide 98Cd RADIOACTIVITY 98Cd(EC), (β+) [from Sn(p, X), E=600 MeV]; measured Eγ, Iγ, γγ-, γ(X-ray)-coin; deduced Q(EC). 98Ag deduced levels, relative Iγ, ICC, J, π, Gamow-Teller transition strength, γ-multipolarity. Shell model.
1992SI14 J.Phys.(London) G18, 1377 (1992) J.Sinatkas, L.D.Skouras, D.Strottman, J.D.Vergados Shell-Model Calculations in the A = 80-100 Mass Region: I. A study of the N = 50 nuclei NUCLEAR STRUCTURE 94Ru, 92Mo, 90Zr, 88Sr, 86Kr, 84Se, 93Tc, 91Nb, 89Y, 87Rb, 95Rh; calculated levels, B(λ). 96Pd; calculated levels. Shell model.
doi: 10.1088/0954-3899/18/8/012
1992SI15 J.Phys.(London) G18, 1401 (1992) J.Sinatkas, L.D.Skouras, D.Strottman, J.D.Vergados Shell-Model Calculations in the A = 80-100 Mass Region: II. A study of the N = 49, 48 nuclei NUCLEAR STRUCTURE 91Mo, 89Zr, 93Ru, 87Sr, 90Nb, 88Y, 92Ru, 90Mo, 88Zr, 86Sr, 91Tc, 89Nb; calculated levels, B(λ). 87Y; caluclated levels. Shell model.
doi: 10.1088/0954-3899/18/8/013
1991BO05 Phys.Rev. C43, R952 (1991) D.Bonatsos, L.D.Skouras, J.Rikovska Successive Energy Ratios in Medium- and Heavy-Mass Nuclei as Indicators of Different Kinds of Collectivity NUCLEAR STRUCTURE A=74-248; analyzed level energy ratio systematics; deduced different kinds of collectivity.
doi: 10.1103/PhysRevC.43.R952
1991BO06 J.Phys.(London) G17, 63 (1991) D.Bonatsos, L.D.Skouras, J.Rikovska Tests of Phenomenological Collective Models Based on Energy Ratios and Staggering Systematics NUCLEAR STRUCTURE A=74-248; analyzed band structure, level systematics; deduced collective models applicability.
doi: 10.1088/0954-3899/17/1/006
1991BO13 J.Phys.(London) G17, 865 (1991) D.Bonatsos, L.D.Skouras, J.Rikovska Systematics of Energy Differences as Signs of Intruder Bands and Parameter Independent Tests of Interacting Boson Models for Octupole States NUCLEAR STRUCTURE 160,162,164Dy, 164,166,168Er, 166,168Yb, 232Th, 234U; calculated energy level difference ratio; analyzed systematics; deduced intruder bands role.
doi: 10.1088/0954-3899/17/6/009
1991BO45 J.Phys.(London) G17, 1803 (1991) D.Bonatsos, L.D.Skouras, P.Van Isacker, M.A.Nagarajan An Application of the Democratic Mapping to the sd and fp Shells NUCLEAR STRUCTURE 20Ne, 42Sc, 44Ti; calculated levels. Democratic mapping method.
doi: 10.1088/0954-3899/17/12/004
1991CI09 J.Phys.(London) G17, 1363 (1991) O.Civitarese, H.Muther, L.D.Skouras, A.Faessler Single β+ Decay in 26Mg: A comparison between the shell model and quasiparticle random phase approximation RADIOACTIVITY 26Mg(β+); calculated β+ strength distribution. Shell, quasiparticle RPA models comparison.
doi: 10.1088/0954-3899/17/9/010
1991MU04 J.Phys.(London) G17, L27 (1991) Correlations and the Radii of Nuclei NUCLEAR STRUCTURE 16O; calculated binding energy, radius; deduced correlations role. Microscopic model.
doi: 10.1088/0954-3899/17/3/001
1991SK02 Nucl.Phys. A534, 128 (1991) Effective Transition Operators in the sd Shell NUCLEAR STRUCTURE 17O; calculated effective E2, M1 transition matrix elements. Matrix-inversion techniques.
doi: 10.1016/0375-9474(91)90560-S
1990SK04 Nucl.Phys. A513, 239 (1990) A Study of the Mass-18 Nuclei and the Effective Interaction in the sd Shell NUCLEAR STRUCTURE 16,17,18O; A=18, 19; calculated levels. Q-box techniques.
doi: 10.1016/0375-9474(90)90097-6
1990SK05 Nucl.Phys. A513, 264 (1990) The Effective Interaction in the p-Shell NUCLEAR STRUCTURE 5He, 6,7,8Li, 8,9Be, 10,11,12B, 12,13C, 14N, 15O; calculated levels. Q-box techniques.
doi: 10.1016/0375-9474(90)90098-7
1990SK07 Nucl.Phys. A515, 93 (1990) Effective Intraction Derived from the Bagel Approach NUCLEAR STRUCTURE 16,17O, 18F; calculated projected space eigen values. Matrix inversion techniques, shell model.
doi: 10.1016/0375-9474(90)90324-F
1990SK08 Nucl.Phys. A516, 255 (1990) L.D.Skouras, P.Van Isacker, M.A.Nagarajan A Democratic Mapping between the Shell Model and the Interacting Boson Model NUCLEAR STRUCTURE 44,45,46Ti, 46,47V, 48Ca; calculated levels. Shell model, interacting boson model connection.
doi: 10.1016/0375-9474(90)90308-9
1988SI03 Phys.Rev. C37, 1229 (1988) J.Sinatkas, L.D.Skouras, J.D.Vergados Shell Model Nuclear Matrix Elements for Double β Decay RADIOACTIVITY 76Ge, 80,82Se, 86Kr(2β); calculated β-decay matrix elements; deduced neutrino mass limits. Shell model.
doi: 10.1103/PhysRevC.37.1229
1986AD04 Phys.Rev. C34, 791 (1986) E.Adamides, J.Sinatkas, L.D.Skouras, A.C.Xenoulis, E.N.Gazis, C.T.Papadopoulos, R.Vlastou Structure of 96Ru NUCLEAR REACTIONS 96Ru(p, p'γ), E=7 MeV; measured Eγ, Iγ, γγ-coin, DSA, γ(θ), oriental nuclei. 96Ru deduced levels, J, π, γ-branching, B(λ), δ(E2/M1).
doi: 10.1103/PhysRevC.34.791
1983SK04 Phys.Rev. C28, 2122 (1983) Double β-Decay Nuclear Matrix Elements for the A = 48 and A = 58 Systems NUCLEAR STRUCTURE 48Ca, 58Ni; calculated double β-decay matrix elements; deduced β+-decay T1/2 for A=58, lepton violating parameters for A=48.
doi: 10.1103/PhysRevC.28.2122
1981AD03 Phys.Rev. C23, 2016 (1981) E.Adamides, L.D.Skouras, A.C.Xenoulis Structure of Low-Lying States in 94Mo NUCLEAR REACTIONS 94Mo(p, p'), E=4.8, 5 MeV; measured Eγ, Iγ(θ), DSA. 94Mo deduced levels, B(λ), T1/2, δ, γ-branching ratio. Enriched target, Ge(Li) detector. NUCLEAR STRUCTURE 94Mo; calculated levels, B(λ), T1/2, branching ratios. Shell model.
doi: 10.1103/PhysRevC.23.2016
1981AD08 Phys.Rev. C24, 1429 (1981) E.Adamides, L.D.Skouras, A.C.Xenoulis Structure of 94Tc NUCLEAR REACTIONS 94Mo(p, nγ), E=5-8 MeV; measured Eγ, Iγ, γγ-, nγ-coin, DSA, γ(θ), oriented nuclei. 94Tc deduced levels, γ-branching, T1/2, δ, B(λ). Shell model. NUCLEAR STRUCTURE 94Tc; calculated levels, γ-branching, T1/2, B(λ). Shell model.
doi: 10.1103/PhysRevC.24.1429
1979KA22 Z.Phys. A292, 153 (1979) C.A.Kalfas, A.C.Xenoulis, E.Adamides, S.Papaioannou, L.D.Skouras Properties of Electromagnetic Transitions from High-Spin States in 94Mo RADIOACTIVITY 94Tc [from 94Mo(p, n), E=8 MeV]; measured γγ(θ). 94Mo levels deduced δ, J, π. Shell model interpretation of 6+ levels.
doi: 10.1007/BF01441622
1977DE09 Phys.Lett. 66B, 417 (1977) The Even Parity States of 94Mo NUCLEAR STRUCTURE 94Mo; calculated even parity levels.
doi: 10.1016/0370-2693(77)90574-3
1977MA20 Phys.Rev. C16, 895 (1977) H.A.Mavromatis, L.D.Skouras, C.Dedes Effective Three-Body Interaction in 93Tc, 93Mo, and 94Ru NUCLEAR STRUCTURE 93Tc, 93Mo, 94Ru; calculated effective 3-body interaction.
doi: 10.1103/PhysRevC.16.895
1977SK01 Phys.Rev. C15, 1873 (1977) Even-Parity States of 95Tc NUCLEAR STRUCTURE 95Tc; calculated levels, T1/2, B(λ), γ-branching.
doi: 10.1103/PhysRevC.15.1873
1976SK03 J.Phys.(London) G2, 709 (1976) Even Parity States of 36S NUCLEAR STRUCTURE 36S; calculated low-lying even-parity levels, T1/2, δ, γ-branching.
doi: 10.1088/0305-4616/2/10/005
1975SK03 J.Phys.(London) G1, 438 (1975) Even Parity States of 46Ti NUCLEAR STRUCTURE 46Ti; calculated levels, T1/2, γ-mixing, γ-branching.
doi: 10.1088/0305-4616/1/4/008
1974SK03 Nucl.Phys. A220, 604 (1974) The Even Parity Spectrum of 44Ca NUCLEAR STRUCTURE 44Ca; calculated levels, J, π, B(E2), S, γ-branching.
doi: 10.1016/0375-9474(74)90138-9
1973TH11 J.Phys.(London) A6, 1763 (1973) A Study of 42Sc Using the 40Ca(α, d)42Sc Reaction NUCLEAR REACTIONS 40Ca(α, d), E=25.5 MeV; measured σ(Ed, θ). 42Sc deduced levels, J, π.
doi: 10.1088/0305-4470/6/11/013
1970SK01 Phys.Lett. 21B, 439 (1970) Even Parity States of 38Ar NUCLEAR STRUCTURE 38Ar; calculated even-parity states, T1/2. Mixing of 2h, 2p-4h configurations.
doi: 10.1016/0370-2693(70)90147-4
1969FL03 Nucl.Phys. A136, 353 (1969) Deformed State Admixtures in Mass-42 Nuclei NUCLEAR STRUCTURE 42Ca, 42Sc; calculated levels, transition rates. Shell model, deformed state admixtures.
doi: 10.1016/0375-9474(69)90059-1
1968FL07 Nucl.Phys. A116, 529 (1968) Deformed States in 42Ca NUCLEAR STRUCTURE 42Ca; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0375-9474(68)90389-8
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