NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = G.Pantis Found 32 matches. 2003SI09 Phys.Rev. C 68, 014309 (2003) F.Simkovic, M.Smotlak, G.Pantis Quasiparticle random phase approximation with a nonlinear phonon operator
doi: 10.1103/PhysRevC.68.014309
2002PA28 Czech.J.Phys. 52, 629 (2002) G.Pantis, M.Smotlak, F.Simkovic A Schematic Calculation of the ββ-Decay Matrix Element within the Green Function Approach
doi: 10.1023/A:1015334032468
2001PA13 Phys.Rev. C63, 044009 (2001) G.Pantis, I.E.Lagaris, S.A.Sofianos Forbidden States and the Three-Body Bound State Collapse
doi: 10.1103/PhysRevC.63.044009
2000PA25 Nucl.Phys. A663-664, 825c (2000) Higher Order Terms of the Nucleon Current in the Neutrino Mass Mechanism of Neutrinoless Double Beta Decay RADIOACTIVITY 76Ge, 82Se, 96Zr, 100Mo, 116Cd, 128,130Te, 136Xe, 150Nd(2β); calculated oν-accompanied 2β-decay nuclear matrix elements; deduced limits on lepton number violating parameters.
doi: 10.1016/S0375-9474(99)00778-2
2000PA47 Yad.Fiz. 63, No 7, 1252 (2000); Phys.Atomic Nuclei 63, 1177 (2000) The Effect of Weak Magnetism and Induced Pseudoscalar Coupling in Neutrinoless Double-Beta Decay RADIOACTIVITY 76Ge, 82Se, 96Zr, 100Mo, 116Cd, 128,130Te, 136Xe, 150Nd(2β-); calculated 0ν accompanied 2β decay matrix elements, contributions from weak magnetism and induced pseudoscalar coupling.
doi: 10.1134/1.855763
1999SI04 Yad.Fiz. 62, No 4, 632 (1999); Phys.Atomic Nuclei 62, 585 (1999) Field-Theoretical Approach to Two-Neutrino Double-Beta Decay
1999SI18 Phys.Rev. C60, 055502 (1999) F.Simkovic, G.Pantis, J.D.Vergados, A.Faessler Additional Nucleon Current Contributions to Neutrinoless Double β Decay RADIOACTIVITY 76Ge, 82Se, 96Zr, 100Mo, 116Cd, 128,130Te, 136Xe, 150Nd(2β); calculated 0ν accompanied 2β-decay matrix elements; deduced nucleon current contributions.
doi: 10.1103/PhysRevC.60.055502
1998PA28 Yad.Fiz. 61, No 7, 1311 (1998); Phys.Atomic Nuclei 61, 1211 (1998) G.Pantis, F.Simkovic, A.Faessler QRPA and RQRPA Calculations of Neutrinoless Double-Beta Decay Beyond the Point of Collapse RADIOACTIVITY 76Ge, 100Mo, 116Cd, 128Te, 136Xe(2β); calculated 0ν-accompanied 2β decay T1/2. Renormalized quasiparticle RPA.
1998SI23 Yad.Fiz. 61, No 7, 1318 (1998); Phys.Atomic Nuclei 61, 1218 (1998) F.Simkovic, G.Pantis, A.Faessler Two-Neutrino Double Beta Decay: Critical analysis RADIOACTIVITY 76Ge(2β); calculated 2ν-accompanied 2β decay matrix elements. Operator expansion method.
1998SI33 Prog.Part.Nucl.Phys. 40, 285 (1998) F.Simkovic, G.Pantis, A.Faessler Two-Neutrino Double Beta Decay: A study of different approximation schemes RADIOACTIVITY 76Ge(2β-); calculated 2ν accompanied 2β-decay nuclear matrix elements. Quasiparticle RPA.
doi: 10.1016/S0146-6410(98)00037-4
1997SI06 Phys.Lett. 393B, 267 (1997) F.Simkovic, J.Schwieger, M.Veselsky, G.Pantis, A.Faessler Non-Collapsing Renormalized QRPA with Proton-Neutron Pairing for Neutrinoless Double Beta Decay RADIOACTIVITY 76Ge, 100Mo, 128,130Te(2β); calculated 0ν-accompained 2β-decay matrix elements. Renormalized quasiparticle RPA.
doi: 10.1016/S0370-2693(96)01622-X
1996PA02 Phys.Rev. C53, 695 (1996) G.Pantis, F.Simkovic, J.D.Vergados, A.Faessler Neutrinoless Double Beta Decay within the Quasiparticle Random-Phase Approximation with Proton-Neutron Pairing RADIOACTIVITY 48Ca, 76Ge, 82Se, 96Zr, 100Mo, 116Cd, 128,130Te, 136Xe(2β); calculated 0ν-accompanied 2β-decay T1/2, limits on lepton nonconserving parameters. Quasiparticle RPA.
doi: 10.1103/PhysRevC.53.695
1996PA26 Phys.Rev. C54, 1825 (1996) Inverse Scattering for a Specific Resonating Group Model Nonlocality NUCLEAR REACTIONS 4He(n, n), E=50, 100 MeV; 40Ca(n, n), E=100, 150 MeV; calculated phase shifts, equivalent local potenitals. Inverse scattering, resonating group model, specific nonlocality.
doi: 10.1103/PhysRevC.54.1825
1996SI29 Nucl.Phys.(Proc.Suppl.) S48, 257 (1996) F.Simkovic, G.Pantis, J.D.Vergados, A.Faessler The QRPA Study of Neutrinoless Double Beta Decay with and without Proton-Neutron Pairing RADIOACTIVITY 48Ca, 76Ge, 82Se, 96Zr, 100Mo, 116Cd, 128,130Te, 136Xe; analyzed 0ν-accompanied 2β-decay T1/2 data; deduced lepton number nonconserving parameters lower limits. Quasiparticle RPA with, without proton-neutron pairing.
doi: 10.1016/0920-5632(96)00255-1
1995EM02 Nucl.Phys. A592, 581 (1995) Pion Thermalisation in Relativistic Heavy Ion Collisions NUCLEAR REACTIONS 197Au(O, X), E=relativistic; analyzed pion spectra; deduced chemical potential, temperature effects relative role in thermalization.
doi: 10.1016/0375-9474(95)00302-H
1995PA27 J.Phys.(London) G21, 1079 (1995) G.Pantis, H.Fiedeldey, S.A.Sofianos Dispersion Relation for Equivalent Local Potentials with Spurious and Dynamiac Energy Dependence
doi: 10.1088/0954-3899/21/8/006
1994PA01 Phys.Rev. C49, 338 (1994) Azimuthal Distribution in Heavy-Ion Collisions NUCLEAR REACTIONS 197Au, 12C(12C, X), E=50 MeV/nucleon; 51V(40Ar, X), E=35 MeV/nucleon; calculated particle azimuthal distribution; deduced characteristic flow evidence. Boltzmann-Uehling-Uhlenbeck model.
doi: 10.1103/PhysRevC.49.338
1993HO09 Nucl.Phys. A556, 29 (1993) L.L.Howell, S.A.Sofianos, H.Fiedeldey, G.Pantis Nucleon-Alpha Potentials by Marchenko Inversion and Supersymmetry NUCLEAR REACTIONS 4He(n, n), E(cm)=2-1000 MeV; calculated phase shifts; deduced potential parameters. Marchenko inversion method.
doi: 10.1016/0375-9474(93)90236-Q
1993PA15 Nucl.Phys. A559, 266 (1993) G.Pantis, S.A.Sofianos, H.Fiedeldey, R.Lipperheide, P.E.Hodgson Dispersive Correction to the p + 16O Optical Model and the Effective Nucleon-Nucleon Potential NUCLEAR REACTIONS, ICPND 16O(p, p), E=23.4-52.5 MeV; analyzed σ(θ); deduced potential parameters, reaction σ(E). Optical model, dispersive corrections.
doi: 10.1016/0375-9474(93)90191-Y
1993PA26 Nucl.Phys. A565, 628 (1993) G.Pantis, H.Fiedeldey, S.A.Sofianos Dispersion Relation Approach to the Optical Potential Resonating Group Formulation of the n + 40Ca Reaction NUCLEAR REACTIONS 40Ca(n, n), E=11.9-30.3 MeV; analyzed σ(θ); deduced model parameters. Semi-microscopic model, dispersion relation approach.
doi: 10.1016/0375-9474(93)90049-4
1992PA07 J.Phys.(London) G18, 605 (1992) G.Pantis, A.Faessler, W.A.Kaminski, J.D.Vergados Description of the 0νββ Decay of 48Ca, 76Ge, 100Mo, 128,130Te RADIOACTIVITY 48Ca, 76Ge, 100Mo, 128,130Te(2β); calculated 0ν-accompanied 2β-decay T1/2, matrix elements; deduced lepton violating parameters limits. Quasiparticle RPA, no closure approximation.
doi: 10.1088/0954-3899/18/4/003
1992SO03 Nucl.Phys. A540, 199 (1992) S.A.Sofianos, H.Fiedeldey, R.Lipperheide, G.Pantis, P.E.Hodgson Dispersive Corrections to the Resonating Group αα Potential NUCLEAR REACTIONS 4He(α, α), E(cm) ≈ 20-70 MeV; calculated phase shifts vs E. Resonating group method, phenomenological potentials, dispersive corrections.
doi: 10.1016/0375-9474(92)90200-4
1991FA01 Phys.Rev. C43, R21 (1991) A.Faessler, W.A.Kaminski, G.Pantis, J.D.Vergados Double-β-Decay Matrix Elements RADIOACTIVITY 76Ge(2β); calculated 0ν associated 2β-decay matrix elements; deduced closure approximation validity.
doi: 10.1103/PhysRevC.43.R21
1990PA15 Phys.Lett. 242B, 1 (1990) Neutrinoless Double Beta Decay Matrix Elements Beyond Closure Approximation RADIOACTIVITY 48Ca(2β); calculated neutrinoless β-decay matrix elements.
doi: 10.1016/0370-2693(90)91584-X
1989PA08 Nucl.Phys. A499, 209 (1989) G.Pantis, R.Linden, N.Ohtsuka, A.Faessler Effect of 3α-Like States in 12C to 12C - 12C Scattering NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E=360 MeV; calculated σ(θ). Resonating group method, 3α-like states role.
doi: 10.1016/0375-9474(89)90278-9
1987PA24 Phys.Rev. C36, 1408 (1987) Folding Model for Sub-Barrier Interaction between Alpha-Type Nuclei NUCLEAR REACTIONS, ICPND 16O(12C, 12C), E(cm) ≤ 12 MeV; 12C(12C, 12C), E(cm) ≤ 8 MeV; 16O(16O, 16O), E(cm) ≤ 14 MeV; calculated σ(θ=90°), fusion σ, S-factor vs E. Folding model.
doi: 10.1103/PhysRevC.36.1408
1985PA11 Z.Phys. A321, 149 (1985) Analysis of (n, n) and (d, p) Reactions on the Same Target using Phase-Equivalent Potentials NUCLEAR REACTIONS 15N(d, p), E not given; analyzed σ(θ) vs En. 16N levels deduced possible J. Continuum stripping, nonlocal effects.
doi: 10.1007/BF01411958
1985PA14 Phys.Rev. C32, 657 (1985) G.Pantis, K.Ioannides, P.Poirier Importance of the Energy-Dependent Geometry in the 16O + 16O Optical Model Potential NUCLEAR REACTIONS 16O(16O, 16O), E=15-85 MeV; calculated σ(E, θ); deduced optical model parameters. Energy dependent optical model.
doi: 10.1103/PhysRevC.32.657
1981PA05 Can.J.Phys. 59, 225 (1981) G.Pantis, H.Fiedeldey, D.W.L.Sprung The Charge Form Factor of the Model Triton for Two-Particle Interactions with Continuum Bound States NUCLEAR STRUCTURE 3H; calculated charge form factor. Partly nonlocal interactions.
doi: 10.1139/p81-028
1980PA03 Z.Phys. A294, 101 (1980) G.Pantis, H.Fiedeldey, D.W.L.Sprung Three-Particle Bound States for Partly Nonlocal Interactions with Continuum Bound States NUCLEAR STRUCTURE 3H; calculated binding energy. Partly nonlocal interactions.
doi: 10.1007/BF01473126
1979PA02 Can.J.Phys. 57, 132 (1979) Assigment of Jπ = 1- for the 5.048 MeV Level of 16N NUCLEAR REACTIONS 15N(d, p), E=12 MeV; calculated σ(θ), plane wave formalism including off-shell effects, L=0, 2 admixture. 16N level deduced J, π.
doi: 10.1139/p79-017
1978PA05 Can.J.Phys. 56, 659 (1978) Off-Shell Effects in (d, p) Stripping Reactions NUCLEAR REACTIONS 15N(d, p), E=12 MeV; calculated σ(θ). 16N deduced level properties.
doi: 10.1139/p78-083
Back to query form |