NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = N.De Takacsy Found 33 matches. 2014DE06 Phys.Rev. C 89, 034301 (2014) Occupation probabilities from quadrupole moments in the Sn region NUCLEAR STRUCTURE 109,111,113,115,117,119,121,123,125,127,129,131Sn, 103,105,107,109,111,113,115,117,119,121,123,125,127,129Cd; analyzed experimental quadrupole moments; deduced neutron single-particle occupation probabilities. Spherical Bardeen-Cooper-Schrieffer (BCS) model with a weak-coupling approximation. COMPILATION 98,100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130Cd, 100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132Sn; compiled level energy and B(E2) of first 2+ states.
doi: 10.1103/PhysRevC.89.034301
1992MO05 Nucl.Phys. A537, 667 (1992) C.Moisan, N.De Takacsy, J.Barrette, S.K.Mark, G.Ingold, J.Stachel, P.Braun-Munzinger, N.Alamanos, Y.Cassagnou, J.M.Hisleur, J.Julien, R.Lacey, R.Legrain, P.Roussel-Chomaz, V.Bellini, L.Sperduto Neutral Pion Production in the Reactions 16O + 27Al, 58Ni, 208Pb at E(lab) = 95 MeV/Nucleon NUCLEAR REACTIONS 27Al, 58Ni, 208Pb(16O, π0X), E=95 MeV/nucleon; measured σ, σ(θ); deduced pion production, absorption mechanism. Moving thermal source model, fireball model, mean field effects.
doi: 10.1016/0375-9474(92)90373-R
1991AL01 Phys.Rev. C43, 1389 (1991) R.Alvarez del Castillo, N.B.de Takacsy Analysis of Low Energy π+ Scattering to Second 0+ States NUCLEAR REACTIONS 28Si, 12C(π+, π+), (π+, π+'), E=50 MeV; analyzed σ(θ); deduced reaction mechanism. Optical potential with Ericson-Ericson-Lorentz-Lorenz parameter.
doi: 10.1103/PhysRevC.43.1389
1989CO04 Phys.Lett. 220B, 17 (1989) Suppression of High Intermediate Momenta in the π-Nucleus Interaction NUCLEAR REACTIONS 16O(p, π+), E=200 MeV; 17O(π0, π0), E=50 MeV; calculated σ(θ). High intermediate momenta suppression.
doi: 10.1016/0370-2693(89)90005-1
1989DE29 Phys.Rev. C40, 1842 (1989) Skin Thickness in the Te Isotopes NUCLEAR STRUCTURE Te; calculated effective skin thickness vs deformation for isotopes; deduced effect on charge densities. Two-parameter Fermi type nuclear density.
doi: 10.1103/PhysRevC.40.1842
1988DE29 Phys.Lett. 208B, 45 (1988) Pairing Deformation and Nuclear Radii NUCLEAR STRUCTURE 100,102,104,106,108,110,113,114,118,120,122,124,126,128,130,132Sn; analyzed rms radii data; deduced pairing deformation role.
doi: 10.1016/0370-2693(88)91200-2
1988TU02 Phys.Rev. C38, 487 (1988) Charge Radii in the 50 ≤ N, Z ≤ 82 Region NUCLEAR STRUCTURE 120,122,124,126,128,130,132,134,136,138Ba; calculated deformations. N ≥ 50, Z ≤ 82; calculated rms radii. Shell model, semi-realistic effective interaction.
doi: 10.1103/PhysRevC.38.487
1986LE11 Phys.Lett. 174B, 147 (1986) L.Lee, T.E.Drake, L.Buchmann, A.Galindo-Uribarri, R.Schubank, R.J.Sobie, D.R.Gill, B.K.Jennings, N.De Takacsy Evidence for the Suppression of Multiple Scattering in 12C(π, π') at Low Energies NUCLEAR REACTIONS 12C(π+, π+), (π+, π+'), E=50 MeV; measured σ(θ). 12C transition deduced multiple scattering suppression, Ericson-Ericson Lorentz-Lorenz effect evidence.
doi: 10.1016/0370-2693(86)90730-6
1984SO12 Phys.Lett. 143B, 338 (1984) R.J.Sobie, T.E.Drake, J.Gaydos, R.R.Johnson, R.Tacik, D.R.Gill, B.K.Jennings, N.de Takacsy Study of the Pion-Nucleus Reaction Mechanism with 12C(π, π'γ) NUCLEAR REACTIONS 12C(π+, π+'), E=65, 90 MeV; measured σ(θ(π), θγ); deduced nuclear matter density role, pion-nuclear reaction mechanism role.
doi: 10.1016/0370-2693(84)91478-3
1983JE05 Phys.Lett. 124B, 302 (1983) Further Evidence for the EELL Effect NUCLEAR REACTIONS 12C(π+, π+), (π+, π+'), E=67.5 MeV; analyzed σ(θ); deduced multiple scattering suppression. DWBA, Coulomb distortions.
doi: 10.1016/0370-2693(83)91458-2
1980DE09 Nucl.Phys. A339, 54 (1980) Exact Calculations and a Fermion Pair Description of the s-Bosons Used in the Interacting Boson Approximation NUCLEAR STRUCTURE 108,116Sn; calculated ground state energy. Wave functions from correlated J=0 fermion pairs.
doi: 10.1016/0375-9474(80)90241-9
1979BE49 Phys.Rev. C20, 2439 (1979) Relation between the Interacting Boson Approximation and the Quasiparticle Formalism NUCLEAR STRUCTURE 120Sn; calculated energies of low lying levels; deduced relation between interacting boson, quasiparticle formalisms. Hamiltonian, realistic nucleon-nucleon interaction.
doi: 10.1103/PhysRevC.20.2439
1979EW03 Phys.Rev. C20, 1145 (1979) Angular Momentum Projected Quasiboson States for Triaxial Nuclei NUCLEAR STRUCTURE 130,132,134,136Ba; calculated levels, J, π, B(E2), quadrupole moments. Angular momentum projected triaxial quasiboson formalism.
doi: 10.1103/PhysRevC.20.1145
1978EW01 Phys.Rev. C17, 303 (1978) Angular Momentum Projected Quasiboson States in Transitional Nuclei NUCLEAR STRUCTURE 130,132,134,136,138Ba; calculated levels, J, π, B(E2), quadrupole moment. Tabakin interaction, angular momentum projected quasiboson formalism.
doi: 10.1103/PhysRevC.17.303
1977BE49 Nucl.Phys. A289, 397 (1977) R.Behrman, S.Das Gupta, N.de Takacsy The Structure of 12C and 16O in a Cluster Model with Varying Hinge Angle NUCLEAR STRUCTURE 12C, 16O; calculated levels. Cluster model.
doi: 10.1016/0375-9474(77)90042-2
1976DE04 Phys.Rev. C13, 399 (1976) Calculations in the 50 < N, Z < 82 Region with an Interaction Derived from the Tabakin Potential NUCLEAR STRUCTURE A=100-150; Ba; calculated levels, J, π. Semi-realistic forces, combination of Hartree-Fock, BCS methods.
doi: 10.1103/PhysRevC.13.399
1976DE17 Nucl.Phys. A263, 237 (1976) Structure Calculations for the Odd-Mass Pd Isotopes NUCLEAR STRUCTURE 101,103,105Pd; calculated levels, J, π, S, B(E2). Renormalized Tabakin potential in a deformed Hartree-Fock calculation followed by a BCS calculation.
doi: 10.1016/0375-9474(76)90170-6
1975DA03 Nucl.Phys. A240, 293 (1975) An Analysis of BCS Solutions with Realistic Interactions NUCLEAR STRUCTURE 110,120Sn; calculated binding energy.
doi: 10.1016/0375-9474(75)90332-2
1974DA25 Phys.Rev. C10, 1220 (1974) Negative-Parity States in Odd-Mass Lanthanum Isotopes NUCLEAR STRUCTURE 129La; calculated levels as function of deformation.
doi: 10.1103/PhysRevC.10.1220
1974DE38 Nucl.Phys. A231, 243 (1974) On the Contribution from a Two-Step Mechanism, Involving the Sequential Transfer of Two Neutrons, to the Calculation of (p, t) Reaction Cross Sections NUCLEAR REACTIONS 208Pb(p, d), (p, t); 30Si(p, t), E=35 MeV; 208Pb(d, t), E=17 MeV; 50Ti(p, t), E=23 MeV; 48Ca(p, t), E=39 MeV; 28Si(p, d), E=33.6 MeV; 28Si(d, t), E=21.6 MeV; calculated σ(θ).
doi: 10.1016/0375-9474(74)90520-X
1973DE36 Phys.Rev.Lett. 31, 1007 (1973) Two-Step Mechanism in the Reaction 208Pb(p, t) NUCLEAR REACTIONS 208Pb(p, t); calculated σ(Et, θ). 206Pb level deduced excitation mechanism.
doi: 10.1103/PhysRevLett.31.1007
1973SI11 Nucl.Phys. A205, 97 (1973) R.N.Singh, N.De Takacsy, S.I.Hayakawa, R.L.Hutson, J.J.Kraushaar Multi-Step Processes in the 12C(3He, α)11C Reaction NUCLEAR REACTIONS 12C(3He, 3He'), 12C(3He, α); E(lab)=42 MeV, measured σ(θ).
doi: 10.1016/0375-9474(73)90123-1
1972DE03 Nucl.Phys. A178, 469 (1972) The Structure of 12C in a Cluster Model with Varying Hinge Angle NUCLEAR STRUCTURE 12C; calculated levels, radius, B(λ), wave functions. Cluster model.
doi: 10.1016/0375-9474(72)90474-5
1972DE29 Phys.Rev. C5, 1883 (1972) Direct Solution of the Hill-Wheeler Equation for Alpha-Alpha Scattering NUCLEAR REACTIONS 4He(α, α), E(cm)=0.5-14.5 MeV; 2n(2n, 2n), E=0-25 MeV; calculated phase shifts. Direct solution of Hill-Wheeler equation.
doi: 10.1103/PhysRevC.5.1883
1972DE58 Phys.Lett. 42B, 1 (1972) On Two Step Mechanisms in the Reaction 48Ca(3He, t)48Sc NUCLEAR REACTIONS 48Ca(3He, t), E=18 MeV; calculated σ(θ).
doi: 10.1016/0370-2693(72)90699-5
1971AN14 Phys.Lett. 37B, 143 (1971) K.Ananthanarayanan, S.Das Gupta, N.de Takacsy Instability of the Four Particle-Four Hole Solution of 16O Against Parity Mixing NUCLEAR STRUCTURE 16O; calculated intrinsic state energy; deduced instability of 4p-4h against parity mixing. Hartree-Fock method.
doi: 10.1016/0370-2693(71)90036-0
1970DE24 Nucl.Phys. A152, 657 (1970) Many-Particle Many-Hole States in 16O NUCLEAR STRUCTURE 16O; calculated 1p-1h, 3p-3h, 4p-4h states.
doi: 10.1016/0375-9474(70)90939-5
1970DE45 Phys.Lett. 33B, 556 (1970) Can the 7.65 MeV 0+ State in 12C Belong to a Linear Chain of α-Clusters (Question) NUCLEAR STRUCTURE 12C; calculated levels, low-lying bands.α-cluster model.
doi: 10.1016/0370-2693(70)90347-3
1969BH03 Phys.Rev. 187, 1347 (1969) Decoupling Parameter in Light Nuclei NUCLEAR STRUCTURE 19F; calculated levels, decoupling parameters for K=1/2 bands.
doi: 10.1103/PhysRev.187.1347
1968DE13 Can.J.Phys. 46, 2091 (1968) Shell-Model Calculations in the 16O Region with the Tabakin Potential
1966DE18 Phys.Letters 23, 260 (1966) Modification of the Effective Particle-Hole Force by Ground State Correlations in Perturbation Theory NUCLEAR STRUCTURE 17F, 16O, 17O; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(66)90176-4
1966MA12 Can.J.Phys. 44, 1431 (1966) Low-Lying Negative Parity States in the A = 17 Nuclei NUCLEAR STRUCTURE 17N, 17O, 17Ne, 17F; measured not abstracted; deduced nuclear properties.
doi: 10.1139/p66-120
1965MA16 Phys.Letters 15, 329 (1965) The Lowest Negative Parity State in F17 and O17 NUCLEAR STRUCTURE 17O, 17F; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(65)91276-X
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