NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = L.Wilets Found 25 matches. 2005GI16 Nucl.Phys. A761, 22 (2005) B.G.Giraud, A.Weiguny, L.Wilets Coordinates, modes and maps for the density functional
doi: 10.1016/j.nuclphysa.2005.07.012
1997DA06 Nucl.Phys. A616, 625 (1997) C.A.da Rocha, G.Krein, L.Wilets Ghost Poles in the Nucleon Propagator in the Linear σ Model Approach and Its Role in πN Low-Energy Theorems
doi: 10.1016/S0375-9474(96)00480-0
1997WI05 Phys.Rev. C55, 2067 (1997) The Chromodielectric Soliton Model: Quark self-energy and hadron bags
doi: 10.1103/PhysRevC.55.2067
1997WI07 Phys.Rev. C56, 486 (1997) L.Wilets, M.A.Alberg, S.Pepin, Fl.Stancu, J.Carlson, W.Koepf Quark Substructure Approach to 4He Charge Distribution NUCLEAR STRUCTURE 4He; calculated density distribution; deduced proton size vs density. Realistic nucleonic wave functions, quark substructure, chromodielectric model.
doi: 10.1103/PhysRevC.56.486
1996PE03 Phys.Rev. C53, 1368 (1996) S.Pepin, Fl.Stancu, W.Koepf, L.Wilets Nucleon-Nucleon Interaction in the Chromodielectric Soliton Model: Dynamics
doi: 10.1103/PhysRevC.53.1368
1995KO23 Phys.Rev. C51, 3445 (1995) Quark Model Description of the N-N System: Momentum distributions, structure functions, and the EMC effect
doi: 10.1103/PhysRevC.51.3445
1995WI03 Phys.Rev. C51, 339 (1995) Collapse of Flux Tubes
doi: 10.1103/PhysRevC.51.339
1994AL34 Yad.Fiz. 57, No 9, 1678 (1994); Phys.Atomic Nuclei 57, 1608 (1994) M.A.Alberg, E.M.Henley, L.Wilets, P.D.Kunz A Quark Model of (Lambda-bar)(Lambda) Production in (p-bar)p Interactions NUCLEAR REACTIONS 1H(p-bar, X), E=threshold-1695 MeV/c; analyzed σ, σ(θ), polarization observables data following (lambda-bar)(lambda) production. Quark model.
1994AL51 Nuovo Cim. 107A, 2483 (1994) M.A.Alberg, E.M.Henley, L.Wilets, P.D.Kunz A Quark Model of (Lambda-bar)Lambda Production in (p-bar)p Interactions NUCLEAR REACTIONS 1H(p-bar, X), E=threshold-1.92 GeV/c; calculated σ(θ) for (lambda-bar)(lambda) production. DWBA.
doi: 10.1007/BF02734020
1994BR07 Phys.Rev. C49, 1299 (1994) M.E.Bracco, A.Eiras, G.Krein, L.Wilets Self-Consistent Solution of the Schwinger-Dyson Equations for the Nucleon and Meson Propagators
doi: 10.1103/PhysRevC.49.1299
1994KO22 Phys.Rev. C50, 614 (1994) W.Koepf, L.Wilets, S.Pepin, Fl.Stancu The Nucleon-Nucleon Potential in the Chromodielectric Soliton Model: Statics NUCLEAR STRUCTURE 1H; calculated μ; deduced chromodielectric soliton model parameters. Self-consistent mean field calculation. Model used for NN-interaction.
doi: 10.1103/PhysRevC.50.614
1993AL16 Nucl.Phys. A560, 365 (1993) M.A.Alberg, E.M.Henley, L.Wilets, P.D.Kunz A Quark Model of Antilambda-Lambda Production in (p-bar)p Interactions NUCLEAR REACTIONS 1H(p-bar, X), E at 1436-1695 MeV/c; calculated (lambda)(lambda-bar) production σ(θ), asymmetry; analyzed σ(θ), polarization, spin correlation coefficients data; deduced model parameters. Quark model, DWBA approach.
doi: 10.1016/0375-9474(93)90102-4
1992PO10 Phys.Rev. C46, 2587 (1992) S.J.Pollock, E.N.Fortson, L.Wilets Atomic Parity Nonconservation: Electroweak parameters and nuclear structure NUCLEAR STRUCTURE 202,204,206,208,210Pb; calculated neutron, proton rms radius, ratio; deduced parity nonconservation measurement implications. Realivistic, nonrelativistic model calculations.
doi: 10.1103/PhysRevC.46.2587
1990AL15 Phys.Rev. C41, 2544 (1990) M.A.Alberg, L.Wilets, J.J.Rehr, J.M.de Leon Upper Limits to Fusion Rates of Isotopic Hydrogen Molecules in Pd NUCLEAR REACTIONS 2,1H(d, d), E=low; calculated fusion rates; deduced cold fusion rates upper limits in PdH.
doi: 10.1103/PhysRevC.41.2544
1990FO08 Phys.Rev.Lett. 65, 2857 (1990) Nuclear-Structure Effects in Atomic Parity Nonconservation ATOMIC PHYSICS A=75-105; calculated parity-nonconservation related single electron normalization factor; deduced nuclear effects role, neutron distribution rms radii determination possibility.
doi: 10.1103/PhysRevLett.65.2857
1987BI02 Z.Phys. A326, 89 (1987) M.Bickeboller, M.C.Birse, L.Wilets Self-Consistent Treatment of One-Gluon Exchange in the Soliton Bag Model NUCLEAR STRUCTURE 1H; calculated μ. Self-consistent model, one-gluon exchange, soliton bag model.
1979CA11 Nucl.Phys. A327, 250 (1979) D.J.E.Callaway, L.Wilets, Y.Yariv Classical Many-Body Model for Heavy-Ion Collisions (III). Ne-Ne and Ca-Ca Calculations NUCLEAR REACTIONS 20Ne(20Ne, X), E=800 MeV/nucleon; 40Ca(40Ca, X), E=250 MeV/nucleon; calculated double differential σ. Classical many-body model.
doi: 10.1016/0375-9474(79)90327-0
1976AL03 Ann.Phys.(New York) 96, 43 (1976) M.Alberg, E.M.Henley, L.Wilets Theory of Kaonic Atoms ATOMIC PHYSICS, Mesic-Atoms 10,11B, 12C, 31P, 32S, 35Cl, 27Al, 28Si, Ni, Cu; analyzed theory of kaonic atoms.
doi: 10.1016/0003-4916(76)90111-1
1976HE01 Nucl.Phys. A256, 349 (1976) E.M.Henley, F.R.Krejs, L.Wilets Nuclear Polarization in Muonic He Ions NUCLEAR STRUCTURE 3,4He; calculated polarization effects in muonic atoms.
doi: 10.1016/0375-9474(76)90377-8
1975SC37 Nucl.Phys. A252, 21 (1975) Dynamics and Non-Adiabaticity in the Fission Process NUCLEAR STRUCTURE 40Ca, 238U; calculated deformation.
doi: 10.1016/0375-9474(75)90598-9
1975WI31 Phys.Rev. C12, 2088 (1975) L.Wilets, D.R.Tuerpe, P.K.Haff Calculation of the Mass Parameter in the Theory of Self-Cranked Generator Coordinates NUCLEAR STRUCTURE 108Ru; calculated mean quadrupole moment. Self-cranked generator-coordinate method.
doi: 10.1103/PhysRevC.12.2088
1973BA04 Phys.Rev.Lett. 30, 294 (1973) W.H.Bassichis, D.R.Tuerpe, C.F.Tsang, L.Wilets Consistent Test of the Strutinsky-Nilsson Method NUCLEAR STRUCTURE 108Ru; calculated single-particle energies, shell corrections. Constrained Hartree-Fock, Strutinsky-Nilsson model.
doi: 10.1103/PhysRevLett.30.294
1959WI55 Science 129, 361 (1959) Shape of the Nucleus
doi: 10.1126/science.129.3346.361
1958CH46 Phys.Rev. 110, 1080 (1958) D.M.Chase, L.Wilets, A.R.Edmonds Rotational-Optical Model for Scattering of Neutrons
doi: 10.1103/PhysRev.110.1080
1954WI44 Kgl.Dan.Vidensk.Selsk.Mat.-Fys.Medd. 29, No.3 (1954) Excitation of nuclear rotational states in μ-mesonic atoms NUCLEAR STRUCTURE A=155-185; A>225; calculated interaction of a μ-meson with the rotational states of a nucleus produces splittings of the 2p atomic levels which are comparable in size with the mesonic fine structure splittings.
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