NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = W.D.Myers Found 34 matches. 2019MO01 At.Data Nucl.Data Tables 125, 1 (2019) P.Moller, M.R.Mumpower, T.Kawano, W.D.Myers Nuclear properties for astrophysical and radioactive-ion-beam applications (II) NUCLEAR STRUCTURE Z=8-136; calculated the ground-state odd-proton and odd-neutron spins and parities, proton and neutron pairing gaps, one- and two-neutron separation energies, quantities related to β-delayed one- and two-neutron emission probabilities, average energy and average number of emitted neutrons, β-decay energy release and T1/2 with respect to Gamow-Teller decay with a phenomenological treatment of first-forbidden decays, one- and two-proton separation energies, and α-decay energy release and half-life.
doi: 10.1016/j.adt.2018.03.003
2012MO01 Phys.Rev.Lett. 108, 052501 (2012) P.Moller, W.D.Myers, H.Sagawa, S.Yoshida New Finite-Range Droplet Mass Model and Equation-of-State Parameters NUCLEAR STRUCTURE Z=1-120, A=1-160; calculated masses, symmetry parameters, using finite-range droplet model (FRDM); deduced more accurate FRDM-2011 parameters and constants. Comparison with atomic mass evaluation 2003.
doi: 10.1103/PhysRevLett.108.052501
2001MY01 Phys.Rev. C63, 034318 (2001) Isospin Dependence of the Nuclear Surface Tension
doi: 10.1103/PhysRevC.63.034318
2001MY02 Acta Phys.Pol. B32, 1033 (2001) At the Extremes of Nuclear Charge and Spin NUCLEAR STRUCTURE 94Mo, 108Cd, 140Nd, 168Yb; calculated γ energy vs angular momentum, deformation features. Thomas-Fermi approach. NUCLEAR REACTIONS 208Pb(50Ti, X), (70Zn, X), (86Kr, X), E*=13 MeV; calculated fusion barrier features.
2001NI02 Nucl.Phys. A682, 98c (2001) V.Ninov, K.E.Gregorich, T.N.Ginter, F.P.Hessberger, R.Krucken, D.M.Lee, W.Loveland, W.D.Myers, J.Patin, M.W.Rowe, N.K.Seward, W.J.Swiatecki, A.Turler, P.A.Wilk Production and Structure of the Heaviest Elements
doi: 10.1016/S0375-9474(00)00627-8
2000MY01 Phys.Rev. C62, 044610 (2000) Nucleus-Nucleus Proximity Potential and Superheavy Nuclei NUCLEAR REACTIONS 208Pb(50Ti, X), (70Zn, X), (86Kr, X), 142Ce(136Xe, X), E* ≈ 13 MeV; calculated potential energy vs separation, fusion barrier features. Proximity potential, application to superheavy element production.
doi: 10.1103/PhysRevC.62.044610
1999MY01 Phys.Rev. C60, 014606 (1999) Thomas-Fermi Fission Barriers NUCLEAR STRUCTURE Z=70-100; calculated fission barriers. Self-consistent Thomas-Fermi model. Comparison with data.
doi: 10.1103/PhysRevC.60.014606
1999MY02 Phys.Rev. C60, 054313 (1999) Nuclear Diffuseness as a Degree of Freedom. II. An Improved Approach NUCLEAR STRUCTURE 20Ne, 200Hg; calculated neutron, proton densities. A=20-340; calculated surface diffuseness, related features. Thomas-Fermi approach.
doi: 10.1103/PhysRevC.60.054313
1998MY01 Phys.Rev. C57, 3020 (1998); Erratum Phys.Rev. C 74, 029902 (2006) Nuclear Equation of State
doi: 10.1103/PhysRevC.57.3020
1998MY03 Nucl.Phys. A641, 203 (1998) A Model of Nuclear Rotation NUCLEAR STRUCTURE 152,154,156Dy, 160Er, 172Hf, 178Os, 232Th, 236,238U, 240,244Pu, 194Hg, 194Pb, 132Ce; calculated rotational bands transition energies. 135Nd, 126Xe; calculated binding energy vs spin. Phenomenological model.
doi: 10.1016/S0375-9474(98)00463-1
1998MY04 Phys.Rev. C58, 3368 (1998) Nuclear Diffuseness as a Degree of Freedom
doi: 10.1103/PhysRevC.58.3368
1997MY01 Nucl.Phys. A612, 249 (1997) The Congruence Energy: A contribution to nuclear masses, deformation energies and fission barriers NUCLEAR STRUCTURE A=173-252; calculated congruence energy related corrections to saddle point energies, masses, fission barriers.
doi: 10.1016/S0375-9474(96)00328-4
1997MY02 Acta Phys.Pol. B28, 9 (1997) The Nuclear Thomas-Fermi Model with Angular Momentum: Fission barriers, superdeformations, moments of inertia NUCLEAR STRUCTURE 135Nd, 184Hg; calculated binding energy vs angular momentum, deformation; deduced fission barriers angular momentum dependence. 238U, 172Hf, 194Hg, 152Dy; calculated rotational bands moments of inertia. Thomas-Fermi model.
1996MY01 Nucl.Phys. A601, 141 (1996) Nuclear Properties According to the Thomas-Fermi Model NUCLEAR STRUCTURE 56Fe, 124Sn, 209Bi; calculated Thomas-Fermi charge distributions. 83,120,167Sn; calculated nucleon density distributions. Z=47-66; calculated Thomas-Fermi mass excess with, without shell corrections. A=8-252; calculated fission barriers. Thomas-Fermi model.
doi: 10.1016/0375-9474(95)00509-9
1996MY02 Acta Phys.Pol. B27, 99 (1996) The Rotating Nuclear Thomas-Fermi Model NUCLEAR STRUCTURE 152Dy, 83Sr; calculated fission barrier vs angular momentum, superdeformed nuclei.
1995MO29 At.Data Nucl.Data Tables 59, 185 (1995) P.Moller, J.R.Nix, W.D.Myers, W.J.Swiatecki Nuclear Ground-State Masses and Deformations NUCLEAR STRUCTURE A=16-339; calculated mass excess, ground state deformations. Finite-range droplet macroscopic, folded-Yukawa single particle microscopic models.
doi: 10.1006/adnd.1995.1002
1995MY01 Nucl.Phys. A587, 92 (1995) The Compressibility of Finite Nuclei NUCLEAR STRUCTURE A=10-260; calculated compressibilities for N=Z nuclei. Universal scaling dependence approach.
doi: 10.1016/0375-9474(94)00793-M
1995MY02 Acta Phys.Pol. B26, 111 (1995) The Nuclear Thomas-Fermi Model NUCLEAR STRUCTURE Z=70-108; N=96-156; calculated deformation energies vs constraint parameter. Z=71-98; calculated fission barrier heights. 82,120,170Sn; calculated nucleon density distributions. Statistical Thomas-Fermi model, other nuclei, other aspects studied.
1992MO02 Nucl.Phys. A536, 61 (1992) P.Moller, J.R.Nix, W.D.Myers, W.J.Swiatecki The Coulomb Redistribution Energy as Revealed by a Refined Study of Nuclear Masses NUCLEAR STRUCTURE 16O, 48Ca, 132Sn, 208Pb, 266Mt; calculated Coulomb volume, surface redistribution energies. N ≤ 200; Z ≤ 140; calculated ground state mass vs shape degrees of freedom; deduced Coulomb redistribution energy terms role. Macroscopic, microscopic approach.
doi: 10.1016/0375-9474(92)90245-F
1991MY01 Ann.Phys.(New York) 211, 292 (1991) A Thomas-Fermi Model of Nuclei. II. Fission Barriers and Charge Distributions NUCLEAR STRUCTURE Z=70-108; N=96-156; calculated deformation energies, fission barriers. 56Fe, 124Sn, 208Bi; calculated charge distributions. Thomas-Fermi model.
doi: 10.1016/0003-4916(91)90207-O
1990CH26 Nucl.Phys. A513, 283 (1990) The Charge and Mass Dependence of Nuclear Interaction Cross Sections NUCLEAR STRUCTURE 40Ar, 124Sn, 209Bi; calculated charge distribution. A=10-34; calculated interaction radii. Thomas-Fermi model.
doi: 10.1016/0375-9474(90)90099-8
1990MY01 Ann.Phys.(New York) 204, 401 (1990) A Thomas-Fermi Model of Nuclei. Part I. Formulation and First Results NUCLEAR STRUCTURE 40Ar, 124Sn, 209Bi; calculated Thomas-Fermi charge distributions. Generalized Seyler-Blanchard effective interaction.
doi: 10.1016/0003-4916(90)90395-5
1988MO20 At.Data Nucl.Data Tables 39, 225 (1988) P.Moller, W.D.Myers, W.J.Swiatecki, J.Treiner Nuclear Mass Formula with a Finite-Range Droplet Model and a Folded-Yukawa Single-Particle Potential NUCLEAR STRUCTURE A=16-318; calculated masses. Macroscopic-microscopic model. ATOMIC PHYSICS A=16-318; calculated masses. Macroscopic-microscopic model.
doi: 10.1016/0092-640X(88)90023-X
1987MY01 Nucl.Phys. A470, 107 (1987) The Contribution of Collective Zero-Point Motion to Mean-Square Charge Radii NUCLEAR STRUCTURE 76,77,78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98Rb; calculated rms charge radii, deformations, potential energy surfaces; deduced collective quadrupole zero-point motion contribution.
doi: 10.1016/0375-9474(87)90123-0
1986DO03 Nucl.Phys. A451, 189 (1986) C.O.Dorso, W.D.Myers, W.J.Swiatecki Droplet-Model Electric Dipole Moments NUCLEAR STRUCTURE 222Th, 226Ra; calculated electric dipole moment, proton charge units. Deformed nucleus, droplet model.
doi: 10.1016/0375-9474(86)90410-0
1983MY02 Nucl.Phys. A410, 61 (1983) An Update on Droplet-Model Charge Distributions NUCLEAR STRUCTURE N ≈ 10-150; calculated rms charge radii, differences. Z ≈ 20-90; calculated equivalent sharp charge radius slope vs neutron number with mass dependent factor. 118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,147Cs; calculated rms radii vs neutron number. Droplet model.
doi: 10.1016/0375-9474(83)90401-3
1981HE12 Nucl.Phys. A361, 483 (1981) E.S.Hernandez, W.D.Myers, J.Randrup, B.Remaud Quantal Dynamics of Charge Equilibration in Damped Nuclear Collisions NUCLEAR REACTIONS 92Mo(86Kr, X), E=430 MeV; 197Au(132Xe, X), E=900 MeV; calculated projectile-like fragment mean charge, charge dispersion.
doi: 10.1016/0375-9474(81)90648-5
1981MY01 Phys.Lett. B98, 1 (1981) W.D.Myers, G.Mantzouranis, J.Randrup Adiabacticity Criterion for Charge Equilibration with Application to Fission NUCLEAR STRUCTURE 236U; calculated fission charge widths. Charge equilibration, adiabaticity criterion. NUCLEAR REACTIONS 92Mo(86Kr, X), E=430 MeV; calculated fragment charge distribution width. Charge equilibration, adiabaticity criterion.
doi: 10.1016/0370-2693(81)90353-1
1980MY01 Nucl.Phys. A336, 267 (1980) Droplet-Model Theory of the Neutron Skin NUCLEAR STRUCTURE 16O, 40,48Ca, 90Zr, 116,124Sn, 208Pb; calculatged n, p rms radii differences. Droplet model.
doi: 10.1016/0375-9474(80)90623-5
1978MY01 Nucl.Phys. A296, 177 (1978) A Model for High-Energy Heavy-Ion Collisions NUCLEAR REACTIONS 238U(20Ne, X), E=250, 400 MeV/nucleon; calculated yields.
doi: 10.1016/0375-9474(78)90420-7
1976BO29 Phys.Lett. 63B, 265 (1976) Y.Boneh, J.P.Blocki, W.D.Myers Microscopic and Macroscopic Calculations of One-Body Damping in Fission NUCLEAR STRUCTURE 236U; calculated excitation of neutron levels in fission.
doi: 10.1016/0370-2693(76)90259-8
1976MY01 Phys.Lett. 61B, 125 (1976) The Nuclear Surface Diffuseness NUCLEAR STRUCTURE 208Pb; calculated nuclear surface diffuseness.
doi: 10.1016/0370-2693(76)90605-5
1973MY01 Nucl.Phys. A204, 465 (1973) Geometric Properties of Leptodermous Distributions with Applications to Nuclei NUCLEAR STRUCTURE A=4-208; analyzed nuclear density distributions, optical model potentials; deduced nuclear radius parameter.
doi: 10.1016/0375-9474(73)90388-6
1966MY02 Nucl.Phys. 81, 1 (1966) Nuclear Masses and Deformations
doi: 10.1016/0029-5582(66)90639-0
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