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NSR database version of May 24, 2024.

Search: Author = W.Myers

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2021GO25      Nucl.Sci.Eng. 195, S55 (2021)

J.Goda, C.Bravo, T.Cutler, T.Grove, D.Hayes, J.Hutchinson, G.McKenzie, A.McSpaden, W.Myers, R.Sanchez

A New Era of Nuclear Criticality Experiments: The First 10 Years of Godiva IV Operations at NCERC

doi: 10.1080/00295639.2021.1947103
Citations: PlumX Metrics

2021HA40      Nucl.Sci.Eng. 195, S37 (2021)

D.Hayes, T.Bredeweg, T.Cutler, J.Goda, T.Grove, J.Hutchinson, J.Lamproe, G.McKenzie, A.McSpaden, W.Myers, R.Sanchez, J.Walker

A New Era of Nuclear Criticality Experiments: The First 10 Years of Flattop Operations at NCERC

doi: 10.1080/00295639.2021.1947104
Citations: PlumX Metrics

2021HU22      Nucl.Sci.Eng. 195, S80 (2021)

J.Hutchinson, J.Bounds, T.Cutler, D.Dinwiddie, J.Goda, T.Grove, D.Hayes, G.McKenzie, A.McSpaden, J.Miller, W.Myers, E.Andres O.Ferrer, R.Sanchez, T.Smith, K.Stults, N.Thompson, J.Walker

A New Era of Nuclear Criticality Experiments: The First 10 Years of Radiation Test Object Operations at NCERC

doi: 10.1080/00295639.2021.1918938
Citations: PlumX Metrics

2021HU25      Nucl.Technology 207, s62 (2021)

J.Hutchinson, J.Alwin, A.McSpaden, W.Myers, M.Rising, R.Sanchez

Criticality Experiments with Fast 235U and 239Pu Metal and Hydride Systems During the Manhattan Project

NUCLEAR REACTIONS 235U, 239Pu(n, F), E<20 MeV; analyzed Manhattan Project data; deduced implications on MCNP6 code and ENDF data.

doi: 10.1080/00295450.2021.1908076
Citations: PlumX Metrics

2021KI11      Nucl.Technology 207, s81 (2021)

R.Kimpland, T.Grove, P.Jaegers, R.Malenfant, W.Myers

Critical Assemblies: Dragon Burst Assembly and Solution Assemblies

doi: 10.1080/00295450.2021.1927626
Citations: PlumX Metrics

2021SA45      Nucl.Sci.Eng. 195, S1 (2021)

R.Sanchez, T.Cutler, J.Goda, T.Grove, D.Hayes, J.Hutchinson, G.McKenzie, A.McSpaden, W.Myers, R.Rico, J.Walker, R.Weldon

A New Era of Nuclear Criticality Experiments: The First 10 Years of Planet Operations at NCERC

doi: 10.1080/00295639.2021.1951077
Citations: PlumX Metrics

2021TH11      Nucl.Sci.Eng. 195, S17 (2021)

N.Thompson, R.Sanchez, J.Goda, K.Amundson, T.Cutler, T.Grove, D.Hayes, J.Hutchinson, C.Kostelac, G.McKenzie, A.McSpaden, W.Myers, J.Walker

A New Era of Nuclear Criticality Experiments: The First 10 Years of Comet Operations at NCERC

doi: 10.1080/00295639.2021.1947105
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2014CH44      Nucl.Data Sheets 118, 558 (2014)

A.Chapelle, P.Casoli, N.Authier, W.Myers, J.Hutchinson, A.Sood, B.Rooney

Joint Neutron Noise Measurements on Metallic Reactor Caliban

doi: 10.1016/j.nds.2014.04.134
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2005MA80      J.Radioanal.Nucl.Chem. 266, 159 (2005)

O.Manuel, M.Pleess, Y.Singh, W.A.Myers

Nuclear systematics: Part IV. Neutron-capture cross sections and solar abundance

doi: 10.1007/s10967-005-0887-2
Citations: PlumX Metrics

2002WA24      Phys.Rev. C66, 024317 (2002)

D.Ward, R.M.Diamond, W.J.Swiatecki, R.M.Clark, M.Cromaz, M.A.Deleplanque, P.Fallon, A.Goergen, G.J.Lane, I.Y.Lee, A.O.Macchiavelli, W.Myers, F.S.Stephens, C.E.Svensson, K.Vetter

Search for the Jacobi shape transition in rapidly rotating nuclei

NUCLEAR REACTIONS 50Ti, 64Ni, 96Zr, 124Sn(48Ca, xnypzα), E=195-215 MeV; measured Eγ, Iγ, γγ-coin, multiplicities; deduced quasicontinuum spectrum features, moment of inertia vs angular momentum, possible Jacobi shape transition. 91Nb, 108Cd, 140Nd, 168Yb; deduced collective E2 bump centroids. Gammasphere and 8PI arrays.

doi: 10.1103/PhysRevC.66.024317
Citations: PlumX Metrics

2001MY01      Phys.Rev. C63, 034318 (2001)

W.D.Myers, W.J.Swiatecki

Isospin Dependence of the Nuclear Surface Tension

doi: 10.1103/PhysRevC.63.034318
Citations: PlumX Metrics

2001MY02      Acta Phys.Pol. B32, 1033 (2001)

W.D.Myers, W.J.Swiatecki

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
Citations: PlumX Metrics

2000MY01      Phys.Rev. C62, 044610 (2000)

W.D.Myers, W.J.Swiatecki

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
Citations: PlumX Metrics

1999MY01      Phys.Rev. C60, 014606 (1999)

W.D.Myers, W.J.Swiatecki

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
Citations: PlumX Metrics

1999MY02      Phys.Rev. C60, 054313 (1999)

W.D.Myers, W.J.Swiatecki

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
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1998MY01      Phys.Rev. C57, 3020 (1998); Erratum Phys.Rev. C 74, 029902 (2006)

W.D.Myers, W.J.Swiatecki

Nuclear Equation of State

doi: 10.1103/PhysRevC.57.3020
Citations: PlumX Metrics

1998MY03      Nucl.Phys. A641, 203 (1998)

W.D.Myers, W.J.Swiatecki

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
Citations: PlumX Metrics

1998MY04      Phys.Rev. C58, 3368 (1998)

W.D.Myers, W.J.Swiatecki

Nuclear Diffuseness as a Degree of Freedom

doi: 10.1103/PhysRevC.58.3368
Citations: PlumX Metrics

1997MY01      Nucl.Phys. A612, 249 (1997)

W.D.Myers, W.J.Swiatecki

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
Citations: PlumX Metrics

1997MY02      Acta Phys.Pol. B28, 9 (1997)

W.D.Myers, W.J.Swiatecki

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)

W.D.Myers, W.J.Swiatecki

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
Citations: PlumX Metrics

1996MY02      Acta Phys.Pol. B27, 99 (1996)

W.D.Myers, W.J.Swiatecki

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
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1995MY01      Nucl.Phys. A587, 92 (1995)

W.D.Myers, W.J.Swiatecki

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
Citations: PlumX Metrics

1995MY02      Acta Phys.Pol. B26, 111 (1995)

W.D.Myers, W.J.Swiatecki

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
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1991MY01      Ann.Phys.(New York) 211, 292 (1991)

W.D.Myers, W.J.Swiatecki

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
Citations: PlumX Metrics

1990CH26      Nucl.Phys. A513, 283 (1990)

H.S.Chung, W.D.Myers

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
Citations: PlumX Metrics

1990MY01      Ann.Phys.(New York) 204, 401 (1990)

W.D.Myers, W.J.Swiatecki

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
Citations: PlumX Metrics

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
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1987MY01      Nucl.Phys. A470, 107 (1987)

W.D.Myers, P.Rozmej

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1983MY02      Nucl.Phys. A410, 61 (1983)

W.D.Myers, K.-H.Schmidt

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
Citations: PlumX Metrics

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
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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
Citations: PlumX Metrics

1980MY01      Nucl.Phys. A336, 267 (1980)

W.D.Myers, W.J.Swiatecki

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
Citations: PlumX Metrics

1978ME10      Phys.Rev. C17, 1822 (1978)

R.A.Meyer, A.L.Prindle, W.A.Myers, P.K.Hopke, D.Dieterly, J.E.Koops

Multiparticle Configurations in the Odd-Neutron Nuclei 61Ni and 67Zn Populated by Decay of 61Cu, 67Cu, and 67Ga

RADIOACTIVITY 61,67Cu; measured Eγ, Iγ. 67Ga; measured absolute Iγ, T1/2, Eγ. 61Ni, 67Zn deduced levels, J, π, γ-branching.

doi: 10.1103/PhysRevC.17.1822
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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
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1978MY02      Phys.Rev. C18, 1700 (1978)

W.A.Myers, M.V.Kantelo, R.L.Osborne, A.L.Prindle, D.R.Nethaway

Fast Neutron Fission of 240Pu

NUCLEAR REACTIONS 240Pu(n, F), E=fast; measured yields, σ(A), independent, isomeric yields.

doi: 10.1103/PhysRevC.18.1700
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset10821.

1977MY02      J.Inorg.Nucl.Chem. 39, 925 (1977)


The Half-Life of 169Er

RADIOACTIVITY 169Er; measured T1/2.

doi: 10.1016/0022-1902(77)80236-4
Citations: PlumX Metrics

1977NE10      Phys.Rev. C16, 1907 (1977)

D.R.Nethaway, A.L.Prindle, W.A.Myers, W.C.Fuqua, M.V.Kantelo

Fission of 240Pu with 14.8-MeV Neutrons

RADIOACTIVITY 111Ag; measured absolute Iγ.

NUCLEAR REACTIONS 240Pu(n, F), E=14.8 MeV; measured yields, independent yields, partial isomeric yields; deduced σ(A).

doi: 10.1103/PhysRevC.16.1907
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset10712.

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
Citations: PlumX Metrics

1976MY01      Phys.Lett. 61B, 125 (1976)

W.D.Myers, H.Von Groote

The Nuclear Surface Diffuseness

NUCLEAR STRUCTURE 208Pb; calculated nuclear surface diffuseness.

doi: 10.1016/0370-2693(76)90605-5
Citations: PlumX Metrics

1975MY01      J.Inorg.Nucl.Chem. 37, 637 (1975)

W.A.Myers, M.Lindner, R.S.Newbury

The Isomer Ratio 236Np(l)/236Np(s) in the Reaction 237Np(n, 2n)236Np From Neutrons Produced in Thermonuclear Devices

NUCLEAR REACTIONS 237Np(n, 2n), E=thermonuclear spectrum; measured yield ratio for 236mNp/236Np.

doi: 10.1016/0022-1902(75)80512-4
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset10408.

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
Citations: PlumX Metrics

1973MY02      J.Inorg.Nucl.Chem. 35, 3985 (1973)

W.A.Myers, R.J.Nagle, Jr.

The Half-Life of 181W

RADIOACTIVITY 181W; measured T1/2.

doi: 10.1016/0022-1902(73)80385-9
Citations: PlumX Metrics

1966MY02      Nucl.Phys. 81, 1 (1966)

W.D.Myers, W.J.Swiatecki

Nuclear Masses and Deformations

doi: 10.1016/0029-5582(66)90639-0
Citations: PlumX Metrics

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Note: The following list of authors and aliases matches the search parameter W.Myers: , W.A.MYERS, W.D.MYERS, W.L.MYERS