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Search: Author = T.Werner

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2012SA50      Phys.Rev. C 86, 054316 (2012)

W.Satula, J.Dobaczewski, W.Nazarewicz, T.R.Werner

Isospin-breaking corrections to superallowed Fermi β decay in isospin- and angular-momentum-projected nuclear density functional theory

RADIOACTIVITY ^10,11C, ^13,14N, ^14,15O, ^17,18F, ^18,19Ne, ^21,22Na, ^22,23Mg, ^25,26Al, ^26,27Si, ^29,30P, ^30,31S, ^33,34Cl, ^34,35Ar, ³⁷K, ³⁹Ca, ^41,42Sc, ⁴³Ti, ^45,46V, ⁴⁷Cr, ^49,50Mn, ⁵⁴Co, ⁶²Ga, ⁶⁶As, ⁷⁰Br, ⁷⁴Rb, ⁷⁸Y, ⁸²Nb, ⁸⁶Tc, ⁹⁰Rh, ⁹⁴Ag, ⁹⁸In(β⁺); calculated isospin mixing effects and isospin breaking (ISB) corrections for superallowed β transitions using density functional theory. Unitarity of the CKM matrix. Comparison with experimental data.

doi: 10.1103/PhysRevC.86.054316
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2009SA31      Int.J.Mod.Phys. E18, 808 (2009)

W.Satula, M.Zalewski, J.Dobaczewski, P.Olbratowski, M.Rafalski, T.R.Werner, R.A.Wyss

Global nuclear structure aspects of tensor interaction

NUCLEAR STRUCTURE ^{111,113,115,117,119,121,123,125,127,129}Sn; ^40,48Ca, ⁵⁶Ni; calculated level properties using Skyrme-Hartree-Fock; ^{18,20,22,24,26,30}O, ^40,48Ca, ⁵⁶Ni, ⁹⁰Zr, ¹³²Sn, ²⁰⁸Pb; calculated mass excess and related quantities. Compared to available data.

doi: 10.1142/S0218301309012902
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2009ZA08      Phys.Rev. C 80, 064307 (2009)

M.Zalewski, P.Olbratowski, M.Rafalski, W.Satula, T.R.Werner, R.A.Wyss

Global nuclear structure effects of the tensor interaction

NUCLEAR STRUCTURE ¹⁶O, ^40,48Ca, ⁵⁶Ni, ^80,90Zr, ^100,132Sn, ²⁰⁸Pb; calculated binding energies, mechanism for superdeformed structures, and potential energy curves using energy-density-functional (EDF) methods with spherical and deformed HFB approaches and SLy4T interaction. Z=1-84, N=1-130; calculated tensor contribution to nuclear binding energy. Comparison with experimental data.

doi: 10.1103/PhysRevC.80.064307
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2009ZA11      Eur.Phys.J. A 42, 577 (2009)

M.Zalewski, W.Satula, J.Dobaczewski, P.Olbratowski, M.Rafalski, T.R.Werner, R.A.Wyss

Shell structure fingerprints of tensor interaction

NUCLEAR STRUCTURE ^40,48Ca, ⁵⁶Ni; calculated spin-orbit splittings. Z=2-82; A=4-210; calculated binding energy tensor contributions. Local energy density functional.

doi: 10.1140/epja/i2008-10768-1
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2008ZA02      Phys.Rev. C 77, 024316 (2008)

M.Zalewski, J.Dobaczewski, W.Satula, T.R.Werner

Spin-orbit and tensor mean-field effects on spin-orbit splitting including self-consistent core polarizations

NUCLEAR STRUCTURE ¹⁶O, ^40,48Ca, ⁵⁶Ni, ⁹⁰Zr, ¹³²Sn, ²⁰⁸Pb; calculated single particle energies, spin-orbit splittings, grounds state energies. ¹⁶O, ^40,48Ca, ⁵⁶Ni, ⁹⁰Zr, ^100,132Sn, ²⁰⁸Pb; analyzed single particle levels.

doi: 10.1103/PhysRevC.77.024316
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2002FO02      Nucl.Phys. A697, 703 (2002)

R.Fossion, C.De Coster, J.E.Garcia-Ramos, T.Werner, K.Heyde

Nuclear Binding Energies: Global collective structure and local shell-model correlations

NUCLEAR STRUCTURE Z=50-82; analyzed binding energies, two-neutron separation energies; deduced possible shell, deformation, or configuration-mixing effects. Liquid drop model, shell model, interacting boson model.

doi: 10.1016/S0375-9474(01)01270-2
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2000DO14      Phys.Rev. C62, 014310 (2000)

J.Dobaczewski, J.Dudek, S.G.Rohozinski, T.R.Werner

Point Symmetries in the Hartree-Fock Approach. I. Densities, Shapes, and Currents

doi: 10.1103/PhysRevC.62.014310
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2000DO15      Phys.Rev. C62, 014311 (2000)

J.Dobaczewski, J.Dudek, S.G.Rohozinski, T.R.Werner

Point Symmetries in the Hartree-Fock Approach. II. Symmetry-Breaking Schemes

doi: 10.1103/PhysRevC.62.014311
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1998VE02      Phys.Rev. C57, 3089 (1998)

T.Vertse, A.T.Kruppa, R.J.Liotta, W.Nazarewicz, N.Sandulescu, T.R.Werner

Shell Corrections for Finite Depth Potentials: Particle continuum effects

NUCLEAR STRUCTURE ⁷⁸Ni, ^{90,96,104,106,108,110,122}Zr, ¹²⁴Zr, ¹³²Sn, ¹⁴⁶Gd, ²⁰⁸Pb, ²⁹⁸Fl; calculated neutron shell correction energies. ⁴⁸Ni, ⁹⁰Zr, ^100,132Sn, ¹⁴⁶Gd, ^180,208Pb; calculated proton shell correction energies. ¹⁴⁶Gd, ²⁰⁸Pb calculated smoothed level densities. Smoothing procedure with particle continuum contribution.

doi: 10.1103/PhysRevC.57.3089
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1997WE07      Z.Phys. A358, 169 (1997)

T.R.Werner, J.Dobaczewski, W.Nazarewicz

Drip-Line Nuclei in Self-Consistent Mean-Field Theory

NUCLEAR STRUCTURE Z=20-82; N=90-190; compiled, reviewed nucleon matter radii data, analyses. Z=12-74; N=26-130; compiled, reviewed two-neutron separation energies, other nuclei, other aspects studied.

doi: 10.1007/s002180050296
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1996DA20      Acta Phys.Pol. B27, 155 (1996)

P.J.Dagnall, A.G.Smith, J.C.Lisle, D.H.Smalley, R.Chapman, C.Finck, B.Haas, M.J.Leddy, D.Prevost, N.Rowley, H.Savajols, T.R.Werner, W.Nazarewicz

The Observation of Superdeformed Structure in Mass 80 Nuclei

NUCLEAR REACTIONS ⁵⁸Ni(³⁰Si, X), E=134 MeV; measured γγ-coin. ⁸²Sr, ⁸²Y deduced high-spin levels, J, π, superdeformed bands evidence.

1996DO02      Z.Phys. A354, 27 (1996)

J.Dobaczewski, W.Nazarewicz, T.R.Werner

Neutron Radii and Skins in the Hartree-Fock-Bogoliubov Calculations

NUCLEAR STRUCTURE ^40,48Ca, ^56,64Ni, ⁹⁰Zr, ^116,124Sn, ²⁰⁸Pb; calculated neutron rms radii. A=48-98; calculated two-neutron separation, Ni isotopes. Z=20-82; N=20-82; calculated nucleon rms radii. A ≤ 16; N ≤ 208; calculated neutron rms radii; deduced (N, Z)-localization of nucleon skins. Self-consistent Skyrme-HFB theory.

doi: 10.1007/s002180050009
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1996DO06      Phys.Rev. C53, 2809 (1996)

J.Dobaczewski, W.Nazarewicz, T.R.Werner, J.F.Berger, C.R.Chinn, J.Decharge

Mean-Field Description of Ground-State Properties of Drip-Line Nuclei: Pairing and continuum effects

NUCLEAR STRUCTURE ^{132,120,150,172,100}Sn; calculated neutron, pairing densities, other aspects. Mean-field approach.

doi: 10.1103/PhysRevC.53.2809
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1996GU17      Phys.Rev. C54, 1610 (1996)

M.Gupta, P.Das, S.B.Patel, R.K.Bhowmik, T.Werner, Y.A.Akovali

Single-Particle States in ₆₆¹⁴⁹Dy₈₃ at High Spin

NUCLEAR REACTIONS ¹²²Sn(³²S, 5n), E=163 MeV; measured γγ-coin, Eγ, Iγ, DCO ratios. ¹⁴⁹Dy deduced high-spin levels, J, π, configurations. Shell model.

doi: 10.1103/PhysRevC.54.1610
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1996NA03      Phys.Rev. C53, 740 (1996)

W.Nazarewicz, J.Dobaczewski, T.R.Werner, J.A.Maruhn, P.-G.Reinhard, K.Rutz, C.R.Chinn, A.S.Umar, M.R.Strayer

Structure of Proton Drip-Line Nuclei Around Doubly Magic ⁴⁸Ni

NUCLEAR STRUCTURE ^42,44Cr, ^46,48Fe, ^48,50Ni; calculated 2-proton separation energies, deformations, single-particle levels, diproton partial decay T_1/2. Self-consistent, relativistic mean-field theories.

doi: 10.1103/PhysRevC.53.740
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1996WE02      Nucl.Phys. A597, 327 (1996)

T.R.Werner, J.A.Sheikh, M.Misu, W.Nazarewicz, J.Rikovska, K.Heeger, A.S.Umar, M.R.Strayer

Ground-State Properties of Exotic Si, S, Ar and Ca Isotopes

NUCLEAR STRUCTURE ^28,30Si, ^32,34,36S, ^36,40Ar, ^{40,42,44,46,48}Ca; calculated rms charge radius. Self-consistent.

doi: 10.1016/0375-9474(95)00476-9
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1995BA26      Phys.Rev.Lett. 74, 1946 (1995)

C.Baktash, D.M.Cullen, J.D.Garrett, C.J.Gross, N.R.Johnson, W.Nazarewicz, D.G.Sarantites, J.Simpson, T.R.Werner

First Observation of a Superdeformed Band in the N, Z ≈ 40 Mass Region

NUCLEAR REACTIONS ⁵⁶Fe(³⁰Si, X), E=128 MeV; measured γγ-coin. ⁸³Sr deduced high-spin levels, J, π, superdeformed, rotational bands, dynamical moment of inertia.

doi: 10.1103/PhysRevLett.74.1946
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1995CH56      Phys.Lett. 357B, 281 (1995)

F.Cristancho, D.R.LaFosse, C.Baktash, D.F.Winchell, B.Cederwall, J.Doring, C.J.Gross, P.-F.Hua, H.-Q.Jin, M.Korolija, E.Landulfo, I.Y.Lee, A.O.Macchiavelli, M.R.Maier, W.Rathbun, J.X.Saladin, D.Sarantites, D.W.Stracener, S.L.Tabor, A.Vander Molen, T.R.Werner

Multiple Superdeformed Bands in ⁸¹Sr

NUCLEAR REACTIONS ⁵⁸Ni(²⁹Si, 2pα), E=128 MeV; measured γγ-coin. ⁸¹Sr deduced high-spin levels, J, π, multiple superdeformed bands, moments of inertia. Cranked shell model.

doi: 10.1016/0370-2693(95)00918-B
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1995DO27      Phys.Scr. T56, 15 (1995)

J.Dobaczewski, W.Nazarewicz, T.R.Werner

Closed Shells at Drip-Line Nuclei

NUCLEAR STRUCTURE Z=20-80; calculated average neutron pairing gaps; N=20-125; calculated average proton pairing gaps energies N=20-200; calculated two neutron separation energies, other aspects; deduced role of particle-hole, particle-particle components of effective interaction. Self-consistent spherical HFB.

doi: 10.1088/0031-8949/1995/T56/002
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1995JI08      Phys.Rev.Lett. 75, 1471 (1995)

H.-Q.Jin, C.Baktash, M.J.Brinkman, C.J.Gross, D.G.Sarantites, I.Y.Lee, B.Cederwall, F.Cristancho, J.Doring, F.E.Durham, P.-F.Hua, G.D.Johns, M.Korolija, D.R.LaFosse, E.Landulfo, A.O.Macchiavelli, W.Rathbun, J.X.Saladin, D.W.Stracener, S.L.Tabor, T.R.Werner

Identification and Quadrupole-Moment Measurement of a Superdeformed Band in ⁸⁴Zr

NUCLEAR REACTIONS ⁵⁸Ni(²⁹Si, n2p), E=128 MeV; ⁵⁸Ni(³²S, 2pα), E=135 MeV; measured (charged particle)γγ-coin. ⁸⁴Zr deduced high-spin levels, J, π, superdeformed band transition quadrupole moment, deformation features.

doi: 10.1103/PhysRevLett.75.1471
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1995LA18      Phys.Rev.Lett. 74, 5186 (1995)

D.R.LaFosse, D.G.Sarantites, C.Baktash, P.-F.Hua, B.Cederwall, P.Fallon, C.J.Gross, H.-Q.Jin, M.Korolija, I.Y.Lee, A.O.Macchiavelli, M.R.Maier, W.Rathbun, D.W.Stracener, T.R.Werner

Evidence for Hyperdeformation in ¹⁴⁷Gd

NUCLEAR REACTIONS ¹⁰⁰Mo(⁵¹V, X), E=230 MeV; measured γγ-coin. ¹⁴⁷Gd deduced levels, J, π, hyperdeformation.

doi: 10.1103/PhysRevLett.74.5186
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1995LA21      Phys.Lett. 354B, 34 (1995)

D.R.LaFosse, P.-F.Hua, D.G.Sarantites, C.Baktash, Y.A.Akovali, M.Brinkman, B.Cederwall, F.Cristancho, J.Doring, C.J.Gross, H.-Q.Jin, M.Korolija, E.Landulfo, I.Y.Lee, A.O.Macchiavelli, M.R.Maier, W.Rathbun, J.X.Saladin, D.W.Stracener, S.L.Tabor, A.Vander Molen, T.R.Werner

Characterization of the First Superdeformed Band in the A ≈ 80 Region

NUCLEAR REACTIONS ⁵⁸Ni(²⁹Si, X), E=128 MeV; measured γγ-coin, energy correlations. ⁸³Sr deduced high-spin levels, J, π, superdeformed bands.

doi: 10.1016/0370-2693(95)00499-B
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1995NA20      Phys.Scr. T56, 9 (1995)

W.Nazarewicz, J.Dobaczewski, T.R.Werner

Physics of Exotic Nuclear States

NUCLEAR STRUCTURE Z=18-28; compiled, reviewed two-proton separation energies. Z=8-28; compiled, reviewed charge radii. N=88-120; A=138-170; compiled, reviewed two neutron separation energies. Exotic nuclear states, other aspects discussed.

doi: 10.1088/0031-8949/1995/T56/001
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1995SM08      Phys.Lett. 355B, 32 (1995)

A.G.Smith, P.J.Dagnall, J.C.Lisle, D.H.Smalley, T.R.Werner, R.Chapman, C.Finck, B.Haas, M.Leddy, W.Nazarewicz, D.Prevost, N.Rowley, H.Savajols

Observation of Superdeformation in ⁸²Sr

NUCLEAR REACTIONS ⁵⁸Ni(³⁰Si, 2pα), (³⁰Si, X), E=134 MeV; measured γγ-coin. ⁸²Sr deduced high-spin levels, superdeformed bands, configuration. Cranked Woods-Saxon calculations.

doi: 10.1016/0370-2693(95)00735-4
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1995WE02      At.Data Nucl.Data Tables 59, 1 (1995)

T.R.Werner, J.Dudek

Shape Coexistence Effects of Super- and Hyperdeformed Configurations in Rotating Nuclei II. Nuclei with 42 ≤ Z ≤ 56 and 74 ≤ Z ≤ 92

NUCLEAR STRUCTURE Z=42-56; Z=74-92; compiled, reviewed high-spin data; calculated total energies; deduced superdeformed, hyperdeformed configurations shape coexistence features. Macroscopic-microscopic approach.

doi: 10.1006/adnd.1995.1001
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1994NA16      Phys.Rev. C50, 2860 (1994)

W.Nazarewicz, T.R.Werner, J.Dobaczewski

Mean-Field Description of Ground-State Properties of Drip-Line Nuclei: Shell-correction method

NUCLEAR STRUCTURE ^100,122Zr; calculated neutron, total shell corrections, average level density. ^100,122,124Zr, ^{166,186,206,226}Os; calculated neutron shell corrections vs deformation β₂. N=89-120; calculated one-, two-neutron separation, Fermi energies vs neutron number for Sn isotopes. N=90-184; calculated Fermi energies. Mean-field description, shell correction method.

doi: 10.1103/PhysRevC.50.2860
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1994WE11      Phys.Lett. 335B, 259 (1994)

T.R.Werner, J.A.Sheikh, W.Nazarewicz, M.R.Strayer, A.S.Umar, M.Misu

Shape Coexistence Around ⁴⁴₁₆S₂₈: The deformed N = 28 region

NUCLEAR STRUCTURE ^{28,30,32,34,36,38,40,42,44,46,48,50,52,54}S; analyzed two-neutron separation energies, masses, deformations, radii, single particle level energies; deduced stability features around ⁴⁴S.

doi: 10.1016/0370-2693(94)90347-6
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1994WE13      Nucl.Phys. A578, 1 (1994)

T.R.Werner, J.Dobaczewski, M.W.Guidry, W.Nazarewicz, J.A.Sheikh

Microscopic Aspects of Nuclear Deformation

NUCLEAR STRUCTURE N ≤ 110; calculated equilibrium deformations for Kr, Sr, Zr, Mo, Gd, Er, Hf isotopes. ^92,106Mo; calculated potential energy curves, ground state, deformation energies. Skyrme Hartree-Fock + BCS model based self-consistent approach.

doi: 10.1016/0375-9474(94)90966-0
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1994WE16      Phys.Lett. 333B, 303 (1994)

T.R.Werner, J.A.Sheikh, W.Nazarewicz, M.R.Strayer, A.S.Umar, M.Misu

Shape Coexistence Around ⁴⁴₁₆S₂₈: The deformed N = 28 Region

NUCLEAR STRUCTURE ^{28,30,32,34,36,38,40,42,44,46,48,50,52}S; calculated two-neutron separation energies, quadrupole mass deformations, neutron distribution rms radii. Self-consistent mean field theory.

doi: 10.1016/0370-2693(94)90146-5
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1991BE31      Phys.Lett. 267B, 431 (1991)

B.Belgoumene, J.Dudek, T.Werner

A New Realisation of the Realistic Average Field Approach with Density-Dependent Spin-Orbit Term

NUCLEAR STRUCTURE N=83, Z=51; ²⁰⁸Pb, ¹⁴⁶Gd; calculated single particle excitations. ^{157,159,161,163,165,167,169,171,173}Ho; calculated proton-quasiparticle levels. Realistic average field, density-dependent spin-orbit term.

doi: 10.1016/0370-2693(91)90889-X
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1991WE12      Phys.Rev. C44, R948 (1991)

T.R.Werner, J.Dudek

Superdeformation in the Quasicontinuum: Microscopic view of the excited superdeformed bands and the corresponding level densities

NUCLEAR STRUCTURE ¹⁵²Dy, ¹⁴⁹Gd; calculated rotational, superdeformed bands. Microscopic approach, Woods-Saxon potential, extended Strutinsky method.

doi: 10.1103/PhysRevC.44.R948
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1991ZU01      Phys.Lett. 254B, 308 (1991)

K.Zuber, D.Balouka, F.A.Beck, Th.Byrski, D.Curien, G.De France, G.Duchene, C.Gehringer, B.Haas, J.C.Merdinger, P.Romain, D.Santos, J.Styczen, J.P.Vivien, J.Dudek, Z.Szymanski, T.R.Werner

A Comparative Study of Superdeformation in ^146,147,148Gd. Possible Manifestations of the Pseudo-SU₃ Symmetry, Octupole Shape Susceptibility and Superdeformed Deep-Hole Excitations

NUCLEAR REACTIONS ¹²²Sn(³⁰Si, 5n), E=155 MeV; measured Eγ, Iγ, sum spectra. ¹⁴⁷Gd deduced levels, J, π, superdeformed band features. Model comparison.

doi: 10.1016/0370-2693(91)91160-W
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1990DU10      Phys.Lett. 248B, 235 (1990)

J.Dudek, T.R.Werner, Z.Szymanski

Prediction of Octupole-Deformation Effects in Superdeformed Nuclei of A ≈ 150 and A ≈ 190 Mass Regions and Possible Interrelation with Pseudo-Spin Symmetry

NUCLEAR STRUCTURE ¹⁴⁶Nd, ¹⁴⁸Sm, ¹⁵⁰Gd, ¹⁵²Dy, ¹⁵⁴Er, ¹⁵⁶Yb, ^{186,188,190,192,194,196,198,200,202}Hg; calculated potential energy vs deformation parameter; deduced pronounced octupole effects, superdeformed nuclei.

doi: 10.1016/0370-2693(90)90284-D
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1990ZU02      Nucl.Phys. A520, 195c (1990)

K.Zuber, D.Balouka, F.A.Beck, Th.Byrski, D.Curien, G.Duchene, C.Gehringer, B.Haas, J.C.Merdinger, P.Romain, D.Santos, J.Styczen, J.P.Vivien, J.Dudek, Z.Szymanski, T.Werner

Superdeformed Bands in ¹⁴⁷₆₄Gd₈₃, a Possible Test of the Existence of Octupole Correlations in Superdeformed Bands

NUCLEAR REACTIONS ¹²²Sn(³⁰Si, 5n), E=155 MeV; measured Eγ, Iγ. ¹⁴⁷Gd deduced levels, superdeformed band structure.

doi: 10.1016/0375-9474(90)91147-J
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1988DO08      Phys.Rev.Lett. 60, 2254 (1988)

J.Dobaczewski, W.Nazarewicz, J.Skalski, T.Werner

Nuclear Deformation: A proton-neutron effect ( Question )

NUCLEAR STRUCTURE ^{60,62,64,66,68,70,72,74,76,78,80,82}Ge; calculated deformation energy vs quadrupole moment; deduced quadrupole-quadrupole coupling constant. Hartree-Fock method, Skyrme force.

doi: 10.1103/PhysRevLett.60.2254
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1988DU13      Phys.Rev. C38, 940 (1988)

J.Dudek, B.Herskind, W.Nazarewicz, Z.Szymanski, T.R.Werner

Pairing, Temperature, and Deformed-Shell Effects on the Properties of Superdeformed ¹⁵²Dy Nucleus

NUCLEAR STRUCTURE ¹⁵²Dy; calculated barrier heights, potential energy surfaces, high spin behaviour, deformation, superdeformation properties. Strutinsky model.

doi: 10.1103/PhysRevC.38.940
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1988DU15      Phys.Lett. 211B, 252 (1988)

J.Dudek, T.Werner, L.L.Riedinger

Prediction of Hyperdeformed Nuclear States at Very High Spins

NUCLEAR STRUCTURE ¹⁶⁸Yb; calculated total energy surface; deduced high spin hyperdeformed states evidence. ^{166,168,170,172,174}Yb; calculated total energy vs elongation.

doi: 10.1016/0370-2693(88)90898-2
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1988DU16      Phys.Lett. 213B, 120 (1988)

J.Dudek, T.Werner, L.L.Riedinger

Dependence of the First Saddle-Point Energy on Temperature and Spin in Superdeformed Rare-Earth Nuclei

NUCLEAR STRUCTURE ^{146,152,156,162}Dy, ^{152,154,156,158,160,162}Er, ^{148,150,152,154,156,158}Gd, ^{146,148,150,152,154,156}Sm; calculated saddle point energy vs temperature, spin, superdeformation.

doi: 10.1016/0370-2693(88)91010-6
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1982DU17      Phys.Rev. C26, 1712 (1982)

J.Dudek, Z.Szymanski, T.Werner, A.Faessler, C.Lima

Description of the High Spin States in ¹⁴⁶Gd using the Optimized Woods-Saxon Potential

NUCLEAR STRUCTURE ¹⁴⁶Gd; calculated yrast, yrare levels. Optimized Woods-Saxon potential, BCS, particle number projection.

doi: 10.1103/PhysRevC.26.1712
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1981DU04      Phys.Rev. C23, 920 (1981)

J.Dudek, Z.Szymanski, T.Werner

Woods-Saxon Potential Parameters Optimized to the High Spin Spectra in the Lead Region

NUCLEAR STRUCTURE ²⁰⁴Pb, ²¹²Rn; calculated high spin states; deduced optimum parameters of Woods-Saxon potential spin-orbit term.

doi: 10.1103/PhysRevC.23.920
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1979DU07      J.Phys.(London) G5, 1359 (1979)

J.Dudek, A.Majhofer, J.Skalski, T.Werner, S.Cwiok, W.Nazarewicz

Parameters of the Deformed Woods-Saxon Potential Outside A = 110-210 Nuclei

NUCLEAR STRUCTURE A=40-110, A=210-280; calculated single-particle level spins, particles. Deformed Woods-Saxon potential, adjusted strength, radius of spin-orbit term.

doi: 10.1088/0305-4616/5/10/014
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1978DU18      J.Phys.(London) G4, 1543 (1978)

J.Dudek, T.Werner

New Parameters of the Deformed Woods-Saxon Potential for A = 110-210 Nuclei

NUCLEAR STRUCTURE A=110-210; calculated strength, radius parameter of spin-orbit term in deformed Woods-Saxon potential using experimental level schemes, deformation parameters.

doi: 10.1088/0305-4616/4/10/006
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Note: The following list of authors and aliases matches the search parameter T.Werner: , T.R.WERNER