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NSR database version of May 24, 2024.

Search: Author = S.Cwiok

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2005CW01      Eur.Phys.J. A 23, 387 (2005)

S.Cwiok, W.Dudek, P.Kaszynski, W.Nazarewicz

Shell energy in the heaviest nuclei using the Green's function oscillator expansion method

NUCLEAR STRUCTURE 310126, 262Sg, 270Hs; Z=82-128; calculated shell correction energies. 252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282,284,286,288,290,292Hs; calculated shell correction energies, deformation, two-neutron separation energies. Strutinsky smoothing, Green's function approach.

doi: 10.1140/epja/i2004-10111-0
Citations: PlumX Metrics

2005CW02      Nature(London) 433, 705 (2005)

S.Cwiok, P.-H.Heenen, W.Nazarewicz

Shape coexistence and triaxiality in the superheavy nuclei

NUCLEAR STRUCTURE Z=92-128; calculated deformation parameters, Qα for even-even nuclides. 294120, 290Og, 286,292Lv, 288Fl, 284Cn; calculated potential energy surfaces. Self-consistent approach.

doi: 10.1038/nature03336
Citations: PlumX Metrics

2005DU10      Int.J.Mod.Phys. E14, 377 (2005)

W.Dudek, S.Cwiok, P.Kaszynski

Fission barriers in the heaviest nuclei using the Green's function oscillator expansion method

NUCLEAR STRUCTURE 260Rf, 270Hs, 276Cn; calculated potential energy vs β2 along fission path; deduced fission barrier heights, single-particle continuum effects. 276Cn; calculated shell correction energy vs β2 along fission path. Green's function oscillator expansion method.

doi: 10.1142/S0218301305003156
Citations: PlumX Metrics

2003SA02      Eur.Phys.J. A 16, 51 (2003)

M.Sawicka, J.M.Daugas, H.Grawe, S.Cwiok, D.L.Balabanski, R.Beraud, C.Bingham, C.Borcea, M.La Commara, G.de France, G.Georgiev, M.Gorska, R.Grzywacz, M.Hass, M.Hellstrom, Z.Janas, M.Lewitowicz, H.Mach, I.Matea, G.Neyens, C.O'Leary, F.de Oliveira Santos, R.D.Page, M.Pfutzner, Zs.Podolyak, K.Rykaczewski, M.Stanoiu, J.Zylicz

Isomeric decay of 67Fe -- Evidence for deformation

RADIOACTIVITY 67mFe(IT) [from 9Be(76Ge, X)]; measured Eγ, Iγ, T1/2. 67Fe deduced isomeric level energy, possible J, π, deformation, configuration. Mass separator, comparisons with model predictions.

doi: 10.1140/epja/i2002-10073-1
Citations: PlumX Metrics

2002NA18      Nucl.Phys. A701, 165c (2002)

W.Nazarewicz, M.Bender, S.Cwiok, P.H.Heenen, A.T.Kruppa, P.-G.Reinhard, T.Vertse

Theoretical Description of Superheavy Nuclei

NUCLEAR STRUCTURE 257No, 261Rf, 265Sg, 269Hs, 271Ds, 277Cn; calculated levels, J, π, Qα. Z=120; calculated neutron shell correction energies. Skyrme-Hartree-Fock and relativistic mean-field calculations.

doi: 10.1016/S0375-9474(01)01567-6
Citations: PlumX Metrics

2001HO06      Eur.Phys.J. A 10, 5 (2001)

S.Hofmann, F.P.Hessberger, D.Ackermann, S.Antalic, P.Cagarda, S.Cwiok, B.Kindler, J.Kojouharova, B.Lommel, R.Mann, G.Munzenberg, A.G.Popeko, S.Saro, H.J.Schott, A.V.Yeremin

The New Isotope 270110 and Its Decay Products 266Hs and 262Sg

NUCLEAR REACTIONS 207Pb(64Ni, n), E=317 MeV; measured Eα, αα-, (recoil)α-coin following residual nucleus decay; deduced production σ, evidence for 270Ds, 266Hs, 262Sg. Mass separator.

RADIOACTIVITY 270Ds, 266Hs, 262Sg(α) [from 207Pb(64Ni, n)]; measured Eα, T1/2.

doi: 10.1007/s100500170137
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0896.

2001NO03      Acta Phys.Pol. B32, 1113 (2001)

R.Nowakowski, S.Cwiok, W.Nazarewicz, P.-H.Heenen

Single-Nucleon Densities in Superheavy Nuclei

NUCLEAR STRUCTURE Z=92-124; calculated radii and diffuseness parameters. Skyrme-Hartree-Fock plus BCS theory with zero-range pairing force.

2000KR03      Phys.Rev. C61, 034313 (2000)

A.T.Kruppa, M.Bender, W.Nazarewicz, P.-G.Reinhard, T.Vertse, S.Cwiok

Shell Corrections of Superheavy Nuclei in Self-Consistent Calculations

NUCLEAR STRUCTURE Z=120; calculated neutron single-particle levels, shell corrections. Z=110-130; calculated proton shell corrections, macroscopic energies. Self-consistent Skyrme-Hartree-Fock and relativistic mean field calculations.

doi: 10.1103/PhysRevC.61.034313
Citations: PlumX Metrics

1999CW01      Phys.Rev.Lett. 83, 1108 (1999)

S.Cwiok, W.Nazarewicz, P.H.Heenen

Structure of Odd-N Superheavy Elements

NUCLEAR STRUCTURE 293Og, 289,293Lv, 285,289Fl, 281,285Cn, 277,281Ds, 273,277Hs, 269Sg, 265Rf; calculated single quasiparticle levels, configurations, deformation. Z=96-118; calculated α-decay energies for even-even nuclides. Self-consistent Skyrme-Hartree-Fock-Bogoliubov method with pairing.

doi: 10.1103/PhysRevLett.83.1108
Citations: PlumX Metrics

1999MU05      Phys.Rev. C59, 2009 (1999)

W.F.Mueller, H.Q.Jin, J.M.Lewis, W.Reviol, L.L.Riedinger, M.P.Carpenter, C.Baktash, J.D.Garrett, N.R.Johnson, I.Y.Lee, F.K.McGowan, C.-H.Yu, S.Cwiok

High-Spin Structure in 181, 183Au

NUCLEAR REACTIONS 152Sm(35Cl, 4n), E=170 MeV; 150Sm(35Cl, 4n), E=168 MeV; measured Eγ, Iγ, γγ-coin. 181,183Au deduced high-spin levels, J, π, configurations, rotational band features.

NUCLEAR STRUCTURE 169,171,173,175,177,179Re, 171,173,175,177,179,181,183Ir, 177,179,181,183,185Au; calculated bandhead excitation energies, configurations, deformation parameters. 179Ir, 181,183,185Au; calculated Routhians, B(M1)/B(E2). Macroscopic-microscopic shell correction model.

doi: 10.1103/PhysRevC.59.2009
Citations: PlumX Metrics

1996CW01      Nucl.Phys. A611, 211 (1996)

S.Cwiok, J.Dobaczewski, P.-H.Heenen, P.Magierski, W.Nazarewicz

Shell Structure of the Superheavy Elements

NUCLEAR STRUCTURE Z=108-128; N=150-192; calculated superheavy nuclei potential energy surfaces, ground state deformations, Q(α), α-decay T1/2, fission barriers in some cases. Skyrme-Hartree-Fock with density-independent contact pairing interaction, macroscopic-microscopic approaches.

doi: 10.1016/S0375-9474(96)00337-5
Citations: PlumX Metrics

1996TE04      Phys.Rev.Lett. 77, 32 (1996)

G.M.Ter-Akopian, J.H.Hamilton, Yu.Ts.Oganessian, A.V.Daniel, J.Kormicki, A.V.Ramayya, G.S.Popeko, B.R.S.Babu, Q.-H.Lu, K.Butler-Moore, W.-C.Ma, S.Cwiok, W.Nazarewicz, J.K.Deng, D.Shi, J.Kliman, M.Morhac, J.D.Cole, R.Aryaeinejad, N.R.Johnson, I.Y.Lee, F.K.McGowan, J.X.Saladin

New Spontaneous Fission Mode for 252Cf: Indication of hyperdeformed 144,145,146Ba at scission

RADIOACTIVITY 252Cf(SF); measured γγ-coin, prompt neutron multiplicities, Mo, Ba isotopes correlated fragment pairs yields; deduced new fission mode. 144,145,146Ba deduced hyperdeformed shape evidence at scission.

doi: 10.1103/PhysRevLett.77.32
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13648.

1995NA13      Acta Phys.Pol. B26, 189 (1995)

W.Nazarewicz, S.Cwiok, J.Dobaczewski, J.X.Saladin

Multiclustering and Physics of Exotic Nuclear Shapes

NUCLEAR STRUCTURE 220,224Rn, 222,226,230Ra, 224,228,232Th, 226,230,234U; compiled, reviewed, analyzed potential energy surface predictions; deduced hyperdeformed minimum resemblance to di-nucleus. Multi-cluster model.

1994CW01      Phys.Lett. 322B, 304 (1994)

S.Cwiok, W.Nazarewicz, J.X.Saladin, W.Plociennik, A.Johnson

Hyperdeformations and Clustering in the Actinide Nuclei

NUCLEAR STRUCTURE 220,222Ra, 232Th, 234U; calculated Woods-Saxon-Strutinsky total potential energy vs deformation parameters β2, β3; deduced hyperdeformed minima features. Shell correction approach.

doi: 10.1016/0370-2693(94)91157-6
Citations: PlumX Metrics

1994CW02      Nucl.Phys. A573, 356 (1994)

S.Cwiok, S.Hofmann, W.Nazarewicz

Shell Structure of the Heaviest Elements

NUCLEAR STRUCTURE Z=95-111; N=149-162; compiled, reviewed mass excess, equilibrium deformations, single nucleon states binding energy, Q(α).

doi: 10.1016/0375-9474(94)90349-2
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1993MA40      Phys.Rev. C48, 1686 (1993)

P.Magierski, S.Cwiok, J.Dobaczewski, W.Nazarewicz

Approximate Particle Number Projection for Rotating Nuclei

doi: 10.1103/PhysRevC.48.1686
Citations: PlumX Metrics

1992CW01      Z.Phys. A342, 203 (1992)

S.Cwiok, A.Sobiczewski

Potential Energy and Fission Barriers of Superheavy Nuclei Calculated in Multidimensional Deformation Space

NUCLEAR STRUCTURE 276Cn, 298Fl; calculated potential energy contours vs deformations β2, β4; Z=112-130; N=152-210; calculated β20, β40, β60 equilibrium deformations contour, fission barriers. Macroscopic-microscopic method, multi-dimensional deformation space.

1991CW01      Nucl.Phys. A529, 95 (1991)

S.Cwiok, W.Nazarewicz

Reflection-Asymmetric Shapes in Odd-A Actinide Nuclei

NUCLEAR STRUCTURE 219,221,223,225Fr, 219,221,223,225,227Ac, 221,223,225,227,229Pa, 219,221,223,225Rn, 219,221,223,225,227Ra, 221,223,225,227Th; calculated levels, equilibrium deformations, asymmetry energies, parity contents. Average Woods-Saxon potential, monopole pairing residual interaction, reflection-asymmetric mean field approach.

doi: 10.1016/0375-9474(91)90787-7
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1991EN01      Nucl.Phys. A535, 392 (1991); Erratum Nucl.Phys. A560, 1079 (1993)

P.J.Ennis, C.J.Lister, W.Gelletly, H.G.Price, B.J.Varley, P.A.Butler, T.Hoare, S.Cwiok, W.Nazarewicz

Triaxiality and Isospin-Forbidden E1 Decays in the N = Z Nucleus 64Ge

NUCLEAR REACTIONS 12C(54Fe, 2n), E=165 MeV; 54Fe(12C, 2n), E=37 MeV; measured Eγ, Iγ(θ), γγ-coin; deduced absorption σ. 64Ge deduced levels, J, π. Germanium detector array, recoil separator.

doi: 10.1016/0375-9474(91)90454-E
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1991SA12      Nucl.Phys. A529, 289 (1991)

W.Satula, S.Cwiok, W.Nazarewicz, R.Wyss, A.Johnson

Structure of Superdeformed States in Au-Ra Nuclei

NUCLEAR STRUCTURE 190,192,194,196Hg, 192,194,196,198Pb, 194,196,198,200,202Po, 198,200,202,204,206Rn, 204,206,208,210,212Ra; calculated superdeformed state energies, equilibrium deformations, band head energies, barrier heights, potential energy surfaces. 189,191,193,195,190,192,194,196Tl, 187,189,191,193,195Au; calculated equilibrium deformations. Strutinsky shell correction method.

doi: 10.1016/0375-9474(91)90797-A
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1990BR23      J.Phys.(London) G16, 1735 (1990)

Ch.Briancon, S.Cwiok, S.A.Eid, V.Green, W.D.Hamilton, C.F.Liang, R.J.Walen

A Re-Examination of the Band Structure of 223Ra and Reflection Asymmetry in this Nucleus

RADIOACTIVITY 227Th(α); measured γγ(θ), αγ(θ), γ(θ), oriented nuclei, Eγ, Iγ, recoil distance. 223Ra deduced levels, J, π, band structure, T1/2, ICC, δ.

doi: 10.1088/0954-3899/16/11/021
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1990MA45      Phys.Rev. C42, R811 (1990)

H.Mach, S.Cwiok, W.Nazarewicz, B.Fogelberg, M.Moszynski, J.Winger, R.L.Gill

Strong Octupole and Dipole Collectivity in 96Zr: Indication for octupole instability in the A = 100 mass region

RADIOACTIVITY 96Y(β-) [from 235U(n, F)]; measured βγγ(t). 96Zr level deduced T1/2, B(λ). RPA, deformed shell model calculations.

NUCLEAR STRUCTURE 96Zr; calculated total energy surfaces. Woods-Saxon potential, pairing.

doi: 10.1103/PhysRevC.42.R811
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1989CW01      Nucl.Phys. A491, 281 (1989)

S.Cwiok, P.Rozmej, A.Sobiczewski, Z.Patyk

Two Fission Modes of the Heavy Fermium Isotopes

NUCLEAR STRUCTURE 254,258Fm, 272Hs; calculated fission barrier shapes, potential energy surfaces; deduced deformations role.

doi: 10.1016/0375-9474(89)90703-3
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1989CW02      Nucl.Phys. A496, 367 (1989)

S.Cwiok, W.Nazarewicz

Ground-State Shapes and Spectroscopic Properties of Z ≈ 58, N ≈ 88 Nuclei

NUCLEAR STRUCTURE Z ≈ 58; N ≈ 88; calculated ground state shapes. Deformed shell model.

doi: 10.1016/0375-9474(89)90180-2
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1989CW03      Phys.Lett. 224B, 5 (1989)

S.Cwiok, W.Nazarewicz

Reflection-Asymmetric Shapes in Transitional Odd-A Th Isotopes

NUCLEAR STRUCTURE 219,221,223,225,227,229Th; calculated quasiparticle states, band heads, equilibrium deformations. Reflection-asymmetric mean field theory.

doi: 10.1016/0370-2693(89)91039-3
Citations: PlumX Metrics

1989PA22      Nucl.Phys. A502, 591c (1989)

Z.Patyk, J.Skalski, A.Sobiczewski, S.Cwiok

Potential Energy and Spontaneous-Fission Half-Lives for Heavy and Superheavy Nuclei

NUCLEAR STRUCTURE Z=100-130; N=140-210; calculated potential energies, SF T1/2. Macroscopic-microscopic method.

doi: 10.1016/0375-9474(89)90691-X
Citations: PlumX Metrics

1989SC33      Phys.Rev.Lett. 63, 2645 (1989)

N.Schulz, V.Vanin, M.Aiche, A.Chevallier, J.Chevallier, J.C.Sens, Ch.Briancon, S.Cwiok, E.Ruchowska, J.Fernandez-Niello, Ch.Mittag, J.Dudek

Persisting Domination of the Octupole over the Quadrupole Degrees of Freedom and the New Type of Transitional Nuclei: High-spin behavior of 218Ra

NUCLEAR REACTIONS 208Pb(14C, 4n), E=80 MeV; measured γγ(t), γ-spectra. 218Ra deduced levels, J, π.

doi: 10.1103/PhysRevLett.63.2645
Citations: PlumX Metrics

1989SO03      Phys.Lett. 224B, 1 (1989)

A.Sobiczewski, Z.Patyk, S.Cwiok

Deformed Superheavy Nuclei

NUCLEAR STRUCTURE N=150-190; Z=100-130; calculated equilibrium deformation, deformation energy, total T1/2 contours. Deformed superheavy nuclei.

doi: 10.1016/0370-2693(89)91038-1
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1988RO05      Phys.Lett. 203B, 197 (1988)

P.Rozmej, S.Cwiok, A.Sobiczewski

Is Octupole Deformation Sufficient to Describe the Properties of ' Octupolly ' Unstable Nuclei ( Question )

NUCLEAR STRUCTURE 216,218,220,222,224,226,228Ra; calculated deformation energy, equilibrium deformation.

doi: 10.1016/0370-2693(88)90537-0
Citations: PlumX Metrics

1988SO08      Nucl.Phys. A485, 16 (1988)

A.Sobiczewski, Z.Patyk, S.Cwiok, P.Rozmej

Study of the Potential Energy of ' Octupole '-Deformed Nuclei in a Multidimensional Deformation Space

NUCLEAR STRUCTURE 218,220,222,224,226Ra; calculated potential energy surfaces. 216,218,220,222,224,226Rn, 216,218,220,222,224,226,228Ra, 218,220,222,224,226,228Th, 220,222,224,226,228U, 222,224,226,228Pu, 224,226,228Cm, 226,228,230Cf, 138,140,142,144,146,148Xe, 140,142,144,146,148,150,152Ba, 144,142,146,148,150Ce, 144,146,148Nd; calculated equilibrium deformation, energy. Multi-dimensional deformation space, macroscopic-microscopic method.

doi: 10.1016/0375-9474(88)90519-2
Citations: PlumX Metrics

1987SO03      Phys.Lett. 186B, 6 (1987)

A.Sobiczewski, Z.Patyk, S.Cwiok

Do the Superheavy Nuclei Really Form an Island ( Question )

RADIOACTIVITY Z=104-110(SF), (α); calculated fission barrier heights, T1/2. Liquid-drop energy, shell correction.

doi: 10.1016/0370-2693(87)90502-8
Citations: PlumX Metrics

1986BO37      Z.Phys. A325, 479 (1986)

K.Boning, Z.Patyk, A.Sobiczewski, S.Cwiok

Theoretical Half-Lives for the Heaviest Nuclei

RADIOACTIVITY Z=100-110(SF), (α); calculated SF-decay, α-decay T1/2.

1985CW01      Nucl.Phys. A444, 1 (1985)

S.Cwiok, Z.Lojewski, V.V.Pashkevich

Fission Barriers of Odd-Mass Nuclei and Odd Nuclei with 100 ≤ Z ≤ 111

NUCLEAR STRUCTURE 259,261,257,255,253,251,249,247,245,243Fm, 246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262,263Md, 243,245,246,249,251,253,255,257,259,261,263No, 254,255,256,257,258,259,260,261,262,263,264,265Lr, 251,253,255,257,259,261,263,265Rf, 254,255,256,257,258,259,260,261,262,263,264,265,266,267Db, 257,259,261,263,265,267Sg, 258,259,260,261,262,263,264,265,266,267,268,269,270,271Bh, 259,261,263,265,267,269,271Hs, 262,263,264,265,266,267,268,269,270,271Mt, 263,265,267,269,271,273,275Ds, 267,268,269,270,271,272,273,274,275,276,277,278Rg; calculated deformation energy along fission barrier vs β2, fission barrier vs neutron number. Strutinsky method, realistic Woods-Saxon potential.

doi: 10.1016/0375-9474(85)90288-X
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1985KV02      Czech.J.Phys. B35, 949 (1985)

J.Kvasil, M.M.Chariev, S.Cwiok, P.Holan

Non-Adiabatic Effects and Coriolis Interactions in Odd Deformed Nuclei

NUCLEAR STRUCTURE 235U; calculated levels, rotational band structure. Quasiadiabatic approach.

doi: 10.1007/BF01676358
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1985KV03      Yad.Fiz. 42, 588 (1985)

J.Kvasil, M.Chariev, S.Cwiok, V.Choriev, I.N.Mikhailov

Description of the Negative Parity States in 158Dy and 168Er in the Framework of Random Phase Approximation Based on the Cranking Model

NUCLEAR STRUCTURE 158Dy, 168Er; calculated levels, B(λ). RPA, cranking model.

1985LO05      Nucl.Phys. A436, 499 (1985)

Z.Lojewski, V.V.Pashkevich, S.Cwiok

Excitation Effects on the Nuclear-Fission Process in the Heaviest Elements

NUCLEAR STRUCTURE 260No, 264Rf, 268Sg; calculated fission barriers. Quantum statistical approach, nuclear heating effect.

doi: 10.1016/0375-9474(85)90082-X
Citations: PlumX Metrics

1984KV04      Czech.J.Phys. B34, 1179 (1984)

J.Kvasil, M.M.Chariev, S.Cwiok, I.N.Mikhailov, B.Choriev

Application of the RPA Method Based on the Cranked Hartree-Fock-Bogolubov Model in 168Er and 158Dy

NUCLEAR STRUCTURE 158Dy, 168Er; calculated levels, B(E2). Cranked HFB based RPA.

doi: 10.1007/BF01590065
Citations: PlumX Metrics

1984MI08      Yad.Fiz. 39, 1368 (1984)

I.N.Mikhailov, R.G.Nazmitdinov, S.Cwiok

Evolution of the Shape of Fast Rotating Nuclei and of the γ Spectrum

NUCLEAR STRUCTURE 118Te; calculated potential energy surfaces, shape evolution, Iγ. 118Te deduced γ-multipolarity. Strutinsky method, cranking model.

1983CW01      Nucl.Phys. A410, 254 (1983)

S.Cwiok, V.V.Pashkevich, J.Dudek, W.Nazarewicz

Fission Barriers of Transfermium Elements

NUCLEAR STRUCTURE 242,244,246,248,250,252,254,256,258Fm, 250,252,254,256,258,260,262,264,266No, 254Rf, 256Rf, 258Rf, 260Rf, 262Rf, 264Rf; calculated fission barriers; deduced possible nuclear isomers, fission barrier separation. Strutinsky method.

doi: 10.1016/0375-9474(83)90201-4
Citations: PlumX Metrics

1983CW02      Z.Phys. A314, 337 (1983)

S.Cwiok, I.N.Mikhailov, Ch.Briancon

The Shape of Fast-Rotating Nuclei in the Region of Subshell N = 82

NUCLEAR STRUCTURE 146,148,150,152,154,158Er; calculated free energy surfaces. 154,148Er; calculated moment of inertia vs rotational frequency square. 156,158,160,162,164Er; calculated oblate to prolate spin transition. 158Er; calculated equilibrium deformation. 158Er; calculated stretched E2 transition strengths, yrast line. Strutinsky shell correction, Woods-Saxon potentials, nonaxial hexadecapole deformations.

doi: 10.1007/BF01412930
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1980CW01      Nucl.Phys. A333, 139 (1980)

S.Cwiok, W.Nazarewicz, J.Dudek, J.Skalski, Z.Szymanski

Microscopic Analysis of the Double Backbending in the Nucleus 160Yb

NUCLEAR STRUCTURE 160Yb; calculated double back-bending effects. Cranked Hartree-Fock-Bogoliubov method, deformed Woods-Saxon potential, monopole pairing terms.

doi: 10.1016/0375-9474(80)90019-6
Citations: PlumX Metrics

1980CW02      Phys.Rev. C21, 448 (1980)

S.Cwiok, W.Nazarewicz, J.Dudek, Z.Szymanski

Analysis of the Backbending Effect in 166Yb, 168Yb, and 170Yb within the Hartree-Fock-Bogolyubov Cranking Method

NUCLEAR STRUCTURE 166,168,170Yb; calculated moments of inertia. Cranked Hartree-Fock-Bogoliubov method.

doi: 10.1103/PhysRevC.21.448
Citations: PlumX Metrics

1980CW03      Acta Phys.Pol. B11, 445 (1980)

S.Cwiok, W.Nazarewicz, W.Zych

The Dependence of Coulomb Displacement Energy on Deformation of a Nucleus

NUCLEAR STRUCTURE 149,151Nd, 149,151Pm, 169Er, 169Tm, 169,171Yb, 169,171Lu; calculated Coulomb displacement energies; deduced deformation effects. Woods-Saxon deformed potential, monopole pairing interaction.

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
Citations: PlumX Metrics

1976CW01      Acta Phys.Pol. B7, 375 (1976)

S.Cwiok, W.Zych

Coulomb Displacement Energy in the Isobaric Analog Pairs Ti-V

NUCLEAR STRUCTURE 49Ca, 49Sc;49Ti, 49V;51Ti, 51V; calculated Coulomb displacement energies.

1975CW01      Acta Phys.Pol. B6, 105 (1975)


Spin Vibration States in 120Sn and 208Pb within ΔN = 0 and ΔN = 2

NUCLEAR STRUCTURE 120Sn, 208Pb; calculated levels, wavefunctions, Γ(M1).

1973CW01      Acta Phys.Pol. B4, 233 (1973)

S.Cwiok, M.Wygonowska

Excited States Jπ = 1+ in Spherical Nuclei

NUCLEAR STRUCTURE 55Ni, 114,116,118,120,122,124Sn, 138Ba, 140Ce, 142Nd, 208Pb; calculated levels, level-width.

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