References quoted in the ENSDF dataset: 190HG 160GD(34S,4NG):SD

86 references found.

Clicking on a keynumber will list datasets that reference the given article.


1990BE37

Nucl.Phys. A520, 187c (1990)

J.A.Becker, N.Roy, E.A.Henry, S.W.Yates, A.Kuhnert, J.E.Draper, W.Korten, C.W.Beausang, M.A.Deleplanque, R.M.Diamond, F.S.Stephens, W.H.Kelly, F.Azaiez, J.A.Cizewski, M.J.Brinkman

Level Spin and Moments of Inertia in Superdeformed Nuclei Near A = 194

NUCLEAR STRUCTURE 190,191,192,193,194Hg, 194,196Pb, 193,194Tl; analyzed data; deduced levels, J, superdeformed band parameters. Least-squares fit to rotational formulas.

doi: 10.1016/0375-9474(90)91146-I


1990BO40

Nucl.Phys. A519, 509 (1990)

P.Bonche, J.Dobaczewski, H.Flocard, P.H.Heenen, S.J.Krieger, J.Meyer, M.S.Weiss

Quadrupole Collective Correlations and the Depopulation of the Superdeformed Bands in Mercury

NUCLEAR STRUCTURE 190,192,194,196,198Hg; calculated deformation energy, wave functions, proton quadrupole moments, superdeformed band decay Iγ. Self-consistent generator coordinate method, Hartree-Fock plus BCS wave functions.

doi: 10.1016/0375-9474(90)90443-P


1990CH24

Phys.Lett. 242B, 317 (1990)

R.R.Chasman

The Effects of Pairing on Superdeformed Rotational Bands Near A = 190

NUCLEAR STRUCTURE 190,191,192,193,194Hg, 193,194Tl; calculated superdeformed level second moments of inertia.

doi: 10.1016/0370-2693(90)91768-7


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, 186,188,190,192,194,196,198,200,202Hg; calculated potential energy vs deformation parameter; deduced pronounced octupole effects, superdeformed nuclei.

doi: 10.1016/0370-2693(90)90284-D


1990HO13

Z.Phys. A336, 363 (1990)

J.Holler, S.Aberg

Octupole Instability of Super- and Hyperdeformed Nuclei

NUCLEAR STRUCTURE 152Dy, 190,194Hg, 200Rn; calculated potential energy surfaces; deduced possible superdeformation, hyperdeformation. 146Gd, 152Dy, 194,190Hg, 196Pb, 198Po, 200Rn; calculated octupole softness; deduced possible superdeformation. Cranked Nilsson-Strutinsky model.


1990JA13

Nucl.Phys. A520, 75c (1990)

R.V.F.Janssens, M.P.Carpenter, M.W.Drigert, P.B.Fernandez, E.F.Moore, D.Ye, I.Ahmad, K.B.Beard, I.G.Bearden, Ph.Benet, P.J.Daly, U.Garg, Z.W.Grabowski, T.L.Khoo, W.Reviol, F.L.H.Wolfs

Superdeformation in the Mercury Nuclei

NUCLEAR STRUCTURE 194,196Pb, 193,194Tl, 189,190,191,192,193,194Hg; compiled, analyzed superdeformed band data.

doi: 10.1016/0375-9474(90)91135-E


1991CH36

Phys.Lett. 266B, 243 (1991)

R.R.Chasman

Superdeformed and Hyperdeformed Banana Shaped Nuclides Near A = 190

NUCLEAR STRUCTURE 190Pt, 189,190,191,192Au, 188,189,190,191,192,193,194,195Hg, 189,190,191,192,193,194,195Tl, 190,191,192,193Pb, 193,194,195,196Bi, 194Po; calculated level energy relative to prolate mininum, barrier heights, reflection symmetric shapes; deduced superdeformed, hyperdeformed minima, deformation features.

doi: 10.1016/0370-2693(91)91033-R


1991DR04

Nucl.Phys. A530, 452 (1991)

M.W.Drigert, M.P.Carpenter, R.V.F.Janssens, E.F.Moore, I.Ahmad, P.B.Fernandez, T.L.Khoo, F.L.H.Wolfs, I.G.Bearden, Ph.Benet, P.J.Daly, U.Garg, W.Reviol, D.Ye, R.Wyss

Superdeformed Bands in 189,190Hg

NUCLEAR REACTIONS 160Gd(34S, xn), E=159, 162 MeV; measured Eγ, Iγ, γγ-coin, DSA. 189,190Hg deduced levels, J, π, T1/2, superdeformed band characteristics. Enriched targets, Ge detectors, array of anti-Compton spectrometers, 4π bismuth germanate ball. Cranked Woods-Saxon model calculations.

doi: 10.1016/0375-9474(91)90813-L


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


1992BE25

Phys.Rev. C46, 889 (1992)

J.A.Becker, E.A.Henry, A.Kuhnert, T.F.Wang, S.W.Yates, R.M.Diamond, F.S.Stephens, J.E.Draper, W.Korten, M.A.Deleplanque, A.O.Macchiavelli, F.Azaiez, W.H.Kelly, J.A.Cizewski, M.J.Brinkman

Level Spin for Superdeformed Nuclei Near A = 194

NUCLEAR STRUCTURE 189,190,191,192,193,194Hg, 192,194,196,198Pb, 193,194,195Tl; analyzed superdeformed band transition Eγ; deduced J, π. Power series expansion approach.

doi: 10.1103/PhysRevC.46.889


1992BEZL

Proc.Int.Conf.Nuclear Structure at High Angular Momentum, Ottawa, p.10 (1992); AECL-10613 (1992)

I.G.Bearden, R.V.F.Janssens, M.P.Carpenter, I.Ahmad, P.J.Daly, M.W.Drigert, U.Garg, T.L.Khoo, T.Lauritsen, Y.Liang, W.Reviol, R.Wyss

Higher Superdeformed Band Members in 190Hg: Evidence for a band interaction ( Question )

NUCLEAR REACTIONS 160Gd(34S, 4n), E=159-165 MeV; measured γγ-coin, γ-multiplicity. 190Hg deduced superdeformed band, dynamic moment of inertia, band interaction evidence.


1992FA02

Phys.Lett. 276B, 427 (1992)

P.Fallon, W.Nazarewicz, M.A.Riley, R.Wyss

The Influence of Pairing on the Properties of ' Identical ' Superdeformed Bands in Hg Nuclei

NUCLEAR STRUCTURE 190,191,192,193,194Hg; analyzed band structure data; deduced good reference for superdeformed bands, neutron pairing relative magnitude.

doi: 10.1016/0370-2693(92)91662-S


1992ME01

Phys.Rev. C45, 233 (1992)

M.Meyer, N.Redon, P.Quentin, J.Libert

Superdeformed Single-Particle Orbitals in the A = 190 Region from Hartree-Fock Plus BCS Calculations

NUCLEAR STRUCTURE 192,194,196,198,200Pb, 194,192,190Hg; calculated superdeformed nucleon state components, spectra; deduced particle number symmetry restoration role. Self-consistent axial Hartree-Fock plus BCS.

doi: 10.1103/PhysRevC.45.233


1992WU01

Phys.Rev. C45, 261 (1992)

C.S.Wu, J.Y.Zeng, Z.Xing, X.Q.Chen, J.Meng

Spin Determination and Calculation of Nuclear Superdeformed Bands in A ≈ 190 Region

NUCLEAR STRUCTURE 190,191,192,193,194Hg, 193,194Tl, 194,196Pb; calculated superdeformed bands, transition energies. Two-parameter approach.

doi: 10.1103/PhysRevC.45.261


1993AB08

Nucl.Phys. A557, 17c (1993)

S.Aberg

Superdeformed Nuclei

NUCLEAR STRUCTURE 146,150Gd, 151Tb, 152Dy, 188,190,191,192,193,194Hg; compiled, reviewed superdeformed band related data. 146Gd deduced hyperdeformation evidence. Other nuclei included.

doi: 10.1016/0375-9474(93)90528-6


1993CA23

Nucl.Phys. A557, 57c (1993)

M.P.Carpenter, R.V.F.Janssens, Y.Liang, I.G.Bearden, I.Ahmad, M.W.Drigert, U.Garg, R.G.Henry, J.M.Lewis, T.L.Khoo, T.Lauritsen, S.Pilotte, W.Reviol, L.L.Riedinger, F.Soramel, C.-H.Yu

New Results on Superdeformed Bands in Hg and Tl Nuclei

NUCLEAR REACTIONS 159Tb(36S, 4n), E=165 MeV; 160Gd(37Cl, 5n), E=178, 181 MeV; analyzed data. 191,192Tl, 190Hg deduced levels, J, π, superdeformed bands. Other data input.

doi: 10.1016/0375-9474(93)90530-B


1993HU06

Chin.J.Nucl.Phys. 15, No 1, 45 (1993)

J.Hu, C.Zheng

Spin Determination of Superdeformed Bands, A - 190 and A - 150 Regions

NUCLEAR STRUCTURE 190,191,192,193,194Hg, 193,194Tl, 194,196,198Pb, 146,147,148,149,150Gd, 150,151Tb, 151,152,153Dy; analyzed level spectra, Eγ; deduced superdeformed band states spin. Different methods.


1993LI09

Nucl.Phys. A553, 523c (1993)

J.Libert, J.F.Berger, J.P.Delaroche, M.Girod

Microscopic Description of Superdeformed Bands in 190,192,194Hg

NUCLEAR STRUCTURE 190,192,194Hg; calculated levels, normal, superdeformation bands. Microscopic model.

doi: 10.1016/0375-9474(93)90652-E


1993MI10

Nucl.Phys. A557, 125c (1993)

S.Mizutori, T.Nakatsukasa, K.Arita, Y.R.Shimizu, K.Matsuyanagi

Octupole Correlations in Superdeformed High-Spin States

NUCLEAR STRUCTURE 158,156,154,152,150,148,146,144,142Gd, 184,186,188,190,192,194,196,198,200Hg; calculated curvature against octupole deformation, stretched octupole strengths; deduced octupole instability, superdeformed shape relationship.

doi: 10.1016/0375-9474(93)90536-7


1993NA05

Phys.Lett. 305B, 195 (1993)

W.Nazarewicz

Variety of Shapes in the Mercury and Lead Isotopes

NUCLEAR STRUCTURE 166,168,170,172,174,176,178,180,182,184,186,188,190,192,194,196,198,200Hg, 178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210Pb; calculated shape coexistence configurations excitation energies; deduced prolate, oblate shapes competition. Axial reflection-asymmetric Woods-Saxon model. Other nuclei, intruder states discussed.

doi: 10.1016/0370-2693(93)90107-S


1993PI03

Z.Phys. A345, 7 (1993)

R.Piepenbring, K.V.Protasov

Model of Superfluid Liquid with Triplet Pairing, Cranking Model and Model of Variable Moment of Inertia in Superdeformed Bands in A ≈ 190 Region

NUCLEAR STRUCTURE 189,190,191,193,194Hg, 194,196Pb, 193,194Tl; calculated superdeformed band states transition energies; deduced spin assignments. Triplet pairing model.


1994CR08

Phys.Lett. 333B, 320 (1994)

B.Crowell, R.V.F.Janssens, M.P.Carpenter, I.Ahmad, S.Harfenist, R.G.Henry, T.L.Khoo, T.Lauritsen, D.Nisius, A.N.Wilson, J.F.Sharpey-Schafer, J.Skalski

Superdeformed Band with a Unique Decay Pattern: Possible evidence for octupole vibration in 190Hg

NUCLEAR REACTIONS 160Gd(34S, 4n), E=163 MeV; measured γγ-coin. 190Hg deduced high-spin levels, J, π, superdeformed band transitions, dynamic moment of inertia, shape features.

doi: 10.1016/0370-2693(94)90149-X


1994GA22

Z.Phys. A348, 183 (1994)

B.Gall, P.Bonche, J.Dobaczewski, H.Flocard, P.-H.Heenen

Superdeformed Rotational Bands in the Mercury Region. A Cranked Skyrme-Hartree-Fock-Bogoliubov Study

NUCLEAR STRUCTURE 190,192,194Hg, 194Pb; calculated superdeformed bands moment of inertia, proton, neutron pairing energies, charge quadrupole moments versus angular velocity. Cranked Skyrme-Hartree-Fock-Bogoliubov method.


1994PA29

Phys.Rev. C50, 1924 (1994)

S.K.Patra, S.Yoshida, N.Takigawa, C.R.Praharaj

Shape and Superdeformed Structure in Hg Isotopes in Relativistic Mean Field Model

NUCLEAR STRUCTURE 170,172,174,176,178,180,182,184,186,188,190,192,194,196,198,200Hg; calculated binding energy, quadrupole deformation parameter, hexadecupole moment, charge, rms radii. Relativistic mean field theory.

doi: 10.1103/PhysRevC.50.1924


1994SA41

Phys.Rev. C50, 2888 (1994)

W.Satula, R.Wyss

Coherence of Nucleonic Motion in Superdeformed Nuclei: Towards an understanding of identical bands

NUCLEAR STRUCTURE 190,192,194,196Hg, 192,194,196,198Pb; calculated superdeformed bands dynamical moments of inertia. Cranked Strutinsky-Lipkin-Nogami approach, self-consistent treatment of deformation, pairing effects.

doi: 10.1103/PhysRevC.50.2888


1994SK02

Phys.Rev. C49, 2011 (1994)

J.Skalski

Octupole-Induced Dipole Moments of Very Deformed Nuclei

NUCLEAR STRUCTURE 224Ra, 192Hg; calculated dipole moments vs β2, β3 deformation. 190,192,194Hg, 192,194,196Pb; calculated intrinsic dipole moments at superdeformed shape vs β3 deformation. Shell correction method.

doi: 10.1103/PhysRevC.49.2011


1994ZH40

Chin.J.Nucl.Phys. 16, No 1, 85 (1994)

C.Zhou, T.Liu

Level Spin Assignment of Superdeformed Bands for A ≈ 190 Region

NUCLEAR STRUCTURE 189,190,191,192,193,194Hg, 193,194,195Tl, 192,194,196,198Pb; analyzed superdeformed bands data; deduced J assignment in some cases.


1995BB02

Int.J.Mod.Phys. E4, 385 (1995)

R.Barbier, J.Meyer, M.Kibler

A U(qp)(u2) Rotor Model for Rotational Bands of Superdeformed Nuclei

NUCLEAR STRUCTURE 130La, 132Ce, 134,136Nd, 146,148,150Gd, 152Dy, 190,192,194Hg, 192,194,196,198Pb, 194Tl; analyzed superdeformed band associated transitions Eγ, Iγ. Nonrigid rotor model based on two-parameter U(qp)(u2) quantum algebra.

doi: 10.1142/S0218301395000122


1995CI05

Phys.Rev. C52, 1307 (1995)

J.A.Cizewski, R.Bijker, J.A.Becker, M.J.Brinkman, E.A.Henry, F.S.Stephens, M.A.Deleplanque, R.M.Diamond

Spin-Rotor Interpretation of Identical Bands and Quantized Alignment in Superdeformed A ≈ 190 Nuclei

NUCLEAR STRUCTURE 191,192,193,194Hg, 193,194Tl, 194Pb; analyzed identical bands, superdeformed nuclei; calculated level spectra, γ- transition energies. Pseudo-SU(3) symmetries, supersymmetries.

doi: 10.1103/PhysRevC.52.1307


1995CR02

Phys.Rev. C51, R1599 (1995)

B.Crowell, M.P.Carpenter, R.V.F.Janssens, D.J.Blumenthal, J.Timar, A.N.Wilson, J.F.Sharpey-Schafer, T.Nakatsukasa, I.Ahmad, A.Astier, F.Azaiez, L.du Croux, B.J.P.Gall, F.Hannachi, T.L.Khoo, A.Korichi, T.Lauritsen, A.Lopez-Martens, M.Meyer, D.Nisius, E.S.Paul, M.G.Porquet, N.Redon

Relative Spins and Excitation Energies of Superdeformed Bands in 190Hg: Further evide4nce for octupole vibration

NUCLEAR REACTIONS 160Gd(34S, 4n), E ≈ 158 MeV; measured Eγ, relative Eγ, relative Iγ, γγγ-coin, DCO ratios. 190Hg deduced high-spin levels, J, π, J2 moments of inertia, B(λ), relative excitation energy between two superdeformed bands. Comparison with RPA calculations.

doi: 10.1103/PhysRevC.51.R1599


1995KU17

Phys.Lett. 349B, 253 (1995)

S.Kuyucak, S.C.Li

1/N Expansion Formalism for High-Spin States

NUCLEAR STRUCTURE 190,192,194Hg; calculated dynamic moments of inertia; deduced normal, superdeformed nuclei high-spin states analysis implications.

doi: 10.1016/0370-2693(95)00276-Q


1995TE03

Nucl.Phys. A593, 1 (1995)

J.Terasaki, P.-H.Heenen, P.Bonche, J.Dobaczewski, H.Flocard

Superdeformed Rotational Bands with Density Dependent Pairing Interactions

NUCLEAR STRUCTURE 190,192,194Hg, 194Pb; calculated superdeformed bands charge quadrupole moments, nucleon quasi particle routhians, dynamic moments of inertia. 150Gd; calculated dynamic moments of intertia.

doi: 10.1016/0375-9474(95)00316-S


1996HE02

Phys.Rev. C53, 1035 (1996)

K.Heyde, C.De Coster, P.Van Duppen, M.Huyse, J.L.Wood, W.Nazarewicz

Comment on ' Shape and Superdeformed Structure in Hg Isotopes in Relativistic Mean Field Model ' and ' Structure of Neutron-Deficient Pt, Hg, and Pb Isotopes '

NUCLEAR STRUCTURE 176,178,180,182,184,186,188,190,192,194,196,198Pt, 178,180,182,186,188,190,192,194,196,198Hg; analyzed data, predicted B(λ); deduced quadrupole deformations; deduced prolate, superdeformed bands related conclusions implications. Nonrelativistic approach.

doi: 10.1103/PhysRevC.53.1035


1996KU06

Phys.Rev. C53, 2194 (1996)

S.Kuyucak, M.Honma, T.Otsuka

Description of Superdeformed Nuclei in the Interacting Boson Model

NUCLEAR STRUCTURE 190,192,194Hg, 192,194,196Pb, 148,150Gd, 152,154Dy; analyzed dynamic moment of inertia, B(λ) in some cases, superdeformed nuclei. Interacting boson model.

doi: 10.1103/PhysRevC.53.2194


1996NA07

Phys.Rev. C53, 2213 (1996)

T.Nakatsukasa, K.Matsuyanagi, S.Mizutori, Y.R.Shimizu

Microscopic Structure of High-Spin Vibrational Excitations in Superdeformed 190,192,194Hg

NUCLEAR STRUCTURE 190,192,194Hg; calculated octupole, (γ) vibrations excitation energy, B(λ), superdeformed bands dynamic moments of inertia. Cranked shell model extended by RPA.

doi: 10.1103/PhysRevC.53.2213


1996TA01

Phys.Rev. C53, 1038 (1996)

N.Takigawa, S.Yoshida, K.Hagino, S.K.Patra, C.R.Praharaj

Reply to ' Comment on ' Shape and Superdeformed Structure in Hg Isotopes in Relativistic Mean Field Model ' and ' Structure of Neutron-Deficient Pt, Hg, and Pb Isotopes ' '

NUCLEAR STRUCTURE 176,178,180,182,184,186,188,190,192,194,196,198,200Hg; analyzed predicted binding energy per particle, rms charge radii. 170,172,174Hg, 192,194,196,198,200,202,204,206,208Pb; analyzed predicted rms charge radii; deduced sensitivity to model parameters. Relativistic mean field theory.

doi: 10.1103/PhysRevC.53.1038


1996WI08

Phys.Rev. C54, 559 (1996)

A.N.Wilson, J.Timar, J.F.Sharpey-Schafer, B.Crowell, M.P.Carpenter, R.V.F.Janssens, D.J.Blumenthal, I.Ahmad, A.Astier, F.Azaiez, M.Bergstrom, L.Ducroux, B.J.P.Gall, F.Hannachi, T.L.Khoo, A.Korichi, T.Lauritsen, A.Lopez-Martens, M.Meyer, D.Nisius, E.S.Paul, M.G.Porquet, N.Redon, J.N.Wilson, T.Nakatsukasa

Collective and Quasiparticle Excitations in Superdeformed 190Hg

NUCLEAR REACTIONS 160Gd(34S, 4n), E ≈ 155 MeV; measured γγ-coin, Eγ, Iγ. 190Hg deduced high-spin levels, J, π, B(λ), superdeformed bands.

doi: 10.1103/PhysRevC.54.559


1996WU05

Phys.Rev.Lett. 76, 4132 (1996)

L.-A.Wu, H.-M.Ding, Z.-T.Yan, G.Liu

Unified Description of Collective Bands of Even-Even Nuclei and Fingerprint of the Nuclear γ Shape

NUCLEAR STRUCTURE 156,158,160,162,164Dy; analyzed yrast level data; deduced parameter R. A=80-248; analyzed data; deduced relative root square deviation. 190,192,194Hg; analyzed data; deduced superdeformed bands, parameter R, relative root square deviation.

doi: 10.1103/PhysRevLett.76.4132


1997AM06

Phys.Lett. 413B, 15 (1997)

H.Amro, E.F.Moore, R.V.F.Janssens, G.Hackman, S.M.Fischer, M.P.Carpenter, I.Ahmad, B.Crowell, T.L.Khoo, T.Lauritsen, D.Nisius, J.Timar, A.N.Wilson

Lifetime Measurements and Dipole Transition Rates for Superdeformed States in 190Hg

NUCLEAR REACTIONS 160Gd(34S, 4n), E=159 MeV; measured Eγ, Iγ, γγ-coin, DSA. 190Hg deduced superdeformed levels T1/2, B(λ), quadrupole moment, evidence for octupole vibration.

doi: 10.1016/S0370-2693(97)01113-1


1997DE32

Z.Phys. A358, 181 (1997)

I.Deloncle, M.Kaci, M.G.Porquet, J.Duprat, F.Azaiez, S.Bouneau, C.Bourgeois, H.Sergolle

Highest Spin Reached in the Superdeformed Well in the A ≈ 190 Mass Region

NUCLEAR STRUCTURE 190,192,194Hg, 193,195Tl, 192,194,196,198Pb, 190Po; analyzed superdeformed bands maximum spin vs fissility parameter; deduced linear relationship.

doi: 10.1007/s002180050300


1997FA04

Phys.Rev. C55, R999 (1997)

P.Fallon, F.S.Stephens, S.Asztalos, B.Busse, R.M.Clark, M.A.Deleplanque, R.M.Diamond, R.Krucken, I.Y.Lee, A.O.Macchiavelli, R.W.MacLeod, G.Schmid, K.Vetter, T.Nakatsukasa

Octupole Vibrations and Signature Splitting in Even Mass Hg Superdeformed Bands

NUCLEAR STRUCTURE 190,192,194Hg; analyzed superdeformed bands octupole characteristics.

doi: 10.1103/PhysRevC.55.R999


1997GI06

Z.Phys. A358, 177 (1997)

M.Girod, J.P.Delaroche, J.F.Berger, S.Peru, J.Libert

Microscopic Descriptions of Collective SD Bands in the A = 190 Mass Rgion with the Gogny Force

NUCLEAR STRUCTURE 190,192,194Hg, 194Pb; calculated yrast superdeformed bands moments of inertia. 194Pb calculated excited superdeformed bands. HFB, generator coordinate method, Gaussian overlap approximation, Gogny force.

doi: 10.1007/s002180050298


1997GU28

Mod.Phys.Lett. A 12, 1775 (1997)

R.K.Gupta, D.Bir, S.Dhaulta

Decay Modes of 180-194Hg Nuclei - A New Possibility of Deformed Daughter Radioactivity

RADIOACTIVITY 180,182,184,186,188,190,192,194Hg(α), (8Be), (12C), (14C), (16C), (16O), (18O), (22Ne), (24Ne); calculated deformed, superdeformed states cluster decay T1/2; deduced shell structure effects.


1997HU13

Phys.Rev. C56, 2523 (1997)

Z.X.Hu, J.Y.Zeng

Comparison of the Harris and ab Expressions for the Description of Nuclear Superdeformed Rotational Bands

NUCLEAR STRUCTURE 190,191,192,193,194Hg, 192,193,194,195,196,198Pb, 191Au, 193,195Tl; analyzed superdeformed transition energies; deduced parameters. Harris formula, "ab" expression.

doi: 10.1103/PhysRevC.56.2523


1997LI21

Phys.Rev. C56, 1370 (1997)

Y.-X.Liu, J.-G.Song, H.-Z.Sun, E.-G.Zhao

Description of Superdeformed Nuclear States in the Interacting Boson Model

NUCLEAR STRUCTURE 190,192,194Hg, 192,194,196,198Pb, 148,150Gd, 152,154Dy; calculated superdeformed states transition energies, rotational properties. Interacting boson model, comparison with experiment.

doi: 10.1103/PhysRevC.56.1370


1997PE04

Phys.Rev. C55, 1797 (1997)

S.Perries, D.Samsoen, J.Meyer, M.Meyer, P.Quentin

Collective Gyromagnetic Ratios and the Structure of Odd Superdeformed A = 190 Nuclei

NUCLEAR STRUCTURE 152Sm, 158Gd, 162Dy, 166Er, 174Yb, 178Hf, 182,184W, 188,190,192Os, 194Pt; calculated ground state collective gyromagnetic factors. 190,192,194,196,198,200Pb, 188,190,192,194,196,198Hg; calculated gyromagnetic ratios at superdeformed minima, (g(K)-g(R)/Q0)K. 193Hg, 193Pb, 193,195Tl; calculated superdeformed minima magnetic properties. Microsocopic approach.

doi: 10.1103/PhysRevC.55.1797


1997SU07

Phys.Rev.Lett. 78, 2321 (1997)

Y.Sun, J.-Y.Zhang, M.Guidry

Systematic Description of Yrast Superdeformed Bands in Even-Even Nuclei of the Mass-190 Region

NUCLEAR STRUCTURE 188,190,192,194,196Hg, 190,192,194,196,198Pb; analyzed yrast superdeformed bands Eγ, dynamical moment of inertia. 194Hg; analyzed transition quadrupole moments, g-factors. Projected shell model.

doi: 10.1103/PhysRevLett.78.2321


1997ZH04

Nucl.Phys. A615, 229 (1997)

S.-G.Zhou, C.Zheng, F.Xu, J.Hu

Study of the Superdeformed Nuclei in A = 190 Region with the Cranking Bohr-Mottelson Hamiltonian

NUCLEAR STRUCTURE 189,191,190,192,193,194Hg, 192,194,196,198,193,195Pb, 191,193,195,192,194Tl, 196Bi, 191Au, 198Po; analyzed superdeformed bands transition energies; deduced mass, rigidity parameters. Cranking Bohr-Mottelson Hamiltonian.

doi: 10.1016/S0375-9474(96)00490-3


1997ZH07

Phys.Rev. C55, 2324 (1997)

S.-G.Zhou, C.Zheng

Exponential Model with Pairing Attenuation Applied to Superdeformed Nuclei in the A ∼ 190 Region

NUCLEAR STRUCTURE 191Au, 189,190,191,192,193,194Hg, 191,192,193,194,195Tl, 192,193,194,195,196Pb, 195,197Bi, 198Po; calculated superdeformed bands associated level spins, parameters, Eγ(in some cases), bandhead moment of inertia characteristics. Exponential model.

doi: 10.1103/PhysRevC.55.2324


1998DA20

Phys.Rev. C58, 2068 (1998)

H.Dancer, P.Bonche, H.Flocard, P.-H.Heenen, J.Meyer, M.Meyer

Monopole Strength and Decay Out of Superdeformed Bands in the A = 190 Mass Region from Theories Beyond the Mean Field

NUCLEAR STRUCTURE 190,192,194,196,198Hg, 192,194,196,198,200Pb; calculated E0, E2 transition rates from superdeformed bands; deduced E2 transitions dominance. Generator coordinate method, comparison with two-level model.

doi: 10.1103/PhysRevC.58.2068


1998HE07

Phys.Rev. C57, 1719 (1998)

P.-H.Heenen, J.Dobaczewski, W.Nazarewicz, P.Bonche, T.L.Khoo

Shell Effects in Superdeformed Minima

NUCLEAR STRUCTURE 190,192,194,196Hg, 192,194,196,198Pb, 234,236,238,240Np; calculated two-proton separation energies. 188,190,192,194Pt, 232,234,236,238U, 190,192,194,196Hg, 192,194,196,198Pb, 234,236,238,240Np; calculated two-neutron separation energies, excitation energies of superdeformed minima. Self-consistent Skyrme-HFB method. Comparison with data.

doi: 10.1103/PhysRevC.57.1719


1998LI54

Phys.Rev. C58, 3266 (1998)

S.X.Liu, J.Y.Zeng

Variation of Moments of Inertia with Angular Momentum and Systematics of Bandhead Moments of Inertia of Superdeformed Bands

NUCLEAR STRUCTURE 166Er, 169Lu, 189,190,191,192,193,194,195Hg, 192,193,194Tl, 198Po, 192,193,194,195,196,197,198Pb, 240,242Pu; analyzed superdeformed bands transition energies; deduced bandhead spins.

doi: 10.1103/PhysRevC.58.3266


1998ZH24

Phys.Rev. C58, 868 (1998)

J.-Y.Zhang, Y.Sun, L.L.Riedinger, M.Guidry

Lack of Additivity in Mass-190 Superdeformed Bands

NUCLEAR STRUCTURE 190,191,192Hg, 191,192Tl; analyzed superdeformed bands relative spins; deduced residual interactions. Projected shell model calculations.

doi: 10.1103/PhysRevC.58.868


1999AF04

Phys.Rev. C60, 051303 (1999)

A.V.Afanasjev, J.Konig, P.Ring

Cranked Relativistic Hartree-Bogoliubov Theory: Superdeformed bands in the A ∼ 190 region

NUCLEAR STRUCTURE 192,194,196Pb, 190,192,194Hg; calculated superdeformed bands moments of inertia, transition quadrupole moments. Cranked relativistic Hartree-Bogoliubov theory, comparisons with data.

doi: 10.1103/PhysRevC.60.051303


1999DA30

Nucl.Phys. (Supplement) A654, 655c (1999)

H.Dancer, S.Perries, P.Bonche, H.Flocard, P.-H.Heenen, J.Meyer, M.Meyer

Generator Coordinate Method and Superdeformation in A = 190 Nuclei

NUCLEAR STRUCTURE 190,192,194,196Hg, 192,194,196,198Pb; calculated E0, E2 transition rates for decay out of superdeformed bands; deduced E2 transition dominance.

doi: 10.1016/S0375-9474(00)88520-6


1999FA13

Phys.Rev. C60, 044301 (1999)

P.Fallon, P.-H.Heenen, W.Satula, R.M.Clark, F.S.Stephens, M.A.Deleplanque, R.M.Diamond, I.Y.Lee, A.O.Macchiavelli, K.Vetter

Origin of Unit Alignment in Superdeformed Bands in A ≈ 190 Nuclei

NUCLEAR STRUCTURE 192,193,194,195,196Pb, 192,193,194,195Tl, 190,191,192,193,194Hg; analyzed identical superdeformed bands spin alignments, moments of inertia; deduced relative single-particle, core contributions. Cranked mean-field calculations.

doi: 10.1103/PhysRevC.60.044301


1999JO07

J.Phys.(London) G25, L43 (1999)

R.S.Johal, R.K.Gupta

SUq(2) and Superdeformed Bands in Nuclei

NUCLEAR STRUCTURE 130La, 134Nd, 146Gd, 150Tb, 190Hg, 194Pb; analyzed superdeformed bands; deduced role of SUq(2) symmetry.

doi: 10.1088/0954-3899/25/6/102


1999LI38

Phys.Rev. C60, 054301 (1999)

J.Libert, M.Girod, J.-P.Delaroche

Microscopic Descriptions of Superdeformed Bands with Gogny Force: Configuration mixing calculations in the A ∼ 190 mass region

NUCLEAR STRUCTURE 190,192,194Hg, 192,194,196Pb, 196,198Po; calculated potential energy surfaces, superdeformed bands excitation energies, moments of inertia, transition quadrupole moments, related features. Constrained HFB calculations, Gogny force.

doi: 10.1103/PhysRevC.60.054301


1999ZH12

J.Phys.(London) G25, 819 (1999)

J.-Y.Zhang, Y.Sun, L.L.Riedinger, M.Guidry

Does an Independent Quasiparticle Picture Hold in Mass-190 Superformed Nuclei ?

NUCLEAR STRUCTURE 190,191Hg, 191,192Tl; analyzed superdeformed bands relative spins; deduced deviations from additivity. Projected shell model, independent quasiparticle picture.

doi: 10.1088/0954-3899/25/4/045


2000AF19

Phys.Scr. T88, 10 (2000)

A.V.Afanasjev, P.Ring

Superdeformations in Relativistic and Non-Relativistic Mean Field Theories

NUCLEAR STRUCTURE 58Cu, 60,62Zn, 149Gd, 150,151Tb, 152,153Dy, 190,192,194Hg, 192,194,196Pb; calculated superdeformed bands moments of inertia, effective alignments. Relativistic mean field theory, comparisons with data.

doi: 10.1238/Physica.Topical.088a00010


2000HA63

Acta Phys.Hung.N.S. 12, 191 (2000)

F.Hannachi, A.Korichi, A.N.Wilson, A.Lopez-Martens, M.Rejmund, C.Schuck, Ch.Vieu, G.Chmel, A.Gorgen, H.Hubel, D.Rossbach, G.Schonwasser, M.Bergstrom, B.M.Nyako, J.Timar, D.Bazzacco, S.Lunardi, C.Rossi-Alvarez, P.Bednarczyk, N.Kintz, S.Naguleswaran, A.Astier, D.M.Cullen, J.F.Sharpey-Schafer, T.Lauritsen, R.Wadsworth

Experiments Evidence of Octupole Vibrations in the Superdeformed Well

NUCLEAR REACTIONS 160Gd(34S, 4n), E=156 MeV; measured Eγ, Iγ, γγ-coin, γ-ray polarization. 190Hg deduced octupole vibrational nature of excited superdeformed band. Euroball IV array.


2000SH37

Yad.Fiz. 63, No 9, 1618 (2000); Phys.Atomic Nuclei 63, 1533 (2000)

I.S.Shapiro, V.A.Khangulyan, R.A.Barankov

Triplet Cooper Pairing in Nuclear Matter and Rotational States of Superdeformed Nuclei

NUCLEAR STRUCTURE 197Bi, 198,197,196,195,194,193Pb, 195,194,193,192,191Tl, 195,194,193,192,191,190,189Hg, 191Au, 153Ho, 155,154,153,152,151Dy, 152,151,150,145Tb, 150,149,148,147,146,145Gd, 143,142Eu, 142Sm, 132Nd, 133Pr, 133Pm, 81Sr; analyzed superdeformed rotational bands; deduced bandhead spin, dynamical moment of inertia, band parameters. Superfluid nuclear matter model calculations.

doi: 10.1134/1.1312887


2000VA02

Nucl.Phys. A665, 46 (2000)

A.Valor, J.L.Egido, L.M.Robledo

Approximate Particle Number Projection with Density Dependent Forces: Superdeformed bands in the A = 150 and A = 190 regions

NUCLEAR STRUCTURE 150Gd, 152Dy, 190,192,194Hg, 194Pb; calculated superdeformed bands Eγ, quadrupole moments, related features. Cranked HFB and cranked Lipkin-Nogami approaches, approximate particle number projection.

doi: 10.1016/S0375-9474(99)00430-3


2000VA09

Nucl.Phys. A671, 189 (2000)

A.Valor, J.L.Egido, L.M.Robledo

Implementation of a Variational Approach to Approximate Particle Number Projection with Effective Forces

NUCLEAR STRUCTURE 152Dy, 164Er, 190Hg; calculated normal-deformed, superdeformed rotational bands moments of inertia, related features. Self-consistent calculations, approximate particle number projection with effective forces.

doi: 10.1016/S0375-9474(99)00841-6


2000ZW03

J.Phys.(London) G26, 1723 (2000)

G.Zwartz, T.E.Drake, M.Cromaz, D.Ward, V.Janzen, A.Galindo-Uribarri, D.Prevost, J.Waddington, S.M.Mullins

Investigation of the use of an α + Xn Reaction Channel to Enhance the Population of Superdeformed States in 193Hg and 195Hg

NUCLEAR REACTIONS 184W(18O, 5nα), (18O, 6n), (18O, 7n), E=115, 120 MeV; 186W(18O, 5nα), E=105, 110 MeV; 164Dy(30Si, 4n), E=147 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-coin. 190,193Hg deduced superdeformed bands transitions, relative intensities.

doi: 10.1088/0954-3899/26/11/307


2001BU02

Phys.Rev. C63, 014312 (2001)

B.Buck, A.C.Merchant, S.M.Perez

Transition Quadrupole Moments in Superdeformed Bands

NUCLEAR STRUCTURE 60,62Zn, 80,82Sr, 84,86Zr, 132Ce, 134Nd, 142Sm, 146,148,150Gd, 152,154Dy, 190,192,194Hg, 194,196Pb, 236,238U; calculated superdeformed bands transition quadrupole moments; deduced cluster configuration features. Binary cluster model, comparisons with data.

doi: 10.1103/PhysRevC.63.014312


2001HA15

Acta Phys.Pol. B32, 1083 (2001)

F.Hannachi, A.Korichi, A.N.Wilson, A.Lopez-Martens, M.Rejmund, C.Schuck, Ch.Vieu, G.Chmel, A.Gorgen, H.Hubel, D.Rossbach, G.Schonwasser, M.Bergstrom, B.M.Nyako, J.Timar, D.Bazzacco, S.Lunardi, C.Rossi-Alvarez, P.Bednarczyk, N.Kintz, S.Naguleswaran, A.Astier, D.M.Cullen, J.F.Sharpey-Schafer, T.Lauritsen, R.Wadsworth

Collective Excitations in the Superdeformed Well

NUCLEAR REACTIONS 160Gd(34S, 4n), E=156 MeV; measured Eγ, Iγ, γγ-coin, γ-ray polarization. 190Hg deduced superdeformed bands, multipolarity of inter-band transitions, collective excitation of excited band. Euroball-IV array.


2001KO16

Phys.Rev.Lett. 86, 2746 (2001)

A.Korichi, A.N.Wilson, F.Hannachi, A.Lopez-Martens, M.Rejmund, C.Schuck, Ch.Vieu, G.Chmel, A.Gorgen, H.Hubel, D.Rossbach, G.Schonwasser, M.Bergstrom, B.M.Nyako, J.Timar, D.Bazzacco, S.Lunardi, C.Rossi-Alvarez, P.Bednarczyk, N.Kintz, S.Naguleswaran, A.Astier, D.M.Cullen, J.F.Sharpey-Schafer, T.Lauritsen, R.Wadsworth

Linear Polarization Measurement of Interband Transitions in Superdeformed 190Hg: Model-independent evidence for octupole vibrational structures

NUCLEAR REACTIONS 160Gd(34S, 4n), E=156 MeV; measured Eγ, Iγ, γγ-coin, γ-ray polarization. 190Hg deduced superdeformed bands, multipolarity of interband transitions, octupole collective nature of excited superdeformed band. Euroball IV array.

doi: 10.1103/PhysRevLett.86.2746


2001SH11

Nucl.Phys. A682, 464c (2001)

Y.R.Shimizu, M.Matsuo, K.Yoshida

Theoretical Study of the Decay-Out Spin of Superdeformed Bands in the Dy and Hg Regions

NUCLEAR STRUCTURE 143,144Eu, 144,146,147,148,149,150Gd, 150,151Tb, 151,152Dy, 191Au, 190,191,192,193,194Hg, 193Tl, 193,194,195,196Pb, 197Bi; calculated superdeformed band transition intensities; deduced decay-out spin. Compound mixing model, comparison with data.

doi: 10.1016/S0375-9474(00)00674-6


2001SU05

Phys.Rev. C63, 047306 (2001)

Y.Sun, J.-Y.Zhang, M.Guidry

g Factors and the Interplay of Collective and Single-Particle Degrees of Freedom in Superdeformed Mass-190 Nuclei

NUCLEAR STRUCTURE 188,190,192,194,196Hg, 190,192,194,196,198Pb; calculated superdeformed bands g factors vs spin. Projected shell model.

doi: 10.1103/PhysRevC.63.047306


2002BU13

Yad.Fiz. 65, 701 (2002); Phys.Atomic Nuclei 65, 669 (2002)

B.Buck, A.C.Merchant, S.M.Perez

Transition Quadrupole Moments in Superdeformed Bands

NUCLEAR STRUCTURE 60,62Zn, 80,82Sr, 84,86Zr, 132Ce, 134Nd, 142Sm, 146,148,150Gd, 152,154Dy, 190,192,194Hg, 194,196Pb, 236,238U; calculated superdeformed bands transition quadrupole moments. Binary cluster approach, comparisons with data.

doi: 10.1134/1.1471271


2002CH62

Chin.Phys.Lett. 19, 1771 (2002)

Y.-J.Chen, Y.-S.Chen, F.-X.Xu

Pairing Field and Moments of Inertia of Superdeformed Nuclei

NUCLEAR STRUCTURE 84Zr, 150Gd, 190Hg; analyzed superdeformed bands dynamic moments of inertia; deduced pairing effects. Harmonic oscillator quadrupole pairing HFB model.

doi: 10.1088/0256-307X/19/12/309


2002NI03

Phys.Rev. C65, 054320 (2002)

T.Niksic, D.Vretenar, P.Ring, G.A.Lalazissis

Shape Coexistence in the Relativistic Hartree-Bogoliubov Approach

NUCLEAR STRUCTURE 176,178,180,182,184,186,188,190,192,194,196,198,200,202,204,206Hg, 184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214Pb; calculated binding energies, deformation effects; deduced role of effective interactions. 208Pb calculated single-particle energies. Relativistic Hartree-Bogoliubov approach.

doi: 10.1103/PhysRevC.65.054320


2003BU11

Phys.Rev. C 68, 024313 (2003)

B.Buck, A.C.Merchant, S.M.Perez

Theory of band comparison in even-even nuclei

NUCLEAR STRUCTURE 142,144,146Ba, 146,148Ce, 146,148,150,152Nd, 150,152,154Sm, 218,220,222,224,226Ra, 222,224,226,228,230,232,234Th, 230,232,234,236,238U, 236,238,240,242,244Pu; calculated rotational bands relative μ, B(E2). 148,150Gd, 152,154Dy, 190,192,194Hg, 194,196Pb; calculated superdeformed bands relative μ, B(E2). 212Pb, 212Po; calculated superdeformed bands features. Cluster model.

doi: 10.1103/PhysRevC.68.024313


2004AD19

Phys.Rev. C 69, 054310 (2004)

G.G.Adamian, N.V.Antonenko, R.V.Jolos, Yu.V.Palchikov, W.Scheid, T.M.Shneidman

Decay out of superdeformed bands in the mass region A ≈ 190 within a cluster approach

NUCLEAR STRUCTURE 190,192,194Hg, 192,194,196Pb; calculated superdeformed rotational band energies, decay-out probabilities. Cluster model.

doi: 10.1103/PhysRevC.69.054310


2004AD31

Yad.Fiz. 67, 1737 (2004); Phys.Atomic Nuclei 67, 1709 (2004)

G.G.Adamian, N.V.Antonenko, R.V.Jolos, Yu.V.Palchikov, W.Scheid, T.M.Shneidman

Superdeformation as Cluster State

NUCLEAR STRUCTURE 190,192,194Hg; calculated normal-deformed and superdeformed bands levels, J, π, decay-out probabilities. Cluster approach.

doi: 10.1134/1.1806911


2006RI03

Int.J.Mod.Phys. E15, 520 (2006)

P.Ring

Covariant density functional theory for collective excitations in nuclei far from stability

NUCLEAR STRUCTURE 152Dy, 190,192,194Hg, 192,194,196,198Pb, 198Po; calculated superdeformed bands moments of inertia. 116,118,120,124Sn; calculated dipole strength distributions. Covariant density functional theory.

doi: 10.1142/S0218301306004478


2007KV02

Phys.Rev. C 75, 034306 (2007)

J.Kvasil, N.Lo Iudice, F.Andreozzi, F.Knapp, A.Porrino

Microscopic structure of deformed and superdeformed collective bands in rotating nuclei

NUCLEAR STRUCTURE 190,192,194Hg, 152Dy; calculated deformed and superdeformed rotational bands energies, configurations, strength distributions for linking transitions. Cranked Nilsson plus quasiparticle RPA approach.

doi: 10.1103/PhysRevC.75.034306


2008KV01

Int.J.Mod.Phys. E17, 196 (2008)

J.Kvasil, N.Lo Iudice, F.Andreozzi, A.Porrino, F.Knapp

Collective bands in superdeformed nuclei

NUCLEAR STRUCTURE 152Dy, 190Hg; analyzed superdeformed bands, and strength of E1 transitions using Cranked Nilsson + QRPA Model.

doi: 10.1142/S0218301308009690


2009AL12

Phys.Rev. C 79, 054324 (2009)

H.H.Alharbi, H.A.Alhendi, F.S.Alhakami

Description of superdeformed nuclei in the A ∼ 190 region by generalized deformed suq(2)

NUCLEAR STRUCTURE 191Au, 189,190,191,192,193,194,195Hg, 189,191,192,193,194,195Tl, 192,193,194,195,196,197,198Pb, 196Bi, 198Po; analyzed superdeformed bands; calculated moments of inertia using generalized deformed suq(2) model calculations.

doi: 10.1103/PhysRevC.79.054324


2010GU10

Nucl.Phys. A834, 87c (2010)

J.-Z.Gu, B.-B.Peng, W.-H.Zou, S.-F.Shen

Decay out of A Superdeformed Band: Chaoticity Dependence and A Microscopic Understanding

NUCLEAR STRUCTURE 188,190,192,194,196Hg; calculated super-deformed bands, E2 transition strengths, angular momentum, deformation using projected shell model with HFB based on Gogny force.

doi: 10.1016/j.nuclphysa.2010.01.026


2010WI02

Phys.Rev.Lett. 104, 162501 (2010)

A.N.Wilson, A.Korichi, S.Siem, A.Astier, D.Bazzacco, P.Bednarczyk, M.H.Bergstrom, S.Chmel, D.M.Cullen, P.M.Davidson, A.Gorgen, F.Hannachi, H.Hubel, N.Kintz, T.Lauritsen, A.Lopez-Martens, S.Lunardi, S.Naguleswaran, B.M.Nyako, M.Rejmund, G.Schonwasser, C.Schuck, J.F.Sharpey-Schafer, J.Timar, R.Wadsworth, J.Libert

Two-Particle Separation Energy Trends in the Superdeformed Well

NUCLEAR REACTIONS 160Gd(34S, 4n), E=156 MeV; measured Eγ, Iγ, γγ-coin.; 190Hg deduced energy and J of superdeformed and normal states, two-proton separation energies, critical tests of nuclear models.

doi: 10.1103/PhysRevLett.104.162501


2011WI12

J.Phys.:Conf.Ser. 312, 092065 (2011)

A.N.Wilson, A.Korichi, S.Siem, A.Astier, D.Bazzacco, P.Bednarczyk, M.H.Bergstrom, S.Chmel, D.M.Cullen, P.M.Davidson, A.Gorgen, F.Hannachi, H.Hubel, N.Kintz, T.Lauritsen, A.Lopez-Martens, S.Lunardi, S.Naguleswaran, B.M.Nyako, M.Rejmund, G .Schonwasser, C.Schuck, J.F.Sharpey-Schafer, J.Timar, R.Wadsworth, J.Libert

Two-Particle Separation Energies in the Superdeformed Well

NUCLEAR STRUCTURE 190,192,194Hg, 192,194,196Pb; calculated superdeformed quasi-vacuum states using HFB with Skyrme and Gogny forces and GCM. 188,190,192,194,196Hg, 190,192,194,196,198Pb; calculated mass excess, 2n and 2p separation energies. Compared with data.

doi: 10.1088/1742-6596/312/9/092065


2013SH34

Int.J.Mod.Phys. E22, 1350053 (2013)

N.Sharma, H.M.Mittal

Systematic study of nuclear softness of superdeformed bands in A = 190 mass region

NUCLEAR STRUCTURE 191Au, 189,190,191,192,193,194,195Hg, 189,191,192,193,194,195Tl, 196,197Bi, 198Po; calculated superdeformed bands, nuclear softness parameter. Comparison with ENSDF and XUNDL databases.

doi: 10.1142/S0218301313500535


2015KH04

Turk.J.Phys. 39, 178 (2015)

A.Khalaf, K.Abdelmageed, M.M.Sirag

Description of the Yrast Superdeformed Bands in Even-Even Nuclei in A ∼ 190 Region Using the Nuclear Softness Model

NUCLEAR STRUCTURE 190,192,194Hg, 192,194,196,198Pb, 198Po; calculated level energies, J, π. Comparison with experimental data.

doi: 10.3906/fiz-1412-3


2018SH19

Chin.Phys.C 42, 054104 (2018)

H.Sharma, H.M.Mittal

Band head spin assignment of superdeformed bands in Hg isotopes through power index formula

NUCLEAR STRUCTURE 189,190,191,192,193,194,195Hg; analyzed available data; deduced transition energies, head spins of super deformed band, moment of inertia using the power index formula.

doi: 10.1088/1674-1137/42/5/054104