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NSR database version of April 11, 2024.

Search: Author = X.T.He

Found 29 matches.

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2023PE11      Phys.Rev. C 108, 014317 (2023)

C.M.Petrache, J.Uusitalo, A.D.Briscoe, C.M.Sullivan, D.T.Joss, H.Tann, O.Aktas, B.Alayed, M.A.M.Al-Aqeel, A.Astier, H.Badran, B.Cederwall, C.Delafosse, A.Ertoprak, Z.Favier, U.Forsberg, W.Gins, T.Grahn, P.T.Greenlees, X.T.He, J.Heery, J.Hilton, S.Kalantan, R.Li, P.M.Jodidar, R.Julin, S.Juutinen, M.Leino, M.C.Lewis, J.G.Li, Z.P.Li, M.Luoma, B.F.Lv, A.McCarter, S.Nathaniel, J.Ojala, R.D.Page, J.Pakarinen, P.Papadakis, E.Parr, J.Partanen, E.S.Paul, P.Rahkila, P.Ruotsalainen, M.Sandzelius, J.Saren, J.Smallcombe, J.Sorri, S.Szwec, L.J.Wang, Y.Wang, L.Waring, F.R.Xu, J.Zhang, Z.H.Zhang, K.K.Zheng, G.Zimba

High-K three-quasiparticle isomers in the proton-rich nucleus 129Nd

doi: 10.1103/PhysRevC.108.014317
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2023SE09      Phys.Rev. C 107, L061302 (2023)

D.Seweryniak, T.Huang, K.Auranen, A.D.Ayangeakaa, B.B.Back, M.P.Carpenter, P.Chowdhury, R.M.Clark, P.A.Copp, Z.Favier, K.Hauschild, X.-T.He, T.L.Khoo, F.G.Kondev, A.Korichi, T.Lauritsen, J.Li, C.Morse, D.H.Potterveld, G.Savard, S.Stolze, J.Wu, J.Zhang, Y.-F.Xu

Nuclear rotation at the fission limit in 254Rf

NUCLEAR REACTIONS 206Pb(50Ti, 2n)254Rf, E=244 MeV from the ATLAS-ANL facility; measured reaction products, prompt γ rays, Eγ, Iγ, Rf Kα and Kβ x-rays, (254Rf implants)γ-coin, (implants)(fission events)γ-coin using the Gammasphere array and the Argonne gas-filled analyzer (AGFA). 254Rf; deduced levels, J, π, ground-state rotational band up to 14+, kinematic moment of inertia. Systematics of ground-state bands in 250Fm, 252,254No, and 254,256Rf, and comparison with particle-number conserving cranked shell model (PNC-CSM) calculations.

doi: 10.1103/PhysRevC.107.L061302
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2023ZH08      Phys.Rev. C 107, 024305 (2023)

J.Zhang, X.-T.He, Y.-C.Li, H.-Q.Zhang

Parity-doublet bands in the odd-A isotones 237U and 239Pu investigated by a particle-number-conserving method based on the cranked shell model

NUCLEAR STRUCTURE 237U, 239Pu; calculated cranked Nilsson levels near the Fermi surface for neutrons and protons, kinematic moments of inertia and alignments of the parity-doublet rotational bands, neutron and proton orbitals occupation probabilities, contributions of protons to the angular momentum alignments, contributions of neutrons to the moments of inertia. Particle-number-con serving method in the framework of the cranked shell model (PNC-CSM) calculations. Comparison to experimental data.

doi: 10.1103/PhysRevC.107.024305
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2022HU21      Phys.Rev. C 106, L061301 (2022)

T.Huang, D.Seweryniak, B.B.Back, P.C.Bender, M.P.Carpenter, P.Chowdhury, R.M.Clark, P.A.Copp, X.-T.He, R.D.Herzberg, D.E.M.Hoff, H.Jayatissa, T.L.Khoo, F.G.Kondev, G.Morgan, C.Morse, A.Korichi, T.Lauritsen, C.Muller-Gatermann, D.H.Potterveld, W.Reviol, A.M.Rogers, S.Saha, G.Savard, K.Sharma, S.Stolze, S.Waniganeththi, G.L.Wilson, J.Wu, Y.-F.Xu, S.Zhu

Discovery of the new isotope 251Lr: Impact of the hexacontetrapole deformation on single-proton orbital energies near the Z=100 deformed shell gap

NUCLEAR REACTIONS 203Tl(50Ti, 2n)251Lr, 205Tl(50Ti, 2n)253Lr, E=237 MeV; measured reaction products, α-decay of the reaction products, Eα, Iα. 251,253Lr; deduced levels J, π, α-decay width. 251,253,255Lr; calculated single-proton levels near the Fermi surface. Calculations with particle-number conserving cranked shell model. Beam delivered to target by ATLAS linear accelerator and recoiling reaction products were separated in the Argonne Gas-Filled Analyzer (AGFA) at (ANL). Decay of the implanted reaction products was measured in pixelized double-sided Si strip detector (DSSD).

RADIOACTIVITY 251,253Lr(α)[from 203,205Tl(50Ti, 2n), E=237 MeV]; measured Eα, Iα; deduced T1/2, Q-value, α-decay branchings and widths. Comparison to other experimental data. and predictions of theoretical models.

doi: 10.1103/PhysRevC.106.L061301
Citations: PlumX Metrics


2022LV04      Phys.Rev. C 105, 044319 (2022)

B.F.Lv, C.M.Petrache, K.K.Zheng, Z.H.Zhang, W.Sun, Z.P.Li, X.T.He, J.Zhang, A.Astier, P.Greenlees, T.Grahn, R.Julin, S.Juutinen, M.Luoma, J.Ojala, J.Pakarinen, J.Partanen, P.Rahkila, P.Ruotsalainen, M.Sandzelius, J.Saren, H.Tann, J.Uusitalo, G.Zimba, B.Cederwall, O.Aktas, A.Ertoprak, W.Zhang, S.Guo, M.L.Liu, H.J.Ong, Z.Y.Sun, J.G.Wang, X.H.Zhou, I.Kuti, B.M.Nyako, D.Sohler, J.Timar, C.Andreoiu, M.Doncel, D.T.Joss, R.D.Page

Refined description of the positive-parity bands and the extent of octupole correlations in 120Ba

NUCLEAR REACTIONS 58Ni(64Zn, 2p), E=255 MeV; measured Eγ, Iγ, γγγ-coin, γγ-coin, γ(θ). 120Ba; deduced levels, J, π, DCO ratios, two-point angular correlation (anisotropy) ratios, multipolarity, B(E1), B(E2), B(E3), high-spin states, bands, configurations, alignments, moments of inertia. Comparison with unpaired cranked shell model (CNS), particle number conserving cranked shell-model (PNC-CSM), and Quadrupole and Octupole Collective Hamiltonian based on the Relativistic Hartree-Bogoliubov Model calculations (QOCH-RHB). Systematics of B(E1)/B(E2) of 7- and 9- states in even-even Xe and Ba (A=116-124). JUROGAM3 array and MARA at K130 cyclotron (JYFL).

doi: 10.1103/PhysRevC.105.044319
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2022ZH45      Phys.Rev. C 106, 024305 (2022)

M.M.Zhang, Y.L.Tian, Y.S.Wang, Z.Y.Zhang, Z.G.Gan, H.B.Yang, M.H.Huang, L.Ma, C.L.Yang, J.G.Wang, C.X.Yuan, C.Qi, A.N.Andreyev, X.Y.Huang, S.Y.Xu, Z.Zhao, L.X.Chen, J.Y.Wang, M.L.Liu, Y.H.Qiang, G.S.Li, W.Q.Yang, R.F.Chen, H.B.Zhang, Z.W.Lu, X.X.Xu, L.M.Duan, H.R.Yang, W.X.Huang, Z.Liu, X.H.Zhou, Y.H.Zhang, H.S.Xu, N.Wang, H.B.Zhou, X.J.Wen, S.Huang, W.Hua, L.Zhu, X.Wang, Y.C.Mao, X.T.He, S.Y.Wang, W.Z.Xu, H.W.Li, Y.F.Niu, L.Guo, Z.Z.Ren, S.G.Zhou

Fine structure in the α decay of the 8+ isomer in 216, 218U

RADIOACTIVITY 216,216m,218,218mU(α)[218U from 182W(40Ar, 4n), E=190 MeV, 184W(40Ca, 2nα), E=206 MeV, 216U from 180W(40Ar, 4n), E=191 MeV]; measured evaporation residues (EVRs), Eα, Iα, (EVR)α12-correlations, T1/2 using position-sensitive strip detectors (PSSDs) for α detection, and SHANS separator at HIRFL-Lanzhou. 216,216m,218,218mU; deduced T1/2, Q-values, α-branching ratio, α-decay hindrance factors. 204Rn, 208,210Ra, 212,214Th(α)[from 216,218U α-decay chains]; measured Eα, T1/2. 212Th; deduced level, J, π, identification of the first 2+ state. 215Ra, 212,213,216Ac, 211,212,213,214,216,216m,217Th, 216,217,217m,218Pa, 217,218,219U; observed Eα from their decays from (EVR)α-correlations. Comparison with previous experimental data.

doi: 10.1103/PhysRevC.106.024305
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2021HE24      Chin.Phys.C 45, 101001 (2021)

X.-T.He, C.Wang, K.-Y.Zhang, C.Shen

Possible existence of bound nuclei beyond neutron drip lines driven by deformation

NUCLEAR STRUCTURE 362,364,366,368,370,372,374,376,378,380,382,384,386,388,390,392,394,396,398,400,402,404Ds; calculated ground state properties, two-neutron separation energies, deformation parameters using the deformed relativistic Hartree-Bogoliubov theory in continuum (DRHBc). deduced possible existence of bound nuclei beyond the neutron drip lines.

doi: 10.1088/1674-1137/ac1b99
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2021ZH22      Phys.Rev.Lett. 126, 152502 (2021)

Z.Y.Zhang, H.B.Yang, M.H.Huang, Z.G.Gan, C.X.Yuan, C.Qi, A.N.Andreyev, M.L.Liu, L.Ma, M.M.Zhang, Y.L.Tian, Y.S.Wang, J.G.Wang, C.L.Yang, G.S.Li, Y.H.Qiang, W.Q.Yang, R.F.Chen, H.B.Zhang, Z.W.Lu, X.X.Xu, L.M.Duan, H.R.Yang, W.X.Huang, Z.Liu, X.H.Zhou, Y.H.Zhang, H.S.Xu, N.Wang, H.B.Zhou, X.J.Wen, S.Huang, W.Hua, L.Zhu, X.Wang, Y.C.Mao, X.T.He, S.Y.Wang, W.Z.Xu, H.W.Li, Z.Z.Ren, S.G.Zhou

New α-Emitting Isotope 214U and Abnormal Enhancement of α-Particle Clustering in Lightest Uranium Isotopes

RADIOACTIVITY 214,216,218U(α) [from 180,182W(36Ar, 4n), 184W(40Ca, 2nα), E<200 MeV]; measured decay products, Eα, Iα; deduced α-decay Q-values and reduced widths, T1/2, abnormal enhancement by the strong monopole interaction between the valence protons and neutrons. Comparison withavailable data, calculations.

doi: 10.1103/PhysRevLett.126.152502
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetS0279. Data from this article have been entered in the XUNDL database. For more information, click here.


2020HE05      Chin.Phys.C 44, 034106 (2020)

X.-T.He, S.-Y.Zhao, Z.-H.Zhang, Z.-Z.Ren

High-K multi-particle bands and pairing reduction in 254No

NUCLEAR STRUCTURE 254No; calculated multi-particle states and rotational properties of the two-particle bands using the cranked shell model with pairing correlations treated by the particle number conserving method.

doi: 10.1088/1674-1137/44/3/034106
Citations: PlumX Metrics


2020HE10      Chin.Phys.C 44, 034106 (2020)

X.-T.He, S.-Y.Zhao, Z.-H.Zhang, Z.-Z.Ren

High-K multi-particle bands and pairing reduction in 254No

NUCLEAR STRUCTURE 254No; calculated Nilsson single-particle levels, J, π, energy levels, moments of inertia, bands using the cranked shell model with pairing correlations treated by the particle number conserving method.

doi: 10.1088/1674-1137/44/3/034106
Citations: PlumX Metrics


2020HE15      Phys.Rev. C 102, 014322 (2020)

X.-T.He, Y.Cao, X.-L.Gan

Effects of high-j orbitals, pairing, and deformed neutron shells on upbendings of ground-state bands in the neutron-rich even-even isotopes 170-184Hf

NUCLEAR STRUCTURE 170,172,174,176,178,180,182,184Hf; calculated neutron and proton levels with Nilsson configurations near the Fermi surface, levels, J, π, neutron and proton occupation probabilities, contribution from the neutron shells to the angular momentum alignment in the ground state bands, neutron kinematic moment of inertia with and without pairing. Cranked shell model with pairing correlations treated by the particle-number conserving method. Comparison with experimental data.

doi: 10.1103/PhysRevC.102.014322
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2020HE28      Phys.Rev. C 102, 064328 (2020)

X.-T.He, Y.-C.Li

Alternating-parity bands of 236, 238U and 238, 240Pu in a particle-number-conserving method based on the cranked shell model

NUCLEAR STRUCTURE 236,238U, 238,240Pu; calculated ratio of rotational frequencies of the positive- and negative-parity bands as function of angular momentum, cranked Nilsson proton and neutron levels near the Fermi surface, kinematic moments of inertia and alignments of the alternating-parity rotational bands, occupation probability of neutron and proton orbitals, contributions of neutron and proton to the angular momentum alignment. Particle-number-conserving (PNC) method in the framework of cranked shell model (CSM) for reflection-asymmetric nuclear systems. Comparison with experimental data.

doi: 10.1103/PhysRevC.102.064328
Citations: PlumX Metrics


2020MA27      Phys.Rev.Lett. 125, 032502 (2020)

L.Ma, Z.Y.Zhang, Z.G.Gan, X.H.Zhou, H.B.Yang, M.H.Huang, C.L.Yang, M.M.Zhang, Y.L.Tian, Y.S.Wang, H.B.Zhou, X.T.He, Y.C.Mao, W.Hua, L.M.Duan, W.X.Huang, Z.Liu, X.X.Xu, Z.Z.Ren, S.G.Zhou, H.S.Xu

Short-Lived α-Emitting Isotope 222Np and the Stability of the N = 126 Magic Shell

NUCLEAR REACTIONS 187Re(40Ar, 5N)222Np, E=198.7 MeV; measured reaction products, Eα, Iα. 220Pa, 219Th; deduced Q-values, T1/2. Comparison with systematics.

doi: 10.1103/PhysRevLett.125.032502
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2020ZH01      Phys.Lett. B 800, 135102 (2020)

M.M.Zhang, H.B.Yang, Z.G.Gan, Z.Y.Zhang, M.H.Huang, L.Ma, C.L.Yang, C.X.Yuan, Y.S.Wang, Y.L.Tian, H.B.Zhou, S.Huang, X.T.He, S.Y.Wang, W.Z.Xu, H.W.Li, X.X.Xu, J.G.Wang, H.R.Yang, L.M.Duan, W.Q.Yang, S.G.Zhou, Z.Z.Ren, X.H.Zhou, H.S.Xu, A.A.Voinov, Yu.S.Tsyganov, A.N.Polyakov, M.V.Shumeiko

A new isomeric state in 218Pa

RADIOACTIVITY 218Pa(α) [from 182W(40Ar, 3np)218Pa, E=190 MeV]; measured decay products, Eα, Iα, Eγ, Iγ; deduced ground and isomeric states T1/2, α and γ-ray energies and intensities, J, π.

doi: 10.1016/j.physletb.2019.135102
Citations: PlumX Metrics


2019HE06      Chin.Phys.C 43, 064106 (2019)

X.-T.He, Z.-L.Chen

High-K isomer and the rotational properties in the odd-Z neutron-rich nucleus M163Eu

NUCLEAR STRUCTURE 163Eu, 162Sm, 164Gd; calculated energy levels, J, π by using the cranked shell model. Comparison with experimental data.

doi: 10.1088/1674-1137/43/6/064106
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2019ZH54      Phys.Rev. C 100, 064317 (2019)

M.M.Zhang, Y.L.Tian, Y.S.Wang, X.H.Zhou, Z.Y.Zhang, H.B.Yang, M.H.Huang, L.Ma, C.L.Yang, Z.G.Gan, J.G.Wang, H.B.Zhou, S.Huang, X.T.He, S.Y.Wang, W.Z.Xu, H.W.Li, X.X.Xu, L.M.Duan, Z.Z.Ren, S.G.Zhou, H.S.Xu

Fine structure in the α decay of 219U

RADIOACTIVITY 219U(α)[from 183W(40Ar, 4n), E=190 MeV]; measured Eα, Iα, αα-coin, (recoils)ααα-correlations, half-life of 219U decay, production σ of 219U using position-sensitive strip detectors (PSSDs) for α detection, and the SHANS separator at the Heavy Ion Research Facility (HIRFL) in Lanzhou. 215Th; deduced levels, J, π, α-branching ratios, α-decay reduced widths. 216,216m,217,219Th, 220Pa(α)[from 183W(40Ar, X), E=190 MeV]; 215Th, 211Ra[from 219U α decay]; measured Eα, half-lives of decays of the isotopes. Discussed α-decay systematics in neighboring nuclides. Comparison with previous experimental data.

doi: 10.1103/PhysRevC.100.064317
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2018HE18      Phys.Rev. C 98, 064314 (2018)

X.-T.He, Y.-C.Li

Insight into nuclear midshell structures by studying K isomers in rare-earth neutron-rich nuclei

NUCLEAR STRUCTURE 158,160,162,164Sm, 160,162,164,166Gd; calculated levels, J, π, K-isomers near the Fermi surface of 160Sm for protons and neutrons, configurations and energies of low-lying multiparticle states, bandhead energies, occupation probabilities of cranked Nilsson orbital near the Fermi surface, kinematic moments of inertia, and B(E2) values using cranked shell model (CSM) with pairing correlation treated by a particle-number-conserving (PNC) method. Systematics of B(E2) values in 156,158,160,162Nd, 158,160,162,164Sm, 160,162,164,166Gd, 162,164,166,168Dy. Comparison with experimental data and other theoretical predictions.

doi: 10.1103/PhysRevC.98.064314
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2018XI03      Chin.Phys.C 42, 054105 (2018)

X.-H.Xiang, X.-T.He

Backbendings of superdeformed bands in 36;40Ar

NUCLEAR STRUCTURE 36,40Ar; calculated Nilsson diagram for protons or neutrons, cranked proton Nilsson levels near the Fermi surface, kinematic moment of inertia of the super deformed bands, occupation probability using cranked shell model (CSM).

doi: 10.1088/1674-1137/42/5/054105
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2015HE03      Phys.Rev. C 91, 015810 (2015)

X.-T.He, F.J.Fattoyev, B.-A.Li, W.G.Newton

Impact of the equation-of-state-gravity degeneracy on constraining the nuclear symmetry energy from astrophysical observables

doi: 10.1103/PhysRevC.91.015810
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2012ZH01      Phys.Rev. C 85, 014324 (2012)

Z.-H.Zhang, X.-T.He, J.-Y.Zeng, E.-G.Zhao, S.-G.Zhou

Systematic investigation of the rotational bands in nuclei with Z ≈ 100 using a particle-number conserving method based on a cranked shell model

NUCLEAR STRUCTURE 240,242,244,246,248,250,252Cm, 242,244,246,248,250,252,254Cf, 244,246,248,250,252,254,256Fm, 246,248,250,252,254,256,258No, 250Bk; calculated quadrupole deformation parameters β2, β4, moment of inertia plots, alignments, occupation probabilities, contribution of neutron and proton major shells to angular momentum alignments. 245Cm, 250Fm; calculated energies of Nilsson orbitals. 241,243,245,247,249Cm, 243,245,247,249,251Cf, 245,247,249,251,253Fm, 247,249,251,253,255No, 243,245,247,249,251Bk, 245,247,249,251,253Es, 247,249,251,253,255Md, 255Lr; calculated bandhead energies of low-lying one-quasiparticle bands, moments of inertia plots of g.s. and excited bands, alignments, occupation probabilities, contribution of neutron and proton major shells to angular momentum alignments. Cranked shell model (CSM), particle-number conserving (PNC) method. Comparison with experimental data.

doi: 10.1103/PhysRevC.85.014324
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2009HE02      Nucl.Phys. A817, 45 (2009)

X.-t.He, Z.-z.Ren, S-x.Liu, E.-g.Zhao

Influence of high-j intruder orbitals in odd mass transfermium nuclei 253No and 251Md

NUCLEAR STRUCTURE 251Md, 253No; calculated rotational band properties, configurations using a cranked shell model and comparison with data.

doi: 10.1016/j.nuclphysa.2008.12.003
Citations: PlumX Metrics


2008HE02      J.Phys.(London) G35, 035106 (2008)

X.-t.He, Z.-z.Ren

Enhanced sensitivity to variation of fundamental constants in the narrow nuclear transitions (II)

doi: 10.1088/0954-3899/35/3/035106
Citations: PlumX Metrics


2008HE09      Nucl.Phys. A806, 117 (2008)

X.-T.He, Z.-Z.Ren

Temporal variation of the fine structure constant and the strong interaction parameter in the 229Th transition

NUCLEAR STRUCTURE 209Pb, 209Bi, 229Th; calculated ground and excited state energies based on relative mean field theory.

doi: 10.1016/j.nuclphysa.2008.03.002
Citations: PlumX Metrics


2008HE18      Int.J.Mod.Phys. E17, Supplement 1, 208 (2008)

X.T.He, Z.-Z.Ren

Particle-number conserving treatment for the ground state bands in even-even transfermium nuclei

NUCLEAR STRUCTURE 250Fm, 252,254No; calculated ground state and high-spin bands, J, π. Cranked shell model.

doi: 10.1142/S0218301308011860
Citations: PlumX Metrics


2007HE17      J.Phys.(London) G34, 1611 (2007)

X.T.He, Z.-Z.Ren

Enhanced sensitivity to variation of fundamental constants in the transitions of 229Th and 249Bk

NUCLEAR STRUCTURE 229Th, 249Bk; calculated transition frequencies between the first excited and ground states, including their sensitivity to the temporal variation of the strong and fine structure constant.

doi: 10.1088/0954-3899/34/7/003
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2006HE18      Eur.Phys.J. A 28, 265 (2006)

X.T.He, S.G.Zhou, J.Meng, E.G.Zhao, W.Scheid

Test of spin symmetry in anti-nucleon spectra

NUCLEAR STRUCTURE 40Ca, 90Zr, 124Sn, 208Pb; calculated radial wave functions of antineutron spin doublets. Relativistic mean-field model.

doi: 10.1140/epja/i2006-10066-0
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2005HE01      Eur.Phys.J. A 23, 217 (2005)

X.T.He, S.X.Liu, S.Y.Yu, J.Y.Zeng, E.G.Zhao

The i13/2 proton intruder orbital and the identical superdeformed bands in 193, 194, 195Tl

NUCLEAR STRUCTURE 193,194,195Tl; calculated superdeformed bands energies, configurations; deduced role of proton blocking. Particle-number-conserving cranked mean-field approach, comparison with data.

doi: 10.1140/epja/i2004-10092-x
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2005HE21      Nucl.Phys. A760, 263 (2005)

X.T.He, S.Y.Yu, J.Y.Zeng, E.G.Zhao

The intruder orbitals in superdeformed bands and alignment additivity of odd-odd nuclei in the A ∼ 190 region

NUCLEAR STRUCTURE 191,192,193Tl, 191,193,194Hg; calculated superdeformed bands configurations, moments of inertia, angular momentum alignment. Particle-number-conserving cranked mean field approach.

doi: 10.1016/j.nuclphysa.2005.06.006
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2004HE11      Chin.Phys.Lett. 21, 813 (2004)

X.-T.He, S.-Y.Yu, S.-X.Liu, Y.-X.Liu, E.-G.Zhao

Identical Bands and Alignment in 193, 194Tl

NUCLEAR STRUCTURE 193,194Tl; analyzed superdeformed bands moments of inertia, relative alignments; deduced role of blocking in identical band mechanism.

doi: 10.1088/0256-307X/21/5/014
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