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The Influence of Triaxiality Parameter γ on the Chiral Doublet Bands with (πg_(9/2))~(-1)(νh_(11/2))~2 Configuration
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作者 亓斌 王守宇 +4 位作者 赵兴言 祝笑颖 孙大鹏 刘晨 徐长江 《Plasma Science and Technology》 SCIE EI CAS CSCD 2012年第7期595-597,共3页
The chiral doublet bands with three-quasiparticle configuration (πg9/2)-1 (vh11/2)2 are studied by the fully quantal triaxial particle rotor model. The energy spectra and B(M1)/B(E2) ratios of the doublet ban... The chiral doublet bands with three-quasiparticle configuration (πg9/2)-1 (vh11/2)2 are studied by the fully quantal triaxial particle rotor model. The energy spectra and B(M1)/B(E2) ratios of the doublet bands with different triaxiality parameter γ are systematically analyzed. It is found that γ is a sensitive parameter for the properties of these doublet bands. 展开更多
关键词 chiral doublet bands triaxiality parameter three-quasiparticle configuration
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Observation of a new isomer in ^(185)Au
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作者 X.Y.Fu Z.Liu +40 位作者 A.N.Andreyev C.F.Jiao R.Y.Dong W.Q.Zhang H.Huang W.Sun Q.B.Chen S.Q.Zhang J.G.Li X.H.Zhou X.H.Yu Q.B.Zeng D.Seweryniak B.Andel S.Antalic A.E.Barzakh M.Block A.Bronis M.P.Carpenter P.Copp J.G.Cubiss D.T.Doherty P.Van Duppen Z.Favier F.Giacoppo B.Kindler F.G.Kondev T.Lauritsen B.Lommel M.Al Monthery P.Mosat C.Raison W.Reviol G.Savard S.Stolze G.L.Wilson B.Ding S.Guo C.Y.Guo Y.B.Yu Y.F.Wu 《Chinese Physics C》 2025年第8期171-176,共6页
Delayed γ-ray spectroscopy of^(185)Au was studied at the Argonne Gas-Filled Analyzer.A new isomer at an excitation energy of 1504.2(4) keV with a half-life of 630(80) ns was identified via γ-γ coincidence analysis,... Delayed γ-ray spectroscopy of^(185)Au was studied at the Argonne Gas-Filled Analyzer.A new isomer at an excitation energy of 1504.2(4) keV with a half-life of 630(80) ns was identified via γ-γ coincidence analysis,decaying via a 294.8(3) keV transition.Based on Weisskopf estimates,the multipolarity of the 295 keV transition is assigned to be E1,M1,E2,or M2.Possible configurations for this new isomer are discussed based on configurationconstrained potential energy surface calculations. 展开更多
关键词 ISOMER shape deformation PES calculation three-quasiparticle state mid-shell
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Signature splitting in three-quasineutron rotational band 3/1[521]_(ν)⊗1/2[660]_(ν)⊗1/2[660]_(ν)of^(155)Dy
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作者 Manpreet Kaur Sushil Kumar +1 位作者 Sukhjeet Singh A.K.Jain 《Chinese Physics C》 2025年第10期234-240,共7页
The signature splitting observed in the 3/2[521]_(ν)↑⊗1/2[660]_(ν)↑⊗1/2[660]_(ν)↑three-quasineutron rotational band of 155 Dy is examined within the framework of axially symmetric three-quasiparticle plus axiall... The signature splitting observed in the 3/2[521]_(ν)↑⊗1/2[660]_(ν)↑⊗1/2[660]_(ν)↑three-quasineutron rotational band of 155 Dy is examined within the framework of axially symmetric three-quasiparticle plus axially symmetric rotor model.The experimental level energies and magnitudes of observed splitting are well-reproduced with RMS deviations of 68.13 keV and 0.58 keV,respectively.The major contributing bands in the observed splitting are K^(π)=7/2^(-):5/2[512]_(ν)↑⊗3/2[651]_(ν)↑⊗1/2[660]_(ν)↓,K^(π)=5/2^(-):5/2[512]_(ν)↑⊗3/2[651]_(ν)↑⊗3/2[651]_(ν)↓,K^(π)=1/2^(-):3/2[521]_(ν)↑⊗1/2[660]_(ν)↑⊗3/2[651]_(ν)↓,K^(π)=1/2^(-):3/2[521]_(ν)↓⊗1/2[660]_(ν)↑⊗3/2[651]_(ν)↑,K^(π)=5/2^(-):3/2[521]_(ν)↑⊗3/2[651]_(ν)↑⊗1/2[660]_(ν)↓,and K^(π)=3/2^(-):3/2[521]_(ν)↑⊗3/2[651]_(ν)↑⊗3/2[651]_(ν)↓,which mix through rotor-particle(ΔK=1)and particle-particle(ΔK=0)couplings among the bands comprising the given basis space.The observed signature splitting is also wellreproduced by the superposition of calculated energy staggering of the strongly interacting bands,which further strengthens the validity of present particle rotor model calculations.Based on the present calculations,we assign the bandhead spin K^(π)=3/2^(-)to the band under discussion.Additionally,the locations of 13 low-lying band members in the spin range I^(π)=3/2^(-)to 23/2^(-)and at 27/2^(-)and 31/2^(-)are predicted,which will be useful for future experimental investigations. 展开更多
关键词 signature splitting rotor-particle coupling particle-particle coupling three-quasiparticle rotational bands three quasiparticle plus rotor model
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