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ΔK = 0 M1 Excitation Strength of the Well-Deformed Nucleus ~(164)Dy from K Mixing

机译:ΔK= 0m1良好变形核的激发强度〜k混合的〜(164)Dy

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摘要

The size of a Delta K = 0 M1 excitation strength has been determined for the first time in a predominantly axially deformed even-even nucleus. It has been obtained from the observation of a rare K-mixing situation between two close-lying J(pi) = 1(+) states of the nucleus Dy-164 with components characterized by intrinsic projection quantum numbers K = 0 and K = 1. Nuclear resonance fluorescence induced by quasimonochromatic linearly polarized gamma-ray beams provided evidence for K mixing of the 1(+) states at 3159.1(3) and 3173.6(3) keV in excitation energy from their gamma-decay branching ratios into the ground-state band. The Delta K = 0 transition strength of B(M1;0(1)(+) - 1(K=0)(+) = 0.008(1)mu(2)(N) was inferred from a mixing analysis of their M1 transition rates into the ground-state band. It is in agreement with predictions from the quasiparticle phonon nuclear model. This determination represents first experimental information on the M1 excitation strength of a nuclear quantum state with a negative R-symmetry quantum number.
机译:已经在主要轴向变形的偶核中首次确定了ΔK= 0m1激发强度的尺寸。从观察核j(pi)= 1(+)态与由内在投影量子数k = 0和k = 1的组件之间的粗LAy-164的近似j(pi)= 1(+)状态之间的罕见k混合情况观察到罕见的k混合情况。 。QuAmoNoomeLy偏振γ射线束诱导的核共振荧光为3159.1(3)和3173.6(3)KeV在激发能量中的k〜3173.6(3)kev中的k混合的证据是从其伽马衰减分支比到地面 - 国家乐队。 ΔK= 0的B(M1; 0(1)(+) - > 1(+) - > 1(+)= 0.008(1)亩(2)(n)被从它们的混合分析推断出来M1过渡率进入地态频段。它与Quasiparticle核模型的预测一致。该确定代表了具有负R-ysummetry量子数的核量子状态的M1激发强度的首先实验信息。

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  • 来源
    《Physical review letters》 |2020年第9期|092501.1-092501.6|共6页
  • 作者单位

    Tech Univ Darmstadt Inst Kernphys D-64289 Darmstadt Germany;

    Tech Univ Darmstadt Inst Kernphys D-64289 Darmstadt Germany|Yale Univ Wright Nucl Struct Lab New Haven CT 06520 USA;

    Tech Univ Darmstadt Inst Kernphys D-64289 Darmstadt Germany;

    Duke Univ Dept Phys Durham NC 27708 USA|Triangle Univ Nucl Lab Durham NC 27708 USA;

    Yale Univ Wright Nucl Struct Lab New Haven CT 06520 USA;

    Tech Univ Darmstadt Inst Kernphys D-64289 Darmstadt Germany|Univ N Carolina Dept Phys & Astron Chapel Hill NC 27599 USA|Duke Univ Triangle Univ Nucl Lab Durham NC 27708 USA;

    Tech Univ Darmstadt Inst Kernphys D-64289 Darmstadt Germany;

    Joint Inst Nucl Res Dubna 141980 Russia|Dubna State Univ Dept Nucl Phys Dubna 141980 Russia;

    Tech Univ Darmstadt Inst Kernphys D-64289 Darmstadt Germany;

    Duke Univ Dept Phys Durham NC 27708 USA|Triangle Univ Nucl Lab Durham NC 27708 USA;

    Tech Univ Darmstadt Inst Kernphys D-64289 Darmstadt Germany;

    Duke Univ Dept Phys Durham NC 27708 USA|Triangle Univ Nucl Lab Durham NC 27708 USA;

    Yale Univ Wright Nucl Struct Lab New Haven CT 06520 USA;

    Univ Kentucky Dept Phys & Astron Lexington KY 40506 USA|Mississippi State Univ Dept Phys & Astron Starkville MS 39762 USA;

    Yale Univ Wright Nucl Struct Lab New Haven CT 06520 USA|Univ Surrey Dept Phys Guildford GU2 7XH Surrey England;

    GSI Helmholtzzentrum Schwerionenforsch GmbH D-64291 Darmstadt Germany;

    Horia Hulubei Natl Inst Phys & Nucl Engn POB MG 6 R-76900 Bucharest Romania;

    Yale Univ Wright Nucl Struct Lab New Haven CT 06520 USA|Univ Delhi Dept Phys & Astrophys Delhi 110007 India;

    Horia Hulubei Natl Inst Phys & Nucl Engn POB MG 6 R-76900 Bucharest Romania;

    Univ Kentucky Dept Chem Lexington KY 40506 USA;

    Univ Kentucky Dept Phys & Astron Lexington KY 40506 USA|Univ Kentucky Dept Chem Lexington KY 40506 USA;

    Univ Kentucky Dept Chem Lexington KY 40506 USA;

    GSI Helmholtzzentrum Schwerionenforsch GmbH D-64291 Darmstadt Germany;

    US Naval Acad Dept Phys Annapolis MD 21402 USA;

    Univ Cologne Inst Kernphys D-50937 Cologne Germany;

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