<p>Three-quasiparticle <i>K</i>-isomeric states in odd-mass <i>N</i>&#xa0;=&#xa0;106 isotones within the <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(A\,\sim\, 180\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>A</mi> <mspace width="0.166667em" /> <mo>∼</mo> <mspace width="0.166667em" /> <mn>180</mn> </mrow> </math></EquationSource> </InlineEquation> mass region were systematically investigated using configuration-constrained potential energy surface calculations. The calculations successfully reproduced the excitation energies and deformations of the known high-<i>K</i> isomers in nuclei from <sup>175</sup>Tm to <sup>181</sup>Re. For the nuclei closer to the <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(Z=82\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>Z</mi> <mo>=</mo> <mn>82</mn> </mrow> </math></EquationSource> </InlineEquation> shell closure (<sup>183</sup>Ir, <sup>185</sup>Au, and <sup>187</sup>Tl), predictions of the configurations of the observed and yet-to-be-observed isomers are provided. The results reveal strong shape polarization, where the three-quasiparticle states are driven to larger deformations compared to the often shape-soft or spherical ground states. A particularly rich spectrum of shape coexistence is predicted in <sup>187</sup>Tl, where several high-<i>K</i> three-quasiparticle configurations with distinct prolate, oblate, and triaxial shapes are found to coexist at similar excitation energies. Notably, the oblate-deformed <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(K^{\pi }=29/2^{+}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>K</mi> <mi>π</mi> </msup> <mo>=</mo> <mn>29</mn> <mo stretchy="false">/</mo> <msup> <mn>2</mn> <mo>+</mo> </msup> </mrow> </math></EquationSource> </InlineEquation> configuration at <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(E_x = 1839\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>E</mi> <mi>x</mi> </msub> <mo>=</mo> <mn>1839</mn> </mrow> </math></EquationSource> </InlineEquation> keV was proposed to be responsible for a long-lived isomer. This study provides a comprehensive picture of shape evolution and coexistence in high-<i>K</i> multi-quasiparticle states, offering valuable insights for future experimental studies.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Shape polarization and coexistence of high-K three-quasiparticle states in odd-mass N = 106 isotones

  • Run-Yan Dong,
  • Chang-Feng Jiao

摘要

Three-quasiparticle K-isomeric states in odd-mass N = 106 isotones within the \(A\,\sim\, 180\) A 180 mass region were systematically investigated using configuration-constrained potential energy surface calculations. The calculations successfully reproduced the excitation energies and deformations of the known high-K isomers in nuclei from 175Tm to 181Re. For the nuclei closer to the \(Z=82\) Z = 82 shell closure (183Ir, 185Au, and 187Tl), predictions of the configurations of the observed and yet-to-be-observed isomers are provided. The results reveal strong shape polarization, where the three-quasiparticle states are driven to larger deformations compared to the often shape-soft or spherical ground states. A particularly rich spectrum of shape coexistence is predicted in 187Tl, where several high-K three-quasiparticle configurations with distinct prolate, oblate, and triaxial shapes are found to coexist at similar excitation energies. Notably, the oblate-deformed \(K^{\pi }=29/2^{+}\) K π = 29 / 2 + configuration at \(E_x = 1839\) E x = 1839 keV was proposed to be responsible for a long-lived isomer. This study provides a comprehensive picture of shape evolution and coexistence in high-K multi-quasiparticle states, offering valuable insights for future experimental studies.