<p>The proton-rich nucleus <InlineEquation ID="IEq3"><EquationSource Format="TEX">\(^{134}\)</EquationSource></InlineEquation>Sm has been studied up to high spin and the level scheme has been extended beyond the six transitions previously reported in the ground-state band. Levels beyond <i>E</i><InlineEquation ID="IEq4"><EquationSource Format="TEX">\(_{x}\)</EquationSource></InlineEquation> = 4 MeV and up to I<InlineEquation ID="IEq5"><EquationSource Format="TEX">\(^{\pi }\)</EquationSource></InlineEquation> = (16<InlineEquation ID="IEq6"><EquationSource Format="TEX">\(^{+}\)</EquationSource></InlineEquation>) have been identified. The first nucleon alignment in the yrast positive-parity structure has been established at a rotational frequency of <InlineEquation ID="IEq7"><EquationSource Format="TEX">\(\approx\)</EquationSource></InlineEquation> 0.30 MeV, and is attributed to the breaking of a <i>h</i><InlineEquation ID="IEq8"><EquationSource Format="TEX">\(_{11/2}\)</EquationSource></InlineEquation> proton pair. A negative-parity structure with its bandhead at <i>E</i><InlineEquation ID="IEq9"><EquationSource Format="TEX">\(_{x}\)</EquationSource></InlineEquation> = 2061 keV and <i>I</i><InlineEquation ID="IEq10"><EquationSource Format="TEX">\(^{\pi }\)</EquationSource></InlineEquation> = (7<InlineEquation ID="IEq11"><EquationSource Format="TEX">\(^{-}\)</EquationSource></InlineEquation>) has been identified and is attributed to the excitation of protons in the <i>h</i><InlineEquation ID="IEq12"><EquationSource Format="TEX">\(_{11/2}\)</EquationSource></InlineEquation> and <i>g</i><InlineEquation ID="IEq13"><EquationSource Format="TEX">\(_{7/2}\)</EquationSource></InlineEquation> orbitals. Cranked shell model calculations using the Ultimate Cranker code with standard Nilsson parameters indicate a prolate deformed minimum which persists to high frequencies. The calculated proton alignment frequency is in good agreement with the experimental value, and the neutron crossing is expected at a significantly higher frequency on account of the <i>N</i> = 72 deformed subshell gap.</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

Alignment in yrast structure and negative-parity sideband in the proton-rich nucleus \(^{134}\)Sm

  • Sachin K. Singh,
  • S. K. Tandel,
  • Saket Suman,
  • M. Hemalatha,
  • S. G. Wahid,
  • D. Negi,
  • S. Mukhopadhyay,
  • Md. S. R. Laskar,
  • R. Palit

摘要

The proton-rich nucleus \(^{134}\)Sm has been studied up to high spin and the level scheme has been extended beyond the six transitions previously reported in the ground-state band. Levels beyond E\(_{x}\) = 4 MeV and up to I\(^{\pi }\) = (16\(^{+}\)) have been identified. The first nucleon alignment in the yrast positive-parity structure has been established at a rotational frequency of \(\approx\) 0.30 MeV, and is attributed to the breaking of a h\(_{11/2}\) proton pair. A negative-parity structure with its bandhead at E\(_{x}\) = 2061 keV and I\(^{\pi }\) = (7\(^{-}\)) has been identified and is attributed to the excitation of protons in the h\(_{11/2}\) and g\(_{7/2}\) orbitals. Cranked shell model calculations using the Ultimate Cranker code with standard Nilsson parameters indicate a prolate deformed minimum which persists to high frequencies. The calculated proton alignment frequency is in good agreement with the experimental value, and the neutron crossing is expected at a significantly higher frequency on account of the N = 72 deformed subshell gap.