<p>We present a new development in the multireference covariant density functional theory (MR-CDFT) for the low-lying states of odd-mass nuclei by mixing configurations with different intrinsic quadrupole shapes and different <i>K</i> quantum numbers. All configurations are projected onto the good particle numbers and angular momenta. The success of this newly developed framework is illustrated in its application to the low-lying states of <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(^{43}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>43</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>S near the neutron magic number <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(N=28\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>=</mo> <mn>28</mn> </mrow> </math></EquationSource> </InlineEquation> with shape coexistence. Our results indicate that the ground state, <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(3/2^-_1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>3</mn> <mo stretchy="false">/</mo> <msubsup> <mn>2</mn> <mn>1</mn> <mo>-</mo> </msubsup> </mrow> </math></EquationSource> </InlineEquation>, is predominantly composed of the intruder prolate one-quasiparticle (1qp) configuration <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\nu 1/2^-[321]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ν</mi> <mn>1</mn> <mo stretchy="false">/</mo> <msup> <mn>2</mn> <mo>-</mo> </msup> <mrow> <mo stretchy="false">[</mo> <mn>321</mn> <mo stretchy="false">]</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. In contrast, the <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(7/2^-_1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>7</mn> <mo stretchy="false">/</mo> <msubsup> <mn>2</mn> <mn>1</mn> <mo>-</mo> </msubsup> </mrow> </math></EquationSource> </InlineEquation> state is identified as a high-<i>K</i> isomer, primarily built on the prolate 1qp configuration <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\nu 7/2^-[303]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>ν</mi> <mn>7</mn> <mo stretchy="false">/</mo> <msup> <mn>2</mn> <mo>-</mo> </msup> <mrow> <mo stretchy="false">[</mo> <mn>303</mn> <mo stretchy="false">]</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. Additionally, the <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(3/2^-_2\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>3</mn> <mo stretchy="false">/</mo> <msubsup> <mn>2</mn> <mn>2</mn> <mo>-</mo> </msubsup> </mrow> </math></EquationSource> </InlineEquation> state is found to be an admixture dominated by an oblate configuration with <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(K^\pi = 1/2^-\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>K</mi> <mi>π</mi> </msup> <mo>=</mo> <mn>1</mn> <mo stretchy="false">/</mo> <msup> <mn>2</mn> <mo>-</mo> </msup> </mrow> </math></EquationSource> </InlineEquation>, along with a small contribution from a prolate configuration with <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(K^\pi = 3/2^-\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>K</mi> <mi>π</mi> </msup> <mo>=</mo> <mn>3</mn> <mo stretchy="false">/</mo> <msup> <mn>2</mn> <mo>-</mo> </msup> </mrow> </math></EquationSource> </InlineEquation>. These results demonstrate the capability of MR-CDFT to capture the intricate interplay among shape coexistence, configuration mixing, and isomerism in the low-energy structure of odd-mass nuclei around <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(N = 28\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>N</mi> <mo>=</mo> <mn>28</mn> </mrow> </math></EquationSource> </InlineEquation>, without invoking triaxiality.</p>

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Multireference covariant density functional theory for shape coexistence and isomerism in \(^{43}\)S

  • En-Fu Zhou,
  • Xian-Ye Wu,
  • Jian Xiang,
  • Jiang-Ming Yao,
  • Peter Ring

摘要

We present a new development in the multireference covariant density functional theory (MR-CDFT) for the low-lying states of odd-mass nuclei by mixing configurations with different intrinsic quadrupole shapes and different K quantum numbers. All configurations are projected onto the good particle numbers and angular momenta. The success of this newly developed framework is illustrated in its application to the low-lying states of \(^{43}\) 43 S near the neutron magic number \(N=28\) N = 28 with shape coexistence. Our results indicate that the ground state, \(3/2^-_1\) 3 / 2 1 - , is predominantly composed of the intruder prolate one-quasiparticle (1qp) configuration \(\nu 1/2^-[321]\) ν 1 / 2 - [ 321 ] . In contrast, the \(7/2^-_1\) 7 / 2 1 - state is identified as a high-K isomer, primarily built on the prolate 1qp configuration \(\nu 7/2^-[303]\) ν 7 / 2 - [ 303 ] . Additionally, the \(3/2^-_2\) 3 / 2 2 - state is found to be an admixture dominated by an oblate configuration with \(K^\pi = 1/2^-\) K π = 1 / 2 - , along with a small contribution from a prolate configuration with \(K^\pi = 3/2^-\) K π = 3 / 2 - . These results demonstrate the capability of MR-CDFT to capture the intricate interplay among shape coexistence, configuration mixing, and isomerism in the low-energy structure of odd-mass nuclei around \(N = 28\) N = 28 , without invoking triaxiality.