Nuclear-Structure Calculations in <span class="aps-inline-formula"><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mrow><mmultiscripts><mrow><mi mathvariant="normal">F</mi></mrow><mprescripts></mprescripts><mrow></mrow><mrow><mn>18</mn></mrow><mrow></mrow><mrow></mrow></mmultiscripts></mrow></math></span>

M. R. Gunye; S. B. Khadkikar

doi:10.1103/PhysRevC.4.1073

Nuclear-Structure Calculations in ${}^{18}F$

M. R. Gunye

S. B. Khadkikar

Tata Institute of Fundamental Research, Bombay 5, India

Physical Research Laboratory, Ahmedabad 9, India

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Phys. Rev. C 4, 1073 – Published 1 October, 1971

DOI: https://doi.org/10.1103/PhysRevC.4.1073

Abstract

The two intrinsic Hartree-Fock (HF) states, one characterized by isospin $T = T_{z} = \frac{1}{2} (N - Z)$ and the other containing an admixture of $T = T_{z}$ and $T = T_{z} + 1$ , lie energetically very close in the case of light $odd - Z - odd - N$ nuclei. As a result, the low-lying $T = T_{z}$ states of these nuclei have substantial "band mixing." The HF projection formalism is employed to investigate the effect of band mixing on the properties of nuclear states in ${}^{18}F$ by explicitly treating all the nucleons. The results of our calculations are in fair agreement with the experimental data.

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Nuclear-Structure Calculations in ${}^{18}F$

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Nuclear-Structure Calculations in F18

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Nuclear-Structure Calculations in ${}^{18}F$