Abstract

The coexistence of various low-lying deformed states in |$^{42}$|Ca and the |$\alpha $|–|$^{38}$|Ar correlations in those deformed states have been investigated using deformed-basis antisymmetrized molecular dynamics. Wave functions of the low-lying states are obtained via parity and angular momentum projections and the generator coordinate method (GCM). Basis wave functions of the GCM calculation are obtained via energy variations with constraints on the quadrupole deformation parameter |$\beta $| and the distance between |$\alpha $| and the |$^{38}$|Ar clusters. The rotational bands built on the |$J^\pi = 0_2^+$| (1.84 MeV) state as well as the |$J^\pi = 0_3^+$| (3.30 MeV) state are both reproduced. The coexistence of two additional |$K^\pi = 0^+$| rotational bands is predicted; one band is shown to be built on the |$J^\pi = 0_3^+$| state. Members of the ground-state band and the rotational band built on the |$J^\pi = 0_3^+$| state contain |$\alpha $|–|$^{38}$|Ar cluster structure components.

Highlights

  • Drastic structural changes initiated by low excitation energies are a significant characteristic of nuclear systems, and the coexistence of deformed states and cluster structures is a typical phenomenon

  • This rotational band has a large moment of inertia that is similar to the ones of the SD bands in 36Ar and 40Ca, scaled by A5/3[9], which is proportional to square of quadrupole deformation parameter β in the liquid-drop model

  • This paper aims to clarify the structures of excited deformed bands in positive-parity states of 42Ca by focusing on the coexistence of rotational bands with mp-mh configurations

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Summary

Introduction

Drastic structural changes initiated by low excitation energies are a significant characteristic of nuclear systems, and the coexistence of deformed states and cluster structures is a typical phenomenon. In 42Ca, deformed states with mp-mh configurations and clustering behavior have been observed experimentally, and the rotational band built on the Jπ = 0+2 (1.84 MeV) state (Kπ = 0+2 band) has been observed[1, 9]. The α+38Ar orthogonality condition model (OCM) describes 4p2h states with α–38Ar cluster structures, but a rotational band with a 6p4h configuration is not obtained in low-lying states[13]. This paper aims to clarify the structures of excited deformed bands in positive-parity states of 42Ca by focusing on the coexistence of rotational bands with mp-mh configurations. The α–38Ar cluster correlations in low-lying deformed states are discussed.

Wave function
Energy variation
Generator coordinate method
GCM basis obtained by energy variation
E2 transition strengths
Band assignment
Particle-hole configurations and E2 transitions
Findings
Conclusions

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