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H. J. Xia

Publications and source records attributed to H. J. Xia.

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The interplay of single-particle and collective motions in the low-lying states of $^{21}_Λ$Ne with quadrupole-octupole correlations

The beyond mean-field approach for low-lying hypernuclear states is extended by mixing the configurations associated with both single-particle and quadrupole-octupole collective excitations within the generator coordinate method based on a covariant density functional theory. The method is demonstrated in the application to the low-lying states of $^{21}_Λ$Ne, where the configurations with the $Λ$ hyperon occupying the first ($Λ_s$) and second ($Λ_p$) lowest-energy states are considered. The results indicate that the positive-parity states are dominated by the $α+^{12}$C+$α+Λ_s$ structure. In contrast, the low-lying negative-parity states are dominated by a strong admixture of $α+^{16}$O+$Λ_s$ structure and $α+^{12}$C+$α+Λ_p$ structure due to the inclusion of octupole correlations. As a result, the low-lying negative-parity states become much lower than what is expected from the previous studies without the mixing, and the electric multipole transition strengths are significantly quenched.

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Beyond mean-field approach for pear-shaped hypernuclei

We develop both relativistic mean field and beyond approaches for hypernuclei with possible quadrupole-octupole deformation or pear-like shapes based on relativistic point-coupling energy density functionals. The symmetries broken in the mean-field states are recovered with parity, particle-number, and angular momentum projections. We take $^{21}_Λ$Ne as an example to illustrate the method, where the $Λ$ hyperon is put on one of the two lowest-energy orbits (labeled as $Λ_s, Λ_p$), respectively. We find that the $Λ$ hyperon in both cases disfavors the formation of a reflection-asymmetric molecular-like $^{16}$O$+α$ structure in $^{20}$Ne, which is consistent with the Nilsson diagram for the hyperon in $(β_2, β_3)$ deformation plane. In particular, we show that the negative-parity states with the configuration $^{20}$Ne($K^π=0^-)\otimes Λ_s$ are close in energy to those with the configuration $^{20}$Ne($K^π=0^+)\otimes Λ_p$, even though they have very different structures. The $Λ_s$ ($Λ_p$) becomes more and more concentrated around the bottom (top) of the "pear" with the increase of octupole deformation.

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