... channels.¹

As far as we know, the only application of the canonical basis to charge-conserving modes near the drip line is in the relativistic QRPA, see e.g. [61,53].

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... state²

The conjugate state in our HFB code is slightly different: $\vert\overline{\mu m}\rangle = (-)^{j-m+l} \vert\mu -m \rangle$. This definition follows from Eq. (3.24b) of Ref. [60] and the single-particle wave function $\psi_{\mu m}({\mbox{\boldmath$r$\unboldmath}}) = R_{\mu}(r)\sum_{l_z\sigma}Y_{... ...le ll_z {\textstyle \frac{1}{2}} \sigma \vert j m \rangle \vert\sigma\rangle ,$ where $R_\mu(r)$ and $\vert\sigma=\pm 1/2\rangle$ are real radial and spin wave functions. Thus, we multiply all HFB $v_\mu$ by $(-)^{l}$ in the QRPA calculations.

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