Erratum: Effect of pairing correlations on the isospin-mixing parameter in deformed $N=Z$ even-even nuclei [Phys. Rev. C 86, 034332 (2012)]

Figure 2

(The curves in the right panel changed but not the scales.) Convergence of the ground-state structure as a function of the number of pair excitations in the ${}^{48}\mathrm{Cr}$ nucleus. The weights of the components of the correlated wave function (up to the DP excitations) are plotted as a function of $V_0^{(T=1)}$ (left panels) and as a function of $x$ (right panels) for $V_0^{(T=1)}=-200{\mathrm{MeV}\mathrm{fm}}^3$.

Figure 3

(The curves in the right panel changed.) Contributions of the quasivacuum (thick solid lines), SP (thin solid lines with open circles), DP (thin solid lines with full triangles), and TP (thin solid lines with open squares) excitations to the correlated ground state for the four selected $N=Z$ deformed even-even nuclei (${}^{28}\mathrm{Si},{}^{48}\mathrm{Cr},{}^{68}\mathrm{Se}$—oblate and prolate solutions—and ${}^{76}\mathrm{Sr}$ from top to bottom) as functions of $|V_0^{(T=1)}|$ (left panels) and as functions of $x$ for $V_0^{(T=1)}=-300{\mathrm{MeV}\mathrm{fm}}^3$ (right panels).

Figure 4

(The curves in the right panel changed.) Weights of SP quasieigenstates of ${\widehat{\mathbf{T}}}^2$ in the $|{\Psi }_{\mathrm{SP}}\rangle$ contribution to the highly truncated diagonalization approach (HTDA) solution $|\Psi \rangle$ as functions of $|V_0^{(T=1)}|$ (left panel) and as functions of $x$ (right panel). Full squares, circles, and triangles correspond to the sums over clusters of the weights of $|{\Psi }_{01}^{\left(k\right)}\rangle ,|{\Psi }_{02}^{\left(k\right)}\rangle$, and $|{\Psi }_1^{\left(k\right)}\rangle$ states, respectively.

Figure 5

(The curves in the right panel changed.) Variation in the relative $T=2$ contribution to the isospin-mixing parameter with the strength $V_0^{(T=1)}$ of the residual interaction in the $T=1$ channel (left panel) and with $x$ (right panel) for the four selected $N=Z$ deformed even-even nuclei (${}^{28}\mathrm{Si},{}^{48}\mathrm{Cr},{}^{68}\mathrm{Se}$—oblate and prolate solutions—and ${}^{76}\mathrm{Sr}$).

Figure 6

(The curves in the right panel changed.) Variation in the correlation contribution to the isospin-mixing parameter (calculated without the $T=2$ component) with the strength $V_0^{(T=1)}$ of the residual interaction in the $T=1$ channel (left panel) and with $x$ (right panel) for the four selected $N=Z$ deformed even-even nuclei (${}^{28}\mathrm{Si},{}^{48}\mathrm{Cr},{}^{68}\mathrm{Se}$—oblate and prolate solutions—and ${}^{76}\mathrm{Sr}$).

Figure 7

(The curves in the right panel changed.) Decomposition of the correlation contribution to the isospin-mixing parameter (calculated without the $T=2$ component) according to Eq. (44) resulting from the decoupled-cluster approximation including the single-pair ($C_{\mathrm{SP}}$) and double-pair ($C_{\mathrm{DP}}$) contributions only. Left panel: variation with $V_0^{(T=1)}$ and $x=0$. Right panel: variation with $x$ for $V_0^{(T=1)}=-300{\mathrm{MeV}\mathrm{fm}}^3$.

Figure 8

(The curves in the right panel changed.) DCA analysis by $T$ values of the SP (upper row) and DP (lower row) contributions to $\alpha$ in ${}^{76}\mathrm{Sr}$. Left column: variations with $V_0^{(T=1)}$ and $x=0$. Right column: variations with $x$ for $V_0^{(T=1)}=-300{\mathrm{MeV}\mathrm{fm}}^3$.

Figure 9

(The curves in the right panel changed.) Isospin-mixing parameter $\alpha$ of the HTDA ground state obtained in three different calculations: with exact exchange terms in the Coulomb mean field and without residual Coulomb interaction (thick solid line, labeled “Exact MF”), with the Slater approximation to the exchange Coulomb mean field and without residual Coulomb interaction (thin solid line with open circles, labeled “Slater MF”), and with an exact treatment of the full Coulomb interaction (thin solid line with open squares, labeled “Exact MF + res”). Left panel: variation with $V_0^{(T=1)}$; right panel: variation with $x$ for $V_0^{(T=1)}=-300{\mathrm{MeV}\mathrm{fm}}^3$.