We discuss two conditions needed for correct computation of 2νββ nuclear matrix-elements within the realistic shell-model framework. This algorithm yields rapid convergence on the 2νββ matrix-elements, even when neither relevant GT + nor GT − strength distribution is convergent. A significant role of the shell structure is pointed out, which makes the 2νββ matrix-elements highly dominated by the lowlying intermediate states. Experimental information of the low-lying GT ± strengths is strongly desired. Half-lives of T 2ν 1/2 (EC/EC; 36 Ar → 36 S) = 1.7 × 10 29 yr, T 2ν 1/2 (EC/EC; 54 Fe → 54 Cr) = 1.5 × 10 27 yr, T 2ν 1/2 (EC/EC; 58 Ni → 58 Fe) = 6.1 × 10 24 yr and T 2ν 1/2 (β + /EC; 58 Ni → 58 Fe) = 8.6×10 25 yr are obtained from the present realistic shell-model calculation of the nuclear matrix-elements.