Abstract
By using the correlated operators generated within the framework of the first-order perturbation theory, we obtain simultaneously an enhancement of the C6 form factor for 50Ti around the first peak, compared to the single-particle-model predition, and a reduction of the C6 form factor for 52Cr in the same momentum-transfer range, both cases being consistent with the experiments. It is the two-body form of the transition operators that plays a crucial role in elucidating this long-standing puzzle.
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