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(1)(P)=0 for any projector P. Although considerations of such alternative definitions may have some mathematical interest, we believe the present choice is, from a physical point of view, the most natural, as it turns out to be rucible to the mixed-state phase of Ref. [6] for l = 1 [see Eq. (15)] and it can be realized experimentally, at least for l≤2 (see Sec. IV).
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