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Here we work in a basis of spin states in which the λi are diagonal. In a general basis, sums over spin states must be replaced by traces. For example, the term involving (ξ1O)*ξ2O that would appear in Eq. 16 is Tr[(ξ1O)αα'*A1α',2β3γ, 4δ(ξ2O)ββ'(A†)1α,2β'3γ,4δ], where all repeated indices are to be summed over and the numbers 1,..., 4 refer only to the quasiparticle momentum.
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We note that our definition of S(q) differs from that of Schwenk and Friman by a factor of 3.
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We note that our definition of S(q) differs from that of Schwenk and Friman by a factor of 3.
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