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this follows from the perspective of rotation of the static order parameter from SC to Néel. Consequently, Eqs. (23) and (31) in Bruus et al. (Ref. 34), which describe the spin excitations, have gapless Goldstone modes because static SDW is present. This should be contrasted to our Eq. (1.17), whose right-hand side is nonzero, and whose SDW spectrum is gapped
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this follows from the perspective of rotation of the static order parameter from SC to Néel. Consequently, Eqs. (23) and (31) in Bruus et al. (Ref. 34), which describe the spin excitations, have gapless Goldstone modes because static SDW is present. This should be contrasted to our Eq. (1.17), whose right-hand side is nonzero, and whose SDW spectrum is gapped.
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