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2) [4]. In the negative-U case, it was shown that the spin SU(2) symmetry could not be spontaneously broken [13]. Thus we will not consider the spin SU(2) symmetry in this paper. By the term SU(2) symmetry, (if used without any qualification) we will always mean pseudospin symmetry in this paper.
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This inequality can be proven by using the spin-reflection positivity in the ground state of a negalive-U Hubbard model. The proof can be seen in [6, 18]. In the former, we proved the equality part of the inequality; in the latter we proved a similar spin-operator inequality for a positive-U Hubbard model at half-filling, and this inequality for pseudospin operators can easily be obtained by using the partial particle-hole transformation from the positive-U case.
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The superfluid density defined here is related to the penetration depth of an external magnetic field. When it is not equal to zero, the penetration depth is finite and the state is diamagnetic. Usually the CDW states are insulating and the Drude weight should be zero (or the resistance is equal to zero) In this case the quasiparticle spectrum has a gap, and the superfluid density is equal to the Drude weight [21], i.e., the superfluid density in an insulating CDW state is always zero.
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