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In this model, the y component of Q2 kF is π, which may be different from the wave vector of the SDW for certain anions. Nevertheless, our theory is general and does not depend on the wave vector Q2 kF. The key is that the spin and the charge fluctuations have the same wave vector.
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In this model, the y component of Q2 kF is π, which may be different from the wave vector of the SDW for certain anions. Nevertheless, our theory is general and does not depend on the wave vector Q2 kF. The key is that the spin and the charge fluctuations have the same wave vector.
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42349094071
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The definition of the parameters is different from that in Ref. for clarity. (V, V′, V″, Vp) in Ref. corresponds to (V1, V2, V3, Vy) here.
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The definition of the parameters is different from that in Ref. for clarity. (V, V′, V″, Vp) in Ref. corresponds to (V1, V2, V3, Vy) here.
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