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In this paper we assume γ to be constant on the Fermi surface. Recently the form of the coupling constant has been found (see Ref.). The angular dependence of the coupling constant has the form γ (k k′) ik× k′. In the particle-hole channel its angular decomposition contains only even harmonics. For instance, using the above form in the singular vertex, Eq. 7, we obtain (ik× k′) 2 1-cos (2θ-2 θ′). Only the zero harmonic is important in the analysis of density correlation function.
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In this paper we assume γ to be constant on the Fermi surface. Recently the form of the coupling constant has been found (see Ref.). The angular dependence of the coupling constant has the form γ (k k′) ik× k′. In the particle-hole channel its angular decomposition contains only even harmonics. For instance, using the above form in the singular vertex, Eq. 7, we obtain (ik× k′) 2 1-cos (2θ-2 θ′). Only the zero harmonic is important in the analysis of density correlation function.
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There is another branch cut at Im ε1 +Im ε2 =0 which follows from the absorptive part in the Cooper channel. This other channel will not be considered here.
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There is another branch cut at Im ε1 +Im ε2 =0 which follows from the absorptive part in the Cooper channel. This other channel will not be considered here.
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This notation is motivated by apparent similarity with diffusive system where d (ω) = vf2 τ/2=D because S0 -iτ when ω,q vF τ-1. The similarity does not go beyond notation: in marginal Fermi liquid the motion of quasiparticles is not diffusive because Eq. 29 is valid only at ultrasmall momenta q vF ω.
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This notation is motivated by apparent similarity with diffusive system where d (ω) = vf2 τ/2=D because S0 -iτ when ω,q vF τ-1. The similarity does not go beyond notation: in marginal Fermi liquid the motion of quasiparticles is not diffusive because Eq. 29 is valid only at ultrasmall momenta q vF ω.
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