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) 3 ψ k+p + Γμ (k,p ) ψk- where Γμ are matrices which can be deduced from Eq. with Γ0 ( kFω ,0 ) =-iI, Γ1 ( kFω ,0 ) =- σ2, Γ2 ( kFω ,0 ) =-ω σ1.
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) 3 ψ k + p + Γ μ (k, p) ψ k - where Γ μ are matrices which can be deduced from Eq. with Γ 0 (k F ω, 0) = - i I, Γ 1 (k F ω, 0) = - σ 2, Γ 2 (k F ω, 0) = - ω σ 1.
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Wh is defined in the same way as W with an extra infrared cutoff suppressing momenta smaller than Mh
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W h is defined in the same way as W with an extra infrared cutoff suppressing momenta smaller than M h.
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∂2 ∂ λ k,j - ∂ λ k+p,i + Wh (∂α,λ ) |α=λ=0
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∂ 2 ∂ λ k, j - ∂ λ k + p, i + W h (∂ α, λ) | α = λ = 0.
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