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Volumn 82, Issue 12, 2010, Pages

Lattice gauge theory model for graphene

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EID: 77957735366     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.82.121418     Document Type: Article
Times cited : (31)

References (31)
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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.
    • ) 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
    • 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
    • ∂ 2 ∂ λ k, j - ∂ λ k + p, i + W h (∂ α, λ) | α = λ = 0.
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