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The instanton approach to the in-gap fluctuation states is applied to the spectrum of biased bilayer graphene. It is shown that the density of states falls off with energy measured from the band edge as ν(ϵ)∝exp(-|ϵ/ϵₜ|3/2), where the characteristic tail energy, ϵₜ, scales with the concentration of impurities, nᵢ, as nᵢ2/3. While the bare energy spectrum is characterized by two energies: the bias-induced gap, V, and interlayer tunneling, t_⊥, the tail, ϵₜ, contains a single combination V1/3t_⊥2/3. We show that the above expression for ν(ϵ) in the tail actually applies all the way down to the midgap.
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Mkhitaryan et al. (2008) studied this question.
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