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The valley-isotropic Dirac Hamiltonian (1) acts on the spinor ((Equation presented), (Equation presented)) in valley (Equation presented) and ((Equation presented), (Equation presented)) in valley (Equation presented), where (Equation presented) and (Equation presented) are the wave amplitudes on the two triangular sublattices that form the hexagonal lattice of graphene.
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Because the spin degree of freedom is not counted, the conductance quantum is (Equation presented) rather than (Equation presented).
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