Chiral chains with two valleys and disorder of finite correlation length
arXiv:2304.04808 · doi:10.1103/PhysRevB.108.075430
Abstract
In one-dimensional disordered systems with a chiral symmetry it is well-known that electrons at energy avoid localization and simultaneously exhibit a diverging density of states (DOS). For coupled chains with zero-correlation-length disorder, the diverging DOS remains for odd , but a vanishing DOS is found for even . We use a thin spinless graphene nanotube with disordered Semenoff mass and disordered Haldane coupling to construct chiral chain models which at low energy have two linear band crossings at different momenta (two valleys) and disorder with an arbitrary correlation length in units of lattice constant . We find that the finite momentum forces the disorder in one valley to depend on the disorder in the other valley, thus departing from known analytical results which assume having independent disorders (whatever their spatial correlation lengths). Our main numerical results show that for this inter-dependent mass disorder the DOS is also suppressed in the limit of strongly coupled valleys (lattice-white noise limit, ) and exhibits a non-trivial crossover as the valleys decouple () into the DOS shapes of the continuum model with finite correlation length . We also show that changing the intra-unit-cell geometry of the disordered Haldane coupling can tune the amount of inter-valley scattering yet at lowest energies it produces the decoupled-valley behavior () all the way down to lattice white noise.
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