J. J. P. Thompson, D. J. Leech, M. Mucha-Kruczynski Department of Physics, University of Bath, Claverton Down, Bath BA2 7AY, United Kingdom ![]() In monolayer graphene, the wavefunction is a superposition of Bloch states on two sublattices lying on the same plane, in bilayer graphene electrons live on four sites distributed across two layers. In the presence of an external perpendicular magnetic field, electronic states in each of the two otherwise equivalent Brillouin zone corners occupy one of the layers preferentially. We show that such an arrangement results in valley-polarised tunnelling currents due to the difference in distances to arrive at the monolayer graphene electrode. We predict valley polarisations of the order of 80% in magnetic fields B ~1T and because of the chiral nature of the electronic states in graphene, this valley-polarisation can be tuned between the two valleys via the manipulation of applied voltages only. [1] L. Britnell et al., Nature Communications, 4, 1794 (2013). [2] A. Mishchenko et al., Nature Nanotechnology, 9, 808 (2014). ![]() |