AAWSAP DIRD, Quantum Computing and Utilizing Organic Molecules in Automation Technology, December 2010
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UNCLASSIFIED//FOR. OFFI@IAI: l48E OHi:¥ Graphene Disc in Bilayer Graphene Bilayer graphene is the two-layer analog of the single layer. The two sublattices are coupled by the so-called Bernal stacking. A voltage V between the two layers breaks inversion symmetry (like the mass term ti in the single layer) and opens a gap proportional to the voltage. In addition, the combination of a top gate and a back gate allows tuning the gap and the average potential U(r) independently. A central issue, from a computational electronics perspective, is to quantitatively study the condensed state. In materials-based device models, one has an underlying Hamiltonian, such as an ab initio Hamiltonian .m In principle, the excitonic condensate emerges from the interacting particles described by the Hamiltonian. It is shown that both true bound states and quasi-bound states occur, depending on the form of the potentials. In addition, there is a third and most interesting possibility where the character of the states depends on the parameters of the potentials and can be controlled at will. A confinement-de-confinement transition then occurs in which the character of the states changes from oscillatory to exponential as in the Klein paradox for particles with mass. This gives a way of probing the Klein paradox experimentally in a solid state system and numerical studies of the quantum states in a realistic dot model show it is feasible. Further, the same effect could be used to fabricate a graphene dot which has true bound states. This only requires a uniform magnetic field and a gate which can be made lithographically, a geometry that is much easier to fabricate than the non-uniform magnetic field geometry. The relativistic nature of the transmission, exactly 100%, does not depend on E and Vo is a consequence of the zero mass. If the particles had mass mo, the energy-momentum relation would be (E - V) 2 - p 2c2 = mo2c4 and the amplitudes of the wave function components in equations of motion would depend on k or k' and mo. Then the right side amplitude in equations would be different from the left side amplitude, so a reflected wave would have to be introduced to satisfy the boundary condition at x = 0 and the transmission coefficient would not be 100%. bilayer aph · ne op gat f + + + + + + + + Figure 5. Quantum dot in bilayer graphene. m Ab initio Hamiltonian is one derived from first principles. UNCLASSIFIED/;'FOR. 8FFl@IAL U9I!! eHt I 17