Numerical simulations of a box model for quantum annealing reveal residual energy largely independent of landscape roughness and annealing depth, with flat energy gaps proposed to explain diabatic trapping.
(B6), the stationary condition yields h0 2 1 α2 π w0 2 cos 2πx0 w0 e− 1 α π w0 2 = ¯h2 4m − k 4α2 (B9) From Eq
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Box model of quantum annealing
Numerical simulations of a box model for quantum annealing reveal residual energy largely independent of landscape roughness and annealing depth, with flat energy gaps proposed to explain diabatic trapping.