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.
˜Evar = min ⃗ α ⟨ψvar(⃗ α)|H|ψvar(⃗ α)⟩(B1) where ˜Evar is the approximation to the targeted energy
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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.