A shooting technique yields smooth control pulses for quantum gates on spin qudits that are faster than GRAPE, with the advantage growing as system dimension increases, shown in numerical simulations inspired by single molecule magnets.
Accordingly the gradient∇J(M) should be given by ∇J(M) = v1 2(y1 +M 2)v2 (C12) and it is straightforward to verify that the vector in Eq
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Implementation of a shooting technique for quantum optimal control on spin qudits
A shooting technique yields smooth control pulses for quantum gates on spin qudits that are faster than GRAPE, with the advantage growing as system dimension increases, shown in numerical simulations inspired by single molecule magnets.