 For non-commuting observables in a \(n\)-dimensional Hilbert space, one can similarly define an entropic uncertainty in the probability distribution \(\abs{\braket{a_i}{\psi}}^2\) for a given state \(\ket{\psi}\) and a complete set of eigenstates \(\ket{a_i}\), \( (i= 1, \ldots n)\), of the observable \(\bA\): 