Therefore, and K are compatible observables.
In this notation, the kinetic energy operator is
Now note that
Therefore
is therefore a kinetic energy eigenfunction with eigenvalue .
The second part of the problem asks us to solve an inverse problem: Given a target probability, how close can the ``wires'' be?
It should shortly be possible to manufacture circuits whose traces are this far apart. Such devices will not be classical digital computers but will have to account for quantum effects.