  A quantum impulse is a brief but strong perturbation that produces a sudden
change in a wavefunction $\psi(x)$. We develop a theory of quantum impulses,
distinguishing between ordinary and super impulses. An ordinary impulse paints
a phase onto $\psi$, while a super impulse -- the main focus of this paper --
deforms the wavefunction under an invertible map, $\mu: x -> x'$. Borrowing
tools from optimal mass transport theory and shortcuts to adiabaticity, we show
how to design a super impulse that deforms a wavefunction under a desired map
$\mu$, and we illustrate our results using solvable examples. We point out a
strong connection between quantum and classical super impulses, expressed in
terms of the path integral formulation of quantum mechanics. We briefly discuss
hybrid impulses, in which ordinary and super impulses are applied
simultaneously. While our central results are derived for evolution under the
time-dependent Schrodinger equation, they apply equally well to the
time-dependent Gross-Pitaevskii equation, and thus may be relevant for the
manipulation of Bose-Einstein condensates.
