The
molecular dipole polarizability can be decomposed into components
corresponding to the charge flow between atoms and changes in atomic
dipole moments. Such decompositions are recognized to depend on how
atoms are defined within a molecule, as, for example, by Hirshfeld,
iterative Stockholder, or quantum topology partitioning of the electron
density. For some of these, however, there are significant differences
between the numerical results obtained by analytical response methods
and finite field calculations. We show that this difference is due
to analytical response methods accounting for (only) the change in
electron density by a perturbation, while finite field methods may
also include a component corresponding to a perturbation-dependent
change in the definition of an atom within a molecule. For some atom-in-molecule
definitions, such as the iterative Hirshfeld, iterative Stockholder,
and quantum topology methods, the latter effect significantly increases
the charge flow component. The decomposition of molecular polarizability
into atomic charge flow and induced dipole components thus depends
on whether the atom-in-molecule definition is taken to be perturbation-dependent.