  A nonadiabatic scheme for the description of the coupled electron and nuclear
motions in the ozone molecule was proposed recently. An initial coherent
nonstationary state was prepared as a superposition of the ground state and the
excited Hartley band. In this situation neither the electrons nor the nuclei
are in a stationary state. The multiconfiguration time dependent Hartree method
was used to solve the coupled nuclear quantum dynamics in the framework of the
adiabatic separation of the time-dependent Schr\"odinger equation. The
resulting wave packet shows an oscillation of the electron density between the
two chemical bonds. As a first step for probing the electronic motion we
computed the time-dependent molecular dipole and the Dyson orbitals. The latter
play an important role in the explanation of the photoelectron angular
distribution. Calculations of the Dyson orbitals are presented both for the
time-independent as well as the time-dependent situations. We limited our
description of the electronic motion to the Franck-Condon region only due to
the localization of the nuclear wave packets around this point during the first
5-6 fs.
