In the case of the short-range potential [1,5,8,9], the
estimation of the probability of ionization of atoms is carried
along taking into account the approximation (Keldysh
approximation) which states that this kind of potential does not
affect the energy of the final state f of the ejected electron
in the laser field, because the electron is far enough from the
nucleus. When the Coulomb potential is taken into account, it can
be treated as a perturbation to the energy of the final state
[1,10]. Yet, originally [1,10], the Coulomb potential in this kind
of estimation was not included into calculating the turning point.
This was done in [7], but only for the fields below the atomic
field (1016 W/cm2). Now, based on the results [11,12], we
are extending our calculation that included the Coulomb correction
into the estimating the turning point to the fields that are much
stronger (up to 1017 W/cm2). That results in the shift of
the position of the turning point τ. This paper is dealing
with the influence of that shift on the ionization probability for
atoms in the low-frequency electromagnetic field of superstrong
lasers.