  The connection between the neutrinoless double beta ((\beta\beta)_{0 \nu}-)
decay effective Majorana mass, |M_{ee}|, and the branching ratios of the decays
H^{\pm\pm}\to l^\pm {l'}^\pm, l,{l'}= e,\mu, of the doubly charged Higgs boson
H^{\pm\pm} is analysed within the Higgs Triplet Model of neutrino mass
generation. We work in the version of the model with explicit breaking of the
total lepton charge conservation, in which H^{\pm\pm}\to l^\pm {l'}^\pm, l,{l'}
= e,\mu,\tau, are the dominant decay modes of H^{\pm\pm}. It is assumed also
that H^{\pm\pm} are relatively light so that they can be produced at LHC and
the branching ratios of interest measured. Taking into account the current and
prospective uncertainties in the values of the neutrino mixing parameters most
relevant for the problem studied - the atmospheric neutrino mixing angle
\theta_{23} and the CHOOZ angle \theta_{13}, and allowing the lightest neutrino
mass and the CP violating Dirac and Majorana phases to vary in the intervals
[0, 0.3 eV] and [0, 2\pi], respectively, we derive the regions of values of
BR(H^{\pm\pm}\to e^\pm e^\pm) and BR(H^{\pm\pm}\to e^\pm \mu^\pm) for which
|M_{ee}|\geq 0.05 eV, or |M_{ee}| < 0.05 eV. This is done for neutrino mass
spectrum with normal ordering, inverted ordering and in the case when the type
of the spectrum is not known, and i) without using the possible additional data
on BR(H^{\pm\pm}\to \mu^\pm \mu^\pm), ii) using prospective data on
BR(H^{\pm\pm}\to \mu^\pm \mu^\pm). In the latter case results for several
values of BR(H^{\pm\pm}\to \mu^\pm\mu^\pm) are presented.
