We investigate the viability of observing charged Higgs bosons (
H±H^\pm) produced in association with
WW bosons at the CERN large hadron collider, using the leptonic decay
H+ ®t+ ntH^+ \to\tau^+ \nu_\tau and hadronic
WW decay, within different scenarios of the minimal supersymmetric standard model (MSSM) with both real and complex parameters.
Performing a parton level study we show how the irreducible standard model background from
W+2W+2 jets can be controlled by applying appropriate cuts and find that the size of a possible signal depends on the cuts needed
to suppress QCD backgrounds and misidentifications. In the standard maximal mixing scenario of the MSSM we find a viable signal
for large
tanb\tan\beta and intermediate
H±H^\pm masses (
~ mt{\sim} m_t) when using softer cuts (
p^\textmissp_{\perp\text{miss}},
$p_{\perp\tau{\text{jet}}} >$p_{\perp\tau{\text{jet}}} > 50 GeV), whereas for harder cuts (
p^\textmissp_{\perp\text{miss}},
$p_{\perp\tau{\text{jet}}} >$p_{\perp\tau{\text{jet}}} > 100 GeV) we only find a viable signal for very large
tanb\tan\beta (
>~50\gtrsim50). We have also investigated a special class of MSSM scenarios with large mass splittings among the heavy Higgs bosons where
the cross-section can be resonantly enhanced by factors up to one hundred, with a strong dependence on the
CPCP-violating phases. Even so we find that the signal after cuts remains small except for small masses (
<~ mt{\lesssim} m_t) when using the softer cuts. Finally, in all the scenarios we have investigated we have only found small
CPCP-asymmetries.