  We present new results of point-contact Andreev-reflection (PCAR)
spectroscopy in single-phase Mg_{1-x}Al_{x}B_{2} single crystals with x up to
0.32. Fitting the conductance curves of our point contacts with the two-band
Blonder-Tinkham-Klapwijk model allowed us to extract the gap amplitudes
Delta_{sigma} and Delta_{pi}. The gap values agree rather well with other PCAR
results in Al-doped crystals and polycrystals up to x=0.2 reported in
literature, and extend them to higher Al contents. In the low-doping regime,
however, we observed an increase in the small gap Delta_{pi} on increasing x
(or decreasing the local critical temperature of the junctions, T_{c}^{A})
which is not as clearly found in other samples. On further decreasing T_{c}^{A}
below 30 K, both the gaps decrease and, up to the highest doping level x=0.32
and down to T_{c}^{A}= 12 K, no gap merging is observed. A detailed analysis of
the data within the two-band Eliashberg theory shows that this gap trend can be
explained as being mainly due to the band filling and to an increase in the
interband scattering which is necessary to account for the increase in
Delta_{pi} at low Al contents (x < 0.1). We suggest to interpret the following
decrease of Delta_{pi} for T_{c}^{A} < 30 K as being governed by the onset of
inhomogeneity and disorder in the Al distribution that partly mask the
intrinsic effects of doping and is not taken into account in standard
theoretical approaches.
