The excess noise factor due to the nonorthogonality of the transverse
modes of a geometrically stable cavity subject to large diffraction lo
sses is calculated. This calculation is based on an exact determinatio
n of the transverse field distribution of the cavity fundamental eigen
mode. It is shown that when the modes become essentially determined by
diffraction, the transverse modes an far from being orthogonal, leadi
ng to the appearance of a large excess noise factor that must multiply
the standard Schawlow-Townes linewidth. Moreover, in the presence of
two diffracting apertures, the excess noise factor is shown to exhibit
a resonant behavior reminiscent of the one observed in unstable cavit
ies. We estimate that, in the case of circular apertures, excess noise
factors as large as 100 can be experimentally measured using a high-g
ain gas microlaser.