The quantum-limited linewidth of a laser cavity is enhanced above the Schaw
low-Townes value by the Petermann factor K, due to the non-orthogonality of
the cavity modes. The average Petermann factor [K] in an ensemble of cavit
ies with chaotic scattering and broken time-reversal symmetry is calculated
non-perturbatively using random-matrix theory and the supersymmetry techni
que, as a function of the decay rate Gamma of the lasing: mode and the numb
er of scattering channels N. We find for Ai much greater than 1 that for ty
pical values of Gamma the average Petermann factor [K] proportional to root
N much greater than 1 is parametrically larger than unity.