Sonoluminescence spectra of the heavy rare gases are calculated by combinin
g the Hilgenfeldt rt al. model of sonoluminescence [Phys. Fluids 11, 1318 (
1999)] with quantum line-shape calculations of electron-neutral-atom bremss
trahlung spectra [L. Frommhold, Phys. Rev. E 58, 1899 (1998)]. Good agreeme
nt between theoretical and experimental spectra is obtained by choosing val
ues of the ambient radius R-0 and acoustic pressure amplitude P-a that are
compatible with diffusive equilibrium calculations.