The low-frequency (omega less-than-or-equal-to 1200 cm-1) Raman contin
ua of YBa2Cu3Ox single crystals have been measured in both the A1g and
B1g scattering geometries. The A1g continuum is found to be independe
nt of oxygen concentration x for 6.93 < x < 7.00, but the spectral dis
tribution in the B1g continuum depends sensitively on x in this same r
egion. The spectra were also calculated by assuming that the Raman con
tinua arise predominantly from scattering from the electronic excitati
ons in the copper-oxygen planes, and that the band structure for the p
lanes is reasonably reproduced by a two-dimensional tight-binding mode
l. If a superconducting gap function with d-wave symmetry is adopted,
the calculated results for A1g symmetry are found to be in good agreem
ent with the measured A1g spectrum. In contrast, however, the spectrum
calculated in B1g symmetry is inconsistent with the observed spectral
distribution. It is thus suggested that there must be additional sour
ces, for example scattering from spin fluctuations, that contributed t
o the B1g continuum.