A quantum mechanical model is developed for the observed resonance enh
ancement of light scattering by aggregates of electronically interacti
ng chromophores. Aggregate size, monomer oscillator strength, extent o
f electronic coupling, and aggregate geometry are all important determ
inants of intensity in resonance light scattering (RLS) spectra. The t
heory also predicts the value of the depolarization ratio (rho(V)(90))
of RLS for a given aggregate geometry. These results are used to inte
rpret the RLS depolarization ratios of four aggregates: tetrakis(4-sul
fonatophenyl)porphine aggregated at low pH (rho(V)(90) = 0.17 at 488 n
m), ns-bis(N-methylpyridinium-4-yl)-diphenylporphinato copper(II) aggr
egated in 0.2 M NaCl solution (rho(V)(90) = 0.13 at 450 nm) and on cal
f thymus DNA(rho(V)(90) = 0.20 at 454 nm), and chlorophyll a aggregate
s in formamide/water (rho(V)(90) = 0.23 and 0.32 at 469 and 699 nm, re
spectively). The analysis is consistent with a J-aggregate geometry fo
r all four systems. Furthermore, the specific values of rho(V)(90) all
ow us to estimate the orientation of the monomer transition dipoles wi
th respect to the long axis of the aggregate. We conclude that depolar
ized resonance light scattering spectroscopy is a powerful probe of th
e geometric and electronic structures of extended aggregates of strong
chromophores.