The effects of exciton-vibrational coupling and point defects on the absorp
tion and emission of distyrylbenzene nanoaggregates are treated theoretical
ly. Two aggregate types based on a two-dimensional array of cyclic tetramer
s (pinwheels) are considered: type A aggregates, composed of chiral pinwhee
ls, and type B aggregates, composed of achiral pinwheels. The low-energy vi
bronic features in the experimental excitation spectrum arise from vibratio
nally dressed K = (0,0) excitons, while the more intense blue shifted H-ban
d is due to nearly free K = (0,0) excitons. The K = (0,0) features are pola
rized primarily along the herringbone plane normal. The lowest Davydov comp
onent is polarized in the herringbone plane and is due to the lowest energy
K = (pi,pi) exciton. This state is also responsible for the aggregate emis
sion. The 0-upsilon peaks for v >0 are mainly due to indirect transitions t
o the ground electronic state containing v phonons, with wave vector sum eq
ual to (pi,pi). These peaks are largely independent of defect fraction and
are polarized primarily along the herringbone plane normal. In stark contra
st, the 0-0 emission critically depends on the concentration of point defec
ts and is polarized entirely in the herringbone plane. This wavelength depe
ndent emission polarization is in full agreement with experimental observat
ions. Type A aggregates are weakly emissive, with the 0-0 emission peak van
ishing in defect-free aggregates and increasing with defect concentration.
The reverse holds for type B aggregates: the 0-0 intensity scales with the
number of molecules in the aggregate and decreases with defect concentratio
n. Sufficiently large type B aggregates are superradiant, and may be used t
o enhance the quantum yield in optical devices such as light-emitting diode
s. (C) 2001 American Institute of Physics.