  A theory of singlet fission (SF) in carotenoid dimers is applied to explain
the SF in lycopene H-aggregates observed after high energy photoexcitation. The
explanation proposed here is that a high energy, delocalized bright $^1B_u^+$
state first relaxes and localizes onto a single lycopene monomer. The
high-energy intramonomer state then undergoes internal conversion to the
$1^1B_u^-$ state. Once populated, the $1^1B_u^-$ state allows exothermic
bimolecular singlet fission, while its internal conversion to the $2^1A_g^-$
state is symmetry forbidden. The simulation of SF predicts that the
intramonomer triplet-pair state undergoes complete population transfer to the
intermonomer singlet triplet-pair state within 100 ps. ZFS interactions then
begin to partially populate the intermonomer quintet triplet-pair state up to
ca. 2 ns, after which hyperfine interactions thermally equilibrate the
triplet-pair states, thus forming free, single triplets within ca. 0.1 $\mu$s.
