Ultrafast Spectroscopy
and Dynamics of Excitons and
Spin-Correlated Triplet-Pair Intermediates Generated in the Singlet
Exciton Fission of Naphtho-[2,1,8-qra]-tetracene
posted on 2025-11-24, 23:08authored byAkshaya Morye, Prabhat K. Sahu, Sangita Bose, Dipak K. Palit
The search for molecules that undergo efficient singlet
(exciton)
fission (SF) to generate two triplet excitons following absorption
of a single photon and create the possibility of generation of a pair
of charge carriers has been very intense during the last two decades.
Tetracene and its derivatives have shown great potential to become
efficient SF materials. Under this consideration, earlier workers
predicted the potentiality of naphtho-[2,1,8-qra]-tetracene (NpTc),
which nearly satisfies the energetic requirement of SF, to work as
an efficient SF material. But its detailed photophysics and dynamics
of the SF process are yet to be explored. This work provides a comprehensive
account of a detailed investigation of the photophysical properties
of the excited states of the molecule in polycrystalline mediums by
using ultrafast fluorescence and transient absorption (TA) spectroscopic
techniques to resolve the intricate mechanism of the SF process. Generation
of a pair of free triplet (T<sub>1</sub>) excitons in the SF process
has been found to follow a mechanism of two sequential and one parallel
step after the population of the singlet (S<sub>1</sub>) exciton
state. Two sequential steps consist of the ultrafast decay of the
S<sub>1</sub> exciton populating the spin-correlated interacting triplet
pair state (CTP1), in which two T<sub>1</sub> excitons reside on two
molecules at neighboring sites in the crystal. In turn, the CTP1 undergoes
the spatial separation of two triplets to create a spin-correlated
but noninteracting spin correlated triplet pair, the CTP2 state, in
which the triplet excitons are spatially separated beyond their neighboring
sites. In the last step of the SF process, the disappearance of the
CTP2 state follows a parallel step, in which two T<sub>1</sub> excitons
either get separated into two free T<sub>1</sub> excitons or undergo
triplet fusion to generate back one S<sub>1</sub> exciton and one
molecule in the S<sub>0</sub> state. The overall lifetime of completion
of the SF process (or generation of two free T<sub>1</sub> excitons)
in 45 nm thin films is about 31 ps. However, the SF rate decreases
upon increasing the thickness of the film, for which one of the possible
reasons may be attributed to reduction in intermolecular electronic
coupling energy in thicker films.