posted on 2016-05-16, 00:00authored byDuncan John Mowbray, Annapaola Migani
Optimizing the photovoltaic
efficiency of dye-sensitized solar
cells (DSSC) based on staggered gap heterojunctions requires a detailed
understanding of sub-band gap transitions in the visible from the
dye directly to the substrate’s conduction band (CB) (type-II
DSSCs). Here, we calculate the optical absorption spectra and spatial
distribution of bright excitons in the visible region for a prototypical
DSSC, catechol on rutile TiO2(110), as a function of coverage
and deprotonation of the OH anchoring groups. This is accomplished
by solving the Bethe–Salpeter equation (BSE) based on hybrid
range-separated exchange and correlation functional (HSE06) density
functional theory (DFT) calculations. Such a treatment is necessary
to accurately describe the interfacial level alignment and the weakly
bound charge transfer transitions that are the dominant absorption
mechanism in type-II DSSCs. Our HSE06 BSE spectra agree semiquantitatively
with spectra measured for catechol on anatase TiO2 nanoparticles.
Our results suggest deprotonation of catechol’s OH anchoring
groups, while being nearly isoenergetic at high coverages, shifts
the onset of the absorption spectra to lower energies, with a concomitant
increase in photovoltaic efficiency. Further, the most relevant bright
excitons in the visible region are rather intense charge transfer
transitions with the electron and hole spatially separated in both
the [110] and [001] directions. Such detailed information on the absorption
spectra and excitons is only accessible via periodic models of the
combined dye-substrate interface.