HOPV12 - Blogs
HOPV12 - Blogs
HOPV12 - Blogs
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4 th Hybrid and Organic Photovoltaic Conference -Uppsala 2012 121<br />
C20 - Modelling of Energy and Hole Transfer in Co-sensitized Dye-Sensitized TiO2:<br />
Electronic structure, optical properties and FRET<br />
Mariachiara Pastore, Filippo De Angelis<br />
ISTM-CNR, Via Elce di sotto, 8, Perugia, 6123, IT<br />
Dye-sensitized solar cells (DSSCs) 1 are attracting a wide-spread interest as low-cost<br />
alternatives to conventional photovoltaics. A possible way to increase the power conversion<br />
efficiency in DSSCs is to enhance the light harvesting in the near–infrared portion of the solar<br />
spectrum by co-sensitization of TiO2 with organic dyes having high NIR absorption; this<br />
strategy was recently investigated by Hardin et al. 2 employing a zinc naphthalocyanine-based<br />
dye (AS02) and the Ru(II) C106 dye The main drawback of co-sensitization is the usually low Voc<br />
due to higher recombination rates of NIR dyes. 3 Higher Voc can be obtained by insulating the<br />
NIR dye from the oxide surface thus using it as an energy rely dye (ERD), able to absorb energy<br />
and undergo Forster resonant energy transfer (FRET) to the sensitizing-dye (SD). To enhance<br />
the FRET efficiency and reduce the voltage losses, a careful tuning of the optical and structural<br />
properties of the NIR-ERD is required: it should have intense absorption and high<br />
photoluminescence quantum efficiency, its emission spectrum should largely overlap the<br />
absorption spectrum of SD, its HOMO should be lower than the redox mediator potential to<br />
have fast regeneration and finally, it should intimately mix and interact with the SD. Motivated<br />
by the work of Hardin et al. 2 and by the great interest in the design of new NIR-ERDs having<br />
the proper electronic and structural properties, we carried out a computational investigation<br />
of (AS02+C106) co-sensitized TiO2 models based upon DFT, Time-Dependent (TD) DFT and ab<br />
initio MP2 calculations.<br />
Figure 1 Model of AS02 and C106 co-adsorption on a grid of Ti atoms representing the TiO2 anatase (101) surface.<br />
On the basis of our experience in the computational prediction of the optical properties of<br />
organic 4 and inorganic 5 sensitizers and in the modeling of dye/TiO2 heterointerfaces 6-7 we<br />
calculated the electronic absorption and emission spectra of the dyes in solution and grafted<br />
to the titania surface, determined the preferred adsorption geometry of the AS02 and C106<br />
dyes onto the semiconductor surface and the relative energy level alignments with respect to<br />
the semiconductor CB. Employing a larger TiO2 model, we modeled the coadsorption of AS02<br />
and C106 dyes, evaluating at MP2 level of theory the relative stability of various co-adsorption<br />
patterns and then the associated optical response.<br />
Owing to our high-level computational methodology, we are able to provide new insights<br />
into the energy transfer mechanisms in co-sensitized solar cells, suggesting guidelines to<br />
design new ERDs with extended NIR absorption and the proper energy level alignment to<br />
suppress hole transfer processes.<br />
© SEFIN 2012