Solid state Dye Sensitized Solar Cells (ssDSCs)
[1] are very promising photovoltaic devices, potentially
stable, economical, and easy to integrate into
existing architectural elements. A ssDSC is based
on the fine intermixing between an electron- and a
hole-conductor, often a thin nanostructured titanium
dioxide layer onto which a monolayer of molecular
organic dye (generally Ru-based) is chemisorbed,
and an organic material (usually P3HT or Spiro-
OmeTAD). The whole nanostructured composite, 2-
3 μm thick, is sandwiched between two electrodes
and encapsulated by a transparent sealant. Despite
an intense investigation aimed at improving the
macroscopic performance of these devices, many
fundamental aspects of their behavior still need to
be addressed. In particular charge diffusion through
the nanostructured composite film must to be understood
and modelled to drive the optimization
of the device. The entire cell is usually modelled
using drift-diffusion equations for both electrons
and holes in an effective medium framework. By
effective medium we mean that the real structure of
the mesoporous materials are not explicitly taken
into account in the model, and an effective material
is used instead [2]. However, the real structure
between electron- and hole-conductor materials is
far more complex.
«
Solid state Dye Sensitized Solar Cells (ssDSCs)
[1] are very promising photovoltaic devices, potentially
stable, economical, and easy to integrate into
existing architectural elements. A ssDSC is based
on the fine intermixing between an electron- and a
hole-conductor, often a thin nanostructured titanium
dioxide layer onto which a monolayer of molecular
organic dye (generally Ru-based) is chemisorbed,
and an organic material (usually P3HT or Spiro-
OmeTAD). The whole nanostructured comp...
»