Ordered Bulk Heterojunction Photovoltaic Cells
January 2004 - August 2007 (Completed)
Investigator
Michael McGehee, Department of Materials Science and Engineering, Stanford University
Objective
This project will involve making efficient photovoltaic (PV) cells
with semiconducting polymers that could be deposited in reel-to-reel
coaters. Careful analysis and optimization of each process that occurs
in bulk heterojunction PV cells will be carried out and devices based
on ordered interpenetrating networks of organic and inorganic
semiconductors will be created. Specifically this research will lead to
devices that will efficiently split excitons and carry charge to
electrodes, that will have improved packing of the molecules in the
organic semiconductor to enhance its ability to carry charge, and that
will have a modified organic-inorganic interface to prevent
recombination of electrons and holes. It is anticipated that charge
recombination in the cells will be almost completely eliminated and
energy conversion efficiencies in the range of 10-15% will be obtained.
Background
Figure 1: Schematic energy diagram of a bulk heterojunction PV cell
Currently the best commercially available PV cells are made of
crystalline silicon and have an energy conversion efficiency of 12%.
The cost of these cells is $3 per Watt of power generated under solar
AM 1.5 conditions. These costs need to be reduced by an order of
magnitude to around $0.3 per Watt for PV cells to be competitive with
other energy generation systems and be manufactured on a large scale. A
revolutionary breakthrough in reducing the costs of PV cells may be
achieved if the semiconductor were deposited from solution onto large
flexible substrates in reel-to-reel coating machines similar to those
used to make food packaging. Manufacturing costs would be much lower
because reel-to-reel coaters use very little energy and have an
exceptionally high throughput. Installation costs would be lower
because lightweight flexible PV cells could be handled more easily than
heavy silicon panels.
The processes involved in operating a bulk heterojunction PV device
are shown in Figure 1. To optimize performance of these cells, the
desirable processes (1. light absorption, 2. exciton diffusion, 3.
forward electron transfer, and 4. charge transport) should be
maximized, while the undesirable recombination processes (5. geminate
recombination and 6. back electron transfer) should be limited. This
can be achieved by improving charge carrier mobility and slowing down
the rate of back electron transfer so that photogenerated charge
carriers can escape from the film before recombination occurs, while
maintaining a thick enough film to allow most of the light to be
absorbed.
Approach
In this study, well-ordered interpenetrating networks of organic and
inorganic semiconductors will be made to create bulk heterojunction PV
devices instead of the disordered blends that have been used in the
past. In these structures, electrons and holes will have straight
pathways to electrodes. Consequently these charge carriers will travel
the shortest possible distance and will never be trapped at dead ends.
To make the interpenetrating nanostructures that are needed, nanoporous
films or nanowire brushes will be fabricated using an inorganic
semiconductor and the pores or brush will be filled in with a
semiconducting polymer. There are many combinations of inorganic
semiconductors and semiconducting polymers that have suitable energy
levels for light absorption and electron transfer. The approach used
requires addressing three different issues:
- Patterning of nanostructured films:
The techniques used to pattern the inorganic films will include
titania/block copolymer co-assembly (see Figure 2), growth of nanowires
off of arrays of catalysts to create a nanowire brush, and stamping of
sol-gel oxide precursors. In each case, the size of the polymer region
will be approximately 20-nm so that all of the excitons in the polymer
can diffuse to the polymer/inorganic semiconductor interface. The films
will be approximately 300-nm thick so that they can effectively absorb
light.

Only
two layers of unit cells are shown. A typical film has more than 100
layers. The hydrophobic blocks are shown in green. The hydrophilic
blocks are shown in blue. After a film is made, pores are created by
burning out the block copolymer.
Figure 2: Schematic of a self-assembled block copolymer-titania nanostructure
- Improving hole transport in organic semiconductors:
Hole mobilities in pore structures may change dramatically from values
in pristine films and may directly impact the ability to extract the
holes in the polymer out of the PV cells before they recombine with
electrons in the electron-accepting semiconductor. Several approaches
will be used for filling nanoporous films and nanowire brushes with
organic semiconductors. These include: modification of the chemical
groups on the polymer chains and the inorganic semiconductor surface to
optimize the interactions between the organic and inorganic materials;
use of techniques to electropolymerize conjugated monomers directly in
the pores which may lead to higher absorption cross-sections and better
contact for improved charge transport; and use of discotic liquid
crystals. With each approach, charge carrier mobility measurements will
be made, and the molecular packing will be characterized in order to
determine in a rational way, how to maximize hole mobility.
- Optimizing electron transfer:
Electron transfer plays a critical role in bulk heterojunction PV
cells. The forward transfer from the polymer to the electron accepting
material must occur before the electron and hole in the exciton undergo
geminate recombination, and back electron transfer from the electron
acceptor to the polymer must be inhibited. Photoluminescence quenching
will be used to determine the effectiveness of forward electron
transfer for all of the organic-inorganic combinations developed and
time-resolved photoinduced absorption to measure the rate of back
electron transfer. Retardation of back electron transfer will be
achieved by coating the inorganic surface with a thin, wide-energy-gap
coating with appropriate energy levels.
By following these approaches, it is anticipated that
the small prototype devices developed in this effort may be scaled up
to allow manufacture of stable low-cost PV cells using reel-to-reel
coaters with energy conversion efficiencies of 10-15% at a cost of
around an order of magnitude cheaper than presently available.
Issued March 2004