Programm Photovoltaik Ausgabe 2009 ... - Bundesamt für Energie BFE
Programm Photovoltaik Ausgabe 2009 ... - Bundesamt für Energie BFE
Programm Photovoltaik Ausgabe 2009 ... - Bundesamt für Energie BFE
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Introduction / Project Goals<br />
The concept of the luminescent solar concentrator (LSC) dates back to the 1970s [1]. The basic principle<br />
of operation of a conventional LSC is illustrated in Fig. 1. The device consists of a transparent<br />
plate (usually polymethylmethacrylate PMMA) containing luminescent centers, which absorb light entering<br />
through the face of the plate. A fraction of the subsequently emitted photons is trapped by total<br />
internal reflection and guided to the edges of the plate. As the edge area of the plate is much smaller<br />
than the face area, the LSC operates as a concentrator of light.<br />
Fig. 1 Principle of operation of a LSC. Only one luminescent center is shown. In order to function as<br />
a concentrator, the face area needs to be larger than the edge area.<br />
Conventional LSCs suffer from a series of problems, which lead to low efficiencies and have prevented<br />
commercial application:<br />
� Self-absorption: Organic dyes with high fluorescence quantum yield generally feature a considerable<br />
overlap between absorption and emission spectra. An emitted photon with an energy corresponding<br />
to this spectral overlap has a high probability of being re-absorbed on its path towards<br />
the edge of the LSC plate. Successive re-absorption and re-emission steps lead to a larger path<br />
length and thus to a higher susceptibility towards the various loss mechanisms, including radiationless<br />
deactivation or emission into the escape cone.<br />
� Escape cone losses: The angle of the escape cone depends on the refractive index of the material.<br />
In the case of PMMA, an escape probability of 26 % is calculated for isotropic absorption and<br />
emission.<br />
� Stability: Problems with stability are mainly associated with the non-sufficient photostability of the<br />
luminescent centers. To become commercially viable, a LSC should be stable enough to ensure<br />
efficient operation over a period of more than 10 years.<br />
We have developed a concept based on dye-zeolite composites that has the potential of solving the<br />
above problems [2]. The goal of the project is the preparation of prototypes according to this new design<br />
concept and the evaluation of the performance of the devices.<br />
General Concept<br />
The use of zeolite L as a host system offers possibilities to obtain high local concentrations of<br />
supramolecularly organized monomeric dye molecules. Zeolite L is an aluminosilicate with onedimensional<br />
channels running parallel to the c-direction of the crystals (Fig. 2). The morphology of the<br />
crystals is typically cylindrical with channel entrances located at the base surfaces. A crystal with a<br />
diameter of 500 nm contains approximately 66'000 parallel channels. Dye molecules can be included<br />
by cation exchange or adsorption from the gas phase. As dye molecules cannot pass each other in<br />
the channels, sequential introduction of different dyes results in defined dye domains. This allows for a<br />
transport of electronic excitation energy along the channels by means of Förster resonance energy<br />
transfer (FRET) [3]. The supramolecular organization of the dyes in the zeolite channels and the<br />
option of extending this organization to the macroscopic scale by preparing layers of oriented crystals<br />
is at the center of our concept for an advanced LSC. Zeolite-polymer hybrid materials can be prepared<br />
with high transparency [4].<br />
164/290<br />
Luminescent concentrators based on inorganic/organic nanomaterials, D. Brühwiler, University of Zurich<br />
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