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  • About
  • The Global ETD Search service is a free service for researchers to find electronic theses and dissertations. This service is provided by the Networked Digital Library of Theses and Dissertations.
    Our metadata is collected from universities around the world. If you manage a university/consortium/country archive and want to be added, details can be found on the NDLTD website.
1

Organische p-i-n Solarzellen

Männig, Bert 03 January 2005 (has links) (PDF)
In this work a p-i-n type heterojunction architecture for organic solar cells is shown, where the active region is sandwiched between two doped wide-gap layers. The term p-i-n means here a layer sequence in the form p-doped layer, intrinsic layer and n-doped layer. The doping is realized by controlled coevaporation using organic dopants and leads to conductivities of 10-4 to 10-5 S/cm in the p- and n-doped wide gap layers, respectively. The conductivity and field effect mobility of single doped layers can be described quantitatively in a self-consistent way by a percolation model. For the solar cells the photoactive layer is formed by a mixture of phthalocyanine zinc (ZnPc) and the fullerene C60 and shows mainly amorphous morphology. The solar cells exhibit a maximum external quantum efficiency of 40% between 630nm and 700nm wavelength. With the help of an optical multilayer model, the optical properties of the solar cells are optimized by placing the active region at the maximum of the optical field distribution. The results of the model are largely confirmed by the experimental findings. The optically optimized device shows an internal quantum efficiency of around 85% at short-circuit conditions and a power-conversion efficiency of 1.7%.
2

Organische p-i-n Solarzellen

Männig, Bert 10 December 2004 (has links)
In this work a p-i-n type heterojunction architecture for organic solar cells is shown, where the active region is sandwiched between two doped wide-gap layers. The term p-i-n means here a layer sequence in the form p-doped layer, intrinsic layer and n-doped layer. The doping is realized by controlled coevaporation using organic dopants and leads to conductivities of 10-4 to 10-5 S/cm in the p- and n-doped wide gap layers, respectively. The conductivity and field effect mobility of single doped layers can be described quantitatively in a self-consistent way by a percolation model. For the solar cells the photoactive layer is formed by a mixture of phthalocyanine zinc (ZnPc) and the fullerene C60 and shows mainly amorphous morphology. The solar cells exhibit a maximum external quantum efficiency of 40% between 630nm and 700nm wavelength. With the help of an optical multilayer model, the optical properties of the solar cells are optimized by placing the active region at the maximum of the optical field distribution. The results of the model are largely confirmed by the experimental findings. The optically optimized device shows an internal quantum efficiency of around 85% at short-circuit conditions and a power-conversion efficiency of 1.7%.

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