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Plenarvorträge - DPG-Tagungen

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Symposium Organic and Hybrid Systems for Future Electronics Donnerstag<br />

carriers in organic solar cells. In this study photoelectron spectroscopy<br />

is applied to determine the electronic properties of the ITO surface. By<br />

treating the ITO substrates with phosphoric or periodic acid these properties<br />

are adjusted to those of the following organic layer. Evidence of adsorbed<br />

acid ions on the electrode surface is found in x-ray photoelectron<br />

spectra. Their inelastic cutoff was determined to calculate work functions.<br />

The work function values are correlated with the performance of<br />

Zn-Phthalocyanine-C60 solar cells. The influence of acid treatments on<br />

the solar cell parameters is compared to the effect of a conventional PE-<br />

DOT:PSS buffer layer.<br />

SYOH 5.42 Do 18:00 B<br />

High efficiency vacuum deposited solar cells using single or multiple<br />

p-i-n architecture. — •Steffen Grundmann, Jens Drechsel,<br />

Bert Männig, Wenge Guo, Karl Leo, and Martin Pfeiffer<br />

— Insitut für Angewandte Photophysik, TU Dresden, D-01062 Dresden,<br />

Germany<br />

We introduce a p-i-n type heterojunction architecture for organic solar<br />

cells where the active region (i) is sandwiched between two doped widegap<br />

layers (p and n). The photoactive layer is formed by a mixture of<br />

zinc phthalocyanine (ZnPc) and the fullerene C60. In the blend layer, the<br />

ZnPc is found in an amorphous morphology while C60 forms nanocrystallites<br />

of less than 10nm size. The solar cells exhibit an external quantum<br />

efficiency of around 40% between 630nm and 700nm wavelength. With<br />

the help of an optical multilayer model, we optimize the optical properties<br />

of the solar cells by placing the active region at the maximum of the<br />

optical field distribution. The results of the model are largely confirmed<br />

by the experimental findings. For an optically optimized device, we find<br />

an internal quantum efficiency of around 85% at short-circuit conditions.<br />

Adding 10nm thick layer of the red material PTCBI to the active region,<br />

a power conversion efficiency of 2% is obtained. Such optically thin cells<br />

with high internal quantum efficiency are an important step towards high<br />

efficiency tandem cells. First tandem cells, which are not yet optimized,<br />

already show 2.4% power conversion efficiency. Moreover, we present first<br />

promising results on device lifetime under simulated AM 1.5 conditions.<br />

SYOH 5.43 Do 18:00 B<br />

Numerical simulation of photovoltaic devices based on organic<br />

materials — •Fryderyk Kozlowski, Wenge Guo, Bert Maennig,<br />

Jens Drechsel, Martin Pfeiffer, and Karl Leo for the H.<br />

Hope collaboration — Institut für Angewandte Photophysik,01069 Dresden,<br />

Germany<br />

We have modelled the optical and electrical behaviours of organic (pi-n)<br />

and (p-i-i-n) solar cells fabricated in our laboratory by numerical<br />

simulations. In the cells with structure (p-i-n), the dissociation of exitons<br />

and free carrier creation occurrs in a photoactive mixed layer (i) e.g. zinc<br />

phthalocyanine mixed with fullerene (ZnPc:C60). The photovoltaic devices<br />

based on a photoactive donor-acceptor heterojunction with a p-i-i-n<br />

architecture consist of the same organic materials. Here however, exitons<br />

are formed in bulk materials and the dissociation of the excitons takes<br />

place at the interface of neat ZnPc and C60 layers. In the numerical model<br />

describing the electrical properties, we took into account effects like bipolar<br />

charge carrier drift and diffusion, bulk and interface recombination,<br />

trapping, creation, diffusion and quenching of exitons. The distribution<br />

of generated free carriers in the mixed layer or the generation profile of<br />

exitons in heterojunctions, respectively, is calculated from optical simulations.<br />

By including trap-mediated recombination for (p-i-n) solar cells,<br />

we are able to simulate the linear dependence of the short circuit current<br />

on light intensity. Furthermore, we study the optimum thickness of the<br />

active layer and compare it with experimental data. Finally, we show the<br />

temperature dependence of short circuit current and open circuit voltage.<br />

SYOH 5.44 Do 18:00 B<br />

Photocurrent action spectra and X-ray diffraction on diindenoperylene/pentacene<br />

heterostructures — •D. Kurrle,<br />

S. Hirschmann, and J. Pflaum — III. Physikalisches Institut,<br />

Universität Stuttgart, Germany<br />

As a new candidate for photovoltaic applications, thin films of the<br />

organic semiconductors diindenoperylene (DIP, C32H16) and pentacene<br />

(C22H14) were prepared and examined by measuring the absorption and<br />

photocurrent action spectra.<br />

Samples of different structures were grown by thermal evaporation, using<br />

ITO and silver as electrode materials. DIP/pentacene double layers<br />

as well as co-evaporated mixed layers were studied (both 100-250 nm<br />

in total thickness), both yielding considerable photocurrents up to 50<br />

nA/cm 2 under the applied conditions.<br />

Furthermore, X-ray diffraction and AFM were carried out to obtain<br />

additional information on the structure of the films. The growth of the<br />

DIP/pentacene bilayers showed a pronounced structural dependence on<br />

the substrate temperature (140-400 K) and the underlying electrode material,<br />

whereas the impact on the photocurrent emerged to be minor.<br />

SYOH 5.45 Do 18:00 B<br />

Optical and Electronic Contributions in Thin Film Organic Solar<br />

Cells — •Helmut Hänsel 1 , Heiko Zettl 1 , Georg Krausch 1 ,<br />

Roman Kisselev 2 , Mukundan Thelakkat 2 , and Hans-Werner<br />

Schmidt 2 — 1 Universität Bayreuth, Physikalische Chemie II —<br />

2 Universität Bayreuth, Makromolekulare Chemie I,D-95447 Bayreuth<br />

We investigate the photocurrent of a (ITO/CuPc/perylene dye/Al)<br />

cell and a (ITO/CuPc/perylene dye/TiO2/Al) cell as a function of the<br />

perylene dye layer thickness. In addition to the experimental data, we<br />

present a model that describes the short circuit current of these cells.<br />

The charge generation probability is estimated from the intensity profile<br />

that is calculated via a matrix transfer algorithm taking into account the<br />

full illumination spectrum. We find that the TiO2 layer modifies the short<br />

circuit current by two effects: Optically, by shifting the charge transfer<br />

interface with respect to the light intensity profile, and electronically, by<br />

introducing a second heterojunction where additional charge transfer can<br />

occur. Thickness dependent studies can clearly separate these two effects<br />

and can yield an estimate of the ratio of the exciton diffusion lengths<br />

in the absorbing media. The high accuracy in thickness variation that is<br />

necessary for such study is achieved by the combinatorial fabrication and<br />

testing of the devices. We can furthermore show that the introduction of<br />

the TiO2 layer leads to a faster and stronger degradation.<br />

SYOH 5.46 Do 18:00 B<br />

Multilayer solar cells based on polymer nanoparticles —<br />

•Thomas Kietzke 1 , Katharina Landfester 2 , and Dieter<br />

Neher 2 — 1 University of Potdam, Institute of Physics, Am Neuen<br />

Palais 10, D-14469 Potsdam — 2 University of Ulm, Institute of<br />

Macromolecular Chemistry, Albert-Einstein-Allee 11, D-89069 Ulm<br />

Recently, we have demonstrated that polymer nanospheres with diameters<br />

in the range of 30 to 250 nm dispersed in water can be prepared<br />

with the miniemulsion process. First solar cells based on layers of<br />

these nanoparticles have shown efficiencies comparable to solvent processed<br />

layers. Formation of films from polymer nanoparticles opens up<br />

new strategies for the deposition of multilayer assemblies, since the semiconducting<br />

polymer nanospheres are dispersed in water. Preparing multilayer<br />

structures of polymers from organic solvents is often difficult if the<br />

polymers of e.g. the second layer is deposited from a solvent, which is also<br />

a good solvent for the underlying polymer. Utilizing dispersions of polymer<br />

nanospheres can help to circumvent this problem. After preparing the<br />

first nanoparticle layer, the sample is thoroughly dried to completely remove<br />

residual water. Then, a second nanosphere layer is deposited on top,<br />

resulting in a multilayer assembly with a well-defined polymer-polymer<br />

interface and no interdiffusion of the polymers in the separate layers. We<br />

show the results on double layer polymer solar cells with ITO and Ca<br />

electrodes as well as devices including a thin TiO2 electron-accepting<br />

layer. Reference: [1] T.Kietzke, D. Neher et. al. Nature Materials, June<br />

2003, 408-412<br />

SYOH 5.47 Do 18:00 B<br />

Organic Photovoltaic Elements - Influence of 100 nm scale<br />

electrode spacing on morphology and efficiency for PF/PANI<br />

conjugated block copolymer — •Jörg Seekamp 1 , R. Güntner 2 ,<br />

V.G. Solovyev 1 , A.P. Kam 1 , A. Goldschmidt 1 , T. Farrell 2 , U.<br />

Scherf 2 , and C.M. Sotomayor Torres 1 — 1 Institute of Materials<br />

Science and Department of Electrical and Information Engineering, University<br />

of Wuppertal, Gauß Straße 20, 42097 Wuppertal, Germany —<br />

2 Fachbereich Chemie, Makromolekulare Chemie, University of Wuppertal,<br />

Gauß Straße 20, 42097 Wuppertal, Germany<br />

The transport properties of organic semiconductors in solar cells are<br />

the object of intense research. The efficiency of these devices crucially<br />

depends on the charge separation and effective transport to metal electrodes.<br />

This work combines closely spaced electrodes and the intrinsically<br />

nanostructured morphology of a block copolymer to improve the<br />

efficiency. The idea is to direct the intrinsic nanostructuring along the

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