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Plenarvorträge - DPG-Tagungen

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Halbleiterphysik Dienstag<br />

Infrared spectroscopic ellipsometry (IRSE) for wave numbers from 333<br />

to 4000 cm −1 is demonstrated as useful technique for characterization<br />

of structural, vibrational, and free-charge-carrier properties of conducting<br />

organic thin layers deposited on electrically conducting as<br />

well as on isolating substrates. Pentacene, poly(3,4-ethylenedioxy thiophene)/poly(styrenesulfonate)<br />

(PEDOT:PSS), C60 and polyfluorene are<br />

studied exemplarily. For all materials the infrared dielectric functions<br />

are reported, which can serve as fingerprints for multiple-layer structures<br />

analysis. PEDOT:PSS layers deposited onto n-type and p-type silicon<br />

substrates reveal different conductivity response, indicative for charge<br />

transfer at the semiconductor/polymer interface, whereas the IRSE data<br />

show that the pentacene layers on glass are rendered highly resistive.<br />

HL 23.7 Di 18:15 H13<br />

Ultrafast excitonic relaxation processes in perylene derivatives<br />

— •E. Engel, M. Koschorreck, M. Hoffmann, T. W. Canzler,<br />

T. Hasche, and K. Leo — Institut für Angewandte Photophysik, TU<br />

Dresden, 01062 Dresden, Germany, www.iapp.de<br />

Perylene derivatives are interesting model systems because of<br />

their quasi-1D organic molecular crystal structure, their strong<br />

molecular interaction and their potential for use in low-cost optoelectronic<br />

devices. We investigated polycrystalline thin films of<br />

N-N’-dimethyl-perylene-3,4,9,10-dicarboximide (MePTCDI) and<br />

perylene-3,4,9,10-tetracarboxylic-dianhydride (PTCDA). Using ultrafast<br />

pump-probe spectroscopy, we temporally resolved the relaxation process<br />

of free excitons from the absorbing states down to the indirectly emitting<br />

states. The time constant, measured by photoinduced absorption, is<br />

about 30fs. Furthermore, we investigated signal contributions from<br />

stimulated emission and ground state bleaching. The relaxation<br />

processes are discussed within the framework of an exciton band<br />

structure model[1].<br />

HL 24 Photovoltaik I<br />

[1] M. Hoffmann, Z. G. Soos and K. Leo, Nonlinear Optics 29, 227<br />

(2002)<br />

HL 23.8 Di 18:30 H13<br />

Ultrafast Relaxation between Davydov Components in<br />

Crystalline N-N’-dimethyl-perylene-3,4,9,10-dicarboximide<br />

(MePTCDI) — •Marco Koschorreck, Egbert Engel,<br />

Karl Leo, and Michael Hoffmann — Institut für Angewandte<br />

Photophysik, TU Dresden, 01062 Dresden, Germany, www.iapp.de<br />

We investigated polarization anisotropies in polycrystalline films of the<br />

organic semiconductor N-N’-dimethyl-perylene-3,4,9,10-dicarboximide<br />

(MePTCDI) by means of pump-probe and time-resolved luminescence<br />

measurements. The timescale of the observed processes range from tens<br />

of femtoseconds to several picoseconds.<br />

On the shorter timescale (50fs), the equilibration process of the initially<br />

differently populated Davydov components was observed. The<br />

textbook model for polarization anisotropies was extended to the case<br />

of two coupled Davydov components. Through this it is possible to<br />

predict the remaining anisotropy after this very fast relaxation process.<br />

The experimental results agreed well with the theoretical values. The behavior<br />

at longer timescales (100ps) could be explained by exciton diffusion<br />

between randomly oriented crystallites. While crossing the crystallite<br />

boundaries, the excitons lose their polarization memory and the polarization<br />

anisotropy goes to zero. Temperature dependent measurements<br />

indicate an incoherent thermally activated hopping process.<br />

HL 23.9 Di 18:45 H13<br />

N,N’-perarylated -2,2’-bithiophene - as a new typ of hole transporting<br />

materials — •Olaf Zeika — Novaled GmbH 01069 Dresden<br />

Zellescher Weg 17<br />

Synthesis, characterisation and possible use in OLED<br />

Zeit: Dienstag 17:45–19:15 Raum: H15<br />

HL 24.1 Di 17:45 H15<br />

Doping experiments with HfSxSe2−x — •Steffen Duhm, Ralf<br />

Severin, Alicia Krapf, Christoph Janowitz, and Recardo<br />

Manzke — Institut f. Physik, Humboldt-Unversität zu Berlin,<br />

Newtonstr. 15, 12489 Berlin<br />

HfSxSe2−x is an indirect semiconductor of the group of transition metal<br />

dichalcogenides, the band-gap of which ranges from 1.1 eV (HfS2) to 2<br />

eV (HfSe2) with a nearly linear dependence on x. Due to this property it<br />

can be used as a source material for a two junction cell (ideal band-gap<br />

1.1 eV and 1.8 eV). In the present work, niobium doped HfS1Se1 (bandgap<br />

∼ 1.5 eV) crystals with different doping concentrations were grown<br />

by chemical vapour transport (CVT). The crystals were characterized by<br />

energy dispersive X-ray analysis (EDX) and absorption measurements.<br />

Despite the indirect band-gap of HfSxSe2−x the absorption coefficient is<br />

very high and enables thin-film solar cells. The quasi two-dimensional<br />

character of HfSxSe2−x prevents surface states and dangling bonds. As<br />

the material is thus highly suitable for a Schottky contact, the work<br />

function was measured using a Kelvin probe.<br />

HL 24.2 Di 18:00 H15<br />

Investigation of the chemical and electronic properties of the<br />

ZnO/Cu(In,Ga)(S,Se)2 interface in thin film solar cells — •G.<br />

Storch 1 , L. Weinhardt 1 , C. Heske 1 , E. Umbach 1 , S. Visbeck 2 ,<br />

T.P. Niesen 2 , and F. Karg 2 — 1 Experimentelle Physik II, Universität<br />

Würzburg, Am Hubland, D-97074 Würzburg — 2 Shell Solar, 81739<br />

München<br />

Thin film solar cells based on Cu(In,Ga)(S,Se))2 (CIGSSe) commonly<br />

contain a CdS buffer layer between the absorber and the (i-ZnO/n-ZnO)<br />

window layer. For environmental reasons, it is desirable to replace the<br />

Cd-containing buffer, either by alternative materials or by direct deposition<br />

of the window layer on the absorber. However, depositing the standard<br />

window layer directly on the absorber results in poor efficiencies.<br />

In contrast, the use of (Zn,Mg)O instead of i-ZnO leads to cells showing<br />

satisfactory performance. Until today, the reason for this discrepancy is<br />

unknown. As a first step towards an understanding, we have investigated<br />

the i-ZnO/CIGSSe interface by using X-ray photoelectron spectroscopy<br />

(XPS), X-ray emission spectroscopy (XES) and UV-photoelectron spectroscopy<br />

(UPS) combined with inverse photoemission (IPES). The result-<br />

ing chemical and electronic picture of the interface, including the band<br />

alignment in both the valence and conduction band, will be discussed and<br />

compared to results from related interfaces (e.g., i-ZnO/CdS) as well as<br />

alternative preparation methods.<br />

HL 24.3 Di 18:15 H15<br />

Band alignment at the i-ZnO/CdS interface in Cu(In,Ga)(S,Se)2<br />

thin film solar cells — •L. Weinhardt 1 , C. Heske 1 , E. Umbach 1 ,<br />

S. Visbeck 2 , T.P. Niesen 2 , and F. Karg 2 — 1 Exp. Physik II, Universität<br />

Würzburg — 2 Shell Solar GmbH, Munich<br />

In solar cells based on Cu(In,Ga)(S,Se)2 (CIGSSe) one potential target<br />

for further optimization of cell performance is the commonly used ZnO<br />

window layer. Today, an n-ZnO/i-ZnO structure is generally used, separated<br />

from the CIGSSe absorber by a CdS buffer layer. Apart from important<br />

bulk parameters of the ZnO layer, such as window transmission and<br />

resistivity, particularly the properties of its interface to the CdS buffer<br />

layer represent a crucial component for the optimization of solar cells. For<br />

a further improvement of this interface a detailed understanding of the<br />

chemical and electronic properties is needed. We have thus investigated<br />

the ZnO/CdS interface using X-ray photoelectron spectroscopy to probe<br />

its chemical properties, and we have used UV and inverse photoemission<br />

for a direct determination of the band gaps and band alignments at the<br />

heterojunction. The results will be discussed in view of a level alignment<br />

model for the complete CIGSSe thin film solar cell device, taking into<br />

account the previously found electronic and chemical structure of the<br />

CdS/CIG(S)Se interface [1,2] as well as new results for absorbers with<br />

varied sulfur content at the surface.<br />

[1] L. Weinhardt et al., Proc. 17th EPSEC Munich 2001, p. 1261.<br />

[2] M. Morkel et al., Appl. Phys. Lett. 79 (2001) 4482.<br />

HL 24.4 Di 18:30 H15<br />

Formation mechanism of the metastable defect in Cz-silicon solar<br />

cells — •Karsten Bothe, Rudolf Hezel, and Jan Schmidt<br />

— Institut für Solarenergieforschung Hameln/Emmerthal (ISFH), Am<br />

Oherberg 1, D-31860 Emmerthal<br />

The efficiency of solar cells made on boron-doped oxygen-contaminated<br />

crystalline silicon decreases under illumination or minority-carrier injection<br />

in the dark by up to 10 % relative. This performance degradation has

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