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Plenarvorträge - DPG-Tagungen

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Dünne Schichten Dienstag<br />

DS 22.48 Di 14:30 Poster B<br />

Temperature-dependent surface photovoltage of polycrystalline<br />

Cu(In,Ga)Se2 from photoemission studies using synchrotron radiation<br />

— Thomas Schulmeyer, Ralf Hunger, and •Andreas<br />

Klein — Technische Universität Darmstadt, Petersenstrasse 23, D-<br />

64287 Darmstadt<br />

A deep insight of surfaces and interfaces is essential for improving<br />

the knowledge of the complex interface behaviour of Cu-chalcopyrites.<br />

In this contribution, temperature-dependent photovoltage measurements<br />

with synchrotron radiation induced photoelectron emission of polycrystalline<br />

Cu(In,Ga)Se2 surfaces and Cu(In,Ga)Se2/CdS interfaces are presented.<br />

Clean Cu(In,Ga)Se2 surfaces are prepared with the Se de-capping<br />

procedure. Additionally, defined oxidized Cu(In,Ga)Se2 and de-capped<br />

CuGaSe2 absorbers were investigated. All chalcopyrite surfaces show a<br />

Cu-poor surface composition.<br />

DS 22.49 Di 14:30 Poster B<br />

Aluminum-induced crystallization of amorphous silicon: Al/a-<br />

Si-interface influence on seed layer formation — •Jens Schneider,<br />

Juliane Klein, Martin Muske, Stefan Gall, and Walther<br />

Fuhs — Hahn-Meitner-Institut Berlin, Kekuléstr. 5, D-12489 Berlin,<br />

Germany<br />

Crystallization of seed layers on inexpensive foreign substrates and<br />

their subsequent epitaxial thickening is a promising approach for the formation<br />

of thin-film crystalline silicon cells. Such seed layers can be formed<br />

by Al-induced crystallization of an amorphous silicon (a-Si) layer. The kinetics<br />

of Al-induced crystallization of a-Si are studied by variation of the<br />

thickness of an Al-oxide layer between the initial Al and a-Si films. The<br />

results show that the thickness of this Al-oxide layer strongly determines<br />

the nucleation time and the number of Si-grains (nucleation) and has only<br />

little influence on the growth velocity of the grains. The diameter of the<br />

grains increases in good approximation linearly with time and is strongly<br />

influenced by the annealing temperature. The general behavior suggests<br />

that the process kinetics of the aluminum-induced layer exchange are determined<br />

by the silicon diffusion across the interface which can be altered<br />

by the thickness of the oxide layer.<br />

DS 22.50 Di 14:30 Poster B<br />

Development system for advanced CdTe Thin Film Solar Cells<br />

— •Jochen Fritsche, Daniel Kraft, Bettina Späth, Andreas<br />

Thißen, Andreas Klein, and Wolfram Jaegermann — Darmstadt<br />

University of Technology, Institute of Materials Science, Surface<br />

Science Division, Germany<br />

CdTe thin film solar cells promise a high potential to reach good conversion<br />

efficiencies with a low cost production process. A large scale production<br />

of CdTe modules (120 cm × 60 cm) is realized by ANTEC Solar<br />

Energy GmbH with average conversion efficiencies of 6,7 %. In the production<br />

a layer sequence is used, which is based on empirical development.<br />

However, the highest obtained efficiency with CdTe is 16,5 %. We have<br />

analyzed electronic and chemical properties of surfaces und interfaces<br />

in the CdTe solar cell. Major obstacles to obtain higher efficiencies and<br />

lower production costs within this system are related to interfacial issues<br />

as barrier heights for charge transport, interface recombination and film<br />

nucleation. A better understanding of these properties will help to prepare<br />

improved front and back contacts as well as to reduce the CdS and<br />

CdTe layer thickness. In order to explore possible advanced cells with<br />

a better control and knowledge about interface properties, we have set<br />

up DAISY-Sol (DArmstadt Integrated SYstem for Solar cell research),<br />

which combines a full vacuum production of CdTe solar cells with an<br />

in-situ analysis to investigate and modify the electrical and chemical<br />

properties of all surfaces and interface.<br />

DS 22.51 Di 14:30 Poster B<br />

CuInS 2 Solar Cells Deposited by Reactive Magnetron Sputtering<br />

— •Thomas Unold, Jan Hinze, and Klaus Ellmer — Hahn-<br />

Meitner Institut, Glienicker Str. 100, D-14109 Berlin, Germany<br />

We have deposited CuInS 2 films in a reactive magnetron sputtering<br />

system, specially designed for the deposition of sulfides by sputtering<br />

in Ar-H2S mixtures. The substrate temperature was varied from<br />

350 to 500C and the deposition rate was about 50 nm/min. The magnetron<br />

plasma was excited by a DC power supply. The contacts (Mo,<br />

ZnO/ZnO:Al) and the buffer layer (CdS) were prepared by the standard<br />

processes of the Hahn-Meitner-Institut. Up to now solar cell efficiencies<br />

of up to 8.1 have been obtained. The electronic and optical properties<br />

of the solar cell devices were analyzed by dark and illuminated current-<br />

voltage characteristics, quantum efficiency and photoluminescence measurements.<br />

We find that although the short circuit current is comparable<br />

to that of cells prepared by the two-step process (sulfurization of sputtered<br />

precursor metals), the open-circuit voltage is about 100meV lower.<br />

This is consistent with the quantum efficiency analysis where we find a<br />

decreased collection efficiency at long wavelengths compared to cells from<br />

the two-step process. From photoluminescence we conclude that the efficiency<br />

of our cells is limited by the defect density in the absorber layer.<br />

DS 22.52 Di 14:30 Poster B<br />

Epitaxial growth and characterization of Cu0.5In0.5Se (Te)<br />

films grown on GaAs by pulsed laser deposition. — •Liudmila<br />

Roussak, Gerald Wagner, and Klaus Bente — Institute of Mineralogy,<br />

Crystallography and Materials Science, Linnestr. 3-5 (TA), D-<br />

04103 Leipzig<br />

Alloys of Cu0.5In0.5Se(Te), as an attractive material for solar cell applications,<br />

have been grown on (001) oriented GaAs substrates by pulsed<br />

laser deposition (PLD). Epitaxial growth was found to occur for substrate<br />

temperatures ranging between 380 and 600 ◦ C. The structural, compositional,<br />

morphological and electrical properties of the Cu0.5In0.5Se(Te)<br />

films depend strongly on the substrate temperature, laser energy density<br />

and deposition rate. Applying optimized growth conditions it is possible<br />

to obtain the films of required electrical and structural characteristic.<br />

The detailed examination of late the absorber and buffer forming the heterostructure<br />

as well as their interface are very important for the efficient<br />

of thin film solar cells.<br />

DS 22.53 Di 14:30 Poster B<br />

Influence of the substrate preparation on the low-temperature<br />

epitaxy of Si by electron-cyclotron resonance chemical vapor<br />

deposition — •Patrick Clemens, Björn Rau, Ina Sieber, Stefan<br />

Gall, and Walther Fuhs — Hahn-Meitner-Institut, Abt. Silizium<br />

Photovoltaik, Kekuléstr. 5, D-12489 Berlin<br />

We report on a study of substrate preparation for the low-temperature<br />

Si homo-epitaxy by electron-cyclotron resonance chemical vapor deposition<br />

(ECRCVD). The background of the research is the development of<br />

a low-temperature epitaxial thickening process for Si thin-film solar cells<br />

on large-grained polycrystalline Si seed layers on glass.<br />

Different from conventional high-temperature Si deposition methods<br />

the conditions of the substrate surface, its crystal orientation and its<br />

contamination are very critical for the successful epitaxial growth of Si<br />

at substrate temperatures below 600 ◦ C. Both, wet chemical surface pretreatments<br />

and in-situ treatments are applied to obtain an ideal substrate<br />

surface for Si epitaxy. Using a HF/alcohol instead of HF/water solution<br />

the roughness of the surface of Si wafers decreases, the surface contaminations<br />

are reduced, and the H-termination of the Si surface is improved.<br />

During substrate heating in-situ H-treatment is used to increase the stability<br />

of this surface and prevent reoxidation. This substrate preparation<br />

leads to a successful epitaxial growth of Si on Si(100) wafers at low temperatures.<br />

The influence of the preparation on the Si epitaxy is analyzed<br />

by structural and electrical characterizations of the grown films.<br />

DS 22.54 Di 14:30 Poster B<br />

Majority-carrier properties of low-temperature epitaxial Si —<br />

•S. Brehme, U. Knipper, B. Rau, and W. Fuhs — Hahn-Meitner-<br />

Institut Kékulestr. 5 12489 Berlin<br />

In this contribution we report the results of electrical investigations on<br />

thin Si films grown epitaxial at temperatures below 600 ◦ C. Such films<br />

are possible candidates for absorber layers in thin-film solar cells on glass.<br />

Films were grown by Electron Cyclotron Resonance Chemical Vapor Deposition<br />

(ECR-CVD) on Si substrates. n- and p-type wafers of varying<br />

conductivity were used in the same run to render possible different types<br />

of electrical measurements such as capacitance voltage (CV), Hall effect<br />

(HE), and Deep Level Transient Spectroscopy (DLTS). The nominally<br />

undoped thin films were found to have room temperature electron concentrations<br />

in the range 10 16 cm −3 to 10 17 cm −3 depending on certain details<br />

of the growth process. From CV measurements similar results were<br />

obtained. Hall mobilities in the range 400 to 700 cm 2 /Vs were observed.<br />

Considering the ratio R of experimentally observed mobilities to values<br />

in a Si wafer of the same doping level, R values of typical 50 % are found<br />

in thin films with doping levels Nd of about 1 × 10 16 cm −3 . For layers<br />

with higher Nd R increases indicating different degrees of compensation.<br />

DLTS measurements show the presence of several electron-emitting trap<br />

levels with a dominant peak P1 at EC - 0.27 eV. Concentrations of P1

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