Tobias Stubhan

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Organization: University of Erlangen-Nuremberg
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Co-reporter:Tobias Stubhan, Ivan Litzov, Ning Li, Michael Salinas, Matthias Steidl, Gerhard Sauer, Karen Forberich, Gebhard J. Matt, Marcus Halik and Christoph J. Brabec  
Journal of Materials Chemistry A 2013 vol. 1(Issue 19) pp:6004-6009
Publication Date(Web):08 Apr 2013
DOI:10.1039/C3TA10987A
Intrinsic zinc oxide (ZnO) is widely used as an electron extraction layer (EEL) for inverted polymer solar cells. Despite the excellent device performance, a major drawback for large area production is its low conductivity. Using microscopic simulations, we derived a technically reasonable threshold value of 10−3 S cm−1 for the conductivity required to overcome transport limitations. For conductivity values typical for ZnO we observed the interface layer thickness restriction at only a few tens of nanometers, either as a fill factor drop due to serial resistance, eventually accompanied by a second diode behavior, or by the need for light soaking. Higher conductive aluminum-doped zinc oxide (AZO), which was introduced earlier, meets the desired conductivity threshold, however, at the cost of high temperature processing. High annealing temperatures (>150 °C) significantly improve the electrical properties of ZnO, but prohibit processing on plastic substrates or organic active layers. Here we report on AZO layers from a sol–gel precursor, which has been already reported to give sufficiently high conductivities at lower processing temperatures (<150 °C). We investigate the influence of different precursor compositions on the electrical properties of the thin films and their performance in inverted poly(3-hexylthiophene):[6,6]-phenyl-C61-butyric acid methyl ester (P3HT:PCBM) solar cells. Low temperature AZO layers with thicknesses up to 680 nm maintained comparable performance to devices with thin AZO layers.
Co-reporter:Tobias Stubhan;Michael Salinas;Alexer Ebel;Frederick C. Krebs;Andreas Hirsch;Marcus Halik;Christoph J. Brabec
Advanced Energy Materials 2012 Volume 2( Issue 5) pp:532-535
Publication Date(Web):
DOI:10.1002/aenm.201100668
Co-reporter:Tobias Stubhan;Ning Li;Norman A. Luechinger;Samuel C. Halim;Gebhard J. Matt;Christoph J. Brabec
Advanced Energy Materials 2012 Volume 2( Issue 12) pp:1433-1438
Publication Date(Web):
DOI:10.1002/aenm.201200330

Abstract

We demonstrate solution-processed tungsten trioxide (WO3) incorporated as hole extraction layer (HEL) in polymer solar cells (PSCs) with active layers comprising either poly(3-hexylthiophene) (P3HT) or poly[(4,4'-bis(2-ethylhexyl)dithieno[3,2-b:2′,3′-d]silole)-2,6-diyl-alt-(4,7-bis(2-thienyl)-2,1,3-benzothiadiazole)-5,50-diyl] (Si-PCPDTBT) mixed with a fullerene derivative. The WO3 layers are deposited from an alcohol-based, surfactant-free nanoparticle solution. A short, low-temperature (80 °C) annealing is sufficient to result in fully functional films without the need for an oxygen-plasma treatment. This allows the application of the WO3 buffer layer in normal as well as inverted architecture solar cells. Normal architecture devices based on WO3 HELs show comparable performance to the PEDOT:PSS reference devices with slightly better fill factors and open circuit voltages. Very high shunt resistances (over 1 MΩ cm2) and excellent diode rectification underline the charge selectivity of the solution-processed WO3 layers.

Co-reporter:Tobias Stubhan, Johannes Krantz, Ning Li, Fei Guo, Ivan Litzov, Matthias Steidl, Moses Richter, Gebhard J. Matt, Christoph J. Brabec
Solar Energy Materials and Solar Cells 2012 107() pp: 248-251
Publication Date(Web):
DOI:10.1016/j.solmat.2012.06.039
Co-reporter:Tobias Stubhan, Hyunchul Oh, Luigi Pinna, Johannes Krantz, Ivan Litzov, Christoph J. Brabec
Organic Electronics 2011 Volume 12(Issue 9) pp:1539-1543
Publication Date(Web):September 2011
DOI:10.1016/j.orgel.2011.05.027
In this article, we demonstrate a route to solve one of the big challenges in the large scale printing process of organic solar cells, which is the reliable deposition of very thin layers. Especially materials for electron (EIL) and hole injection layers (HIL) (except poly(3,4-ethylene dioxythiophene):(polystyrene sulfonic acid) (PEDOT:PSS)) have a low conductivity and therefore require thin films with only a few tens of nanometers thickness to keep the serial resistance under control. To overcome this limitation, we investigated inverted polymer solar cells with an active layer comprising a blend of poly(3-hexylthiophene) (P3HT) and [6,6]-phenyl-C61-butyric acid methyl ester (PCBM) with solution processed aluminum-doped zinc oxide (AZO) EIL. Devices with AZO and intrinsic zinc oxide (i-ZnO) EIL show comparable efficiency at low layer thicknesses of around 30 nm. The conductivity of the doped zinc oxide is found to be three orders of magnitude higher than for the i-ZnO reference. Therefore the buffer layer thickness can be enhanced significantly to more than 100 nm without hampering the solar cell performance, while devices with 100 nm i-ZnO films already suffer from increased series resistance and reduced efficiency.Graphical abstractHighlights► We made solution-processed polymer solar cells in the inverted structure. ► We compared doped and intrinsic zinc oxide (ZnO) as electron injection layer (EIL). ► Al doped ZnO shows three orders of magnitude higher conductivity than intrinsic ZnO. ► The impact of these EILs with increased thickness on the efficiency was determined. ► We demonstrate efficient solar cells with over 100 nm thick Al doped ZnO layers.
Co-reporter:Tobias Stubhan, Ivan Litzov, Ning Li, Michael Salinas, Matthias Steidl, Gerhard Sauer, Karen Forberich, Gebhard J. Matt, Marcus Halik and Christoph J. Brabec
Journal of Materials Chemistry A 2013 - vol. 1(Issue 19) pp:NaN6009-6009
Publication Date(Web):2013/04/08
DOI:10.1039/C3TA10987A
Intrinsic zinc oxide (ZnO) is widely used as an electron extraction layer (EEL) for inverted polymer solar cells. Despite the excellent device performance, a major drawback for large area production is its low conductivity. Using microscopic simulations, we derived a technically reasonable threshold value of 10−3 S cm−1 for the conductivity required to overcome transport limitations. For conductivity values typical for ZnO we observed the interface layer thickness restriction at only a few tens of nanometers, either as a fill factor drop due to serial resistance, eventually accompanied by a second diode behavior, or by the need for light soaking. Higher conductive aluminum-doped zinc oxide (AZO), which was introduced earlier, meets the desired conductivity threshold, however, at the cost of high temperature processing. High annealing temperatures (>150 °C) significantly improve the electrical properties of ZnO, but prohibit processing on plastic substrates or organic active layers. Here we report on AZO layers from a sol–gel precursor, which has been already reported to give sufficiently high conductivities at lower processing temperatures (<150 °C). We investigate the influence of different precursor compositions on the electrical properties of the thin films and their performance in inverted poly(3-hexylthiophene):[6,6]-phenyl-C61-butyric acid methyl ester (P3HT:PCBM) solar cells. Low temperature AZO layers with thicknesses up to 680 nm maintained comparable performance to devices with thin AZO layers.
Clevios P-VP-AI 4083
1-((3-chlorophenyl)sulfonamido)cyclohexane-1-carboxylic acid
2-ethenylbenzenesulfonic acid
Formamide, N,N-dimethyl-