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One of the substrate layouts for our organic solar cells
Credit: AFMD Group

Moritz Riede

Professor of Soft Functional Nanomaterials

Research theme

  • Photovoltaics and nanoscience

Sub department

  • Condensed Matter Physics

Research groups

  • Advanced Functional Materials and Devices (AFMD) Group
moritz.riede@physics.ox.ac.uk
  • About
  • Research
  • Teaching
  • Publications

2-(2-Methoxyphenyl)-1,3-dimethyl-1H-benzoimidazol-3-ium iodide as a new air-stable n-type dopant for vacuum-processed organic semiconductor thin films.

J Am Chem Soc 134:9 (2012) 3999-4002

Authors:

Peng Wei, Torben Menke, Benjamin D Naab, Karl Leo, Moritz Riede, Zhenan Bao

Abstract:

2-(2-Methoxyphenyl)-1,3-dimethyl-1H-benzoimidazol-3-ium iodide (o-MeO-DMBI-I) was synthesized and employed as a strong n-type dopant for fullerene C(60), a well-known n-channel semiconductor. The coevaporated thin films showed a maximum conductivity of 5.5 S/cm at a doping concentration of 8.0 wt% (14 mol%), which is the highest value reported to date for molecular n-type conductors. o-MeO-DMBI-I can be stored and handled in air for extended periods without degradation and is thus promising for various organic electronic devices.
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Erratum: Highly efficient semitransparent tandem organic solar cells with complementary absorber materials (Applied Physics Letters (2011) 99 (043301))

Applied Physics Letters 100:9 (2012)

Authors:

J Meiss, T Menke, K Leo, C Uhrich, WM Gnehr, S Sonntag, M Pfeiffer, M Riede
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In-situ conductivity and Seebeck measurements of highly efficient n-dopants in fullerene C60

Applied Physics Letters 100:9 (2012)

Authors:

T Menke, D Ray, J Meiss, K Leo, M Riede

Abstract:

We present two organic dimetal complexes Cr2(hpp)4 and W2(hpp)4 as n-dopants investigated in the model system of fullerene C60 for the application in organic electronic devices. Conductivity and Seebeck measurements on doped layers are carried out in vacuum at different doping concentrations and various substrate temperatures to compare the two dopants. Very high conductivities of up to 4 S/cm are achieved for both organic dopants. The thermal activation energy of the conductivity as well as the measured Seebeck coefficient are found to decrease with increasing doping concentration, indicating a shift of the Fermi level towards the electron transport level of the n-doped C60. © 2012 American Institute of Physics.
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Interrelation between crystal packing and small-molecule organic solar cell performance.

Adv Mater 24:5 (2012) 675-680

Authors:

Roland Fitzner, Chris Elschner, Matthias Weil, Christian Uhrich, Christian Körner, Moritz Riede, Karl Leo, Martin Pfeiffer, Egon Reinold, Elena Mena-Osteritz, Peter Bäuerle

Abstract:

X-ray investigations on single crystals of a series of terminally dicyanovinyl-substituted quaterthiophenes and co-evaporated blend layers with C(60) give insight into molecular packing behavior and morphology, which are crucial parameters in the field of organic electronics. Structural characteristics on various levels and length scales are correlated with the photovoltaic performance of bulk heterojunction small-molecule organic solar cells.
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The effect of barrier performance on the lifetime of small-molecule organic solar cells

Solar Energy Materials and Solar Cells 97 (2012) 102-108

Authors:

M Hermenau, S Schubert, H Klumbies, J Fahlteich, L Müller-Meskamp, K Leo, M Riede

Abstract:

In this work, we use different encapsulations to protect vacuum-evaporated small molecule organic solar cells with a simple p-i-i-stack for lifetime studies. Our devices use ZnPc and C60 as active materials. Lifetimes (T50) in a range from 300 h for un-encapsulated devices to 4000 h for glass-encapsulated have been observed. We use a model to distinguish between the water vapor transmission rate (WVTR) of the barrier and an additional WVTR of the aluminum top electrode. For all observed devices a loss of 50% of initial efficiency is observed when 10 mg m-2 water entered the device. The losses are related to a reduction of short circuit current density only, whereas open circuit voltage and fill factor remains unaffected. We relate this to an interaction of the water molecules with C60. © 2011 Elsevier B.V.
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