Investigation of Driving Forces for Charge Extraction in Organic Solar Cells: Transient Photocurrent Measurements on Solar Cells Showing S‐Shaped Current–Voltage Characteristics

The role of drift and diffusion as driving forces for charge carrier extraction in flat heterojunction organic solar cells is examined at the example of devices showing intentional S‐shaped current–voltage (J‐V) characteristics. Since these kinks are related to energy barriers causing a redistribution of the electric field and charge carrier density gradients, they are suitable for studying the limits of charge extraction. The dynamics of this redistribution process are experimentally monitored via transient photocurrents, where the current response on square pulses of light is measured in the μs to ms regime. In combination with drift‐diffusion simulation data, we demonstrate a pile‐up of charge carriers at extraction barriers and a high contribution of diffusion to photocurrent in the case of injection barriers. Both types of barrier lead to S‐kinks in the J‐V curve and can be distinguished from each other and from other reasons for S‐kinks (e.g. imbalanced mobilities) by applying the presented approach. Furthermore, it is also helpful to investigate the driving forces for charge extraction in devices without S‐shaped J‐V curve close to open circuit to evaluate whether their electrodes are optimized.

[1]  P. Mendels,et al.  Extension of the zinc paratacamite phase diagram: Probing the effect of spin vacancies in an S = 1/2 kagome antiferromagnet , 2012 .

[2]  Karl Leo,et al.  Influence of Hole‐Transport Layers and Donor Materials on Open‐Circuit Voltage and Shape of I–V Curves of Organic Solar Cells , 2011 .

[3]  Martin Pfeiffer,et al.  Organic p-i-n solar cells , 2004 .

[4]  K. Leo,et al.  Open circuit voltage and IV curve shape of ZnPc:C60 solar cells with varied mixing ratio and hole transport layer , 2011 .

[5]  Martin A. Green,et al.  Solar cell efficiency tables (version 39) , 2012 .

[6]  K. Leo,et al.  Small-molecule solar cells—status and perspectives , 2008, Nanotechnology.

[7]  L. Onsager Initial Recombination of Ions , 1938 .

[8]  Mm Martijn Wienk,et al.  Influence of injected charge carriers on photocurrents in polymer solar cells , 2012 .

[9]  Amy M. Ballantyne,et al.  Recombination Dynamics as a Key Determinant of Open Circuit Voltage in Organic Bulk Heterojunction Solar Cells: A Comparison of Four Different Donor Polymers , 2010, Advanced materials.

[10]  C. Leung,et al.  Charge accumulation induced S-shape J–V curves in bilayer heterojunction organic solar cells , 2011 .

[11]  Y. Filinchuk,et al.  Tetrahedra system Cu4 OCl6 daca4: High-temperature manifold of molecular configurations governing low-temperature properties , 2008, 0801.1507.

[12]  J. Staudigel,et al.  A quantitative numerical model of multilayer vapor-deposited organic light emitting diodes , 1999 .

[13]  K. Leo,et al.  Imbalanced mobilities causing S-shaped IV curves in planar heterojunction organic solar cells , 2011 .

[14]  Yang Yang,et al.  Dipole induced anomalous S-shape I-V curves in polymer solar cells , 2009 .

[15]  Mariusz Wojcik,et al.  Accuracies of the empirical theories of the escape probability based on Eigen model and Braun model compared with the exact extension of Onsager theory. , 2009, The Journal of chemical physics.

[16]  Yuya Tanaka,et al.  Identification of different origins for s-shaped current voltage characteristics in planar heterojunction organic solar cells , 2012 .

[17]  C. McNeill,et al.  Photocurrent transients in all-polymer solar cells: Trapping and detrapping effects , 2009 .

[18]  Christoph J. Brabec,et al.  Design Rules for Donors in Bulk‐Heterojunction Solar Cells—Towards 10 % Energy‐Conversion Efficiency , 2006 .

[19]  D. Rauh,et al.  S-shaped current-voltage characteristics of organic solar devices , 2010, 1005.5669.

[20]  C. Tang,et al.  Hole-transport limited S-shaped I-V curves in planar heterojunction organic photovoltaic cells , 2011 .

[21]  J. Bisquert,et al.  Diffusion-Recombination Determines Collected Current and Voltage in Polymer:Fullerene Solar Cells , 2012 .

[22]  J. Bisquert Beyond the quasistatic approximation: Impedance and capacitance of an exponential distribution of traps , 2008 .

[23]  S. Züfle,et al.  Nanosecond response of organic solar cells and photodetectors , 2009 .

[24]  Andrew J. Medford,et al.  The effect of post-processing treatments on inflection points in current–voltage curves of roll-to-roll processed polymer photovoltaics , 2010 .

[25]  Martin Pfeiffer,et al.  Origin of open circuit voltage in planar and bulk heterojunction organic thin-film photovoltaics depending on doped transport layers , 2008 .

[26]  T. Lahm Bradykinin and the heart: left, right, or both? , 2011, The Journal of surgical research.

[27]  Karl Leo,et al.  Impedance model of trap states for characterization of organic semiconductor devices , 2012 .

[28]  N. S. Sariciftci,et al.  A review of charge transport and recombination in polymer/fullerene organic solar cells , 2007 .

[29]  Charles L. Braun,et al.  Electric field assisted dissociation of charge transfer states as a mechanism of photocarrier production , 1984 .

[30]  N. S. Sariciftci,et al.  Charge transport and recombination in bulk heterojunction solar cells studied by the photoinduced charge extraction in linearly increasing voltage technique , 2005 .

[31]  Kristian O. Sylvester-Hvid,et al.  Efficiency limiting factors of organic bulk heterojunction solar cells identified by electrical impedance spectroscopy , 2007 .