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1991, Advanced Materials
AI
The paper discusses the potential of organic solar cells as a regenerative energy source, comparing their efficiencies and mechanisms with inorganic semiconductor cells. Although organic solar cells have shown significant progress since the 1970s, achieving efficiencies of up to 0.5%, challenges remain due to their complex energy-band structures and lower charge-carrier mobilities. The article provides an overview of organic solar cell structures, fabrication methods, characteristics, and presents a qualitative understanding of their operational principles using classical semiconductor theories.
physica status solidi (RRL) - Rapid Research Letters, 2013
Applied Physics Letters, 2012
Applied Physics Letters, 2016
Accounts of Chemical Research, 2009
O rganic photovoltaics, which convert sunlight into elec- tricity with thin films of organic semiconductors, have been the subject of active research over the past 20 years. The global energy challenge has greatly increased interest in this technology in recent years. Low-temperature processing of organic small molecules from the vapor phase or of polymers from solution can confer organic semiconductors with a critical advantage over inorganic photovoltaic materials since the high-temperature processing requirements of the latter limit the range of substrates on which they can be deposited. Unfortunately, despite significant advances, the power conversion efficiency of organic solar cells remains low, with maximum values in the range of 6%. A better understanding of the physical processes that determine the efficiency of organic photovoltaic cells is crucial to enhancing their competitiveness with other thin-film technologies. Maximum values for the photocurrent can be estimated from the light-harvesting capability of the individual molecules or polymers in the device. However, a better understanding of the materials-level processes, particularly those in layerto-layer interfaces, that determine the open-circuit voltage (V OC ) in organic solar cells is critical and remains the subject of active research. The conventional wisdom is to use organic semiconductors with smaller band gaps to harvest a larger portion of the solar spectrum. This method is not always an effective prescription for increasing efficiency: it ignores the fact that the value of V OC is generally decreased in devices employing materials with smaller band gaps, as is the case with inorganic semiconductors. In this Account, we discuss the influence of the different interfaces formed in organic multilayer photovoltaic devices on the value of V OC ; we use pentacene-C 60 solar cells as a model. In particular, we use top and bottom electrodes with different work function values, finding that V OC is nearly invariant. In contrast, studies on devices incorporating hole-transport layers with different ionization potentials confirm that the value of V OC depends largely on the relative energy levels of the donor and acceptor species that form the essential heterojunction. An analysis of the properties of solar cells using equivalent-circuit methods reveals that V OC is proportional to the logarithm of the ratio of the photocurrent density J ph divided by the reverse saturation current density J 0 . Hence, an understanding of the physical origin of J 0 directly yields information on what limits V OC . We assign the physical origin of J 0 to the thermal excitation of carriers from the donor to the acceptor materials that form the organic heterojunction. Finally, we show that the solution to achieving higher power conversion efficiency in organic solar cells will be to control simultaneously the energetics and the electronic coupling between the donor and acceptor materials, in both the ground and excited state.
Physical Review Applied, 2014
Interfaces play an important role in emerging organic electronic applications. In order to optimize and control the performance in organic devices such as organic solar cells, a comprehensive understanding of the contacts is essential. However, despite the vast progress made, a fundamental theory of the physical processes taking place at the contacts is still lacking. In this work, a numerical device model is used to clarify the effect of imperfect contacts in organic bulk heterojunction solar cells. The effect of increased injection barriers, reduced surface recombination, interfacial minority carrier doping, and traps for majority carriers at the electrodes causing reduced efficiencies is simulated. Two distinctly different underlying mechanisms leading to different S-shaped features are found, both leading to an effective shift of the builtin voltage. In the case of an extraction barrier to majority carriers at the contact, such as reduced surface recombination, the S kink is due to an induced diffusion potential. In the case of interfacial doping or traps, the S kink results from band bending caused by the fixed or trapped space charge. We derive analytical expressions describing the effective reduction of the built-in voltage and the (effective) open-circuit voltage providing means to quantify and distinguish the mechanisms. We show how to experimentally differentiate between these effects and provide tools to extract the relevant physical parameters.
Advanced Materials
The energy of the charge-transfer state formed between electron-donating and electronaccepting materials, a state that directly absorbs, largely determines the limit of the open-circuit voltage in organic photovoltaic devices. This is described in work by Aram Amassian, Michael D. McGehee and co-workers on page 6076.
ACS Nano, 2012
I n organic photovoltaic devices, outer interface structures play a significant role in establishing optimal contact conditions for efficient extraction (or blocking) of charge carriers. Buffer layers of different nature are currently employed to enhance both power conversion efficiency (PCE) and cell stability by improving contact performance. Several materials have been explored to enhance the electron selectivity of the cathode contact: alkali metal compounds (LiF, etc.), metal oxides (TiO x , ZnO, etc.), and low molecular weight organic compounds have been reported to contribute to the overall PCE and solar cell lifetime, as reviewed in recent reports. 1À3 Among those approaches, the effect of the dipole moment associated with self-assembled monolayers (SAM) attached to the interface, which alter the energy level alignment between the cathode metal and the bulk of the blend, 4 is particularly interesting, as well as the inclusion of conjugated polyelectrolyte interlayers. 5 In all of these cases, the energy shift induced by the charge dipole built up at interface layers enables the use of air-stable high work function metals. It is then inferred that electrostatic mechanisms occurring at the nanometer scale, both in the active layer bulk and at interfaces, have a great influence on the overall device operation. Interface dipole layers are regarded as a determining ingredient of the metal/organic contact equilibration. 8À12 Several models have been proposed to account for the energy level alignment at interfaces, depending on the degree of interaction between the metal contact and the deposited organic layer. When the chemical interaction between the metal and contacting conjugated molecules or polymers is not negligible, it is expected that molecules attached to the metal surface undergo both a shift and a broadening of their molecular energy levels. Energy distribution of the attached molecules should be modeled by a specific interfacial density of states (IDOS) which differs from that encountered in the bulk of the organic layer. The situation is ABSTRACT Electronic equilibration at the metalÀorganic interface, leading to equalization of the Fermi levels, is a key process in organic optoelectronic devices. How the energy levels are set across the interface determines carrier extraction at the contact and also limits the achievable open-circuit voltage under illumination. Here, we report an extensive investigation of the cathode energy equilibration of organic bulk-heterojunction solar cells. We show that the potential to balance the mismatch between the cathode metal and the organic layer Fermi levels is divided into two contributions: spatially extended band bending in the organic bulk and voltage drop at the interface dipole layer caused by a net charge transfer. We scan the operation of the cathode under a varied set of conditions, using metals of different work functions in the range of ∼2 eV, different fullerene acceptors, and several cathode interlayers. The measurements allow us to locate the charge-neutrality level within the interface density of sates and calculate the corresponding dipole layer strength. The dipole layer
Faraday discussions, 2014
opened the discussion of the paper by Jenny Nelson: A viable explanation for the initial long-range charge separation step in organic photovoltaic cells is via extremely high non-equilibrium charge mobilities of charge pairs initially formed high in the density of states (DOS). In this model, charge separation would be enhanced by some degree of disorder, including possibly the disorder induced by the packing with the fullerene at the heterojunction.
physica status solidi (b), 2008
Over the past decade organic solar cells dragged lot of attention and research interest due to its wide potential and advantages such as low cost, made of abundant earth materials, simple manufacturing techniques and ability to incorporate various technologies. Although a lot amount of research and development is required to effectively tackle the foreseen advantages. This paper reviews basic fundamental physics of organic solar cells, working mechanism and recent developments in the field.
Applied Physics Letters, 2009
Applied Physics Letters, 2011
Structure dependence in hybrid Si nanowire/poly(3,4-ethylenedioxythiophene):poly(styrenesulfonate) solar cells: Understanding photovoltaic conversion in nanowire radial junctions Appl. Phys. Lett. 100, 023112 (2012) Dependence of recombination mechanisms and strength on processing conditions in polymer solar cells APL: Org. Electron. Photonics 4, 279 (2011) Dependence of recombination mechanisms and strength on processing conditions in polymer solar cells Appl. Phys. Lett. 99, 263301 (2011) Crystal particle Raman-scattering and applications for improved solar cell performance Appl. Phys. Lett. 99, 251109 (2011) Effects of aging on the mobility and lifetime of carriers in organic bulk heterojunction solar cells J. Renewable Sustainable Energy 3, 063111 (2011) Additional information on Appl. Phys. Lett.
Physical Review B, 2013
The ac admittance of solar cells under illumination is investigated under open-circuit conditions. Open-circuit conditions are imposed by inserting a probe capacitor into the circuit. The capacitance and conductance of the cells are investigated as function of frequency and continuous illumination intensity. Results are compared with numerical and analytical modeling of charge recombination and transport. In bulk heterojunction solar cells with [6,6]-Phenyl-C 61 (C 71 )-butyric acid methyl ester as acceptor and poly(3-hexylthiophene) or poly[2methoxy-5-(2 -ethylhexyloxy)-p-phenylene vinylene] as electron donor, the high-frequency capacitance C and conductance G follow a power-law dependence on intensity of white light I, with G(I) ∝ I 3/4 and C(I) ∝ I 1/4 . The modeling shows that these dependencies can be explained in terms of space-charge-limited current in combination with Langevin type recombination of carriers. For poly [2,1,3-benzothiadiazole-4,7-diyl[4,4-bis(2ethylhexyl)-4H-cyclopenta[2,1-b:3,4-b ]dithiophene-2,6-diyl]] the capacitance shows a weaker dependence on intensity, indicating fast recombination of photogenerated carriers. Results indicate that the fill factor of relatively well performing polymer solar cells can still be limited by space charge effects and can be improved by enhancing the charge carrier mobility or by reducing the bimolecular Langevin recombination.
Journal of Applied Physics, 2010
The microscopic states and performance of organic solar cell are investigated theoretically to explore the effect of the carrier mobility. With Ohmic contacts between the semiconductor and the metal electrodes there are two origins of carriers in the semiconductor: the photocarriers generated by photon absorption and the dark carriers diffused from the electrodes. The power efficiency of the solar cell is limited by the recombination of a carrier with either the photocarrier or a dark carrier. Near the short-circuit condition the photocarrier recombination in the semiconductor bulk decreases as the mobility increases. Near the open-circuit condition the dark carrier recombination increases with the mobility. These two opposite effects balance with one another, resulting in an optimal mobility about 10−2 cm2/V s which gives the highest power conversion efficiency. The balance of the electron and hole mobilities are not necessary to maintain the optimal efficiency also because of the ...
Advanced Materials, 2012
Plastic solar cells are the subject of an extensive research effort because of their potential as cheap, printable, and fl exible solar energy converters. As a result, continuous improvements in device effi ciencies are being made, highlighted by power conversion effi ciencies in excess of 10%. [ 1 ] An important step towards the realization of widespread commercialization is attainment of higher effi ciencies in the best cells, and improvements of the scale-up process. Both objectives are possible only through a more complete understanding of factors limiting the device performance; one of the limiting factors is the presence of chemical impurities. Chemical impurities can result from reaction side products, [ 2 ] residual catalysts, [ 3 ] and effects of atmospheric oxygen. [ 4 ] Although impurities have been identifi ed as a signifi cant hindrance to device performance, [ 5 , 6 ] it has also been suggested that intentional dopants could increase performance under special circumstances, for example, when carrier mobilities are highly imbalanced. [ 7 ] The effect of impurities on solar cell performance is related to the discussion regarding the role of energetic disorder on the performance of solar cells [ 8 ] and the properties of organic semiconductor devices in general. [ 9 ] However, the mechanisms by which impurities reduce performance is still a subject of discussion, the resolution of which could enable more targeted troubleshooting of the synthetic and fabrication steps necessary to build a high performing device. To investigate the effect of impurities on the solar cell performance, they are added in a controlled manner, and their effects were investigated using various techniques. The two impurity molecules are 14,14,8,8-teracyanoquinodimethane (TCNQ) and [6,6]-phenyl-C 84-butyric acid methyl ester (PC 84 BM), both of which function as electron traps (Figure 1). [ 5 , 6 , 10 ] More specifi cally, both have larger electron affi nities than the electron www.advmat.de www.MaterialsViews.com
Advanced Functional Materials, 2011
An energy mismatch in the HOMOs leads to kinks in the I-V curves in the cases for which V oc is independent of the HTL.
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