# Bulk Heterojunction Organic Solar Cell Area-Dependent Parameter Fluctuation

Authors: A. J. Trindade; L. Pereira
Journal: International Journal of Photoenergy
 (2017)

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## Abstract

Organic solar cell efficiency is known to be active area dependent and is usually a problem in the upscale factor for market applications. In this work, a detailed study of organic photovoltaic devices with active layer based on poly(3-hexylthiophene) (P3HT) and 1-(3-methoxycarbonyl)-propyl-1-phenyl-(6,6)C61 (PCBM) is made, evaluating the effect of the change on the active area from 10−2 to 4 cm4. The device structure was kept simple in order to allow the understanding of the physical effects involved. Device figures of merit were extracted from the equivalent circuit using a genetic-based algorithm, and their relationship with the active area was compared. It is observed that the efficiency drops significantly with the active area increase (as the fill factor) while the parallel and series resistance, adjusted to the active area, seems to be relatively constant and increases linearly, respectively. The short circuit current and the generated photocurrent also drop significantly with the active area increase. The open circuit voltage does not show major changes. These results are discussed considering the main influences for the observed efficiency data. Particularly, as the basic circuit model seems to fail to explain the macroscopic results, the behavior can be related with the enlargement of defect interaction.


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## Body

## 1. Introduction

As organic solar cells are achieving efficiencies and lifetimes closer to the minimum required for commercialization, there is the need to study different modulus disposition, size, electrical connections, and individual cell behavior [1–17]. While high efficiency modules have been reported, these (as a rule of thumb) only seem to occur on small-scale laboratory devices. While such areas are not practical for mass production and reveal a highly complex and costly manufacturing process, there is the need to optimize and model the cells’ behavior on a real-world real-size scale. While other architectures can lead to efficiency increase and better charge collection at the electrodes, the methods and materials used are expensive and highly reactive, degrade quickly, and add a higher level of complexity to the final device [18–20]. All of which comes at a price for the consumer and to the manufacturing yield. Different architectures emerged on the last years trying to bring a new answer to the limitations of charge transport of the organic materials. Even with its own limitations, the most promising is still the bulk heterojunction type, where some experimental results point to a maximum efficiency of about 13% [21] although in a very complex structure and in a small size active area.Bulk heterojunction (BHJ) solar cells have been extensively studied considering applications in the market [22–25]. However, there is still extensive work to be done regarding the study of their electrical behavior. While efficiency records (in more realistic structures) near 10% have been reported [26–28], these seem to occur on very small laboratory-scale devices. At this moment, the major studies with organic solar cells need to be focused in general device structure and/or composition of the active layers [29–33] as well some novel materials with improved performance [34–37]. As this is not compatible with industrial scales and mass production, there is the need to study the effects of the upscale of such devices and address the loss of performance, efficiency (η), fill factor (FF), and fluctuations on the parallel (RP) and serial (RS) resistances. Also, the diode ideality (n), the generated photocurrent (JPH), and the typical open circuit voltage (VOC) and short circuit current (JSC) must be addressed.Several studies have been done to understand the influence of the BHJ active area on the device properties. Such studies involve in particular the relationship between the serial resistance and the BHJ performance [38, 39]. Recent analytical and experimental work shows that the degradation of the solar cell performance can be attributed to the higher series resistance associated with the active area increase [40–43]. Some physical studies were also made showing that other factors besides the series resistance must be also responsible for the changes in the BHJ device with the increase of the active area [44].In the present work, the simplest BHJ device architecture was made on a substrate with an indium tin oxide (ITO) anode/hole-injection layer (PEDOT:PSS)/bulk heterojunction layer (P3HT:PCBM)/the cathode of aluminum. The analysis of the solar cell parameter fluctuation towards the increase of active illuminated areas is performed and related to the increasing bulk recombination which occurred in the process. The solar cell equation parameters regarding the device characteristics (η, RS, RP, n, FF, JPH, VOC, and JSC) were adjusted and proven to be area dependent. The data shows a slight dependence of the open-circuit voltage (VOC) value that can be correlated with some light intensity as the area increases. The fill factor of the solar cell decreases significantly with the area increase mostly due to both drastic drops in the produced photocurrent contrasting with the inferior VOC increase. The electric power produced increases accordingly with the VOC increase as the latest is area and light intensity dependent. The diode ideality factor (n) also grows as the active area increases, representing the increase of intrinsic defects that behave as existing recombination centers. The parallel resistance (RP) plummets on this situation. This shows the ever growing leakage currents within the device that drives the excitons to a recombination state where the photo-generated holes and electrons no longer exist as separate entities to be collected throughout the material. Finally, we can verify that the typical equivalent electrical circuit partially fails to represent all these parameters fluctuations.All these fluctuations between real device and physical parameters need to be accounted when considering the active area increase for a real-life product application to the end consumer.


## 2. Experimental

The bulk heterojunction solar cells were fabricated using indium thin oxide- (ITO-) coated glass (Delta Technologies) having a 12–14 Ω/cm2 sheet resistance and a maximum active area of 2 × 2 cm2. Substrates were first cleaned through an ultrasonic bath using detergent (10 min), acetone (20 min), isopropanol (20 min), and distilled water (20 min). The different layers composing the device were deposited sequentially. A hole-injection layer (HTL) of PEDOT:PSS (Agfa, high conductivity) was spin coated at 3.000 rpm during 30 seconds followed by thermal annealing at 120°C for 15 minutes in the oven (~50 nm by perfilometry measurements). The active layer is composed of P3HT and PCMB (Sigma-Aldrich, sublimated) on a ratio 1 : 1 in chloroform (20 mg/ml), spin-coated at 2000 rpm for 30 seconds. The thermal annealing conditions were performed in order to minimize surface roughness and allow for the best conformation possible for the polymer chains. The used solvent was therefore evaporated at 50°C during 1 hour (~250 nm by perfilometry measurements). The aluminum cathode was thermally evaporated on the active layer through a shadow mask at <10−6 Torr, and the devices were not encapsulated. Figure 1 shows a schematic diagram of the layer deposition sequence and final device architecture.Figure 1
(a) Device layout overview and dimensions. (b) Sequentially deposited layers. (c) Example of the final device and active area mapping increase from the initial dimension (0.1 × 0.1 cm2) to the maximum available active area (2 × 2 cm2).Current-voltage data was acquired using a Keithley K2410 Voltage Source Meter at room temperature using an AM1.5 Global Oriel NRC-96000 Solar Simulator, and the active area increase was performed using black cardboard masks avoiding the well-known edge effects [45] as only the “nominal” active area is illuminated and tested. In this case, the electrical current is lower than the obtained when the whole region is illuminated (including the edges) but represents a more “real” situation. In Figure 1(c), the performed increase of the measured active area can be seen superimposed on the final device active area.


## 3. Results and Discussion

In order to extract the figures of merit of the device, we can use the one-diode “real” solar cell model (shown in Figure2), typically given by the general equation [46, 47]:
(1)JV=J0expqV−JRSAnkBT−1+V−JRSARP−JPH,where J0 is the diode saturation current density, q the electronic charge, n the diode ideality factor, kB the Boltzmann constant, T the temperature, A the cell active area, and V the device voltage. In this case, we consider JPH voltage independent. A discussion about such question will be done later.Figure 2
(a) Equivalent circuit used to modulate the organic solar cell parameters. (b) Typical current-voltage behavior of a solar cell and the relevant points to be considered in order to calculate all figures of merit and the efficiency. The rectangle inside theI-V curve gives the fill factor as well as the maximum generated power. (c) Simple scheme of the genetic algorithm flow used for the simulations.
(a)
(b)
(c)The resistances included in the equation considerably alter the shape of the curve since the voltageVRS=J×RS decreases along the series resistance, while in parallel adds the current JP=V−J×RS/RP to the current produced. The RP value can be estimated by determining the slope of the J-V curve in the region of voltage values lower than zero voltage, because in the reverse voltage region the diode does not conduct substantially and therefore the current is determined only by resistors RS and RP. The RS can be estimated by the slope of the J-V curve when the applied voltage is higher than the VOC because the current flowing through the diode is higher than the current that flows through RP, whereby the dominant resistance is RS. So, in a first approximation, we can write RP≈V/JAV<0 and RS≈V/JAV>VOC and we use such information for starting points in the genetic algorithm. Series and parallel resistances have been both associated to losses of charge generation (recombination), layer defects from the deposition method, material impurities, interface materials, and energy level misalignment, among other effects reducing charge transport before it can be successfully collected by the electrodes.In order to model the device performance and characteristics, a theoretical simulation based on the acquiredJ-V curves was scripted in Matlab®. The extraction of some parameters is performed initially through adjustments to specific regions of interest in the graphs obtained (ISC, VOC, maximum power (Pmax), and FF). These values are then compared to those obtained from the simulation carried out. The fit to the experimental data was performed using the equations of the real equivalent circuit. The parameters to be obtained from the device allow characterization and quantification of the operating values for the components that comprise the equivalent circuit, these being (scheme indicated in Figure 2(c))
(2)Parameters=n,JPH,J0,RS,RP“realcircuit”.The algorithm was implemented to fit an evolutionary algorithm (genetic algorithm) in order to seek the best fit to the experimental points using the equations used to model inorganic devices. The genetic algorithm method is an optimization and search numerical analysis based on the concept of natural evolution (genetic inheritance and Darwinian strife to survival [48]). Besides such natural approach, the genetic algorithm does not include (contrarily from almost other methods) the calculation of derivatives (that sometimes makes the convergence more problematic) and becomes to be successfully applied in several fields of scientific research and technology, including solid-state devices [49]. Our real problem is to extract the correct information of all device parameters. Using a simplex optimization method, operating limits are established for parameters (Lower and Upper Bounds) restricting the adjustment “evolution.” The population of solutions is randomly generated, and the algorithm searches in the defined domain, a near point for the best solution that take into account a minimization problem of the cost function (error). The simulation performed allowed to inquire about the parameter fluctuation as the active area increases, giving valuable insight regarding final device dimensions for manufacturing and real-module test purposes [50, 51].In the study of the parameter fluctuation, the active area increases from 10−2 cm2 to 4 cm2 in squared shapes increasing millimeter by millimeter side until the maximum active area. As a first result, we can see a global drop in current production and a small gain in the open-circuit voltage. The J-V shape changes indicate, in a first approximation, that the RS increases as the active area increases. Naturally, this kind of behavior will change significantly the overall solar cell figures of merit. The simulated total photocurrent by the device is (as seen in Figure 3(a)) always paired with the short-circuit current. Increase in the measured short-circuit causes the algorithm to recognize a higher produced photocurrent from the device, resulting in a better overlap of the experimental and simulated J-V curves.Figure 3
(a) Extrapolated short-circuit current and simulated photocurrent from the device. (b) Open-circuit voltage of the device regarding the measured active area.
(a)
(b)On an ideal device, these two parameters (JPH and JSC) would be completely matching one another. However, since JPH comes from the numerical simulation, it must account for the losses occurring on the device performance (weighted within the device equation) and is usually higher than the measured short-current density. However, for the minimum area (10−2 cm2)—and for this type of architecture—the maximum current is achieved (~10 mA/cm2); once the area increases, a strong decay in the produced photocurrent is observed, going to values near half of the maximum initially achieved and even much less for higher active areas. The observed decay occurs as more material gets exposed to the incident radiation, demonstrating that an increase in the active area does not always translate on a higher current production but results in a higher number of recombination occurring in the material. With the active area increase, the extra produced photocurrent still surpasses the lost photocurrent due to recombination in the device and seems to slowly decay for areas superior to 1.82 cm2. The nonuniformity of the cells for the large area can contribute, in a first approximation, significantly to this result. The value of the J0 exhibits a relatively large fluctuation, changing from 1 to near 100 μA/cm2 and cannot be correlated with any device area dependency. Such variations in that order of magnitude can be attributed in a first approximation to the algorithm minimization procedures, and due to its randomness with the device area, we expected no physical relationship.Regarding the open-circuit voltage (VOC)—as it has been proven before by [52, 53]—this parameter is incidentally radiation dependent but not necessarily dependent on the solar cell area [44]. As seen in Figure 3(b), gains in the open-source voltage from the initial area can add up to +0.2 V on the final device behavior, providing a significant increase in the device power production. In the first approximation, we expect that the amount of radiation-exposed material that comprises the device is crucial for an efficient open-source voltage (VOC) generation; but, as well known, the value of VOC is much dependent on the junction properties of the donor and acceptor layers and on the difference of the work functions between the electrodes [54, 55]. Therefore, it tends to be relatively constant (independent) with the active area. Although the changes are not much higher, such independence is not observed. The increase is not, however, linearly dependent, and in each initial dimension, increase from the original 10−2 cm2 results in a steady increase of VOC. The highest value measured occurred for the maximum area tested (4 cm2), where 0.6 V were achieved. This result can be simply explained, if we consider that some physical properties of the solar cells are not independent on the active area, confirmed also by changes in the JSC/JPH and (as discussed later) in n. Such parameters are known to be related with the junction properties of the active layer [56]. We must also remember that VOC, along with the JSC, is crucial for the increase in the solar cell efficiency and, on an ideal condition, to allow the cell to have an even higher, although theoretical, power production.One of the key points of a solar cell performance is the maximum power point (MPP) where the cell produces the highest electrical power. This is obtained by multiplying both the produced current and voltage throughout the entireJ-V curve. The highest value resulting from this product, in the curve region where electric power is actually produced, is the MPP, and Jmax and Vmax are the current density and the voltage at the MPP, respectively. Taking into account that this parameter is current and voltage dependent and considering that the current density J (and therefore Jmax) drops significantly while VOC is smoothly increasing the widening of the J-V curve on the voltage axis, the new Vmax points are relatively constant. The result is a decrease in the Pmax by area (W/cm2).The observed losses results on a serious crop on the performance of the device. As more intrinsic defects play a role on the carrier generation/transport, once these are exposed to the incident radiation, the effect can be seen through the curve shape as the device gradually loses its ability to maintain a good fill factor. A solar cell fill factor can be easily obtained by [57, 58]Fillfactor=Jmax×Vmax/JSC×VOC. From the initial 55.7% of FF (Figure 4(a)), as the active area rises, the rectification of the device decreases rapidly substituting the desired “L-shape” of the J-V curve by a line that resembles a linear J-V behavior.Figure 4
(a) Fill factor decay as active area increases. (b) Device efficiency decay towards a higher active area.
(a)
(b)The efficiency of a solar cellη can be easily given by [51, 57] η=Pmax/PIN=VOC×JSC/PIN×FF where PIN is the incident solar power by area. In our case, the active area increase causes a nearly exponential drop of η as seen in Figure 4(b) going from the initial 2.8% to 0.5% efficiency.Despite the increase in open-circuit voltage, the losses in the current seriously affect the device fill factor as it can be seen in Figure4(a). Usually, bulk recombination and intrinsic defects modeled by the parallel resistance (RP) are the major precursor for the FF drop, and we expect that the series resistance increases its value to cause some device performance fluctuations. In Figure 5(a), the increase in the RS (adjusted by area, i.e., RS×area) with the increase of the device area (in a linear relationship) is shown, while in Figure 5(b), we can observe that the value of RP (in the same conditions) was kept relatively constant with the area increase. Since parallel resistances model leakage currents occurring in the device and recombination on the bulk heterojunction, it is clear from Figure 5(b) that the increase of active area does not add much more recombination and, in the first explanation, is not responsible for the lowering of the efficiency.Figure 5
(a) Device series resistance value related to the active area. A linear relationship betweenRs and device area is observed. (b) Device parallel resistance was kept almost constant with active area increase.
(a)
(b)To retrieve information regarding the diode quality, its ideality factor (n) gives a good feedback regarding the molecular conformation and device efficiency on electron hole pair generation and can be seen to be linked to both FF and cell efficiency. The ideality factor seems also to be dependent when the area increases, although not represented here. As widely known, n=1 represents a perfect crystalline mesh with no structural defects [59]. Usually, we consider that the ideality factor is related with the diode behavior with the applied voltage when considering the open situation and the diode recombination behavior [60]. In the case of BHJ solar cells, the cases of n>2 are usually treated as tunneling effects [61] or eventually related with the reduced mobility typical from disordered materials. Considering the fact that organic material conformation is difficult if not impossible to control, in the smallest area, an ideality factor of 2.1 was achieved, which is a relatively good demonstration, for amorphous materials, of the local conformation where this device area was initially studied. As soon as the area is increased, the density of defects under illumination on the device increases as well quickly “reducing” (increasing) the ideality factor from its ideal value (for an area of 4 cm2, n is about 6 in a relatively linear relationship). Such behavior suggests that other mechanisms can be responsible for the recombination losses at the bulk heterojunctions. For instance, nonoverlapping orbitals or different environmental conformations can lead to the existence of several charge traps that end up reducing drastically charge transport through the different donor-acceptor molecular hopping.Considering now the overall figures of merit from our devices, we can see that bothJSC (and JPH) and FF decrease significantly while VOC remains relatively constant. The reduction of the JSC can be easily attributed to the possible existence of inhomogeneity in the thin film morphology that reduces the exciton separation. Taking into account such possible nonuniformities in the active area that increases the series resistance, it seems to be also correct to list the decrease of η as arising from the FF behavior, which clearly decreases while increasing the active area. Considering the behavior of JSC, FF, and η, a logarithmic plot of their normalized values can be made (Figure 6) and it is obvious that the changes in η seem to be more correlated with the JSC behavior than the observed in FF. Nevertheless, both depends on exciton separation (JPH related) and must be the focus. The relationship with FF can be an outlined way for a final assumption.Figure 6
Normalized logarithmic scale for efficiency (η), FF, and JSC. See text for more information.Some other factors must be taken into account. Several attempts to explain the efficiency versus area behavior of organic solar cell has been made namely a poor film quality with the effect of the series resistance [42, 43, 52, 62]. On the other hand, we must also take into account the possible joint effect of the series resistance with some possible physical factors that can accelerate the donor-acceptor recombination, usually related with structural defect states in the polymers used to build the BHJ device [44]. From Figure 6, it is very interesting to extract the fitting parameters giving a simple empirical variation. We have ηarea=0.32exp−0.29×area, FFarea=0.56exp−0.2×area, and Jscarea=0.4exp−0.26×area. Obviously, this kind of device can give a real idea about what we can expect in the scaling up.The decrease ofJSC is naturally related with JPH behavior (Figure 3(a)). As reported by some authors (e.g., [52]), JPH is usually dependent on voltage, particularly under high power light excitation (for instance above one Sun). This behavior is the natural consequence of the loss in exciton separation, a typical and well-known problem in organic photovoltaics, mainly due to the decrease of the charge transfer state generation dissociation (CTS, creation of free electron hole pairs) leading to a decrease of JPH (and therefore changing the remaining figures of merit accordingly). This effect becomes more important as the active area increases. In fact, while increasing the active area, the electrical filed across the OPV becomes much more nonuniform (mainly due to the ITO distributive resistance) and this effect limits the JPH with further loss in JSC. Even in the simplified case of JPH voltage independent ((1)), we should expect a decrease of overall figures of merit. Moreover, we expect that when JSC decreases, it will follow, according the abovementioned discussion, the JPH behavior. This is observed in our case, and for an analytical comparison at low illumination power (up to one Sun), (1) can be used. On the other hand, when increasing the active area, additional loss mechanisms appear, if nonuniform illumination effects become more pronounced. It is interesting to note that with the changes in contacts resistance distribution by means of different device structures, in a similar way, the present work can be extracted [63, 64]. Although much relevant with solar panels where contacts geometry is important, or efficiency of sun concentrators, we cannot discard such influences on our case, in spite of the low incident light power and similar contacts geometry for all devices. The problem can be focused on organic layer inhomogeneity as discussed.Some influence of the active area inhomogeneity can be partially reduced when we analyze theJSC/JPHR, where JPHR is the J at relatively high reverse bias. Some similar approach was successfully made by some authors [44]. In Figure 7, the relationship JSC/JPHR is shown, in addition to JSC and ∣J∣@−5VJPHR. From the typical J-V model, we expect that JSC/JPHR must be kept constant. This is not really observed. However, the JSC and FF does not reduce linearly with the area increase. Therefore, in a good approximation, we can consider that the reduction in JSC (JPH related and, by consequence, FF) is the main factor for lowering the efficiency and not the series resistance. As a simple conclusion (and considering the J-V model circuit), the basic system fails to describe the area dependence results. The loss of JSC can be therefore related to an “accelerated” D-A recombination probably due to defect states where collection charge depends on the local environment found at the active area (and light incidence dependent). Moreover, the carrier generation (JPH) is correlated with this assumption. As an overall conclusion, the final efficiency of an OPV “reliable area” depends on the active film internal recombination process: CTS dissociation (free electron hole pairs) and charge transport. In increasing active areas, such process governs the overall OPV macroscopic behavior and can be related with the enlargement of defect interaction in electrically molecular active overlapping.Figure 7
J
S
C
/
J
P
H
R and JSC, JPHR as a function of device active area.Independently, on the pure physical intrinsic behavior of organic layers mentioned above, the contact distributive resistance effect is evident in large active areas and will be always a real question. Although it is not the focus of the present work (the device structure/shape is always the same for all areas in order to keep a common line), changing the shape contact structure and/or unitary cell can help to reduce the loss in a large area OPV. The decrease ofJPH will always be a constraint. Nevertheless, a uniform electrical field at electrodes (and in this case the ITO) can give some solution. Our recent work in simulation of charge distribution at ITO surface covered with gold metal grid (or even in PEDOT:PSS instead ITO) shows a more uniform distributed resistance up to active areas near 1 cm2, but although with less influence, the problem persists for high active areas. On the other side, to avoid high losses in JPH, (and therefore in JSC and efficiency) in a simple OPV device (without any particular “ordered” HBJ layer), the final optimization towards a “useful” active area must fulfil the requirements of low trapping defect density (as also suggested by our previous results with small signal and capacitance-voltage data). The local molecular conformation can be improved by using careful postthermal annealing and changing the deposition layer parameters/polymer solution properties, as our actual work on continuous roll-to-roll depositions shows.


## 4. Conclusions

The use of small-area laboratory devices is important for performing the initial analysis of materials and other physical studies regarding the performance of organic bulk heterojunction solar cells. However, such dimensions are not appropriate when considering architectures for large-scale final devices or prototypes. In this study, we approached the active area growth from a typical lab scale to a manufacturing scale using the simplest architecture for a BHJ device. The behaviors of the cells were successfully modeled using our algorithms and allowed for a comparison of the cell behavior evolution with the area increase. The significant drop in efficiency, as cell active area increases, can be assigned to the decrease ofJSC/FF, both correlated with the generated photocurrent. There seems to be always a trade-off whenever considering the advantages of small area cells and large area cells, and from the reported experimental data, this has been proven. Further studies and optimizations to the morphology of these devices must consider the data now analyzed to decide strategies to approach these materials/architecture limitations.



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