International Journal of Photoenergy

International Journal of Photoenergy / 2015 / Article

Research Article | Open Access

Volume 2015 |Article ID 893916 | 7 pages | https://doi.org/10.1155/2015/893916

Investigation of Poly(3,4-ethylenedioxythiophene):Poly(styrenesulfonate) Hole Transport Layer for Solution-Processed Polymer Solar Cells

Academic Editor: Zhibin Yu
Received24 Jun 2015
Accepted10 Sep 2015
Published05 Oct 2015

Abstract

The inverted polymer solar cell was prepared by self-made spray-coating system, and the poly(3,4-ethylenedioxythiophene):poly(styrenesulfonate) (PEDOT:PSS) hole transport layer was studied. 220 nm poly-(3-hexylthiophene):[6,6]-phenylC61butyric-acid methyl-ester (P3HT:PCBM) and 40 nm PEDOT:PSS were deposited on ZnO thin film subsequently by solution spray coating. Different volume of isopropyl alcohol was introduced into PEDOT:PSS to decrease the contact angle and obtain the optimum Marangoni flow. The surface morphology and roughness of PEDOT:PSS films were characterized by atomic force microscopy with varied deposition temperature from 70°C to 160°C. The improvement of power conversion efficiency (PCE) was attributed to the enhancement of vertical phase separation in PEDOT:PSS film, which improved the charge transfer in the bulk cell. The highest PCE of spray-coated PSCs reached 2.80% after postannealing for 10 min.

1. Introduction

Polymer solar cell (PSC) has been intensively investigated over the past decade, due to its superior properties such as mechanical flexibility, light weight, low-cost fabrication, and easily large-area manufacturing compatibility [14]. Power conversion efficiency (PCE) surpassing 10% is a milestone of polymer solar cell devices for prospects of commercialization [5, 6]. As a classic PSC polymeric materials, poly-(3-hexylthiophene) (P3HT) and -phenylC61butyric-acid methyl-ester (PCBM) system has shown a praiseworthy potential in increasing PCE. Single-junction bulk-heterojunction (BHJ) solar cells possess interpenetrating networks of electron donor and acceptor, presenting the maximum homogeneous donor/acceptor interfacial area, resulting in more efficient charge separation under illumination. In recent years, the PCE of P3HT:PCBM based PSC has reached 5% [7].

Various approaches have been used to realize an efficient fabrication of the multilayer structure configuration, such as spin coating [8, 9], screen printing [10], ink-jet printing [11], and spray coating [12, 13]. For solution processed method, most of the attention has been captured on spin coating, but it is unsuitable for large-area device or efficient-economical roll-to-roll manufacturing. Spray-coating method can overcome the above drawbacks, which enables uniform thin film and a large-area coating [14].

The inverted PSCs with a configuration of ITO/electron transport layer (ETL)/active layer/hole transport layer (HTL)/metal are widely used. Poly-(3,4-ethylene-dioxythiophene):poly(styrenesulfonate) (PEDOT:PSS) is quite promising as HTL material. The positive effect of PEDOT:PSS layer on device performance is attributed to four reasons: improving the selectivity of anode, higher work function than ITO, smooth contact of electrode/active layer, and facilitating the holes transportation [15]. In addition, aqueous precursor of PEDOT:PSS makes it possible to realize all-solution-processed PSC [16]. Although PEDOT:PSS is widely used in inverted PSC, it is still worth noting that PEDOT:PSS layer cannot flat well on P3HT:PCBM, due to the different polarity (PEDOT:PSS is highly hydrophilic and P3HT:PCBM is hydrophobic).

Herein, we reported a facile spray-coating approach to prepare PEDOT:PSS HTL. The surface morphology of PEDOT:PSS film was investigated and prepared by isopropyl alcohol- (IPA-) diluted PEDOT:PSS solution. It was found that the uniformity and roughness of PEDOT:PSS film was affected by the deposition temperature, and the PCE was improved due to the enhancement of vertical phase separation in PEDOT:PSS film. Significantly, after a series of optimizations, the PCE of 2.80% was achieved in this study.

2. Experiment

2.1. Fabrication of PSCs

The device configuration is ITO/ZnO/P3HT:PCBM/PEDOT:PSS/Ag (Figure 1(a)). PSC devices were fabricated on ITO glass substrates (6.7 Ω/sq). The glass was cleaned in ultrasonic bath containing detergent, deionized water, IPA, and acetone (10 min each step) consecutively. Prior to deposition of the ZnO, ITO glass substrates were treated by ultraviolet light for 10 min. Zinc-ammonia precursor was prepared with zinc acetate (Zn(CH3COO)2, 99.9%, 3 g, Aldrich, USA), and the ZnO layer was sprayed from the zinc-ammonia precursor on ITO glass substrate with a N2 flow rate of 12 L/min, and then the film was annealed at 200°C for 30 min in air. The photoactive layer precursor that consists of 1 : 1 of P3HT (99.9%, Aldrich) and PCBM (99.9%, Lumtec, USA) was dissolved into 1, 2-dichlorobenzene (DCB) at a concentration of 10 mg/mL and the solution was kept stirring for 12 h at 80°C. The P3HT:PCBM layer was sprayed on the top of ZnO layer at a substrate temperature of 80°C and then annealed at 130°C for 10 min in N2 atmosphere. PEDOT:PSS dispersion (Heraeus Clevios PH1000) mixed with different volume IPA and 1% Zonyl FS-300 fluorosurfactant was sprayed onto P3HT:PCBM layer at 130°C with a solution injection rate of 0.2 mL/min. The PEDOT:PSS and P3HT:PCBM layers were both deposited with a N2 flow rate of 10 L/min. Finally, Ag electrode was thermally evaporated in vacuum at 2 × 10−4 Pa through a mask to define five separate cells on each substrate.

2.2. Characterization

The morphology of PEDOT:PSS layer was characterized by atomic force microscope (AFM 5500, Keysight, Inc.) and scanning electron microscope (FEI Quanta 250). The thickness of each layer was monitored using the Alphastep D-100 stylus profiler. The active area of each fabricated PSC was 0.03 cm2. The photocurrent density-voltage (-) curves measurements of PSCs were performed with the xenon lamp (CHF-XM35, Beijing) under a calibrated illumination power of 100 mW/cm2. All the measurements were carried out in air ambient circumstance.

3. Results and Discussion

3.1. Optimizing of Spray-Coating Parameters

The self-made spray-coating system is shown in Figure 1(b). The nozzle is connected to calibrated syringe pump for solution transporting and N2-supplier equipment (upper N2-connector is for pushing up the pin inside and the other is for gas flow controlling). Deposition temperature which plays a crucial role of fabricating HTL is accurately controlled by a thermal couple. The precursor was broken up into small droplets by nozzle and directly sprayed onto temperature controlled ITO substrate.

To form a full wet and continuous PEDOT:PSS layer, the distance between nozzle and substrate was investigated which affected film homogeneity notably. When the height was higher than 8 cm, the small droplets were evaporated completely before reaching hot substrate, thus resulting in a relatively smooth and dry film surface. However, if the height was below 4 cm, the spray-coated PEDOT:PSS film remained wet, resulting in particle aggregation and nonhomogeneous film surface. The best spray distance between nozzle and substrate was 6 cm, at which a continuous and homogeneous film was obtained.

In this work, a computer drove X-Y hotplate stage allows a reproducible thickness of deposited film. The deposition temperature and thickness of each function layer in PSC are summarized in Table 1. By optimizing spray-coating parameters, a better control over the spray-coating processing allowed for improving the performance of PSC.


LayerDeposition temperature (°C)Layer thickness (nm)

ZnO20050 nm
P3HT:PCBM40220 nm
PEDOT:PSS70, 100, 130, 16040 nm
Ag120 nm

3.2. Effect of IPA and Fluorosurfactant Doping on PEDOT:PSS Films

During PEDOT:PSS deposition, coffee ring effect and Marangoni flow are paramount factors to determine the morphology of PEDOT:PSS film. The Marangoni flow can be defined as follows: the solute would accumulate at the rim of a drying droplet under the influence of a surface tension gradient. The Marangoni velocity was given bywhere is viscosity of the film, is surface tension, is volume fraction of low surface tension solvent, and are evaporation velocity, and and are activity coefficient of the low and high surface tension solvent, respectively [17]. IPA is a favorable candidate to dilute PEDOT:PSS dispersion, since it can improve contact properties effectively between PEDOT:PSS and P3HT:PCBM and ensure full coverage of HTL. Moreover, 1% Zonyl FS-300 fluorosurfactant was added to PEDOT:PSS solution to further reduce the contact angle and enhance spreading on the hydrophobic P3HT:PCBM layer.

It was found that volume ratio of PEDOT:PSS and IPA was 1 : 14 and could not only reduce the contact angle of solution but also control Marangoni flow and convective flows during deposition process, obtaining a relatively homogeneous film. Besides, Girotto et al. [12] elaborated the relationship between contact angle and surface tension, which proved that the diluted PEDOT:PSS solution was beneficial to produce a homogeneous film.

The surface morphologies of PEDOT:PSS films are shown in Figure 2. The original PEDOT:PSS dispersion could not flat well onto P3HT:PCBM layer (Figure 2(a)); however, films prepared with the IPA-diluted solution exhibited a distinguish surface morphology. A network surface was formed (Figure 2(b)), due to the well-flatten droplets on the P3HT:PCBM layer. The network surface could benefit exciton separation at P3HT:PCBM and PEDOT:PSS interface and facilitate charge carrier transporting efficiently to the electrodes. The contact angle was decreased during the preparation of diluted PEDOT:PSS layer and the Marangoni flow was under control. When prepared by adding 1% Zonyl FS-300 fluorosurfactant, PEDOT:PSS film surface was smooth (Figure 2(c)). However, the network structure may provide better pathway for charge carrier transferring than smooth surface, thus resulting in the higher conductivity than that of the other two samples.

In practice, the conductivity of PEDOT:PSS film was also modified with IPA and fluorosurfactant (as shown in Figure 3). With IPA-diluted ratio increasing from 1 : 6 to 1 : 18, the PEDOT:PSS films conductivities were improved from 4.5 × 10−3 S/cm to 1.8 × 10−2 S/cm. However, the films conductivities were decreased to 1.2 × 10−2 S/cm and 3.1 × 10−3 S/cm, respectively, with adding 0.5% and 1% Zonyl FS-300 into PEDOT:PSS solution ((PEDOT:PSS) : IPA = 1 : 14), due to the fact that Zonyl FS-300 fluorosurfactant cannot conduct electricity. Despite this, fluorosurfactant could improve solution ductility and well reduce the contact angle, leading to the well contact between HTL and ETL and the improvement of PCE.

3.3. Effect of Deposition Temperature on the Performance of PSCs

PEDOT:PSS HTL surface topography was significantly influenced by droplets drying rate. Actually, real drying condition of sprayed droplets is a result of extremely complex situation. To estimate the relationship between deposition temperature and drying rate, the average drying rate () (dimensions mass/time) is expressed as follows [18]:where is thermal conductivity of liquid droplet, is average droplet diameter, ΔT is mean temperature difference between droplet surface and surrounding air, and λ is latent heat of vaporization. , , and λ can be considered as fixed parameters due to the usage of same solution (in this part, the IPA-diluted solution (PEDOT:PSS) : IPA = 1 : 14 and 1% Zonyl FS-300 fluorosurfactant were utilized); thus, the drying rates are dominantly related to . Therefore, we can assume that the film surface morphology is dominantly related to deposition temperature.

To further control PEDOT:PSS HTL morphology and solution evaporation process, the temperature effect on film surface morphology was also investigated from 70°C to 160°C. Figure 4 show AFM images and vertical phase separation models of PEDOT:PSS films prepared under varied deposition temperatures. The different root mean square (RMS) roughness suggested a variation in surface morphology for PEDOT:PSS films. At 70°C, PEDOT:PSS film exhibited the minimum surface roughness with a RMS of 1.0 nm and less phase separation of PEDOT:PSS [16] (Figure 4(a)). When the deposition temperature improved to 100°C, the PEDOT:PSS film exhibited rougher surface with a RMS of 2.0 nm (Figure 4(b)). Further increasing deposition temperature to 130°C, inner PSS moved to film surface and gathered together, giving rise to vertical phase separation effect and forming larger grains (Figure 5(c)). During this process, the contact area between P3HT:PCBM and PEDOT:PSS film interface was enlarged, increasing the possibility of holes in P3HT:PCBM transporting to PEDOT:PSS. Hence, the carriers could be transported through the conductive pathway rather than being recombined with each other in P3HT:PCBM or trapped in PEDOT:PSS HTL [19, 20]. At 160°C, PEDOT:PSS/IPA solution could not wet onto whole P3HT:PCBM layer surface completely due to the escalation of solution evaporation rate. As shown in Figure 4(d), a largest film surface RMS of 7.0 nm was obtained because of the larger grain size caused by high deposition temperature. At this temperature, PSS was completely separated from PEDOT section, leading to the destruction of holes transportation (Figure 5(d)). Furthermore, quite a few defects in PEDOT:PSS/P3HT:PCBM interface caused by rough HTL film could deteriorate device FF and limit the PCE.

The - curves of PSCs for PEDOT:PSS deposited with different temperatures are shown in Figure 6 and the detailed photovoltaic parameters are listed in Table 2. With temperature increasing from 70°C to 130°C, was improved by 30% from 7.05 to 9.17 mA/cm2 and FF was enhanced from 39.4% to 49.1%, and this rising trend in and FF made a contribution to PCE improvement, from 1.57% to 2.55%. The enhancement could be ascribed to the formation of vertical phase separation between PSS and PEDOT chains which benefited hole transferring from P3HT:PCBM to HTL. Meanwhile, Yeo et al. [21] reported that vertical phase separation in PEDOT:PSS film could increase conductivity and work function of the anode. However, the PCE decreased to 1.40% when deposition temperature was 160°C. On one hand, rougher PEDOT:PSS HTL (as shown in Figure 4(d)) could introduce quite a few defects which might trap hole during the transferring process. On the other hand, the larger PEDOT-rich grains formed by high deposition temperature were completely separated from PSS, deteriorating the conductive pathway for holes migrating and leading to a decrease of and FF. As a result, the optimal deposition temperature to spray PEDOT:PSS solution was 130°C.


TEM (°C) (V) (mA/cm2)FF (%)η (%)

700.557.0539.41.57
1000.567.8047.02.01
1300.609.1749.12.55
1600.557.4534.71.40

To further improve interface contact area between PEDOT:PSS and P3HT:PCBM, devices were postannealed on hot plate for 10 min. After that, the best performance of PSC device was 2.80%, which demonstrated a close similar performance to that of spin-coating device [22].

4. Conclusions

In this experiment, a simple spray-coating process for PEDOT:PSS HTL deposition was demonstrated. In order to take advantage of Marangoni flows to control HTL morphology, IPA and fluorosurfactant were used to tune PEDOT:PSS dispersion. The best conductivity was 1.56 × 10−2 S/cm when PEDOT:PSS/IPA ratio was 1 : 14. The vertical phase separation and roughness of HTL were further tuned by varied deposition temperatures. The carriers could transfer through the HTL rather than being recombined with each other in P3HT:PCBM or trapped in HTL. It was found that the vertical phase separation was reinforced with deposition temperature increasing from 70°C to 130°C. Moreover, PSCs were allowed to post-anneal for another 10 min to further improve PCE. After a series of optimizations, the highest PCE of 2.80% was achieved.

Conflict of Interests

The authors declare that there is no conflict of interests regarding the publication of this paper.

Acknowledgments

This research is supported by Chongqing Science and Technology Commission (Grant no. cstc2013 jcyjys50001), Chongqing Education Committee (Grant no. KJ1401113), and Science Projects of Chongqing University of Arts and Sciences (R2013CJ08, Y2013CJ29, XSKY2015123, M2014 ME05).

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Copyright © 2015 Chengxi Zhang et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

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