Silver Nanoparticles in PEDOT:PSS Layer for Polymer Solar Cell Application

Iwan, Agnieszka; Boharewicz, Bartosz; Tazbir, Igor; Sikora, Andrzej; Zboromirska-Wnukiewicz, Beata

doi:https://doi.org/10.1155/2015/764938

International Journal of Photoenergy

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Abstract Introduction Materials Results and Discussion Conclusions Acknowledgments References Copyright Related Articles

Research Article | Open Access

Volume 2015 | Article ID 764938 | https://doi.org/10.1155/2015/764938

Silver Nanoparticles in PEDOT:PSS Layer for Polymer Solar Cell Application

Agnieszka Iwan,¹Bartosz Boharewicz,¹Igor Tazbir,¹Andrzej Sikora,¹and Beata Zboromirska-Wnukiewicz¹

Academic Editor: Mohammad Muneer

Received29 Oct 2014

Accepted19 Jan 2015

Published02 Mar 2015

Abstract

We compare the performance of polymer solar cells based on poly(3-hexylthiophene) (P3HT) and [6,6]-phenyl-C61-butyric acid methyl ester (PCBM) with silver nanoparticles (Ag NPs) incorporated in poly(3,4-ethylenedioxythiophene):poly(styrenesulfonate) (PEDOT:PSS). The structure of constructed solar devices was ITO/PEDOT:PSS:Ag NPs/P3HT:PCBM/Al. Typical polyol chemistry was used to synthesize silver in water solution. Ag nanoparticles were investigated by UV-vis, atomic force microscopy (AFM), and dynamic light scattering (DLS) methods. We investigated influence of amount of silver in a hole transporting layer on the performance of bulk heterojunction polymer solar cells. The value of power conversion efficiency (PCE), equal to 2.16% under simulated 100 mW/cm² AM 1.5G irradiation, was found for device created in air with 60 µL of Ag NPs added to 1 mL of PEDOT:PSS. Along with the increase amount of Ag NPs from 60 to 150 µL, the PCE decrease was found. Stability of solar cells with Ag was also investigated. The loss in value of PCE after 8 months was found in the range 13–47% depending on the device architecture. The solar cells were additionally measured with impedance spectroscopy.

1. Introduction

Recent development in organic solar cells (OSCs) is addressed to increase value of power conversion efficiency (PCE) by different plasmonic nanoparticles (NPs) introduction [e.g., [1, 2]]. This kind of organic solar cells is classified as fourth generation of photovoltaic devices and could include such NPs as carbon nanotubes, graphene, graphene oxide and their chemical modifications, quantum dots, various oxides such as , MoO₃, V₂O₅, or ZnO, or different metals (Ag, Au, Pt). NPs could be applied as component of (i) active layer, (ii) hole transporting layer, (iii) electrodes, and (iv) interlayer in OSCs (e.g., [1–6]).

Poly(3,4-ethylenedioxythiophene):poly(styrenesulfonate) (PEDOT:PSS) has high work function, high transparency, and good conductivity and is most popular hole transporting layer (HTL) in polymer solar cells [7]. PEDOT:PSS suffers from the following reasons: (i) aggregates of particles in water solution of PEDOT:PSS, (ii) strong acid character of PSS in PEDOT:PSS, and (iii) hydrophilic character of PEDOT:PSS causing nonhomogeneity of the film morphology and electrical properties along with term stability of polymer devices [8]. To solve these problems various inorganic compounds such as V₂O₅, WO₃, NiO, MoO₃, and organic compounds (poly(styrene sulfonic acid) grafted with polyaniline, polypyrrole-polystyrene sulfonate, or PEDOT:PSS with amphiphilic surfactant Surfynol 104 series, new polymer with carbazole and PO₃ moieties, graphene oxide) are proposed instead or together with PEDOT:PSS in polymer solar cells [2, 7–13].

Moreover, various metal nanoparticles (NPs) such as Ag, Au, or mixture of both are investigated in organic solar cells and can enhance the light absorption [1, 2]. The various NPs are applied in HTL or in organic layer of polymer solar cells for light trapping [14]. It is known that several techniques such as inclusion of periodic nanostructures, diffraction gratings, metallic nanoparticles, or combination of NPs and gratings are proposed [14]. NPs in OSCs can be tested in HTL, active layer or on the layer [e.g., [15–19]].

In this work, we presented influence of amount of silver nanoparticles in PEDOT:PSS layer on the performance of BHJ polymer solar cells based on poly(3-hexylthiophene) (P3HT) as a donor and [6,6]-phenyl-C61-butyric acid methyl ester (PCBM) as an acceptor. We show here that, along with the decrease of the Ag amount in hole transporting layer from 150 to 60 μL, the performance of polymer solar cells increased. As a result, we achieved a high PCE of 2.16% for constructed BHJ polymer solar cell with 60 μL of Ag NPs in 1 mL PEDOT:PSS.

2. Materials and Synthesis Procedure

General Comments. Chloroform, P3HT, PCBM, AgNO₃, and 1,5-pentanediol were purchased from Sigma-Aldrich and used as received. ITO and PEDOT:PSS (5–12 cP) were purchased from Ossila company. Surface resistance of ITO was about 20 ohms/square.

2.1. Synthesis of Silver Nanoparticles

Silver nanoparticles (Ag NPs) were obtained by typical polyol chemistry based on synthesis described in [17]. Briefly, silver nitrate (0.09 g) and poly(vinylpyrrolidone) (0.09 g) were disolved in water and next 1,5-pentanediol (12 mL) was added. Solution was mixed at 140°C for 1 h. Obtained Ag NPs were collected by means of centrifugation with the addition of acetone, water, and ethanol. Ag NPs in water solution were investigated in polymer solar cells.

2.2. Construction of Polymer Solar Cells

Solar cells were constructed on an indium tin oxide- (ITO) coated glass substrate, with the structure ITO/PEDOT:PSS:Ag NPs/P3HT:PCBM/Al, in air atmosphere. The ITO coated glass substrate was first cleaned with deionised water and then ultrasonicated in isopropanol for about 20 minutes. PEDOT:PSS:Ag NPs was spin cast (2000 rounds per minute, 25 sec. and annealed for 10 minutes at 130°C) from aqueous solution, to form a film on the ITO substrate. We added from 60 to 150 μL of Ag NPs dispersed in water to 1 mL of PEDOT:PSS. A mixture of P3HT:PCBM in chloroform solution with weight ratio 1 : 0.7 was then spin cast on top of the PEDOT:PSS layer. An aluminum electrode was deposited by thermal evaporation in vacuum of about 5 × 10⁻⁵ Torr. Then solar cells were annealed for 30 minutes at 130°C.

2.3. Characterization

UV-vis spectra in chloroform, water solution and in film were recorded with Jasco V670 spectrophotometer. Size of Ag nanoparticles was determined by dynamic light scattering (DLS) method. The measurements were performed by Zetasizer Analyzer Nano ZS, Malvern Instruments, at temperature of 25, 35, and 45°C. The basic distribution from the DLS measurement method is the distribution of intensity. The AFM measurements were performed using intermittent contact mode in air and room temperature (25°C, RH = 35%). The Innova instrument from Bruker (former Veeco) was used. Typical probes were utilized to perform the measurements (about 40 N/m and <10 nm tip radius). Acquired data was analyzed using SPIP software from Image Metrology [20].

Conductivity of PEDOT:PSS with Ag NPs layers was measured for ITO/PEDOT:PSS:Ag NPs/Al structure at 25°C for 100, 200, and 500 mV. The thickness of the PEDOT:PSS:Ag NPs layer was determined by AFM technique by measuring the height of the edge developed using sharp copper blade.

Current density-voltage (J-V) characteristics of the solar cells were measured using Solar Simulator Model SS100AAA with AM 1.5G. For simulation of solar irradiation a xenon lamp with irradiation intensity of 100 mW/cm² was used. The area of one photovoltaic pixel was 4.5 mm². The solar cells were also measured with impedance spectroscopy by Solartron precision LCR meter Model SI1260, in the frequency range of 1 Hz to 1 MHz with 20 mV test signal under illumination (halogen lamp).

3. Results and Discussion

3.1. Characterization of Ag NPs, PEDOT:PSS:Ag NPs, P3HT, and P3HT:PCBM

Figure 1 presents the chemical structure of P3HT, PCBM, and PEDOT:PSS. Silver nanoparticles were obtained by polyol chemistry [17] and characterized by UV-vis, DLS, and AFM study.

The AFM images showed that the size of Ag NPs and the thickness of PEDOT:PSS layer are about 55 and 59 nm, respectively, which indicate that Ag are imbedded with PEDOT:PSS. The same observation was found in [10] for Ag and Au NPs. The thickness of PEDOT:PSS layer with Ag NPs was approximately 60 nm. Figure 2 shows AFM images of PEDOT:PSS and Ag NPs.

(a)

(b)

(c)

(d)

(e)

(f)

(g)

One can notice the presence of Ag particles on the surface. Sobel transform reveals efficiently even such small objects on large surfaces with complex morphology [12, 21]. It should be noted that, due to immersion of the particles in the compound, only their top parts are exposed and detected by the scanning tip. As a consequence, the histograms present the diameter values of the particles significantly smaller than expected and determined using DLS method. One can however notice a specific distribution of the size, indicating typical depth of the particles immersion, which may be related with specific immersion depth balance due viscosity of the compound. As the distributions differ for each sample, one can argue if it is caused by fine fluctuations of the preparation conditions. Such an approach may allow explaining no correlation between the particles count on the surface and the particles amount for each material.

Typical parameters of topography, such as roughness (, ), for the investigated surfaces are presented in Table 1.

The root-mean-squared () roughness of PEDOT:PSS and P3HT layers on glass substrate was about 1.27 and 2.37 nm, respectively. Values of for PEDOT:PSS with Ag NPs decrease along with increase in the amount of silver nanoparticles from 1.24 nm for 60 μL of silver to about 1.05 nm for 120 μL of silver NPs. As is shown in Table 1 almost no differences were observed in the values of for 90 and 120 μL of silver in PEDOT:PSS layer. Probably during the film casting some of the Ag NPs aggregated and formed on the top of the PEDOT:PSS layer randomly distributed Ag clusters. Similar conclusion was presented by Wang et al. [17]. Only in the case of 150 μL of silver in PEDOT:PSS layer increase in comparison with other samples with and without Ag NPs (see Table 1). This behavior suggested that probably in the case of 150 μL of silver NPs the Ag NPs are mainly located on the PEDOT:PSS layer so that the roughness increased as is presented in Table 1. In the cases of 60 μL of silver in PEDOT:PSS layer almost the same value of was observed and suggested that probably all the Ag NPs are located within the PEDOT:PSS layer. Similar effect was found by Lu et al. [10].

In Figure 3 angular spectra of PEDOT:PSS:Ag NPs for the scanning field 1 μm × 1 μm are presented. The texture direction () is defined as the angle of the dominating texture in the image. For images consisting of parallel ridges, the texture direction is parallel to the direction of the ridges. This parameter is only meaningful if there are morphological objects oriented in privileged direction. The texture direction index () is a measure of how dominant the dominating direction is, and is defined as the average amplitude sum divided by the amplitude sum of the dominating direction.

For all investigated materials the presence of submicron level of organization was observed. Additionally, the and factors indicate certain level of ordering of the features, which changes along with the morphological properties during the adding various amount of Ag NPs to 1 mL of PEDOT:PSS. The increase of the ordering (decrease of parameter) is visible along with decrease in the amount of silver in HTL layer. Value of was the lowest for PEDOT:PSS with 60 μL of Ag NPs (0.432).

Additionally, we investigated size of Ag NPs by DLS method. Average size of silver NPs at 25°C was found about 65 nm (standard deviation ~ 2.4 nm) and had negative zeta potential at −2.17 mV (see Figure 4).

It is known that the Ag NPs can aggregate. To confirm this hypothesis we investigated by DLS method size of Ag NPs at 35 and 45°C. Average size of Ag NPs at 35 and 45°C was found to be about 70 and 94 nm, respectively. Moreover, Ag NPs at 35 and 45°C had negative zeta potential at −1.90 and −0.17 mV, respectively. This fact confirmed that the Ag NPs can aggregate.

Figure 5(a) shows UV-vis absorption spectra of synthesized Ag NPs, PEDOT:PSS, and PEDOT:PSS with different amount of Ag NPs. Silver NPs have two maxima of absorbance at 264 and 426 nm. Aqueous solutions of PEDOT:PSS and PEDOT:PSS with different amount of Ag NPs have one main absorption band at 261 nm and shoulder in the range 300–350 nm which could be seen in UV-vis spectra. Moreover, broad absorption band was observed at about 900 nm for PEDOT:PSS and PEDOT:PSS with different amount of Ag NPs (see Figure 5).

(a)

(b)

In our case silver NPs do not influence the big changes in UV-vis spectra of PEDOT:PSS in aqueous solution. However, influence on the changes in electrical properties of constructed devices is presented below. UV-vis spectra of PEDOT:PSS with and without Ag NPs look similar, however different the UV-vis spectrum of Ag NPs. Similar behavior was presented by Lu et al. [10] and Wang et al. [17]. In [17] authors presented UV-vis spectra of film without and with Ag NPs (40 nm size) in active layer PCDTBT:PC₇₀BM and did not observe differences in shape and absorbance maxima. In [10] Ag NPs were incorporated to PTB7:PC₇₀BM layer and also no big differences in UV-vis spectra were observed. This part of our work needs more investigations.

Additionally, in Figure 5(b) UV-vis spectra of P3HT and P3HT:PCBM in chloroform solution and in film in the region 350–800 nm are presented. In chloroform solution both P3HT and P3HT:PCBM exhibited bathochromic shift of the maximum of absorption bands in comparison with their films. P3HT in solution exhibited two absorption bands at 451 and 600 nm, while in the film two bands were found at 548 and 605 nm. UV-vis spectra of P3HT:PCBM exhibited one bond below 350 nm corresponding to PCBM (at 329 and 335 nm, resp., in solution and in film) and are not showed in Figure 5(b). In the region of 350–800 nm in the P3HT:PCBM mixture exhibited one maximum band at 454 nm (in chloroform solution) and at 492 nm (in film) (see Figure 5).

The conductivity () of P3HT was approximately 6.2 × 10⁻⁸ S/cm at 100 mV. Along with increase of voltage from 100 to 500 mV increases in conductivity of the polymer were found. The conductivity at 200 mV was 6.5 × 10⁻⁸ S/cm, while at 500 mV was 1.3 × 10⁻⁷ S/cm.

Moreover, we investigated the influence of Ag NPs on the conductivity of PEDOT:PSS. The conductivity of PEDOT:PSS was approximately 2.0 × 10⁻⁷ S/cm at 100 mV. The conductivity at 200 mV was 2.1 × 10⁻⁷ S/cm, while at 500 mV was 2.4 × 10⁻⁷ S/cm. Silver nanoparticles increase the conductivity value in the range of 29–85% as is presented in detail in Table 2.

3.2. Photovoltaic Characterization

Polymer solar cells with the glass/ITO/PEDOT:PSS:Ag NPs/P3HT:PCBM/Al architecture were fabricated and measured under AM 1.5G illumination at 100 mW/cm². We tested devices without and with 60, 90, 120, and 150 μL of silver NPs in 1 mL of PEDOT:PSS layer. Table 3 provides a summary of PV parameters.

Along with increase amount of Ag NPs decrease in power conversion value (PCE) was observed. The highest PCE was found for the device with 60 μL of silver NPs in 1 mL of PEDOT:PSS layer. After adding various amounts of Ag NPs into PEDOT:PSS layer open circuit voltage () was the same (0.60 V), except device with 150 μL of silver NPs. Value of short circuit current density () decreases along with increase in the amount of Ag NPs in PEDOT:PSS layer (see Table 3). Fill factor (FF) increased along with decrease in the amount of Ag NPs. As a result, PCE is enhanced from 1.80% for 150 μL of silver to 2.16% for 60 μL of Ag NPs. As we can see the maximum PCE value was observed for the device with 60 μL of silver NPs in 1 mL of PEDOT:PSS layer. Our preliminary study showed that for device with 30 μL of Ag NPs in 1 mL of PEDOT:PSS layer the value of PCE was lowest (1.24%) compared to that for the device with 60 μL of Ag NPs (2.16%). Moreover, our study showed that for the device without Ag NPs the PCE value was found at 2.77% (see Table 3). It shows that the addition of Ag NPs to PEDOT:PSS decreases the PCE value of devices.

To check if Ag NPs influence the lifetime of constructed polymer solar cells after 8 months all devices (encapsulated devices were kept in laboratory in air atmosphere) were again tested. The lowest loss in PCE was found for device with 90 μL of silver NPs in 1 mL of PEDOT:PSS layer. It is about 13% and refers to the PCE value of new device (2.05%) (see Table 3). For the device without Ag NPs measurement after eight months 30% loss in value of PCE was found (see Table 3).

The J-V (current density-voltage) characteristics of BHJ solar cells with Ag NPs constructed in air atmosphere are presented in Figure 6.

Electrochemical impedance spectroscopy (EIS) was applied to measure constructed polymer solar cells with Ag NPs under illumination. Nyquist plots for devices are presented in Figure 7 along with equivalent circuits of ITO/PEDOT:PSS:Ag NPs/P3HT:PCBM/Al devices. EIS experiments were analyzed based on the published papers [22, 23].

Figure 7

Impedance spectra of ITO/PEDOT:PSS:Ag NPs/P3HT:PCBM/Al device with 60, 90, 120, and 150 μL of silver NPs in 1 mL of PEDOT:PSS layer under illumination devices along with fit results and equivalent circuit of devices. represents the series resistance, is capacitance between anode and cathode, is resistance, and is constant phase element of investigated layer, where and are parameters. When then the parameters correspond to some distribution of charge transport processes rather than to a single one.

All studied devices exhibited semicircles in Nyquist plots. Moreover, noticeable drop in values of the real part () and the imaginary part () of the complex impedance along with increase in the amount of Ag NPs could be seen as a result of decreasing the diameter of the semicircles (see Figure 7). The diameter of the semicircle for the BHJ solar cells with 60 μL of silver NPs in 1 mL of PEDOT:PSS layer is the largest and also value of PCE of this device is the highest in comparison with the devices with 90, 120, and 150 μL of silver NPs in 1 mL of PEDOT:PSS layer as presented in Table 3. Moreover, the device with 150 μL of silver NPs in 1 mL of PEDOT:PSS layer exhibited the smallest diameter of the semicircle and also the lowest value of PCE (1.80%), which indicates also the lowest impedance. Fitting parameters of the equivalent circuit are presented in Table 4.

Also, along with the increase of the Ag NPs amount, the decrease of resistance values ( and ) of the devices was found (see Table 4). For the device with 60 μL of silver NPs in 1 mL of PEDOT:PSS layer values of and and were higher in comparison to the other devices.

The mean relaxation times , where : and : ( is constant phase element of the investigated layer, , and corresponds to the relaxation time of processes that occur within the active layer and at the interface, resp.) were calculated (see Table 4). The highest relaxation time was found for device with 60 μL of silver NPs in 1 mL of PEDOT:PSS layer.

4. Conclusions

To conclude, we have demonstrated the influence amount of silver nanoparticles in hole transporting layer on the performance of polymer solar cell based on P3HT:PCBM. Ag NPs were synthesized by polyol chemistry with 60 nm nanoparticles. For device created in air with 60 μL of Ag NPs added to 1 mL of PEDOT:PSS the highest value of PCE, equal to 2.16%, was found. After 8 months device with 60 μL of Ag NPs in PEDOT:PSS exhibited 28% loss in PCE compared with “new” device.

Conflict of Interests

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

Acknowledgments

Agnieszka Iwan expresses her gratitude to the National Centre for Research and Development for a supplementary financial support under the 2012–2015 Project no. PBS1/A5/27/2012. Authors thank Mr. K. Parafiniuk for Ag NPs synthesis.

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Copyright © 2015 Agnieszka Iwan 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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