Dyakonov, Vladimir

Hummelen, Jan C.

Lutsen, Laurence

Parisi, Jürgen

Riedel, Ingo

Vanderzande, Dirk

English

We have studied the influence of temperature and light intensity on the current-voltage characteristics of polymer-fullerene bulk-heterojunction solar cells. The open-circuit voltage varies linearly with temperature in the range 200K-300K and approaches a value of 930mV at T=80K. Strictly positive temperature coefficients were found for both, the short-circuit current density and the fill factor. These cause the device efficiency to increase steadily with temperature up to T=330K. The short-circuit current density increases almost linearly with light intensity. The fill factor is not significantly influenced by the incident light intensity in the temperature range from 260K to 330K. At lower temperatures, a negative slope of the fill factor is observed. Since the maximum power point varies sublinearly with light intensity, a decrease of the power efficiency is obtained at light intensities higher than 3mW/cm2

ARTS repository - University of Groningen

   University of GroningenCurrent-Voltage Characteristics of Polymer-Fullerene Solar CellsRiedel, Ingo; Dyakonov, Vladimir; Parisi, Jürgen; Lutsen, Laurence; Vanderzande, Dirk;Hummelen, Jan C.Published in:Conference Record of the Twenty-Ninth IEEE Photovoltaic Specialists Conference, 2002IMPORTANT NOTE: You are advised to consult the publisher's version (publisher's PDF) if you wish to cite fromit. Please check the document version below.Document VersionPublisher's PDF, also known as Version of recordPublication date:2002Link to publication in University of Groningen/UMCG research databaseCitation for published version (APA):Riedel, I., Dyakonov, V., Parisi, J., Lutsen, L., Vanderzande, D., & Hummelen, J. C. (2002). Current-Voltage Characteristics of Polymer-Fullerene Solar Cells. In Conference Record of the Twenty-Ninth IEEEPhotovoltaic Specialists Conference, 2002 (pp. 1322-1325). University of Groningen, Stratingh Institute forChemistry.CopyrightOther than for strictly personal use, it is not permitted to download or to forward/distribute the text or part of it without the consent of theauthor(s) and/or copyright holder(s), unless the work is under an open content license (like Creative Commons).The publication may also be distributed here under the terms of Article 25fa of the Dutch Copyright Act, indicated by the “Taverne” license.More information can be found on the University of Groningen website: https://www.rug.nl/library/open-access/self-archiving-pure/taverne-amendment.Take-down policyIf you believe that this document breaches copyright please contact us providing details, and we will remove access to the work immediatelyand investigate your claim.Downloaded from the University of Groningen/UMCG research database (Pure): http://www.rug.nl/research/portal. For technical reasons thenumber of authors shown on this cover page is limited to 10 maximum.Download date: 08-06-2022CURRENT-VOLTAGE CHARACTERISTICS OF POLYMER-FULLERENE SOLAR CELLS lngo Riedel'.', Vladimir Dyakonov', Jurgen Parisi', Laurence Lutsen', Dirk Vanderzande', Jan C. Hummelen3 Department for Energy and Semiconductor Research, Faculty of Physics, University of Oldenburg, D-26111 Oldenburg 'Institute for Materials Research, Limburg University Center, Science Park 1, 8-3590 Diepenbeek Stratingh Institute and MSC, University of Groningen, Nijenborgh 4, NL-9747 AG Groningen 1 3 ABSTRACT We have studied the influence of temperature and light intensity on the current-voltage characteristics of polymer- fullerene bulk-hetemjunction solar cells. The open-circuit voltage varies linearly with temperature in the range 200K-300K and approaches a value of 930mV at T=80K. Strictly positive temperature coefficients were found for both, the shod-circuit current density and the fill factor. These cause the device efficiency to increase steadily with temperature up to T=330K. The short-circuit current density increases almost linearly with light intensity. The fill factor is not signiflcantly influenced by the incident light intensity in the temperature range from 260K to 330K. At lower temperatures, a negative slope of the fill factor is observed. Since the maximum power point varies sublinearly with light intensity, a decrease of the power efficiency is obtained at light intensities higher than 3mw/cm2. 1. INTRODUCTION Semiconducting, conjugated polymem are promising candidates for the realization of cheap, non-toxic photovoltaic (PV) devices. Whilst mechanical flexibility and the option of modifying the optical band gap by chemical engineering are commonly desired for solar cells, the main advantage brought with these compounds is their solubility in organic solvents. This feature does not require any vacuum or high temperature processing steps for the semiconductor deposition, one makes instead use of simple and cost effective deposition techniques, such as spin-coating, screen- or even ink-jet printing [1,2]. Furthermore, these techniques are well suited for large area applications, making conjugated polymers quite attractive for PV applications. In polymer light absorbers, an efficient charge carrier generation may be realized by blending the polymer, which acts as an electron donor upon photoexcitation, with acceptor type materials. The underlying photophysics may be described by an ultrafast formation of molecularly separated charge carrier species, i.e.. a polymer cation and a fullerene anion. This photoinduced electron transfer within donor-acceptor heterojunction takes place on a sub-picosecond time scale and results in a metastable, charge separated state [3]. One of the most promising device concepts makes use of a bulk-heterojunction absorber in which the donor and acceptor moieties form a phase segregated, interpenetrating network. supporting both, efficient charge canier generation in the whole absorber volume and charge transpod within the respective subnetworkS141. A selective charge carrier collection at the opposite electrodes Is provided by the use of contact materials with different work functions. They form ohmic contacts to the appropriate semiconductor and block the minority charge carriers. For organic solar cells with light absorbers based on the sulfinyl-route synthesized conjugated polymer OCICIWPPV (3,7dimethyl-octoxy-methyloxy poly- [phenylene-vinylene]) and the fullerene PCBM ([6,6]- phenyl Ca butyric acid methyl ester), power conversion efficiencies of 3% were demonstrated under AM1.5 white light illumination (51. We present a study on the influence of temperature T and white light intensity PWt on the currentdensity vs. voltage (J-V) characteristics of such polymer-fullerene bulk-heterojunction solar cells. From the J-V- measurements, we have calculated the main photovoltaic parameters. namely, the open-circuit voltage VOC, the short-circuit current density JSC. the fill factor FF, and the power conversion efficiency, and represented them as function of T and Prght. 2. EXPERIMENTAL 2.1 Device preparation and characterization The devices were built up on thoroughly cleaned glass substrates, coated with a thin, transparent film of indium tin oxide (ITO), which acts as a window electrode. Onto the substrates, a thin layer of poly-[ethylene dioxy thiophene]: poly- [styrene sulfonate] (PEDOT:PSS, BAYTRON P. BAYER AG, Germany) was deposited. in order to form an optional interface layer. The light absorber was spin cast from an o-chlorobenzene solution of OClC10-PPVPCBM (weight ratio 1:4), forming a 100nm thin film. In the case of PED0T:PSS and the composite material, spin coating was carried out in a dry nitrogen atmosphere. Subsequently the aluminum top electrode was thermally evaporated in a vacuum chamber by shadow masking technique. The corresponding device scheme is shown in Fig. 1. Corresponding author: Inao.Riedel@uni-oldenbura.de. Phone ++49-441-798-3991, Fax -3326 0-7803-7471-1/02/%17.M) 02002 IEEE 1322 . . .  . . .  lght I PEWTPSS Fig. 1. Typical device configuration for a ITOIPEDOT PSS/OC~C~~-PPVPCBMlAl bulk-hetemjunction solar cell. The device characterization was carried out in a variable temperature cryostat with a cooling-heating facility, which allows one to adjust temperatures from 77K to 400K. The samples inside the cryostat were illuminated through a sapphire window by white light of a xenon arc lam , whose maximum intensity was calibrated to 100mWIcm by means of a reference photodiode. At a fixed temperature, the incident light intensity was stepwise reduced by a set of neutral density filters, whose transmission coefficients cover three orders of magnitude. P 3.2 Temperature Dependences An interesting feature of polymer-fullerene composite solar cells is found in the temperature dependence of the basic solar cell parameters. Fig. 2 displays JSC as function a of temperature T. A monotonic increase (10pAmi2K') of this magnitude was found for all incident light intensities up to 300K. For T>300K, JSC saturates and breaks down at the point of the glass transition (T,) for OCICIVPPV ( Ts =330K). Fig. 2. Short-circuit current density as a function of 2.8 . >  . , . , .  2.6 A 0 . 1  "E 2 E 7 0.4 0.0 0.2 ----4--d- 50 100 150 200 250 300 350 4W T I  K temperature. The legend indicates the incident light intensity in units of mW/cm2. The strong influence of temperature on JSC is quite unusual, when concerning conventional inorganic solar cells. Instead for disordered media like polymer or fullerene networks, the thermally assisted hopping transport is typical [SI and might contribute to an enhanced conductivity at elevated temperatures. The transport properties of the composite material are also mirrored in the fill factor, which represents the series and parallel resistance in the equivalent circuit of a solar celi. The fill factor increases monotonically with T and saturates at higher temperatures (See Fig. 4). When 0-7803-7471-1/02/$17.00 02002 IEEE reaching the glass transition at 330K, FF breaks down dramatically. A convergence to FF=42% is observed at higher temperatures close to 300K for different light intensities. 45,  I 50 100 150 200 250 3W 350 400 T I K  Fig. 3. Fill factor (FF) as a function of temperature for different light intensities in units of mW/cm2 (shown In the legend). The open-circuit voltage decreases approximately linear in the temperature range 200K-330K (see Fig. 4). For Tc200K a saturation at Voc=0.93V becomes visible for intensities between 20mWIcm' and 100mWlcm2. This saturation value is close to the value of quasi-Fermi levels splitting of donor and acceptor, i.e., close to the thermodynamic limit, determined by the materials energetics. For OCIClrPPV:PCBM composites,'. this energetic gap is close to 1.2eV. This discrepancy is not clarified at the moment and subject to further investigations. 400 \ 300 \----. -/-.---. ' " " ' ' " ' 50 100 150 200 250 300 350 400 T IK Fig. 4. Temperature dependence of the open-circuit voltage at different light intensities. The arrow indicates the direction of increasing Plbhl. from 0.1 to 100mW/cm2. Calculating the device power conversion efficiency, one ObSeNeS that the decrease of VOC with temperature is overcompensated by the positive temperature coefficients of the short-circuit current density and the fill factor (see Fig. 2 and Fig. 3.). Thus, the device efficiency increases with temperature until the glass transition is reached. The 1323 50 100 150 200 250 3W 350 T I K  Fig. 5. Power conversion efficiency as function of temperature T at different light intensities. Power conversion efficiency is shown in Fig. 5. Note that the maximum efficiency is obtained for light intensities around 3mW/cmz and a highest temperature of 330K. This finding will be discussed more detailed in the following section. 3.3 Light intensity dependences A first insight into the complex loss mechanisms in organic semiconductors may be obtained when investigating the relationship between the short-circuit current density and the light intensity. At higher generation rates, a recombination of electrons and holes of bimolecular type is oflen the case. The latter would lead to a square root dependence for Jsc(Plight). However, we do not observe such behavior in the devices studied. Fig. 6 shows the short-circuit current density as a function of light intensity in a double-logarithmic scale. ro-‘t.,y , , , , ,,,,, , , , , , ,,,, , , , , , ,,,, 4 0.1 1 10 100 plight I mWlcm2 Fig. 6. Intensity dependence of the short-circuit current density for different temperatures, as indicated in the legend. The slopes are typically between 0.9 and 0.95. Thus, bimolecular recombination does not significantly limit the device operation in this intensity range. However, a slight decrease of the slope can be noticed at intensities between 3mW/cm2 and 100mWIcm’. 0-7803-7471-1/02/%17.00 2002 IEEE 0.4 1 0.3 t S I  t 260K t 300K 0.1 -330%  + 0.1 380K 1 10 100 P , ~ ( , ~  I mW/cm2 Fig. 7. Variation of the fill factor with incident light intensities for different temperatures, as indicated in the legend. Fig. 7 proves that the fill factor of the studied polymer- fullerene solar cells depends only weakly on the incident light intensity in the range 260K-330K. At lower temperatures a decrease of FF with light intensity becomes visible. For a solar cell, the relationship between the open- circuit voltage and the incident light intensity is given by equation (1). V,ocCln -+1 , (1) (? I where the Jph means the photocurrent density of the solar cell and is oflen taken equal to the short-circuit current density JSC. JO is the saturation current density, which might be dependent on temperature and light intensity. As follows from Fig. 6, J p h ~ J ~ ~ ~ P ~ g h t ,  so that VOC is expected to follow a logarithmic trend. However, this is not seen in Fig. E ,  where VE is plotted against Plight in a semi- logarithmic representation. A logarithmic scaling law can be recognized only in the intensity range from 3mW/cmz to 100mW/cmz. whereas a saturation at lower temperatures is pronounced. Although the discussed magnitudes increase or at least remain constant with increasing light intensity, the device efficiency breaks down at light intensities above moderate values of approximately 3mW/cmz. 1324 900 800 > 700 8 600 500 400 E > . 0.1 1 10 100 P,,~, / mW/cm2 Fig. 8. Open-circuit voltage as a function of incident light intensity. 1.6 -..., . . . . . . . . ,  . . . . . . . . ,  . . . . . . . . ,  t 80K 1.2 - t 260K .- 0.8 - 0.4 - 0.2 ,,'.-.I- 0.1 1 10 100 Fig. 9. Light intensity dependence of the device efficiency in a semi-logarithic representation. This may originate from a weak shifl of the maximum power point of the J-V characteristics at different light intensities, which may be the result of poor conductivity of the absorber materials, as well as a not optimized active layer morphology. 4. Conclusion We found that the device efficiency of polymer- fullerene bulk-heterojunction solar cells with an OC&-PPV:PCBM light absorber shows a strict positive temperature coefficient in the range 80K- 330K independent of the incident light intensity. The transport properties of the respective semiconductors are strongly affected by temperature, resulting in positive slopes of the short- circuit current density and the fill factor. These overcompensate the decrease of the open-circuit voltage towards higher temperatures. However, a limiting factor for the investigated material is the glass transition at approximately T=60"C. Concerning the influence of light intensity we found a nearly linear increase of JSc with Plight, underlining that bimolecular relaxation of charge carriers is of minor importance. Although the fill factor remains almost independent of Plight at temperatures close to 300K and the open-circuit voltage increases monotonically with Plight. the power conversion efficiency reaches the highest value at 3mW/cm2. The loss mechanisms of the material used may be reduced by using conjugated polymers with enhanced transport properties, e.g. a less defect density, higher mobility and by improving the active layer morphology in order to create a larger geometrical interface between the donor and acceptor moieties. Acknowledgment This work was financially supporled by the German Council for Education and Research (Bundesministerium fiir Bildung und Forschung, BMBF) with support codes 01SF0026 and OlSFO119. Further funding by the European Commission (HPRN-CT-2000-00127 RTN) is acknowledged. The authors gratefully thank C.J. Brabec (Siemens AG, Erlangen. Germany) for fruitful discussions. References S.E. Shaheen. R. Radspinner, N. Peyghambarian,G.E. Jabbour, 'Fabrication of bulk heterojunction plastic solar cells by screen printing" Appl Phs. Lett. 79 (2001) pp. 2996- 2998 S.P. Speakman. G.G. Rozenberg. K.J. Clay, W.I. Milne, A. Me, LA. Gardner. E. Bresler. J.H.G. Steinke, 'High perfonance organic semiconducting thin films: Ink jet printed polyihiophene [rr-PJHT]" Og. Necfr. 2 (2001) pp. 65-73 N.S. Sariciftci, L. Smilowitz, A.J. Heeger, F. Wudl. "Photoinduced electron transfer from a conducting polymer to buckminsterfullerene" Science 258 (1992) pp. 1474-1476 G. Yu, J. Gao, J.C. Hummelen. F. Wudl, A.J. Heeger, "Polymer photovoltaic cells: enhanced efficiencies via a network of internal donor- acceptor heterojunctions' Science 270 (1995) pp. 1789-1 791 T. Munters et al., "A comparison between state- of-the-art 'gilch' and 'sulphinyl' synthesized MDMO-PPWPCBM bulk hetero-junction solar cells" Thin Solid Films 403404 (2002) pp. 247- 251 L. Bozano. S.A. Carter, J.C. Scott, G.G. Malliaras. P.J. Brock, " Temperature- and field- dependent electron and hole mobilities in polymer light-emitting diodes" Appl. Phys. Lett. 74 (1999) pp. 1132-1 134 0-7803-7471-1/02/$17.00 02002 IEEE 1325 

Current-Voltage Characteristics of Polymer-Fullerene Solar Cells

https://pure.rug.nl/ws/files/14537626/2002ConfRecPVSCRiedel.pdf

Current-Voltage Characteristics of Polymer-Fullerene Solar Cells

Abstract

Similar works

Full text

Available Versions

ARTS repository - University of Groningen