Accelerated aging test for carbon composite counter electrodes based dye sensitized solar cells

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    ACCELERATED AGING TEST FOR CARBON COMPOSITE COUNTER

    ELECTRODES BASED DYE SENSITIZED SOLAR CELLS

    Authors: Syed Ghufran Hashmi, Janne Halme and Peter Lund

    Email: [email protected]

    New Energy Technologies Group, Department of Applied Physics, Aalto University, P.O. BOX15100, FI-00076 Aalto (Espoo), Finland

    ABSTRACT: We report here an accelerated aging test for carbon composite catalyst layer based

    dye sensitized solar cells (DSSCs) that was performed under artificial light intensity (1000W/m

    2) equivalent to 1 Sun and at 60 C for 1000 hours in the presence of significant fraction of

    UV light intensity. The performance of the reference DSSCs with thermally platinized counter

    electrodes degraded almost completely due to severe electrolyte bleaching, which is an expected

    result of UV light induced degradation of DSSCs. The performance loss was also accompaniedby an increase in the counter electrode charge transfer resistance (RCT). However, DSSCs with

    counter electrodes based on carbon composite catalyst layers exhibited markedly more stable

    photovoltaic performance, showed no visible bleaching of the electrolyte, and their catalyticactivity even improved with a gradual decrement in RCT (from 6 cm

    2to 2.6 cm

    2). The

    efficiency of the carbon composite based DSSCs was reduced by 35% from the initial efficiency

    due to a slight degradation in N719 dye and the corrosion at the silver contacts which caused a

    small increase in the total cell resistance in both types of DSSCs. The resistance of these carboncomposites counter electrode based DSSCs against UV light may potentially reduce the overall

    manufacturing cost by partially or completely relaxing the need for UV filters in complete DSSC

    assembly, but this hypothesis as well as the physical and chemical origin for the effect should beinvestigated and verified by further studies.

    Keywords: Dye sensitized solar cells, stability, carbon composites and counter electrodes.

    1. INTRODUCTIONDye sensitized solar cells (DSSCs) propose

    variety of cheap materials to be tested in

    different combinations[1]

    . However, longterm operation of these inexpensive

    materials in the cell is critical for the reliable

    commercialization of DSSCs[2]

    . The

    composites of carbon have been tested as analternative to replace the expensive platinum

    (Pt) catalyst layer in several studies

    [3-7]

    .Nevertheless accelerated aging tests for

    these composites are rarely reported[8, 9]

    andmore precisely, their long term

    electrochemical impedance performance is

    mostly missing in the literature. In thiscontribution, we present an accelerated

    aging test that was performed under artificial

    light intensity (1000 W/m2) equivalent to 1

    Sun and at 60 C to see the potential of

    carbon composites catalyst layers to beimplemented in the durable DSSCs. The

    illumination of the solar cells in the aging

    test included also significant UV light

    component, which is known to be significantaging factor of DSSCs. The performance of

    these carbon catalyst layers in an acceleratedaging test was evaluated in terms of

    photovoltaic parameters (IV),electrochemical impedance spectroscopy

    (EIS measurements) and incident photon to

    collected electron efficiency (IPCE) andcompared with reference thermally

    platinized counter electrodes (TPCE).

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    ethanol and acetone solutions (5 min each).

    All the substrates were dried via compressed

    air before placing them in a UV-O3Chamber (Bio-force nano sciences UV

    Ozone Pro Cleaner, 20 minutes) for further

    cleaning. After UV-O3 cleaning step, thesubstrates were immersed into a 40 mMTiCl4 solution container box and placed for

    30 minutes in a preheated oven at 70 C.

    After that the substrates were again washedwith deionized water (DIW) and ethanol

    solution sequentially and dried with

    compressed air. Sequential screen printing

    steps of commercial nano crystalline TiO2paste (18NR-T Dyesol) and TiO2 scattering

    paste (WER2-0 Dyesol) were performed to

    get 9-10 m and 2-4 m thick filmsrespectively with mesh T-61. Each layer was

    dried at 110C for 5-10 minutes after the

    deposition. The TiO2 printed layers were

    then sintered at 500 C for 30 minutes andwere cooled down to room temperature in

    the oven. After sintering the TiCl4treatment

    step was again performed (with abovementioned sequence till the drying with

    compressed air) and the substrates were re-

    sintered at 500 C (for 30 minutes) and were

    again cooled down to room temperature tocomplete the process. These TiCl4 treated

    substrates were sensitized in the 0.32 mM

    cis bis (isothiocyanato) bis (2, 20-bipyridyl-4, 40-dicarboxylato)-ruthenium (II) bis

    tetrabutyl ammonium (N-719, Solaronix)

    and ethanol (99.5 wt %) solution for 16hours before the cell assembly.

    2.2.3 Cell assembly

    Both PE and CE were assembled in

    sandwich type fashion by separating them

    through a 50 m thick Bynel foil (Dupont).

    The (I/I3) redox based electrolyte (HSE-Dyesol) was injected into the cell channel

    via drilled holes at PE side. Finally these

    cell holes were sealed with a 25 m thickBynel foil (Dupont) and a thin glass cover

    piece. The cell contacts were made by

    applying the conductive copper tape and

    spreading silver ink at the in-active area ofthe cell. The contacts were then protected

    with a slow drying epoxy. All the cells were

    soaked for 1 day in 1 Sun light intensity(1000W/m2) for initial stabilization before

    the initial measurements.

    3. RESULTS AND DISCUSSIONS

    3.1 Initial photovoltaic performance

    Table 1 represents the initial photovoltaicperformance of both thermally platinized

    counter electrodes (TPCE) and carbon

    composite counter electrodes (CCE) basedDSSCs. The sample to sample variations are

    presented in the form of standard deviation

    for each type of DSSCs (Table 1). Both

    types of DSSCs exhibited almost equalefficiencies (Avg ~ 6.5%) however, the

    TPCE based DSSCs showed ~ 8% higher

    currents (JSC), 3% higher fill factor (FF) and~ 20% lower cell resistance (RCELL).

    Nevertheless the CCE based DSSCs

    exhibited 8% higher open circuit voltage

    (VOC

    ). Additionally the high fill factors ineach type of DSSCs suggest good adhesion

    of catalyst layers over the substrates.

    Table 1:Initial photovoltaic performance of

    4-5 cells of each type of DSSC along with

    their standard deviations.

    Cell type*JSC

    (mA/cm2)

    VOC

    (mV)

    FF

    (%)

    (%)

    RCELL

    (cm2)

    GPEGTPCE15.6 0.2 690 4 61 2 6.6 0.2 11 0.8

    GPEGCCE 14.4 0.4 750 14 59 1 6.3 0.2 14 0.4

    * GPEGPTCE = Glass photo electrode

    Glass thermal platinum counter electrode.GPEGCCE= Glass photo electrode Glass

    carbon composite counter electrode.

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    3.2 Initial electrochemical impedance

    response

    Figure 1:Typical EIS spectra of each type

    (*GPEGTPCE and **GPEGCCCE) DSSCs

    used in this study. a) Nyquist plot, as b)imaginary impedance Z as a function of

    frequency f. *GPEGTPCE = Glass photo

    electrode Glass thermally platinized

    counter electrode. **GPE GCCE = Glassphoto electrode Glass carbon composite

    counter electrode.

    The initial measurement results regarding

    electrochemical impedance response of each

    type of DSSCs are summarized in Table 2.

    These measurements were performed atopen circuit voltage and in the solar

    simulator with same light intensity (1000

    W/m2) as was used for measuring the

    photovoltaic parameters. The measured

    frequency range was from 100 mHz to 100kHz. In this frequency range, the traditional

    TPCE exhibits three semi circles[10, 11]

    (Figure 1a). Each semicircle can bedistinguished according to its unique peakposition (Figure 1b). The first semicircle for

    TPCE is associated with charge transfer

    resistance (RCT) which appears at very highfrequency (> 1 kHz) range

    [10, 11] (Figure

    1b). Additionally the second adjacent

    semicircle corresponds to the recombination

    resistance of the photo electrode (RPE) andits characteristic frequency appeared around

    20-30 Hz[10]

    (Figure 1b). The third small

    semicircle that appeared at very lowfrequency (~ 1 Hz, Figure 1a-b) is

    associated with the diffusion resistance (RD)

    of the cell[10, 11]

    .

    The case is different for CCE in which a

    large semi-circle results from the

    overlapping of RCT and RPE responses atlower frequency (10-20 Hz, Figure 1b)

    range. Hence it is difficult to estimate the

    exact value of RCTfor CCE. One possibility

    is to subtract the RPE

    value of TPCE basedDSSC since the same photo-electrode

    geometry was employed in fabrication of the

    each type of DSSCs[12, 13]

    . Based upon thisassumption, the RCT values of CCE are

    calculated and presented in Table 2. In

    addition to that one small semicircleadjacent to the large semicircle (Figure 1a)

    can be seen in the CCE spectrum which

    appears at very high frequency (~10 kHz,

    Figure 1b) and is distinguished as in-porediffusion resistance (RPORE) or contact

    resistance [13, 14]. The value of RPORE was

    added in the RCTvalues to calculate the total

    charge transfer resistance (RCT-TOTAL) ofCCE

    [12, 15]. Table 2 summarizes the EIS

    parameters of each type of DSSCs.

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    The main conclusion that can be drawn from

    initial EIS performance is; almost equal

    series resistance (AvgRS= 4.6 0.4 cm2)

    for each type of DSSCs due to the sameFTO Glass substrate (RSHEET = 15 /)

    however, the TPCE exhibited lowerR

    CT(2.2 0.5 cm2) than CCE (6.0 0.2 cm

    2).

    Table 2: Initial average values of 4-5 cells

    of each type along with their standarddeviations representing electrochemical

    impedance performances.Cell type* *GPEGPTCE **GPEGCCE

    RS(cm2) 4.7 0.6 4.5 0.2

    RCT (cm ) 2.2 0.5 5.2 0.5

    RREC(cm ) 2.7 0.4

    RPORE (cm2) 0.8 0.2

    RREC+RCT(cm ) 7.9 0.5RCT-TOTAL(cm ) 6.0 0.2

    * GPEGPTCE = Glass photo electrode Glass thermally platinized counter electrode.

    ** GPE GCCE = Glass photo electrode

    Glass carbon composite counter electrode.

    3.3 Photovoltaic performance of DSSCs

    with accelerated aging

    Figure 2 represents the short circuit current

    density (J

    SC), open circuit voltage (V

    OC), fillfactor (FF) and overall efficiency ()recorded for each type of DSSC during this

    study (from 0 h to 1000 h). During the entire

    period of study, both types of DSSCexhibited different trends compared to each

    other. During the whole study, JSCof TPCE

    based DSSCs was continuously decreased

    (Figure 2a) due to the bleaching of theelectrolyte (Figure 3 b-c). The bleaching of

    the electrolyte solution is well known

    problem in traditional TPCE based DSSCswhen exposed to real or artificial sunlightand is mainly associated with loss of tri-

    iodide ion in the electrolyte solution[16-20]

    .

    This loss of tri-iodide ion has further beenassociated with a reaction between UV light

    and the electrolyte solution that generates an

    irreversible reaction for iodine[21, 22]

    unless a

    UV blocking filter is used to prevent the

    reaction. Since in this work no UV blocking

    filter was employed we assume the

    aforementioned cause is responsible for theloss of tri-iodide ions here as well. Figure 4

    shows the photon flux spectrum of the lampsused in the light soaking system (Philips13117), confirming the presence of UV light

    (below 400 nm).

    Surprisingly, no visible bleaching of

    electrolyte occurred in CCE based DSSCs

    and theJSCvalues were only fractionally (~

    8%, Figure 2 a) decreased from the initialvalue. It should be noted again that in each

    type of DSSCs, the same photo electrode

    and electrolyte composition was used andthe only difference was in the catalyst layer

    i.e. thermal platinum and carbon composite.

    This raises a hypothesis that the irreversible

    reaction between the electrolyte and UVlight was minimized or stopped by the

    carbon composite.

    In addition to that, a continuous drop in

    open circuit voltage (VOC) for CCE based

    DSSCs was observed whereas it was

    recovered up to 90% in case of TPCE basedDSSCs (Figure 2b). The drop in open circuit

    voltage is mainly associated with the

    resistance of photo electrode (RPE) which isinvestigated and further discussed in section

    3.4. Nevertheless, over the whole 1000 h

    period, the voltage decreased by 13% and7% in case of CCE and TPCE based DSSCs

    respectively (Figure 2b).

    Also the FF did not remain stable butdecreased by 11% in case of TPCEs and

    19% for CCE based DSSCs (Figure 2 c).

    These drops in FFs are resulted due to an

    increase in total cell resistance (RCELL 74%increase for TPCE and 26% increase for

    CCE based DSSCs) of the cells (Figure 5 a).

    The RCELLdepends upon various factors forinstance charge transfer resistance at counter

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    electrode (RCT), ideality factor of photo

    electrode, contact resistance of the contacts,

    sheet resistance (RSH) of the substrates and

    electrolyte diffusion. These parameters areinvestigated in detail in section 3.4. Due to

    the decrease inFF

    andV

    OC, the efficiency ofCCE based DSSCs was reduced from 6.3 0.2% to 4.1 0.2 (i.e. by 35 %) whereas the

    efficiency of the TPCE based cells dropped

    linearly by 85% mainly due to the UVinduced, electrolyte bleaching reaction

    (Figure 2 d).

    Figure 2:Photovoltaic parameters of *GPE GTPCE (red squares) and **GPE GCCE

    (black circles) cells. a) Short circuit current

    density (JSC) (b) Open circuit voltage (VOC)

    (c) Fill factor (FF) and (d) Efficiency () of

    the cells. *GPE GTPCE = Glass photoelectrode Glass thermally platinized

    counter electrode. **GPE

    GCCE = GlassPhotoelectrode Glass carbon compositecounter electrodes.

    Figure 3: Bleaching of the electrolyte in

    *TPCEs based DSSCs was observed duringthe entire period. a) Fresh electrolyte with

    dark yellow color. b) Semi bleached

    electrolyte losing yellow color. c)

    Completely colorless/bleached electrolyte.* Thermally platinized counter electrodes.

    Figure 4: Spectrum of lamps used in the

    light soaking system.

    3.4 Electrochemical performance of

    DSSCs with accelerated aging

    Some of the critical factors which determinethe performance of counter electrodes are

    also investigated with electrochemical

    impedance spectroscopy (EIS). Theseparameters are presented in Figure 5 b-d. As

    discussed in earlier section, both types of

    DSSCs exhibited almost equal initial seriesresistance (RS). However, the TPCE based

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    - visible bleaching, the carbon composite

    counter electrodes exhibited improving

    catalytic performance: their RCT gradually

    decreased (down to 58%) throughout thestudy (Figure 5 c).

    In addition to that, gradual increase in theresistance of photo electrode (RPE) has also

    been observed (Figure 5 d). This confirms

    the reason for the degradation in the opencircuit voltage (VOC) that was discussed in

    section 3.2). The possible factor of these

    deviations in the RPEcan be the degradation

    in the photo electrode. This hypothesis wasfurther studied with incident photon to

    collected electron efficiency (IPCE)

    measurements and discussed in the nextsection.

    3.5 Incident photon to collected electron

    efficiency (IPCE) of DSSCs.

    Figure 6:Average IPCE spectra of *TPCE

    and *CCE based DSSCs. *Thermally

    platinized counter electrodes. **Carbon

    composite counter electrode.

    The in-situ IPCE measurements of TPCE

    and CCE based DSSCs was also performed

    to investigate the possibility of degradationin N719 dye used in this work. The initial

    and final average IPCE spectra of CCE

    based DSSCs are presented in Figure 6whereas it was not possible to present the

    final IPCE spectrum of TPCE based DSSCs

    due to the complete bleaching of the

    electrolyte as shown in Figure 3 b-c.

    However an idea can be obtained from the

    initial IPCE spectrum of TPCE basedDSSCs since the same photo electrodegeometry was used in each type of DSSCs.

    Both types of DSSCs revealed almost equal

    (~ 72 - 74%) initial peak IPCE valueshowever these efficiencies were reduced to

    ~ 65% confirming degradation in photo

    electrodes. The possible hypothesis can

    either be desorption of N719 dye moleculeswhich has been observed at high (60-80 C)

    temperatures[2, 27]

    or penetration of water

    inside the cell. Here the aging wasperformed at 60 C and 20% humidity and

    N719 dye is known to be hydrophilic dye[2]

    .

    3.6 Short comparison of thermally platinizedcounter electrodes and carbon composite

    counter electrodes based DSSCs.

    An interesting comparison between TPCE

    and CCE based DSSCs has been obtained at

    the end of the study. The reference TPCEbased DSSC exhibited higher initial

    performance in terms of ~ 8% higher JSC,3% higher FF, ~ 5% higher efficiency and270% lower RCT than CCEs based DSSCs.

    However in the accelerated aging test, TPCE

    based DSSCs were unable to maintain theabove mentioned performance and their

    efficiency dropped below that of CCE based

    cells due to almost complete failure via

    electrolyte bleaching. Despite of lowerinitial performance, the CCE based DSSCs

    were able to retain ~ 92% of initial JSC, 87%

    VOC, 81% FFand 65% overall efficiency andthus showed clear superiority over TPCEbased DSSCs in this aging experiment.

    Interestingly, the RCT also was remarkably

    decreased from 6 0.2 cm2 to 2.6 0.1

    cm2.

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    The key observation of this study was the

    absence of electrolyte bleaching in the CCE

    based DSSCs under halogen lamp light

    without a UV filter. At the same time,equally prepared but TPCE based DSSCs

    degraded due to complete loss of tri-iodide.It is also noteworthy that the CCE showedstable catalytic performance. In fact, their

    RCTwas significantly reduced from its initial

    value which means no degradation at thesecounter electrodes. The study raises

    interesting questions such as why bleaching

    did not occur in CCE based DSSCs. It is

    important to verify and investigate it withmore sophisticated techniques such as

    camera imaging[16]

    , limiting current density

    analysis

    [28]

    and selective application of UVfilters. The degradation at the photo

    electrode was established here through IPCE

    measurement; however, more sophisticated

    setup for instance Raman Spectroscopy[2]

    orIR spectroscopy

    [2]is suggested for a future

    study.

    4. CONCLUSIONS

    Stability of carbon composite based catalystlayers was tested under artificial light

    intensity (1000 W/m2) equivalent to 1 Sun at60 C. The efficiency of these carboncomposite based dye sensitized solar cells

    were only reduced by 35% from the initial

    efficiency compared to the referencethermally platinized counter electrodes

    based DSSCs which completely degraded

    due to severe bleaching of the electrolyte.

    On the other hand, no bleaching of theelectrolyte occurred in carbon composite

    counter electrode based DSSCs. The

    catalytic activity of the carbon compositecounter electrodes was also improved with agradual decrement in their charge transfer

    resistance (from 6 0.2 cm2

    to 2.6 0.1

    cm2). Moreover, the critical reasons for

    35% reduction of efficiency in CCE based

    DSSCs was not the carbon composite

    counter electrodes themselves but a slight

    degradation in the N719 dye at the

    photoelectrode and the corrosion at the

    silver contacts which occurred in both types

    of DSSCs. These results speak for theviability of inexpensive carbon composite as

    an alternative to expensive platinum catalystlayer for stable high performance dyesensitized solar cells.

    5. ACKNOWLEDGEMENT

    Ghufran Hashmi thanks Fortum Foundation

    and Tekniikan edistmissti (Finnish

    Foundation for Technology Promotion) fortravel grants.

    6. REFERENCES

    [1] G. Hashmi, K. Miettunen, T. Peltola, J.

    Halme, I. Asghar, K. Aitola, M. Toivola,and P. Lund, Renew. Sust. Energ. Rev 15

    (2011) 3717-3732.

    [2] M. I. Asghar, K. Miettunen, J. Halme, P.

    Vahermaa, M. Toivola, K. Aitola, Energy

    Environ Sci 3(2010) 418-426.

    [3] Y. Jo, J. Y. Cheon, J. Yu, H. Y. Jeong,

    C. H. Han, Y. Jun, S. H. Joo, Chem.Commun 48(2012) 8057-8059.

    [4] S. J Thompson, J. M. Pringle, X. L.

    Zhang, Y. B. Cheng,J. Phys. D: Appl. Phys46 (2013) 024007.

    [5] D. Y. Kim, J. Kim, J. Kim, A. Y. Kim,

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    [6] X. Miao, K. Pan, Q. Pan, W. Zhou, L.Wang, Y. Liao, G. Tian, G. Wang,Electrochimica Acta96(2013) 155-163.

    [7] C. T. Hsieh, B. H. Yang, W. Y. Chen,Int. J. Photo. Energ, (2012)

    doi:10.1155/2012/709581

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