Assessment of Ruthenium Dye N 719 Adsorption Kinetics in Mesoporous TiO 2 Films of Dye-Sensitized Solar Cells via Nanoplasmonic Sensing

A dyemonolayer formation on a semiconductor surface is critical for efficient dye-sensitized solar cells.(e role of dye is to absorb light and convert it to photoelectrons, which are injected into the semiconductor conduction band as device current.Wemeasured dye N719 adsorption via optical techniques including indirect nanoplasmonic sensing. (e adsorption rate constant of dye N719 in mimic TiO2 photoelectrodes is determined as ka � 983M s. Dye adsorption for ruthenium dyes N3, N749, and Z907, coated onto TiO2 photoelectrodes of varying thicknesses ranging from 3 μm to 10 μm, was conducted and related to fabricated dyesensitized solar cell efficiency. Analytical studies included scanning electron microscopy and ellipsometry, X-ray diffraction, and UV-Vis spectroscopy, as well as quantum efficiency and current-voltage device characterizations. (e results show greatest enhancement of device performance for dye N719 in spite of multilayer formation, which often is underestimated when addressing the dynamic competing factors that reverse thick-film device performance.


Introduction
e photovoltaic research community has focused on optimization of the photovoltaic device structure and material properties to enhance the conversion efficiencies [1].Among the intensively researched photovoltaic device structures, the dye-sensitized solar cell (DSSC) provided an electrochemical research platform for converting light to electricity at large scale [2,3].DCCS main parts include a bandgap semiconductor film, a monolayer of organic dye molecules absorbed onto the semiconductor film, and a liquid electrolyte, which interpenetrates the dye-coated nanoparticles [4].Electrons are injected into the conduction band of the wide bandgap semiconductor film, due to excitation energy introduced by incident photons, and then transferred through the film towards a current collector where they reduce the triiodide of the electrolyte [5].A monolayer and uniform dye coverage by the semiconductor film is critical to improve the light harvesting efficiency.Excess dye loading can lead to multilayer formation, which causes quenching of the photoexcited electrons and leads to a reduction of charge injection [6].On the contrary, poor dye coverage leads to the low photoactive surface area and an increased concentration of electron trap sites.Ono et al. [7] have shown that the agglomeration of dye molecules on titania surfaces causes high charge transfer resistance.e electron diffusion length is limited by a dynamic competition between electron diffusion and lifetime [8].A high electron diffusion coefficient and a low recombination rate constant are key requirements for fabricating highly efficient dye-sensitized solar cells [9].
e impregnation of the dye on the titania films occurs by soaking the matrix in a dye solution for several minutes to hours [11,12].e dye is adsorbed to the surface of titania by carboxylate groups that bind in different anchoring modes [13].In order to fully characterize device performance with respect to dye coverage, it is essential to probe dye concentration throughout the entire film surface.Ellis-Gibbings et al. [14] used depth profiling to determine dye N719 multilayer formation on dye-sensitized solar cell photoelectrodes.Although a nondestructive absorbance technique can allow measurement of dye concentration for thin films, indirect nanoplasmonic sensing enables detecting diffusion at the lower interface of TiO 2 photoelectrodes by using nanoplasmonic gold sensors [15,16].
In this paper, we probe dye N719 diffusion and adsorption kinetics via optical techniques including indirect nanoplasmonic sensing (INPS).Furthermore, we fabricate dye-sensitized solar cells using photoelectrodes of various thicknesses and impregnate them with ruthenium dyes N3, N749, and Z907 as well as with dye N719.We assess multilayer formation of dye N719 based on its adsorption kinetics and performance of fabricated devices in comparison with other dyes.

TiO 2 Photoelectrode
Preparation.Titania films of various thicknesses were pasted using spin coating solutions Tinanoxide T(L)/SC for 700-775 nm mesoporous titania onto nanoplasmonic sensors (mimic photoelectrodes for nanoplasmonic analysis), 3-5 μm mesoporous titania on FTO glass utilizing a spin coater TOP8, and a screen-printing paste of Tinanoxide T/SP for 7-10 μm by the doctor blade method with the scotch tape (photoelectrodes for device fabrication).e thickness of the titania films was measured using Filmetrics F20 thin-film analyzer and VASE Ellipsometer VB-400 (Figure S1, Supporting Information).Anatase phase of titania is confirmed using XRD PANalytical X'Pert PRO (Figure S2, Supporting Information).Device films were fabricated with the same area of 0.384 cm 2 .After the titania is applied, the mimic photoelectrodes were sintered on a hot plate at 100-500 °C, while the device photoelectrodes were sintered at 500 °C, all for 30 min.

Dye Impregnation and Device
Fabrication.Solutions with a 3.0 × 10 −4 M concentration of N3, N749, Z907, and N719 dyes are, respectively, prepared using 1 : 1 vol% acetonitrile/t-butanol mixture.e 3, 5, 7, and 10 μm films prepared are impregnated at times varying from 3 to 60 hours at a film temperature of 55 °C, while the dye is kept at room temperature.Dye uptake is measured by taking sample readings of dye absorbance on solid titania films using UV-Vis Spectrometer Lambda 950 Perkin Elmer following a procedure described elsewhere [17].Devices are constructed following a previous work by Rajab [18] using 60 μm spacers and characterized using a solar simulator IV-16 solar cell I-V measurement system from PV Measurements and QEX7 solar cell spectral response/quantum efficiency/IPCE measurement system from PV Measurements.

Nanoplasmonic Sensing of Dye Impregnation.
Dye coverage is characterized by UV-Vis spectroscopy, and hence, uniform coverage is assessed for any particular film thickness.We fed 3.0 mM of N719 dye via a peristaltic pump of Insplorion XNano into mimic photoelectrodes to monitor the nanoplasmonic peak shifts (Figure 1).We were able to increase the effect of dye multilayer formation by using titania that can be sintered at a low temperature of 100 °C revealing adsorption and desorption processes using a single dye loading in 60-90 minutes, (Figure S3(a), Supporting Information).We then use titania solution of typical sintering temperature at up to 500 °C.e relatively slower adsorption kinetics of N719 dye on thicker films (faster saturation) is seen as lower slope of dye absorbance at 525 nm in Figure S3(b) (Supporting Information).We should mention that typical nanoplasmonic response of dye Z907 adsorption and desorption processes at TiO 2 photoelectrodes using Au nanosensors required Gusak et al. [19] to apply multiple dye loading and rinsing cycles.For dye N719, the absorbance spectra on 10 μm TiO 2 photoelectrodes in Figure 3(b) are slightly higher than those of dye Z907 where their quantum efficiency spectra in Figure 3(c) are comparable.As mesoporous TiO 2 film thickness is increased, dye Z907 device efficiency improved by 24.2% due to 40.2% increase in short-circuit current with 2.9% drop in open-circuit voltage (see (b) in Table 1).Device quantum efficiency of dye Z907 dropped from 40% to 7% at 330 nm and from 50% to 8% at 520 nm (Figures 2(c) and 3(c)).However, dye N719 device efficiency improved 10 folds compared with dye Z907 due to increase in both short-circuit current and open-circuit voltage (see (a) and (b) in Table 1).Device quantum efficiency of dye N719 dropped from 42% to 6% at 330 nm but only from 11% to 8% at 520 nm (Figures 2(c) and 3(c)).e reduction of electron collection efficiency at (330 nm) is indifferent for both dyes Z907 and N719, whereas the reduction at 520 nm is more substantial for dye Z907, though their sensitization capability is similar of up to 750 nm. e proportional increase for dye N719 compared with dye Z907 with the increasing mesoporous surface area is a double effect of the low performance of dye N719 on 3 μm TiO 2 photoelectrode and of dye Z907 on 10 μm TiO 2 photoelectrodes.e latter is attributed to recombination effects resulting from multilayer formation of the bulky dye Z907 and comprised two hydrophobic groups.Gusak et al. used the INPS approach to determine the rate of adsorption of Z907 in similar porous titania films as 1384 M −1 s −1 [20].

Results and Discussion
For dye N719, however, recombination at longer wavelengths in both thin and thick TiO 2 photoelectrodes is likely due to multilayer formation hindering injection kinetics of low energy electrons.By inspection of the similar structure of dye N3, which lacks tetrabutyl ammonium salts, its 10 μm TiO 2 photoelectrode devices yield lowest quantum efficiency and device efficiency of 0.91% due to reduction in both shortcircuit current and open-circuit voltage by 15.4 and 5.6%, respectively, in Figure 3(a)-3(c) and see in (b) Table 1. is shows that multilayer formation is likely indifferent for both dyes N3 and N719 on thick titania films.Gusak et al. [21] reported that dye N3 adsorption rate constant, k a , ranges from 40 to 1000 M −1 s −1 .e partial enhancement of dye N719 is due to the additional two groups of tetrabutyl ammonium salt, which enhances its light absorption.In order to inspect the adsorption kinetics of dye N719, we used INPS to confirm the effect of sintering on multilayer formation and to determine the adsorption kinetics of dye N719.
Typical SEM images of Au sensor nanostructures and the as-coated mesoporous TiO 2 film are shown in Figures S3(c)-S3(d) (Supporting Information).As the mesoporous TiO 2 film is infiltrated with dye N719 solution, a resonance wavelength is used to reflect changes taking place at the surrounding environment of the bottom interface of the TiO 2 photoelectrode.is is referred to as nanoplasmonic peak shift, which plateaus upon saturation confirming dye diffusion to the lower TiO 2 interface.
Sintering of mesoporous films at high temperatures indeed minimizes film porosity and dye multilayer formation (Figure 4(a)), where the nanoplasmonic peak shifts of films sintered at varying temperatures show faster saturation for films sintered at higher temperatures.Dye N719 rate of adsorption is obtained by measuring the initial adsorption slope of N719 dye concentration (per film surface area), where the nanoplasmonic peak shift is inversely proportional to film thickness (Figure 4(b)).Dye N719 rate of adsorption, k a , is determined as 983 M −1 s −1 (Figure 4(c)) confirming similar diffusion kinetics and multilayer formation to dye N3.For enhanced dye diffusion and electron

Conclusion
Ruthenium dye adsorption in mesoporous titania films is characterized using optical techniques by measurement of dye absorbance on TiO 2 photoelectrodes and indirect nanoplasmonic sensing.e kinetics of dye N719 adsorption via indirect nanoplasmonic sensing confirm multilayer formation similar to dye N3 that can be overlooked by the overall enhancement of electron collection efficiency of dye N719 devices.While multilayer formation is dominant for thick-TiO 2 photoelectrode devices, dye N719 device performance is improved due to its tetrabutyl ammonium groups.
e dynamic data obtained via indirect nanoplasmonic sensing allow assessment of dye adsorption

Data Availability
e data used to support the findings of this study are available from the corresponding author upon request.

Figures 2 (
Figures 2(b) and 2(c) show correlation of device quantum efficiency with ruthenium dyes absorption on 3 μm TiO 2 photoelectrodes.Devices with highest dye absorbance on solid titania films show highest short-circuit current and open-circuit voltage, corresponding with 3.72% of device efficiency (Figure 2(a) and see (a) in Table1).Devices with dyes N749 and N3 and dye N719 show similar correlation of dye absorbance on TiO 2 photoelectrodes with short-

Figure 1 :
Figure 1: Nanoplasmonic response shows adsorption upon injection of dye into mesoporous titania on Au sensors followed by desorption upon rinsing with pure solvent.

Figure 2 :Figure 3 :
Figure 2: (a) IV and (c) quantum efficiency characteristic curves of devices fabricated with 3 μm mesoporous TiO 2 films using various ruthenium dyes N3, N749, Z907, and dye N719.(b) Absorbance at dye peaks on solid 3 μm mesoporous TiO 2 films show correlation with device quantum efficiency of respective dyes.Both device quantum efficiency in (b) and absorbance in (c) of dyes N3 and N749 show intersection at 585 nm.