A new nondestructive quantitative method is developed to measure the adsorption of dyes in solid titania films for dye-sensitized solar cells. UV-vis spectroscopy study showed that the absorbance of dye in the solid film can be directly related to the absorbance measured by the typical destructive method used to quantify concentration. Concentrations of N-719 and N-749 dyes on solid titania films were successfully extracted using molar extinction coefficients of dye on solid titania films with value of 6916 and 6454 L·cmˉ
1·molˉ
1 respectively determined using the spectral peaks at 512 and 586 nm.
UV-Vis Spectroscopy Dye Adsorption Titania Solar Cells1. Introduction
Dye-sensitized solar cells (DSSCs) are not limited by the high purities and, consequently, high capital costs associated with silicon-based devices [1] . In fact, DSSCs are promising devices for converting light to electricity at large scale because of their high efficiency, potential low-cost and simple assembly technology [2] [3] . These devices involve a chromophore sensitizer, typically a ruthenium-based dye, that harvests photons. Photons absorbed by the dye are excited to the lowest unoccupied molecular orbital, where an electron can then be injected into the conduction band of a large band gap semiconductor, which is typically titania. A majority of the research work on DSSCs has focused on the use of the photosensitive dyes N-719 [bis(tetrabutylammonium)- cis-di(thiocyanato)-N, NA-bis(4-carboxylato-4A-carboxylic acid-2,2A-bipyridine) ruthenium (II)] and N-749 [(2,2’:6’,2”-terpyridine-4,4’,4”-tricarboxylate) ruthenium (II) tris (tetrabutylammonium) tris (isothiocyanate)].
The impregnation of the dye on the titania films occurs by soaking the matrix in a dye solution for several hours. The dye is adsorbed to the surface of titania by carboxylate groups that bind in different anchoring modes. It is important to obtain uniform dye coverage on titania to ensure enhanced electron transfer and low recombination rates. Excess dye loading can lead to multilayer formation, which causes quenching of the photoexcited electrons and leads to a reduction of charge injection. On the other hand, poor dye coverage leads to low photoactive surface area and an increased concentration of electron trap sites [4] .
Although the dye is critical to the operation of DSSCs, often the dye concentration is not reported or correlated to device performance. The reason for this lack of such valuable information is that the dye concentration is typically obtained by dissolving the dye in a base solution, destroying the cell. The destructive analysis method is simple, but expensive dyes and devices are wasted in the process. In many cases, residual dye amounts remains in the films after completion of the dissolution step of the destructive method, introducing an inherent source of error in determining the concentration or dye coverage. In addition, the molar concentration of dye is also a significant parameter in models that describe the performance of DSSCs [5] [6] . Furthermore, obtaining accurate measurements of dye coverage is of importance for investigating the influence of dye solvents on the performance of DSSCs [7] [8] .
In this paper, a new nondestructive method is developed to calculate the molar extinction coefficients of N-719 and N-749 dyes in titania films, and to quantify the dye concentration on films spanning a range of thicknesses. This technique has multiple benefits, including the possibility of enabling studies to establish a correlation of dye concentration with device performance without having to sacrifice functioning solar cells.
2. Materials and Methods2.1. Materials
A paste containing ~18 wt% nanocrystalline titanium dioxide (Ti Nanoxide T/SP) as well as N-719 and N-749 Ruthenium-based dyes were purchased from Solaronix. The particle size of the titanium dioxide is reported to be 13 nm. Fluorine-doped tin oxide films (FTO) on glass substrates were obtained precut. Acetonitrile and ethanol were purchased from Fisher Scientific. Sodium hydroxide (97%) was purchased from Sigma Aldrich.
2.2. Titania Film Preparation and Dye Impregnation
Titania films of various thicknesses were pasted onto FTO substrates, as described previously [9] . Briefly, a titania paste is used to make 7, 10 and 20 μm thick films (surface area of 0.384 cm2) using a simple doctor blade method. After the titania is pasted onto the FTO, the films are sintered in a tube furnace (Barnstead type 79,300 Thermolyne tube furnace) at a pressure of 5.3 × 10−2 kPa at 450˚C for 30 minutes, and are then annealed at the same temperature on a hot plate until they become transparent. Finally, the films are cooled to room temperature at a controlled rate of 10˚C/min. This method has been shown to prepare defect-free titania films for thicknesses ranging from 7 to 25 μm [9] . Dye-solvent solutions of 0.3 mM were prepared by dissolving N-749 and N-719 dyes in acetonitrile and ethanol, respectively. Titania films were impregnated by soaking in the dye solution for times ranging between 18 to 48 hours.
2.3. Determining the Molar Extinction Coefficient of the Dyes in a NaOH Solution
The liquid extinction coefficient was obtained experimentally. The dyes N-719 and N-749 were dissolved in a mixture of 0.1 M sodium hydroxide and ethanol (1:1 vol%). UV-vis spectra were collected at different dye concentrations for each sample by further dilution with the NaOH solution. The pH values of the solutions were 13.09 and they did not change during dilution.
The absorbance at a spectral peak was plotted as a function of concentration, which yielded straight lines, as expected by Beer’s Law. Applying Beer’s law for the dye solution yields the relationship
where is the absorbance of the dye, εdye is the extinction coefficient of dye, is the path length of the optical cuvette (1 cm), and Cdye is the molar dye concentration in the NaOH solution. The slope of the straight line defined by Equation (1) is the product, from which the extinction coefficient can be readily extracted. The experimental data with their corresponding straight-line fits are shown in Figure 1(a) and Figure 1(b).
Absorbance spectra with their corresponding straight-line fits for determining the molar extinction coefficients in NaOH solutions for (a) N-719 dye and (b) N-749 dye.
2.4. Measurement of Molar Extinction Coefficients in the Solid State
The thickness of titania films on FTO substrates were measured using surface profilometry and Scanning Electron Microscopy. Figure 2 shows the thickness of a titania film of 7 µm using surface profilometry. Figure 3 shows the thickness of a titania film of 20 µm using Scanning Electron Microscopy. UV-vis spectroscopy of the titania films or dye solutions were collected from 350 to 650 nm in a Perkin-Elmer Lambda 9 UV/VIS/NIR spectrometer. The spectra for dyes in the titania films were measured first. The titania films were mounted on an X-Z translational stage (Newport), and multiple measurements (~15) of the initial (unimpregnated) and impregnated titania film were obtained. The spectra of the initial and impregnated titania films were averaged for anal-
Surface Profilometryshows titania film thickness of 7 μm on FTO substrate
Scanning Electron Microscopyshows titania film thickness of 20 μm on FTO substrate
ysis. The titania films were then dissolved in 4 mL of 0.1 M solution of NaOH in ethanol (1:1 vol%) for 30 minutes for spectral analysis. It is worth noting that the spectra used to obtain the molar extinction coefficients were taken from a set of data that showed complete dissolution of the dye, with no residual dye remaining on the substrate.
3. Results and Discussion
Figure 4 shows the absorption spectra for N-719 and N-749 dyes in the NaOH solution and in the solid titania films. The solid line in Figure 4(a) displays the characteristic peaks of the N-719 dye at 375 and 512 nm in an NaOH solution, while the solid line in Figure 4(b) shows the characteristic peaks of the N-749 dye at 397 and 586 nm. Figure 4(a) and Figure 4(b) demonstrate that the spectra for each dye red-shifts once they are adsorbed onto the titania films. For example, the peaks used to determine the molar extinction coefficients of each dye shifted to 525 and 620 nm for N-719 and N-749, respectively. Shifts in peak position can be expected because of the effect of the localized environment on the excited state [10] . Table 1 shows the molar extinction coefficients of each dye in the NaOH solution using the 512 and 586 nm peaks for N-719 and N-749, respectively.
Although the spectra of each dye adsorbed onto the titania has shifted, Beer’s Law can still be used to measure the concentration, provided there are no other optical effects that alter the transmission of light. Figure 5 shows the absorbance for each dye measured in the NaOH solution and in solid titania. The slope of each straight line in Figure 5 yields the absorbance ratio, where the subscripts and s correspond to the liquid NaOH and solid titania film, respectively. This ratio equals ~3 and ~9 for the N-719 and N-749 dyes, respectively. The linearity of the plots indicates that ancillary optical effects are negligible.
Absorbance spectra for (a) N-719 and (b) N-749 dyes in an NaOH solution (solid line, marker “1”) and in solid titania (dashed line, marker “2”).
Absorbance of N-719 (square markers) and N-749 (circle markers) dyes or dissolved in NaOH and adsorbed onto the solid titania film
Measured molar extinction coefficients ε for each dye in an NaOH solution and in a solid titania film. The wavelength λ of the spectral peaks used for calculation of the extinction coefficients are shown
N-719 dye
N-749 dye
λ (nm)
ε (L∙cm−1∙mol−1)
λ (nm)
ε (L∙cm−1∙mol−1)
NaOH solution ()
512
12406
586
6321
titania film (s)
525
6916
620
6454
It is now convenient to rewrite Beer’s Law (1) in the equivalent form
where is number of moles of dye and V is the volume of the medium hosting the dye. In the suite we introduced the subscript in the notation and to denote the absorbance and extinction coefficient of the dye in the liquid NaOH solution. Analogously, we introduce the subscripts to denote the analogous quantities in the solid titania films. It should be noted that both the absorbance and the extinction coefficient are functions of the wavelength. If the dye adsorbed onto the titania film is dissolved completely in the NaOH solution, then the number of moles of dye in the NaOH solution (denoted) must be equal to the number of moles in the solid titania film (). This observation leads to the equalities
where is the thickness of the titania film.
By rearranging Equation (3) and writing, where is the planar surface area of the film and t the film thickness, the following expression for the molar extinction coefficient of the dye adsorbed onto the solid titania films is obtained:
Equation (4) shows that the molar extinction coefficient for the dye adsorbed onto the titania films, , is a function of the constants, , , and, and of the ratio of dye absorbances. Furthermore, Equation (4) is the basis for the new nondestrictuve technique for dye concentration analysis advanced in this work. The quantities bearing the subscript on the right-hand side of the equation can be obtained by carrying out measurements on standard liquid solutions prepared with known dye concentrations in a NaOH sample. The quantities bearing the subscript refer to the solid titania film, and can be measured in a nondestructive fashion.
Equation (4) was then used to determine the molar extinction coefficients of each dye adsorbed onto the titania films, as reported in Table 1. These molar extinction coefficients can be used to calculate the concentration of dye adsorbed onto the titania film. As shown in Figure 6, the molar extinction coefficients obtained using Equation (4) are able to accurately determine the amount of dye adsorbed at a variety of concentrations and film thicknesses.
4. Conclusion
The molar extinction coefficients of both N-719 and N-749 dyes adsorbed onto titania were determined. These
Comparison of the concentration of N-719 (open markers) and N-749 (solid makers) dye determined by measuring the absorbance in the solid state or NaOH solution for titania films ranging in thickness from 7 to 20 μm. The circle markers denote 7 µm, the square markers 10 µm and the triangle markers 20 µm thick films. The dashed line represents equimolar values
molar extinction coefficients can be used to determine the concentration of dye adsorbed in films of varying thickness without destroying the film. This nondestructive technique provides an accurate measurement of the dye adsorbed onto titania. The new technique presented in this work opens up opportunities for future research directions, for example, conducting studies that seek to relate dye concentration with internal quantum efficiency of DSSCs without destroying the devices.
Acknowledgements
The author would like to acknowledge the support of the Ministry of Higher Education, Kingdom of Saudi Arabia for this research through a grant (PCSED-004-11) under the Promising Center for Sensors and Electronic Devices (PCSED) and a grant (NU 54/12) under the deanship of scientific research at Najran University, Kingdom of Saudi Arabia. The author acknowledges insights provided by Prof. K.J. Ziegler at University of Florida, and funding received from the National Science Foundation. Doctor blades were donated by the Incision Tech Company.
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