Functional Devices for Clean Energy and Advanced Sensor Applications
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Theoretical Studies of Electronic Structure and Photophysical Properties of a Series of Indoline Dyes with Triphenylamine Ligand
Abstract
To design efficient organic sensitizer, a series of DπA indoline dyes with different donor parts have been investigated by density functional theory (DFT) and timedependent DFT (TDDFT) approach. The molecular geometries, frontier molecular orbitals, and absorption spectra of these dyes have been systematically investigated to provide comprehensive understanding of the structureproperty relationships. Compared with D149, our designed dyes have proper HOMO and LUMO energy level, narrowed HOMOLUMO energy gap, and broadened absorption band by introducing the N(CH_{3})_{2} and N(phenyl)_{2} groups at the donor part. Furthermore, the dimeric dyes and dye(TiO_{2})_{6} systems have been optimized by DFT method to simulate the intermolecular interactions, as well as interaction between the dyes dimmers and semiconductor interface, respectively. Through the analyses of absorption energies (), energy levels of the HOMO and LUMO, light harvesting efficiency (LHE), and the driving force of electrons injections (), it is found that the designed dyes should have improved optical properties by importing the N(CH_{3})_{2} group. This work is hoped to provide a theoretical guiding role in design of new dyes for dyesensitized solar cells.
1. Introduction
Due to increasing energy demands and concerning global warming, scientists have paid tremendous effort on developing cheap and easily accessible renewable energy sources. Dyesensitized solar cells (DSSCs) have been regarded as one of the most promising nextgeneration photovoltaic cells due to their potentially low fabrication costs, easy production, and flexibility compared to traditional siliconbased solar cells [1]. A typical DSSC is constructed with the dye sensitizer, dyeabsorbed nanocrystalline semiconductor oxide (such as TiO_{2} or ZnO), electrolyte containing redox couples, and closed circuit. Obviously, the sensitizer plays a significant role for improving the efficiency of DSSCs. Therefore, considerable synthetic works have been carried out on Rubased sensitizers [2–4] and metalfree organic dye sensitizers [5–10]. Among them, indoline dye sensitizers [11] have attracted much attention because of their high molar extinction coefficient, relatively less expensive, and low pollution of environmental. Although the significant progress has been made in the organic dyes, the conversion efficiency of indoline type dyes is still lower than the Rubased sensitizer [12]. Therefore, the investigation on the organic dye is very important for realizing largescale commercial production.
Except the massive synthesized research, theoretical studies have been accepted as extremely powerful and comparably lowcost tools for revealing the effect of chemical modifications on the optical properties [13–18]. In spite of outstanding electronic and optical properties of triphenylamine derivatives in solar cell [19–22], to our knowledge, there is no detailed study on indolinecontaining materials coupled with triphenylamine as donor part. Consequently, in order to reveal the role of triphenylamine on the photophysical properties and develop more efficient dyes, the donor part of D149 dye is replaced by triphenylamine unit. Then, triphenylaminecontaining indoline dyes are designed by introducing the N(CH_{3})_{2}, N(phenyl)_{2}, and CF_{3} at the donor part of D149 in this work (see Figure 1). A systematic comparison and analysis of the geometries, frontier molecular orbitals, and absorption spectra of these dyes are carried out. Furthermore, the light harvesting efficiency (LHE) and the driving force of electrons injections () are calculated to estimate the shortcircuit photocurrent density. In addition, the electron coupling of dimeric dyes and dye(TiO_{2})_{6} systems is simulated by DFT method to testify the electron injection efficiency. This work is expected to reveal the effect of chemical modification on the DSSCs efficiency and provide valuable guidance for developing efficiency dyes.
2. Computational Details
All calculations were performed with the Gaussian 09 program package [23]. The density functional theory DFT (B3LYP) approach had been successfully used to calculate the ground geometries in indoline dye sensitizers [13–15, 24]. Therefore, in this work, the geometries structures of monomer and dimer dyes were fully optimized at the DFT level of B3LYP method [25, 26] using the 631G(d) basis set. Following the optimized geometry, the vibrational frequencies were calculated and the results confirmed that all the optimized monomer geometries were stable geometric structures. The absorption spectra of these dyes were investigated by TDDFT with the B3LYP approach associated with the polarized continuum model (PCM) [27, 28] in methanol media.
To investigate the electronic coupling interaction between these dyes and TiO_{2} nanoparticles, the absorption geometries of dyes/(TiO_{2})_{6} clusters were calculated by B3LYP method. The 631G(d) basis sets were used for C, H, O, N, S, and F atoms and LANL2DZ for Ti atom. Although (TiO_{2})_{6} cluster is a simplistic model, it was believed to qualitatively reproduce the trend of the charge distribution [29]. The absorption energies () of dyes/(TiO_{2})_{6} were calculated by the following equation:
The , , and were the total energies of dyes, (TiO_{2})_{6} cluster, and dye/(TiO_{2})_{6}, respectively.
The shortcircuit current density () which is closely connected to the energy conversion efficiency () of the solar cell [30] can be determined by the following equation [31]: where is the lightharvesting efficiency at a given wavelength [31], is the electron injection efficiency to the semiconductor substrate, and is the electron collection efficiency. can be assumed as a constant in the same DSSCs with sole different dyes [32]. As a result, the enhancement of should focus on improving the and . The is related to the driving force for the electron injection. According to Preat’s method [33], the of electron injections from the excited states of dyes to semiconductor surface are calculated.
The lightharvesting efficiency can be calculated withwhere is the oscillator strength of the maximum absorption spectra of dyes.
3. The Molecular Geometries of Dyes
The sketch map and the optimized geometries of D149 and D1–D4 are shown in Figures 1 and 2, respectively. The triphenylamine moiety, indoline and rhodanine group, and CH_{2}COOH act as an electron donor (D), electron conductor (), and acceptor (A), respectively. As shown in Figure 2, the dihedral angle of C_{4}C_{3}N_{2}C_{2} for D149 is 25.26°. D2 and D3 have steric obstruction conformation by gradually adding the N(phenyl)_{2} groups in D1. For example, the dihedral angle of C_{4}C_{3}N_{2}C_{2} for D1–D3 is calculated to be 29.3°, 32.4°, and 37.1°, respectively. Note that the dihedral angle of C_{4}C_{3}N_{2}C_{2} increases from 37.1° (D3) to 43.3° (D4) by introducing the CF_{3} group at the end of triphenylamine. Obviously, the steric obstruction can be justified by proper functional group and thus avoids the unfavorable dye aggregation on the TiO_{2} surface. Besides the dihedral angle of C_{4}C_{3}N_{2}C_{2}, the bond length C_{1}–N_{1} between the D and part increases in the following order: D4 (1.408 Å) < D3 (1.412 Å) < D2 (1.413 Å) < D1 (1.416 Å),indicating the bond conjugation ability decreases in the same order. This can be explained by the NBO charges on the C_{1} and N_{1} atoms. The NBO charges on N_{1} atom of D2–D4 are similar with D1. But for atom, it decreases dramatically in the following order: D4 (0.148e) > D3 (0.133e) > D2 (0.127e) > D1 (0.117e), suggesting the bond conjugation ability has been enhanced by introducing N(phenyl)_{2} and CF_{3} substitutions.
3.1. Frontier Molecular Orbital Analysis
The energy levels of the HOMO and LUMO, as well as the HOMOLUMO gaps, are drawn in Figure 3, together with the energy levels of TiO_{2} semiconductor conduction band (−4.00 eV) [34] and the redox potential of (−4.80 eV) [35].
As drawn in Figure 3, the HOMO and LUMO energy levels of D1–D3 increase remarkably (−4.39 eV and −2.17 eV for D1, −4.53 eV and −2.24 eV for D2, and −4.63 eV and −2.29 eV for D3) compared with D149 obtained by us (−5.07 eV and −2.36 eV) and previous work [24] (−5.009 eV and −2.408 eV), which means that the energy level of molecular orbital can be greatly changed by introduction of triphenylamine into the donor part. Although the introduction of triphenylamine unit increases the HOMO values relative to D149, the HOMO level of D1–D3 still approaches the redox potential of (−4.80 eV). The HOMO level of D4 (−5.11 eV) decreases dramatically by importing the CF_{3} group at the end of the triphenylamine group, which is lower by 0.31 eV than redox potential. This means that the studied dyes ensure efficient dye regeneration. In addition, the LUMO energy of D1–D4 is higher than the conduction band edge of TiO_{2}, which would provide enough driving force for electron injection for ultrafast excitedstate electron injection [36]. Thus, it is a good approach to enhance the ability of dye regeneration by introducing the N(CH_{3})_{2} and N(phenyl)_{2} substitutions at the donor part, especially for CF_{3} group. With the dramatically stabilized HOMO energy, the HOMOLUMO energy gap of these dyes increases in the following order: D1 (2.22 eV) < D2 (2.28 eV) < D3 (2.34 eV) < D4 (2.66 eV). The energy gaps of our designed dyes D1–D3 are much smaller than the famous D149. As reported by previous work [37, 38], the sensitizers that have smaller energy gap values may show higher efficiency in the DSSCs. Thus, it can be inferred that our designed molecules may have improved light harvesting ability.
As drawn in Figure 3, the electron densities of the HOMO of D149 is mainly located on the donor part and indoline ring; the electron densities of its LUMO are mainly distributed around the group. It suggests that the HOMO to LUMO transition is a good charge separated state. The electron distributions of the HOMOs and LUMOs for D1–D4 have the similar features. Both the HOMOs and LUMOs of D1–D4 possess and orbital delocalization. Therefore, it can be confirmed that the intramolecular charge transfer (ICT) may occur when electron excitation occurs from the HOMO to LUMO in these dyes.
3.2. The Absorption Spectra
On the basis of the optimized ground state geometries, the absorption spectra of dyes are calculated by TDDFT/B3LYP method with PCM in methanol media. The simulated electronic absorption spectra are depicted in Figure 4, and the corresponding absorption data are collected in Table 1.

Figure 4 shows the absorption spectrum of D1–D3 displaying three major absorption bands in their UV/Vis spectra, the lowest energy absorption band (in the region of 600.0–800.0 nm), lower energy absorption band (in the region of 450.0 to 600.0 nm), and higher energy absorption band (in the region of 300.0 to 450.0 nm). Compared with D1–D3, the absorption spectra of D4 are different in the band locations and intensity, due to importing the electronwithdrawing CF_{3} groups. From Figure 4 and Table 1, the lowest lying distinguishable absorption speak () of these dyes exhibits dramatically blue shift tendency: D1 (735.1 nm) > D2 (693.5 nm) > D3 (661.5 nm) > D4 (600.2 nm) > D149 (556.1 nm), which is closely related to the increased HOMOLUMO energy gaps of these compounds (see Figure 3). Based on the analysis of electron density of HOMO and LUMO (see Section 3.2), all of the absorption behaviors of the can be ascribed to the intramolecular charge transfer (ICT) character. The maximum absorption speak of D1 and D2 is located at 517.5 and 518.7 nm, respectively, which is contributed by HOMO1 LUMO transition. The HOMO1 of D1 and D2 is contributed by 23.1% (D) + 76.8% () and 53.4% (D) + 42.6% (), respectively. Thus it is reasonable to assign the 517.5 and 518.7 nm for D1 and D2 to ICT character. For D3, the absorption speak with the largest oscillator strength is located at 515.7 nm, which is contributed by HOMO2 LUMO transition. The HOMO2 of D3 is focused on 99.9% (D); therefore, the 515.7 nm of D3 still displays ICT character. With respect to D4, the absorption at 491.5 (attributed by HOMO1 LUMO) and 371.3 nm (attributed by HOMO LUMO+4) are assigned to ICT character. The highenergy absorption speak for D1–D4 is located at 398.5, 362.2, 365.6, and 346.6 nm, respectively, which is ascribed to 19.9% (D) + 79.4% () 98.2% (), 85.1% (D) + 14.5% () 20.8% (D) + 57.9% () + 21.3% (A), 86.9% (D) + 13.1% () 77.1% (D) + 21.2% (), and 58.7% (D) + 41.1% () 83.2% (D) + 16.4% () transitions with the ICT character.
From the above calculations, it can be seen that all the absorption speaks of D1–D4 are covering the entire visible region, which makes these dyes suitable for the application of DSSCs. The location and intensity of the absorption band of these dyes are greatly affected by introducing the N(CH_{3})_{2}, N(phenyl)_{2}, and CF_{3} groups, which means the photophysical properties can be well tuned by proper substitutions. All the intense absorption bands of D1–D4 correspond to the ICT transition, which will play an important role in conversion efficiencies.
3.3. Photoelectric Conversion Efficiency of Dyes
Rapid electron injection from the photoinduced excited states of dyes to the TiO_{2} is desired for high performance of DSSCs. According to Preat’s method [33], the driving force of electrons injections from the excited states of dyes to semiconductor surface is calculated and the results are drawn in Figure 5.
Figure 5 shows that all the values are very negative (in the region of −1.55–−1.86 eV), which suggests that the dye excited state lies above the TiO_{2} conduction band edge. Therefore, it is favorable for electron injection from the excited state dye to the TiO_{2} conduction band edge. Compared with D149 (−1.08 eV), D1–D4 have much more negative values. As expected, the electron injection ability has been improved by replacing the donor part of D149 by triphenylamine. Furthermore, the values of D2 and D3 are −1.74 eV and 1.66 eV, respectively, which are much more positive than D1 (−1.86 eV), indicating that the introduction of diphenylamine at the end of triphenylamine unit results in destabilization of the oxidized dye and therefore reduces the electron injection. In addition, value of D4 (−1.55 eV) is positive than that of D3, indicating it would not be favorable to enhance the electron injection by importing the CF_{3} group at the end of phenylamine. According to (3) in Section 2, the of studied complexes are calculated and the results are also drawn in Figure 5. As depicted in Figure 5, the D1 has larger than D2–D4, which means that D1 has more efficient light harvesting capability than others. As discussed in Section 2, the large values of and are possible approaches to maximize the shortcircuit (). Consequently, it is a promising approach to enhance the efficiency by introducing the N(CH_{3})_{2} group at the donor part.
3.4. Structures and Properties of Dye Dimers
The intermolecular interactions of these dyes dimer are investigated by B3LYP method to predict the stabilization upon dye aggregation. Figure 6 illustrates the optimized geometries of D1 dimer. Further survey of the HOMO and LUMO orbitals of D1 dimer is also collected in Figure 6. The properties of D2D3 dimers are given in Figure S1 in the supporting information (see Supplementary Material available online at http://dx.doi.org/10.1155/2015/605728).
(a)
(b)
As shown in Figure 6 and Figure S1, all these stable molecules have formed intermolecular H⋯O hydrogen bonds. Take D1 dimer as an example, the carboxyl and terminal carbonyl group of thiazolidine form three H⋯O hydrogen bonds. One H⋯O hydrogen bond is 2.568 Å, which is formed by the carboxyl and one terminal H atoms in the ethyl. Another two H⋯O hydrogen bonds are 2.623 and 2.448 Å, which are formed by the two O atoms in the carbonyl group of thiazolidines interact with the two H atoms. In addition, the HOMOs of dimers are mainly located on one monomer, while their LUMO are contributed by another monomeric unit. Clearly, the intermolecular charge transfer process between the dyes dimers may occur for all the dyes. Compared with the isolated dye monomer (see Figure 3), the HOMO energy of D1 dimer slightly increases by 0.06 eV, while the LUMO energy decreases by 0.12 eV, respectively. Because of the dramatically decreased LUMO energy, the HOMOLUMO energy gap of D1 dimer becomes narrowed 0.18 eV compared with monomer. Similarly, the HOMOLUMO energy gap of D2 dimer and D3 dimer decreases by 0.14 eV and 0.18 eV, respectively, compared with corresponding monomer. Normally, the narrowed HOMOLUMO energy gap favors red shifted of absorption spectra. As reported by Pastore and De Angelis [13], the redshift of absorption spectra for indoline dye are due to the dye aggregation. Therefore dye aggregation is expected to be associated with the HOMOLUMO energy gap of dye dimer. Since there are small differences of HOMOLUMO energy gap of these dimers compared with corresponding monomer, introducing the N(phenyl)_{2} substitutions at the donor may play a slightl effect on avoiding unfavorable dye aggregation.
3.5. Dye(TiO_{2})_{6} Complexes
For a better understanding of the effect of the triphenylaminebased donor on the electron coupling, these dyes bound to (TiO_{2})_{6} cluster are optimized by B3LYP method. As well accepted, there are two common absorption models for dyes absorbed on the surface [39, 40]. One is a single TiO monodentate binding mode; another is a bidentate chelating structure mode. In this work, we take D4 as an example to testify which mode is stable absorption configuration. The optimized geometries of D4(TiO_{2})_{6} in different models are drawn in Figure S2. It can be seen that the total energy of bidentatechelating configuration is lower 3.75 kcal/mol than single monodentate mode. This agrees with the previous work; that is, the bidentate chelating structure mode is usually predicted to be stable [13, 41–43]. Therefore, the D149 and D1–D3 absorbed on the surface are optimized under the bidentate chelating structure mode. The optimized geometry, absorption energies (), and the contour plot of the HOMO and LUMO of dye(TiO_{2})_{6} complexes are depicted in Figure 7. The energy level of frontier molecule orbital (eV) of the dye(TiO_{2})_{6} and the energies differences between the dye and dye(TiO_{2})_{6} are drawn in Figure 8.
As shown in Figure 7, the decreased order of for D149 and D1–D4 is D149 (23.68 kcal/mol) > D1 (20.81 kcal/mol) > D2 (15.66 kcal/mol) > D3 (10.32 kcal/mol) > D4 (2.85 kcal/mol), indicating the interactions between the dye and TiO_{2} surface is decreasing in the same order. In particular, for D4, the is so small that D4 is difficult to be chemisorbed on the cluster. After absorption to the (TiO_{2})_{6} cluster, the calculated distances of D1 between the carboxylic oxygen atoms and the (TiO_{2})_{6} cluster (Ti–O bond lengths) are about 2.032 Å and 2.115 Å. By introducing the N(phenyl)_{2} and CF_{3} groups, the two TiO bond lengths increase to 2.032 Å and 2.116 Å for D2, 2.032 Å and 2.117 Å for D3, and 2.032 Å and 2.119 Å for D4. It suggests that the N(phenyl)_{2} and CF_{3} groups have decreased the electron coupling between the dyes and surface, which is consistent with the analyses of .
Molecular orbital spatial distribution shows that the HOMO of dye(TiO_{2})_{6} is mainly localized over the donor part of dyes, while the LUMO is focused on the (TiO_{2})_{6} part. As expected, the interfacial electron injection from the dye to the TiO_{2} surface may successively transfer when the dyes bind on the TiO_{2} film. Furthermore, compared with the isolated sensitizer, the HOMOs have subtle changes (about 0.1 eV) when the D149 and D1–D4 absorb to (TiO_{2})_{6} cluster. The most noticeable difference between the isolated dyes and dye(TiO_{2})_{6} is focused on the LUMO energy. The LUMO energy of (D1–D4)(TiO_{2})_{6} dramatically decreases compared with D149(TiO_{2})_{6}, suggesting that the LUMOs of all designed dyes create relative strong electronic coupling with TiO_{2} film and, as a result, further boost the electron injection. In addition, the LUMO of D1(TiO_{2})_{6} is lower 1.45 eV than that of D1. While the lowerlying energy LUMO of D149(TiO_{2})_{6} (1.35 eV), D2(TiO_{2})_{6} (1.40 eV), and D3(TiO_{2})_{6} (1.37 eV) becomes smaller than that of D1, indicating that the electronic coupling to the TiO_{2} surface decreases by importing the N(phenyl)_{2}.
4. Conclusions
The electronic structures, absorption spectra, and photophysical properties of triphenylaminebased indoline dyes as photosensitizers for application in DSSCs were investigated by density functional theory (DFT) and timedependent DFT (TDDFT). The calculated results demonstrated that the donor parts had great effect on the structure and optical properties. Compared with D149, D1–D3 had proper HOMO and LUMO energy level as well as narrow HOMOLUMO energy gap by introducing the N(CH_{3})_{2} and N(phenyl)_{2} groups at the donor part; therefore D1–D3 may be good DSSC sensitizers. The absorption speaks of D1–D4 covered the entire visible region and the intense absorption bands of them all corresponded to the intramolecular charge transfer transition, which may play an important role in conversion efficiencies. The stable molecule of D1–D3 dimmers were formed by intermolecular H⋯O hydrogen bonds. The data of and the LUMO energy level of dye(TiO_{2})_{6} suggested that D1 had the strongest interactions between the dye and TiO_{2} surface of these dyes. Furthermore, D1 had larger and values than D2–D4, indicating that D1 may have improved energy conversion efficiency by introducing the N(CH_{3})_{2} group at the donor part of triphenylamine. We hope that this work will be helpful for designing the organic dyes with high efficiency.
Conflict of Interests
The authors declare that there is no conflict of interests regarding the publication of this paper.
Acknowledgments
Financial supports were received from NSFC (no. 21243006 and 51304193), the Basic Research Program of Jiangsu Province (no. BK20130172), and the Fundamental Research Funds for the Central Universities (nos. 2013QNA14 and 2010QNA10). A Project funded by the Priority Academic Program Development of Jiangsu Higher Education Institutions is acknowledged. The authors are grateful to the High Performance Computing Center of China University of Mining and Technology for the award of CPU hours to accomplish this work.
Supplementary Materials
The geometries and frontier orbital energy of D2D3 dimers as well as geometries of D4(TiO2)6 in different models are collected in the Supporting information.
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Copyright © 2015 XueFeng Ren 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.