Spectroelectrochemical Characterization of Organic-Inorganic Materials Containing Porous Vanadium (V) Oxide, Poly-o-Methoxyaniline and Poly(Ethylene Oxide)

In this study, the synthesis and spectroelectrochemical analysis of hybrid materials containing poly-o-methoxyaniline/porous V2O5, poly(ethylene) oxide/ porous V2O5 and poly-o-methoxyaniline/poly(ethylene) oxide/porous V2O5, which have high potential for applications in batteries and electronics, is reported. The hybrid materials were obtained by intercalation of the polymers into the porous V2O5 matrix. These new compounds were characterized using dc conductivity, and, for spectroelectrochemical studies, ultraviolet visible (UV-vis) spectroscopy as well as cyclic voltammetry were used. The optical band gap values of the hybrid materials were estimated using Tauc plot. The introduction of organic materials into the inorganic species resulted in the reduction of V ions to V, increasing the dc conductivity and affecting the spectroelectrochemical properties of the samples.


Introduction
Preparation and development of new hybrid materials, containing organic and inorganic structures, have been extensively studied as they introduce the possibility of composite chemical and physical properties that may not be present in the starting components alone [1] [2] [3] [4] [5]. The combination is made by the incorporation of one or more organic species into an inorganic matrix and it occurs mainly though weak interactions, such as van der Waals or electrostatic interactions [6]. In the literature, special emphasis has been placed on hybrid materials prepared from inorganic materials obtained by the sol-gel route followed by intercalation with an organic species [2] [5] [7]- [12]. The sol-gel route is a synthesis that involves the hydrolysis and condensation of metal alkoxides or hydroxylated precursors, followed by an inorganic polymerization reaction [13].
During intercalation reactions, theses precursors can be considered a matrix or host for organic molecules. Vanadium pentoxide (V 2 O 5 ) is an inorganic matrix that presents a lamellar structure and can be used as host material. The combination of V 2 O 5 and an organic material yield new material called as hybrid material with improved properties known as synergic effects [14] [15]. Organic molecules are inserted into the inorganic layered structure and reduction of the oxide induces oxidation as well as polymerization of the organic molecules, resulting in a host-guest compound or hybrid material [1] [16] [17] [18]. Some polymers, such as poly(ethylene oxide), present a ionic conductivity that assist in improving of charge transfer during the electrochemical process. On the other hand, poly-o-methoxianiline is an electric conductivity and once intercalated into the matrix acts on increasing of total charge. The presence of a polymer species in the inorganic host can result in an improvement of the properties, such as electrochemical performance. However, in the solid state, the kinetics of ion insertion/de-insertion during the electrochemical process can be affected, if the hybrid material has a low surface area. To overcome this disadvantage, the surface area can be increased though the use of a highly porous network produced by mesoporous synthesis, which consequently reduces the length of the diffusion path and improves the kinetic performance [19]. Additionally, some hybrid materials undergo a color change during the electrochemical process [20] [21] [22]. This effect can be studied through spectroelectrochemical monitoring of the electrode processes during the redox process [23]. Furthermore, using Tauc's method, it is possible to evaluate the optical absorption of materials. This method is often used to calculate the band gap from results of spectral absorption, which are fitted using a power-law expression. To calculate the band gap, the quantity αhν 1/r (Equation (1)) is plotted against the photon energy. The band gap is determined from the x-intercept of the linear portion of the Tauc plot.
Additionally, the fitted exponent indicates either a direct or indirect electron transition [24] ( ) In Equation (1), α is the absorption coefficient, h is Planck's constant, v is the photon frequency, Eg is the band gap, and B is the slope of the linear portion of the Tauc plot. The value of r depends on the nature of electronic transition: direct allowed transition r = 1/2; indirect allowed transition r = 2; direct forbidden transition r = 3/2; and Journal of Materials Science and Chemical Engineering indirect forbidden transition r = 3.
Based on the literature [25], an exponent of 1/r = 3/2 has been reported for vanadium pentoxide films, suggesting direct, forbidden transitions. To the best of our knowledge, there are few reports of the synthesis, or morphological, electrical, electrochemical, or optical studies of mesoporous V 2 O 5 /polymer hybrid materials [7] [8] [26]. In this context, our interest is to investigate the conductivity and spectroelectrochemical properties of materials produced through intercalation of poly(ethylene oxide) (PEO) and poly-o-methoxyaniline (POMA) into the interlayer space of porous vanadium(V) oxide (VOP); namely the host-guest hybrid materials VOP/PEO and VOP/POMA, respectively, and a ternary hybrid; mesostructured VOP/POMA/PEO.

Materials
All chemical reagents were used as received, unless otherwise specified. Poly (ethylene oxide), PEO (average molecular weight 100,000 g•mol −1 ) was acquired from AcrosOrganics. Acetonitrile (chromatographic grade) was obtained from Fluka. Vanadium(V) oxide powder and the monomer o-methoxyaniline were purchased from Sigma-Aldrich.

Synthesis of the VOP/Polymer Hybrid Materials
The o-methoxyaniline monomer was purified by vacuum distillation before use.
The hybrid material based on poly-o-methoxyaniline (POMA) and VOP was

Equipment and Procedure
The dc conductivity was measured against temperature in the 150 -350 K range. The direct energy gap is calculated using UV-vis spectra and the Tauc Relation (Equation (1)). Additionally, frontier orbitals (HOMO and LUMO) were estimated using Equation (2)

Results and Discussion
To analyze and compare the influence of interactions in the VOP/polymers on the conductivity phenomena after the intercalation reaction, the conductivity values of VOP/PEO, VOP/POMA, and VOP/POMA/PEO were evaluated (Figures 1-3). An increase in conductivity, compared with that of V 2 O 5 , occurred after the intercalation reaction, and had been previously reported by our group [22].    To investigate the spectroelectrochemical behavior were recorded using UVvis spectra and were carried out at potentials determined from cyclic voltammograms (CVs) to fixed potential in redox state. The cyclic voltammograms were previously published by our group [7] Based on the cyclic voltammograms [7], analysis of color transitions at the observed potential changes was carried out with spectroelectrochemical studies. The changes in the UV-vis absorbance spectra of VOP/PEO, VOP/POMA, and VOP/POMA/PEO films, deposited on glass/ITO, as a function of potential applied to the electrode, are shown in Figures 4-6, respectively. In VOP/PEO ( Figure 4) a significant change in absorbance was observed when the potential of working electrode was swept from −0.50 V to 1.0 V. The absorption spectra display broad, intense bands in the visible region, between 280 and 420 nm. This absorption is due to the reduction of the V V sites in the lattice to V IV during the electrochemical process, concomitant with the process of Li + insertion, which leads to the formation of LiV 2 O 5 species [29] [30]. The electrochemical properties of VOP/PEO are similar to those of V 2 O 5 obtained via the sol-gel process [22]. At a potential of +1.0 V, the material appears yellow, which can be attributed to the absorption characteristic of V V . At a potential of 0.0 V, the material appears green, which can be attributed to the absorption characteristic of V V/IV . Finally, at a potential of +0.3 V, the material appears blue, which can be attributed to the absorption characteristic of V IV . PEO is a transparent material which does not influence the UV-vis spectrum during the electrochromic processes in VOP/PEO. As an important point, V 2 O 5 has a yellow coloration and in the redox state associated with cathodic Li-insertion, the LixV 2 O 5 specie formed is pale blue [31]. The electrochemical change in redox state causes an Journal of Materials Science and Chemical Engineering   intense electronic absorption band due to optical intervalence charge transfer. The polymeric species, PEO, is an ionic conductor and a colorless material at different potential values [2]. In Figure 5 and Figure 6 no significant change is observed in the absorption spectra over the potential range; a single band is observed at around 300 nm. These results can be explained by the fact that the in the hybrid compound VOP/POMA, POMA contributes a pale-yellow color, and VOP contributes a blue color associated with the reduction process, resulting in a dark blue color overall. Additionally, in the oxidation process of VOP/POMA, POMA contributes a blue color and VOP contributes a pale yellow color, again resulting in a blue color. It is important to point out that there is a change of absorption for POMA at different potentials due to the different electrochemical doped and undoped states [32]. In its oxidized state, the color of the film is blue, resulting in a blue shift of the absorption peak. However, in its reduced state, the color of the film changes to light yellow [33]. Thus, in the spectroelectrochemical studies, the absorption behavior of the hybrid material VOP/POMA does not change significantly during the redox process. A similar result is observed in VOP/POMA/PEO ( Figure 6) since PEO is a colorless polymer, and thus the colors of VOP and POMA are dominant.
Based on cyclic voltammograms previously published by our group [7] it was possible to identify the highest occupied molecular orbital of VOP/PEO, VOP/ POMA, and VOP/POMA/PEO. The onset oxidation potentials of these materials were observed to be −0.07 V, 0.18 V, and 0.07 V for VOP/PEO, VOP/POMA, and VOP/POMA/PEO, respectively. Furthermore, the HOMO positions were measured from the current onset of the first observed anodic signal. From the Equation (2) Table 1 represent the combination of the cyclic voltammetric studies and the Tauc plot method.
As observed, VOP/PEO has a lower band gap compared to those of VOP/POMA and VOP/POMA/PEO. This value can be attributed to the greater electron injection process, higher available photon flux, and a greater number of electronic interactions involving electrons, photons, and phonons [34]. Furthermore, the lower band gap of VOP/PEO compared to those of VOP/POMA and VOP/ POMA/PEO can be inferred by the presence of structural defects, which promote an increase in localized states of density in the band gap, consequently decreasing the energy gap.