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     . 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 . 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    - . 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 . During intercalation reactions, theses precursors can be considered a matrix or host for organic molecules. Vanadium pentoxide (V2O5) is an inorganic matrix that presents a lamellar structure and can be used as host material. The combination of V2O5 and an organic material yield new material called as hybrid material with improved properties known as synergic effects  . 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    . 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 . Additionally, some hybrid materials undergo a color change during the electrochemical process   . This effect can be studied through spectroelectrochemical monitoring of the electrode processes during the redox process . 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 αhν1/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 
In Equation (1), is the absorption coefficient, is Planck’s constant, 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
indirect forbidden transition r = 3.
Based on the literature , 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 V2O5/polymer hybrid materials   . 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.
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.
2.2. Synthesis of Porous Vanadium(V) Oxide
Vanadium(V) oxide powder was dissolved in 0.1 mol∙L−1 aqueous sodium hydroxide, with stirring, for 24 h, at 50˚C. Subsequently, this solution was combined with an aqueous mixture containing the surfactants cetyltrimethylammonium bromide (CTAB)/hexadecylamine (HDA) at 0.01 mol∙L−1 (1:1), and aqueous magnesium chloride at 0.003 mol∙L−1 and pH = 3. The resulting mixture was stirred at 25˚C, for 24 h, followed by aging at room temperature for 7 days. Subsequently, the resulting brown solid was washed with distilled water until reaching neutral pH, and dried at 60˚C, for 24 h. This mixture (MS) had a molar composition of 1.0:0.03:0.1 (V2O5:MgCl2:surfactants). Then, a black porous material was obtained from MS by removal of the surfactant molecules via thermal treatment (above 350˚C), which afforded the final material, designated VOP. VOP had a molar composition of 1.0 V2O5/0.03 MgCl2.
2.3. 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 prepared by adding VOP (2.2 × 10−3 mol∙L−1) to o-methoxyaniline (8.8 × 10−3 mol∙L−1) both aqueous solution. The combination was stirred for 48 h resulting in the binary material VOP/POMA. To prepare the hybrid material based on PEO and VOP, PEO (160 × 10−7 mol∙L−1) was added to VOP (1.37 × 10−3 mol∙L−1) in aqueous solution, and the mixture was stirred for 48 h, leading to another binary material, VOP/PEO. Finally, the dark green composite containing both polymers (ternary material) was prepared by adding VOP/PEO (0.50 mL) to o-methoxyaniline (0.1 mL), with stirring, for 48 h at room temperature, affording VOP/POMA/PEO.
2.4. Equipment and Procedure
The dc conductivity was measured against temperature in the 150 - 350 K range. The measurements were performed in an evacuated chamber using a dc bias of 1 V between silver electrodes. The ultraviolet visible (UV-vis) spectral measurements were recorded on a spectrophotometer (Varian Cary 50) with the hybrid materials onto an indium tin oxide (ITO) electrode. Cyclic voltammetry experiments were carried out with an Eco Chemie AUTOLAB model PGSTAT30 (GPES/FRA) potentiostat/galvanostat interfaced with a computer. A conventional three-electrode arrangement was used, consisting of an ITO working electrode, a platinum wire auxiliary electrode and a saturated calomel (SCE) reference electrode in 0.1 mol∙L−1 LiClO4 in acetonitrile, at a scan rate of ν = 20 mV∙s−1. The hybrid materials were deposited on the working electrode surface by evaporating 4 µL at room temperature. The experiments were carried out in an inert atmosphere by bubbling N2 through the solution at room temperature. For the spectroelectrochemical experiments, the potentiostat/galvanostat was coupled with the spectrophotometer, and a three-electrode system was assembled in a quartz cell with a 1.00 cm optical path length. An ITO electrode was employed as the working electrode in the presence of a SCE reference electrode, the auxiliary electrode was a platinum wire, and 0.1 mol∙L−1 of LiClO4 in acetonitrile was used as the supporting electrolyte.
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) and Equation (3)  :
3. 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 V2O5, occurred after the intercalation reaction, and had been previously reported by our group . The conductivity values were 5.61 × 10−3, 5.03 × 10−3, and 5.01 × 10−3 (Ω∙cm−1) and the activation energies were 1.09, 0.93, and 1.05 (eV), after introduction of PEO, POMA, and the combined polymers to the VOP structure, respectively. These results are quite similar considering that the structures of the polymers are different. The polymers have a linear structures and interact with VOP through van der Waals forces . However, the variations in conductivity
Figure 1. dc conductivity measurements of VOP/PEO.
Figure 2. dc conductivity measurements of VOP/POMA.
can be attributed to the fact that PEO is an ionic conductor and POMA is an electronic conductor (polarons). In the literature, an increase in the VIV/(VIV + VV) ratio of VOP is observed after intercalation of PEO . So, it is possible to infer that the conductivity of these materials depends on the change in the oxidation state of VOP caused by PEO interaction and/or polaron transport along the POMA backbone.
Figure 3. dc conductivity measurements of VOP/POMA/PEO.
To investigate the spectroelectrochemical behavior were recorded using UV-vis 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 
Based on the cyclic voltammograms , 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 VV sites in the lattice to VIV during the electrochemical process, concomitant with the process of Li+ insertion, which leads to the formation of LiV2O5 species  . The electrochemical properties of VOP/PEO are similar to those of V2O5 obtained via the sol-gel process . At a potential of +1.0 V, the material appears yellow, which can be attributed to the absorption characteristic of VV. At a potential of 0.0 V, the material appears green, which can be attributed to the absorption characteristic of VV/IV. Finally, at a potential of +0.3 V, the material appears blue, which can be attributed to the absorption characteristic of VIV. PEO is a transparent material which does not influence the UV-vis spectrum during the electrochromic processes in VOP/PEO. As an important point, V2O5 has a yellow coloration and in the redox state associated with cathodic Li-insertion, the LixV2O5 specie formed is pale blue . The electrochemical change in redox state causes an
Figure 4. Spectroelectrochemical studies of VOP/PEO.
Figure 5. Spectroelectrochemical studies of VOP/POMA.
Figure 6. Spectroelectrochemical studies of VOP/POMA/PEO.
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 . 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 . 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 . 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  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), the HOMO of VOP/PEO, VOP/POMA, and VOP/ POMA/PEO are −4.77, −4.84, and −4.74 eV, respectively.
From Figures 7-9 (Tauc plots), it was possible to measure the optical band gap and, consequently, to obtain the LUMO level. The optical band gap, LUMO, and HOMO values presented in 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 . 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.
Figure 7. Plot of (αhν)2/3 vs hν for VOP/PEO.
Figure 8. Plot of (αhν)2/3 vs hν for VOP/POMA.
Figure 9. Plot of (αhν)2/3 vs hν for VOP/POMA/PEO.
Table 1. The HOMO-LUMO energy levels and band gap energies of VOP/PEO, VOP/ POMA, and VOP/POMA/PEO.
In this work, the intercalation of POMA and PEO into the porous V2O5 matrix was studied. Intercalation of the polymers into V2O5 affected conductivity. After the insertion of polymers into the porous matrix, the conductivity increased compared to that of pristine V2O5, previously observed in our group. During the spectroelectrochemical process, it was observed that PEO did not influence the absorption during the electrochromic process as it is a transparent material, and therefore, the color changes during the process were exclusively due to the VOP. However, the presence of POMA in the VOP caused a color overlay that meant that during the electrochromic analysis, the color change was not significant. As PEO is a transparent material, VOP/POMA/PEO displayed an electrochromic variation similar to that of VOP/POMA. The Tauc method of determining the band gap of materials was used and the values were found to be 2.65 eV, 3.30 eV, and 3.40 eV for VOP/PEO, VOP/POMA, and VOP/POMA/PEO, respectively. The frontier orbital energies indicate that these materials can be considered as candidates as photosensing components in solar cells.
The authors gratefully acknowledge the fellowship provided by CAPES, FAPESP, FAPEMIG, INEO, and CNPq, which are also acknowledged for financial support. Additionally, this work has been a collaboration research project with members of the Rede Mineira de Química (RQ-MG) supported by FAPEMIG (Project: CEX-RED-00010-14).
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