Synthesis and Characterization of Polymeric (PMMA-PVA) Hybrid Thin Films Doped with TiO 2 Nanoparticles Using Dip-Coating Technique

: We report the synthesis of hybrid thin ﬁlms based on Poly(MethylMethAcrylate) (PMMA) and Poly(VinylAlcohol) (PVA), doped with different concentrations of titanium dioxide nanoparticles (TiO 2 NPs). As-prepared thin ﬁlms of (PMMA-PVA) doped by TiO 2 NPs (wt.% = 2%, 4%, 8%, and 16%) are deposited on glass substrate. Transmittance (T%), reﬂectance (R%), absorption coefﬁcient ( α ), optical constants ( n and k ), and optical dielectric functions ( ε 1 and ε 2 ) are deduced using the experimental transmittance and reﬂectance spectra. Furthermore, a combination of classical models such as Tauc, Urbach, Spitzer-Fan, and Drude models are applied to calculate the optical and optoelectronic parameters and the energy gaps of the prepared nanocomposite thin ﬁlms. The optical bandgap energy of PMMA-PVA thin ﬁlm is found to be 4.101 eV. Incorporation of TiO 2 NPs into PMMA-PVA polymeric thin ﬁlms leads to a decrease in the optical bandgap and thus bandgap engineering is possible. Fourier-transform infrared spectroscopy (FTIR) transmittance spectra of thin ﬁlms are measured and interpreted to identify the vibrational modes. To elucidate the chemical stability, thermogravimetric (TGA) curves are measured. We found that (PMMA-PVA)/TiO 2 NPs polymeric thin ﬁlms are thermally stable below 110 ◦ C enable them to be attractive for a wide range of optical and optoelectronic the optical applications involving thin ﬁlms can be performed at temperatures close to 110 ◦ C. Our detailed and comprehensive investigations of the optical, lattice dynamical, and thermal properties of (PMMAPVA)/TiO 2 nanocomposite thin ﬁlms reveal that they could be utilized in manufacturing realistic scaled optoelectronic and photonic devices. To elucidate a deeper understanding of the vibrational modes of (PMMA-PVA)/TiO 2 nanocomposite thin ﬁlms, we carry out FTIR measurements. We identify and interpret all vibrational bands associated with formation, rotation, and twisting of different bonds involved in the investigated polymerized thin ﬁlms.


Introduction
Hybrid Polymeric nanocomposite thin films have gained much attention owing to their unusual physical, chemical, and optical properties. Merging metal nanoparticles with polymers boosts the optical properties and modifies the mechanical behavior of the polymer composite [1]. The architected polymeric wave guides require a minor adjustment of the refractive index to accomplish total reflectance and henceforward effective wave guiding. Nevertheless, the discrepancy in the values of refractive index between the polymeric matrix and the semiconductor host results in Fresnel losses. This could be compensated by using polymeric material of a high refractive index [2]. The advancement of polymeric composite thin films is basically determined by the selection of ionic fillers and optimum filler loads. Consequently, a nanocomposite thin film of enhanced refractive index is obtained. For high refractive index-polymer to operate effectively, it should also often exhibit higher optical transparency [3][4][5]. Unfortunately, insertion of fillers frequently increases the transparency losses [6]. Additionally, high refractive index polymers are key

Preparation of Titanium Dioxide Nanoparticles (TiO 2 NPs)
To prepare the TiO 2 -NPs using the sol-gel method, we dissolved 5 mL of Titanium (IV) tetraisopropoxide (Ti (OCH (CH3)2)4) with 15 mL of 2-propanol in (beaker A). Beaker A is subsequently placed on a magnetic stirrer for 30 min at room temperature. Next, we dissolve 100 mL distilled water (pH = 8) with 150 mL of 2-propanol in (beaker B) and placed on a magnetic stirrer for 30 min at room temperature. When the solutions in the beaker are ready, we added (beaker A) to (beaker B) and the mixture is left on a stirrer for 15 min to get a homogeneous solution of TiO 2 . The solution should be was centrifuged for 15 min. The as-prepared precipitate is then washed by ethanol three times, centrifuged, and heated at temperatures ranging from 60 to 70 • C for 24 h to obtain TiO 2 -NPs in the powder form. Finally, having obtained TiO 2 -NPs in the powder form, they are then placed in the furnace, and the temperature is gradually raised to anneal the powder at a temperature of 400 • C for 2 h [17].

(PMMA-PVA) Polymeric Thin Films Doped by TiO 2 NPs
The glass substrates are cleaned with warm tap-water, then rinsed with ionized acidic water of (pH = 3.5) to remove the surface oxidized layer and greases, and then dipped in acetone. The substrates are then bathed in the ultrasonic path of distilled water for five minutes and dried with cold air. Then, 1 g of PMMA (m w = 100.12 g/mol) and 1 g of PVA (m w = 86.09 g/mol) are dissolved separately in 200 mL of Chloroform (CHCl 3 ). (PMMA-PVA) solution is obtained by mixing (PMMA and PVA) solutions in a 1:1 volume ratio using a magnetic stirrer for 24 h to enhance the homogeneity. PMMA-PVA solution is then filtered using 0.45 µm millipore filter before dip coating on the glass substrates. The films are synthesized at room temperature of 27 • C under atmospheric pressure [19]. The PVA polymers prevent the aggregation of the TiO 2 -NPs by the organic surface modification and keep the TiO 2 -NPs dispersed in PVA matrix at the nano scale. The final solutions are filtered by paper-filter (0.45 µm in dimension). The viscosity of sol-gel solutions ranges between 1.2079 and 2.8935 Cp. The (PMMA-PVA)/TiO 2 nanocomposite solutions were prepared by adding TiO 2 -NPs into PMMA-PVA solution directly under magnetic stirring for 4 h. The (PMMA-PVA)/TiO 2 nanocomposite solutions are deposited as a thin layer on glass substrate using dip-coating technique by immersing the substrate in the solution for 2 h, forming nanocomposite thin films with average thickness of 500 nm with a maximum standard deviation of 7.5%. The thickness of thin films is confirmed by Scanning Electron Spectroscopy (SEM). The nanocomposite thin films are obtained by allowing the solvent to evaporate for 15 min at 70 • C to evaporate the solvent and organic residues. The withdrawal speed ranged from 10-80 cm min −1 . The multilayers of (PMMA-PVA)/TiO 2 nanocomposites thin films are then analysed and interpreted [19].

Characterization
The average thickness of the as-grown (PMMA-PVA)/TiO 2 nanocomposite thin films is measured to be 500 nm using Scanning Electron Microscopy (SEM, Quanta FEG 450) images obtained at our nanotechnology facility. The room-temperature transmittance and reflectance are obtained using a Double-Beam UV-vis Spectrophotometer (U-3900H). Chemical properties were determined using Fourier Transform Infrared Spectroscopy (FTIR) by KBr technique.

UV-Vis Spectroscopy
A UV-Vis spectrophotometer is employed to investigate the optical properties of the (PMMA-PVA)/TiO 2 nanocomposite thin films with various contents of TiO 2 -NPs. Particularly, we investigate the spectral behavior of transmittance and reflectance. Optical parameters such as absorption coefficient, optical bandgap energy, Urbach energy, optical constants, and optical dielectric functions are measured, analyzed, and interpreted. Moreover, using TGA analysis, we investigate the thermal stability. In addition, FTIR measurements are performed to investigate the vibrational bands. The FTIR results reveal some sorts of interaction between the constituents of nanocomposite thin films as indicated by the induced changes in the vibration modes and the band position. Figure 1 shows the transmittance spectra of (PMMA-PVA)/TiO 2 nanocomposite thin films for various TiO 2 -NPs contents as a function of incident light wavelength. The figure shows a sort of ion transfer mechanism between (PMMA-PVA) polymer composite and TiO 2 -NPs. The transmittance values of undoped (PMMA-PVA) polymeric thin film in the visible region (visible region, λ ≥ 350 nm) is found to be about 91.6%. This behavior indicates an excellent excitation that leads to a sharp electron transition from the valance band to the conduction band. Interestingly, the effect of introducing TiO 2 -NPs contents in (PMMA-PVA) polymeric thin films leads to a decrease in transmittance values in the visible region. This decrease is gradual and nonlinear. Our results indicate that (PMMA-PVA)/TiO 2 nanocomposite thin films (wt.% = 2 and 4%) exhibit transmittance values at λ = 550 nm to 89.8 and 89.6%, respectively. Moreover, increasing the concentration (wt.% = 8 and 16%) of TiO 2 -NPs in (PMMA-PVA) polymeric thin films leads to a further decrease in the transmittance values at λ = 550 nm to 87.6 and 81.3%, respectively. The loss of transparency is attributed to the reflectance and scattering of incident photons by TiO 2 -NPs [6]. Figure 2 shows the reflectance spectra of (PMMA-PVA)/TiO 2 nanocomposite thin films for various TiO 2 -NPs contents as a function of incident light wavelength. At λ ≥ 350 nm, reflectance values decrease slightly as the wavelength is increased. The reflectance values of undoped (PMMA-PVA) polymeric thin film lies in a range of 4.6 up to 8.9 as the wavelength decreases from 700 up to 350 nm. Interestingly, the effect of introducing TiO 2 -NPs contents in (PMMA-PVA) polymeric thin films leads to an increase in reflectance values. As predicted, the reflectance spectrum shows an opposite behavior to those in the transmission spectrum. Our results indicate that (PMMAPVA)/TiO 2 nanocomposite thin films (wt.% = 2 and 4%) exhibit reflectance values at λ = 550 nm about 5.5 and 5.6%, respectively. Moreover, increasing (wt.% = 8 and 16%) of TiO 2 -NPs in (PMMA-PVA) polymeric thin films leads to an increase in the reflectance values at λ = 550 nm to 7 and 13%, respectively. The average of the sum of the transmittance and the reflectance is of the order of unity [15], Therefore, we can neglect the loss of light due to the presence of scattering or absorption of the incident light confirming that the surfaces of the deposited thin films are of good quality and their surfaces are extremely smooth.
Optical absorption measurements provide a straightforward scheme for accurate calculation of optical band gap (E g ). The measurement of absorption coefficient spectra (α) for any polymer, hybrid material, and semiconducting thin films is usually performed in two distinct spectral regions. Mainly, the high energy region, in which α spectrum is associated with the electronic states and the lower energy zone, in which α spectrum is associated with atomic vibrations [20,21]. In this respect, α is calculated as a function of wavelength as, α = (1/d) ln(1/T), where d is the film thickness which is measured to be about 500 nm [19][20][21][22][23]. Figure 3 shows α of (PMMA-PVA)/TiO 2 nanocomposite thin films as a function of wavelength. Clearly, all thin film samples exhibit higher α in the UV region (UV region, λ ≤ 350 nm). Introducing TiO 2 -NPs contents in (PMMA-PVA) polymeric thin films leads to a slight increase in absorption coefficient values. The increase in α values is attributed to the absorption decrease in the interband transition [23]. Interestingly, the accurate determination of α is crucial for the determination of several optical parameters. Typically, the (PMMA-PVA)/TiO 2 nanocomposite thin films have strong absorption in the UV region and strong transmittance in the visible region. Consequently, these films may act as key candidate potential materials for optoelectronic devices operating in the UV spectral region [17].  Optical absorption measurements provide a straightforward scheme for accurate calculation of optical band gap ( ). The measurement of absorption coefficient spectra ( ) for any polymer, hybrid material, and semiconducting thin films is usually performed in two distinct spectral regions. Mainly, the high energy region, in which spectrum is associated with the electronic states and the lower energy zone, in which spectrum is associated with atomic vibrations [20,21]. In this respect, is calculated as a function of wavelength as, (1 ⁄ ) ln(1 ⁄ ), where is the film thickness which is measured to be about 500 nm [19,[20][21][22][23].   Optical absorption measurements provide a straightforward scheme for accurate calculation of optical band gap ( ). The measurement of absorption coefficient spectra ( ) for any polymer, hybrid material, and semiconducting thin films is usually performed in two distinct spectral regions. Mainly, the high energy region, in which spectrum is associated with the electronic states and the lower energy zone, in which spectrum is associated with atomic vibrations [20,21]. In this respect, is calculated as a function of wavelength as, (1 ⁄ ) ln(1 ⁄ ), where is the film thickness which is measured to be about 500 nm [19,[20][21][22][23].  Extinction coefficient (k) indicates the quantity of absorption loss when the electromagnetic wave transmits through the material. k is a crucial parameter for the determination of several related optical parameters, primarily those related to the absorption of light waves in the medium. k value measures the fraction of light lost by scattering and absorption per unit distance of the penetrated medium [24]. The extinction coefficient, k, can be expressed as, k = αλ/ 4π [23]. Figure 4 shows extinction coefficient spectra of (PMMA-PVA)/TiO 2 nanocomposite thin films as a function of wavelength for various TiO 2 -NPs concentrations. k exhibits high values in the UV region, whereas it adopts very low values in the visible region. Moreover, our results indicate that k is directly proportional to the absorption coefficient α. The observed low value of k in the visible range is a strong indication of no light loss due to scattering and as-prepared nanocomposite thin films have excellent optical transparency in this spectral region [23].
Interestingly, the accurate determination of is crucial for the determination of several optical parameters. Typically, the (PMMA-PVA)/TiO2 nanocomposite thin films have strong absorption in the UV region and strong transmittance in the visible region. Consequently, these films may act as key candidate potential materials for optoelectronic devices operating in the UV spectral region [17]. Extinction coefficient ( ) indicates the quantity of absorption loss when the electromagnetic wave transmits through the material. is a crucial parameter for the determination of several related optical parameters, primarily those related to the absorption of light waves in the medium. value measures the fraction of light lost by scattering and absorption per unit distance of the penetrated medium [24]. The extinction coefficient, , can be expressed as, k / 4 [23]. Figure 4 shows extinction coefficient spectra of (PMMA-PVA)/TiO2 nanocomposite thin films as a function of wavelength for various TiO2-NPs concentrations. k exhibits high values in the UV region, whereas it adopts very low values in the visible region. Moreover, our results indicate that is directly proportional to the absorption coefficient . The observed low value of k in the visible range is a strong indication of no light loss due to scattering and as-prepared nanocomposite thin films have excellent optical transparency in this spectral region [23].  Refractive index ( ) is closely related to the electronic polarization of ions and the local field inside optical materials. Accurate calculation of n is crucial for optical application of semi-transparent and transparent polymers, e.g. switches, sensors, filters and modulation, etc. [25]. Therefore, it is of crucial importance to reveal the behavior of n. Several optical parameters are closely correlated to . It can be calculated as, (1 1 ⁄ ) (4 (1 ) ) ⁄ [23]. Figure 5 shows n spectra of (PMMA-PVA)/TiO2 nanocomposite thin films as a function of wavelength for various TiO2-NPs concentrations. In highly absorption region ( 350 ), the incident photon frequency becomes approximately equal to the plasma frequency leading to anomalous dispersion. For ≥ 350 , n decreases slightly as the wavelength is increased. We found that n of (PMMA-PVA) polymeric thin film lies in a range of 1.5 to 1.85, as the wavelength decreases from 700 up to 350 nm. Interestingly, increasing TiO2-NPs contents in (PMMA-PVA) polymeric thin films results in an increase in n values. The effect of introducing wt.% of (2, 4, 8, and 16%) TiO2-NPs into (PMMA-PVA) polymeric thin films on n is found to be nonlinear. The increase in refractive index makes the films denser. Thus, propagation velocity of light traveling Refractive index (n) is closely related to the electronic polarization of ions and the local field inside optical materials. Accurate calculation of n is crucial for optical application of semi-transparent and transparent polymers, e.g. switches, sensors, filters and modulation, etc. [25]. Therefore, it is of crucial importance to reveal the behavior of n. Several optical parameters are closely correlated to n. It can be calculated as, [23]. Figure 5 shows n spectra of (PMMA-PVA)/TiO 2 nanocomposite thin films as a function of wavelength for various TiO 2 -NPs concentrations. In highly absorption region (λ < 350 nm), the incident photon frequency becomes approximately equal to the plasma frequency leading to anomalous dispersion. For λ ≥ 350 nm, n decreases slightly as the wavelength is increased. We found that n of (PMMA-PVA) polymeric thin film lies in a range of 1.5 to 1.85, as the wavelength decreases from 700 up to Crystals 2021, 11, 99 7 of 21 350 nm. Interestingly, increasing TiO 2 -NPs contents in (PMMA-PVA) polymeric thin films results in an increase in n values. The effect of introducing wt.% of (2, 4, 8, and 16%) TiO 2 -NPs into (PMMA-PVA) polymeric thin films on n is found to be nonlinear. The increase in refractive index makes the films denser. Thus, propagation velocity of light traveling through (PMMA-PVA)/TiO 2 nanocomposite thin films decreases considerably [15]. We found that (PMMA-PVA)/TiO 2 nanocomposite thin film containing 2 and 4% of NPs exhibit n values of 1.618 and 1.62 at λ = 550 nm, respectively. Increasing TiO 2 -NPs concentration in (PMMA-PVA) polymeric thin films up to 8 and 16% leads to a further increase in n values at 550 nm to 1.73 and 2.14, respectively. The increase in n values of (PMMA-PVA)/TiO 2 nanocomposite thin films may be attributed to the condensation of smaller nanoparticles into larger clusters [26]. The obtained high n values of the investigated nanocomposite thin films are promising and represent a strong potential indication that the thin films can be used for strong optical confinement and enhance the optical intensities of nonlinear interactions [17,18]. High refractive index values of (PMMA-PVA)/TiO 2 nanocomposite thin films nanocomposite thin films have attracted considerable attention because of their potential applications in advanced optoelectronic devices such as organic light emitting diode devices [7], photoresists for 193-nm immersion lithography [8], high performance substrates for advanced display devices [9], antireflective coatings for advanced optical applications [27] and micro lens components for charge coupled devices or complementary metal oxide semiconductor [10,28]. The optical dielectric constant (ɛ′) is responsible for the suppression of the speed of light in the medium [29]. The optical dielectric loss (ɛ′′) is associated with the absorption of energy from the electric field due to dipole motion [23]. The complex dielectric function (ɛ) can be decomposed as, ɛ ɛ ɛ , with ɛ′ expressed as, ɛ′ and (ɛ′′) is expressed as, ɛ 2 [23]. Figure 6 shows the optical dielectric constant spectra of  Figure 7 shows ɛ′′ spectra of (PMMA-PVA)/TiO2 nanocomposite thin films as a function of wavelength for various TiO2-NPs concentrations. ɛ′′ is found to adopt very low values in the visible range of the spectrum. The observed low value of ɛ′′ The optical dielectric constant (ε ) is responsible for the suppression of the speed of light in the medium [29]. The optical dielectric loss (ε") is associated with the absorption of energy from the electric field due to dipole motion [23]. The complex dielectric function (ε) can be decomposed as, e = e + ie , with e expressed as, e = n 2 + k 2 and (e ) is expressed as, e = 2nk [23]. Figure 6 shows the optical dielectric constant spectra of (PMMA-PVA)/TiO 2 nanocomposite thin films as a function of wavelength for various TiO 2 -NPs concentrations. The value of e of undoped (PMMA-PVA) polymeric thin film is found to be 2.  Figure 7 shows e spectra of (PMMA-PVA)/TiO 2 nanocomposite thin films as a function of wavelength for various TiO 2 -NPs concentrations. e is found to adopt very low values in the visible range of the spectrum. The observed low value of e in the visible ranges indicates less dissipation of absorption energy from the electric field due to frozen molecular dipoles motion indicating that no light loss due to scattering and polarization [30]. Furthermore, increasing TiO 2 -NPs contents in (PMMA-PVA) polymeric thin films leads to an increase slightly of e values in the visible region. The large polarizability of covalent bonds such as C-H, C-C, and C=O, polymeric based thin films demonstrate high dielectric constants [29]. Surprisingly, the values of the real part are relatively larger than those of an imaginary part (ε ε") suggesting that (PMMA-PVA)/TiO 2 nanocomposite thin films exhibit exceptionally small energy dissipation and higher speed of light as light propagates through thin films.     The Tauc plot is commonly used to estimate the optical band gap energy (E g ) of semiconductors. The E g values are obtained by extrapolating the linear part of the relationship of (αhυ) 2 versus hυ to the incident photon energy at which E g equals the incident photon energy (hυ). Tauc plot is based on relating the absorption coefficient with the incident photon energy in eV against (αhυ) 2 as (αhv) 2 = β hv − E g [20,31], where β is constant called band tailing parameter, E g is the band gap energy [17]. Figure 8 indicates that E g of undoped (PMMA-PVA) polymeric thin film is 4.101 eV. As 2 and 4%, of TiO 2 -NPs are introduced into (PMMA-PVA) polymeric thin films, the value of E g decreases slightly to 4.075 and 4.072 eV, respectively. Injection of 8 and 16% of TiO 2 -NPs into (PMMA-PVA) polymeric thin film leads to a further slight decrease in E g to 4.069 and 4.050 eV, respectively. This may be attributed to the tendency to enhance the ion transfer between the constituents of (PMMA-PVA)/TiO 2 nanocomposite thin films [32,33]. Furthermore, some sub-bands are created due to the formation of defect levels leading to the bridge overpass of electrons from valence band maximum (VBM) and conduction band minimum (CBM) [15,17,20,34]. The high transmittance, wide band gap energy, and high refractive index of (PMMA-PVA)/TiO 2 nanocomposite thin films entitle them to be employed in optoelectronic devices applications [3,6]. Furthermore, some sub-bands are created due to the formation of defect levels leading to the bridge overpass of electrons from valence band maximum (VBM) and conduction band minimum (CBM) [15,17,20,34]. The high transmittance, wide band gap energy, and high refractive index of (PMMA-PVA)/TiO2 nanocomposite thin films entitle them to be employed in optoelectronic devices applications [3,6]. Urbach energy ( ) is a result of the structural disorder in an amorphous and lowcrystalline materials [35].
is a measure of the localized density of states extended into the band gap primarily due to presence of defects, impurities, and non-crystallinity energy [18,20]. The relation between , , and , is given by the formula exp( ⁄ ), where is a constant [20].
is calculated by plotting lnα vs . The reciprocal of the slopes of the linear portion, below the optical band gap, gives the value of that is defined as the width of the tail of localized states in the band gap and believed to be a function of the structural disorder [35]. Figure 9 shows the variation of Urbach energy of (PMMA-PVA)/TiO2 nanocomposite thin films as a function TiO2-NPs content in films.
of undoped (PMMA-PVA) polymeric thin film is found to be 190.7 meV. Insertion of (wt.% = 2, 4, 8, and 16%) of TiO2-NPs into (PMMA-PVA)/TiO2 polymeric thin films increases to 191. 3, 192.5, 192.86, and 200 meV, respectively. In addition, tail is closely related to the disorder in the film network. The increase in the values of as TiO2-NPs contents in (PMMA-PVA)/TiO2 polymeric thin films is increased indicates the presence of defects, impurities [18]. Accordingly, it can be easily noticed that the lowering of band gap energy is due to the presence of localized defect states in the band gap energy Urbach energy (E U ) is a result of the structural disorder in an amorphous and low-crystalline materials [35]. E U is a measure of the localized density of states extended into the band gap primarily due to presence of defects, impurities, and noncrystallinity energy [18,20]. The relation between E U , α, and hυ, is given by the formula α = α 0 exp(hv/E U ), where α 0 is a constant [20]. E U is calculated by plotting ln α vs hv. The reciprocal of the slopes of the linear portion, below the optical band gap, gives the value of E U that is defined as the width of the tail of localized states in the band gap and believed to be a function of the structural disorder [35]. Figure 9 shows the variation of Urbach energy of (PMMA-PVA)/TiO 2 nanocomposite thin films as a function TiO 2 -NPs content in films. E U of undoped (PMMA-PVA) polymeric thin film is found to be 190.7 meV. Insertion of (wt.% = 2, 4, 8, and 16%) of TiO 2 -NPs into (PMMA-PVA)/TiO 2 polymeric thin films increases E U to 191. 3, 192.5, 192.86, and 200 meV, respectively. In addition, E U tail is closely related to the disorder in the film network. The increase in the values of E U as TiO 2 -NPs contents in (PMMA-PVA)/TiO 2 polymeric thin films is increased indicates the presence of defects, impurities [18]. Accordingly, it can be easily noticed that the lowering of band gap energy is due to the presence of localized defect states in the band gap energy window [20,35]. Figure 10 shows the relationship between E g and E U of (PMMA-PVA)/TiO 2 nanocomposite thin films for different concentrations of TiO 2 -NPs. Clearly, E U and the band edges of samples exhibit reverse trend. It can be easily noticed that the lowering of band gap in (PMMA-PVA)/TiO 2 nanocomposite thin films is due to the presence of localized defect states in the E g of (PMMA-PVA)/TiO 2 NPs near the VBM and CBM [20]. This decrease leads to a redistribution of states from band to tail, thus permitting a higher number of potential band-to-tail and tail-to-tail transitions [35]. Since Urbach tail parameter is a function of structural disorder and conductivity, the decrease in E U value confirms the alteration of state structure [35]. parameter is a function of structural disorder and conductivity, the decrease in value confirms the alteration of state structure [35].

Optoelectronic Parameters
Optoelectronic parameters of thin films should be accurately measured and appropriately characterized to employ thin films in optoelectronic systems. Refractive index is closely related to both the electronic polarization of ions and the local field inside the optical materials. Remarkably, the refractive index has a normal dispersion in the lower part of the energy spectrum of the incident photons. However, refractive index exhibits an anomalous dispersion in the high energy region. The refractive index dispersion can be Crystals 2021, 11, x FOR PEER REVIEW parameter is a function of structural disorder and conductivity, the decrease in confirms the alteration of state structure [35].

Optoelectronic Parameters
Optoelectronic parameters of thin films should be accurately measured and priately characterized to employ thin films in optoelectronic systems. Refractive

Optoelectronic Parameters
Optoelectronic parameters of thin films should be accurately measured and appropriately characterized to employ thin films in optoelectronic systems. Refractive index is closely related to both the electronic polarization of ions and the local field inside the optical materials. Remarkably, the refractive index has a normal dispersion in the lower part of the energy spectrum of the incident photons. However, refractive index exhibits an anomalous dispersion in the high energy region. The refractive index dispersion can be used to obtain the ratio of the density of states (ratio of free carrier concentrations to the effective mass (N c /m * ) and the high frequency dielectric constant (ε ∞ ). The two optoelectronic parameters are given by the formulation of Spitzer-Fan [36]: Where e is the electronic charge, c is the light speed, N c is the charge carrier density, m * is the effective mass of the carrier, and ε ∞ is the high frequency dielectric constant. Figure 11 shows the variation of the real part of the dielectric function ε = n 2 as a function of the square wavelength for (PMMA-PVA)/TiO 2 nanocomposite thin films to get the high frequency dielectric constant (ε ∞ ) and density of states (N c /m * ). The ε ∞ value of undoped (PMMA-PVA) polymeric thin film is found to be 2.623. Insertion of (wt.% = 2, 4, 8, and 16%) of TiO 2 -NPs in (PMMA-PVA) polymeric thin films leads to an increase in the value of ε ∞ to 2.775, 2.935, 3.353, and 5.268, respectively. The obtained ε ∞ values are found to be greater than the refractive index indicating that, the existence of the free charge carriers in (PMMA-PVA)/TiO 2 nanocomposite thin films are strongly contributing to the polarization process [36]. The N c /m * of (PMMA-PVA)/TiO 2 nanocomposite thin films with TiO 2 -NPs (wt.% = 0, 2, 4, 8, and 16%) is found to increase to 4.273, 5.299, 5.589, 6.440, and 12.525 × 10 +27 atoms/m 3 , respectively. Where is the electronic charge, is the light speed, is the charge carrier density, * is the effective mass of the carrier, and is the high frequency dielectric constant. Figure 11 shows the variation of the real part of the dielectric function( The obtained values are found to be greater than the refractive index indicating that, the existence of the free charge carriers in (PMMA-PVA)/TiO2 nanocomposite thin films are strongly contributing to the polarization process [36]. The * ⁄ of (PMMA-PVA)/TiO2 nanocomposite thin films with TiO2-NPs (wt.% = 0, 2, 4, 8, and 16%) is found to increase to 4.273, 5.299, 5.589, 6.440, and 12.525 ×10 atoms/ , respectively. The relaxation time ( ) measures the time that is required by charge carriers in the semiconducting materials to become neutralized during the conduction process. The value of this time is infinitesimal in the case of metals, but it is small in semiconductors and large for insulators. Drude free electron model demonstrates that both, the real part and imaginary parts of the dielectric function are functions of wavelength of the incident photon according to equation (1) and the relation [36].
(2) The relaxation time (τ) measures the time that is required by charge carriers in the semiconducting materials to become neutralized during the conduction process. The value of this time is infinitesimal in the case of metals, but it is small in semiconductors and large for insulators. Drude free electron model demonstrates that both, the real part and imaginary parts of the dielectric function are functions of wavelength of the incident photon according to Equation (1) and the relation [36].
The imaginary part of the dielectric function (ε ) as a function of the cubic wavelength λ 3 of the incident photon can be analyzed to determine τ as proposed by the Drude model. The N c /m * ratio can be calculated from equation (1). Moreover, Q. Shen et. al. formulates the relationship of m * and m e . This relation gives m * = 0.44 m e [36]. Consequently, free carrier concentrations (N c ) can be evaluated. Figure 12 shows the variation of the ε as a function of the λ 3 for (PMMA-PVA)/TiO 2 nanocomposite thin films. The plot can be utilized to determine τ. The τ constant can be determined from the slope of the plot of ε versus λ 3 and from the density of states calculated previously from the equation (1). τ of (PMMA-PVA)/TiO 2 nanocomposite thin films at (wt.% = 0, 2, 4, 8, and 16%) was found to increase to 2.49, 2.70, 2.76, 2.84, and 3.17 × 10 −14 (s), respectively, compared to that of un-doped thin films.  Finally, from the determination of the , the optical mobility ( ) and the optical resistivity ( ) of thin films can be calculated accordingly as [36], *

(4)
The calculated values of * ⁄ , , , , and are listed in Table 1.  Finally, from the determination of the τ, the optical mobility (µ opt ) and the optical resistivity (ρ opt ) of thin films can be calculated accordingly as [36], The calculated values of N c /m * , N c , τ, µ opt , and ρ opt are listed in Table 1. 3.3. The FTIR Spectra of (PMMA-PVA) Polymeric Thin Films Figure 13 shows Fourier Transform Infrared spectroscopy (FTIR) spectra of (PMMA-PVA) polymeric thin films as a function of wavenumber in the range (500-4000 cm −1 ). Figure 14 shows FTIR spectra of (PMMA-PVA) polymeric thin films measured in the range (500-1500) and (1500-2500) cm −1 . Our results indicate that vibrational frequencies of (PMMA-PVA) polymeric thin films coincide exactly with several vibrational frequencies observed for pure PVA polymer thin films. This observation is attributed to the fact that PVA thin film has dense molecular packing in the polymeric nanocomposite and stronger intermolecular hydrogen bonds in comparison with the PMMA component. The weak intermolecular hydrogen bonds of PMMA is responsible for the disappearance of functional groups of PMMA in the polymer blend [37]. Furthermore, the obtained FTIR spectrum demonstrates shifts of some band positions and changes in the intensities of some other bands compared with pure PMMA and PVA polymeric thin films. These shifts and the increase in intensities of some bands are attributed to the strong intramolecular interactions in (PVA-PMMA) blends. For (PMMA-PVA) polymeric thin films, vibrational band at 667 cm -1 could be ascribed to the (C-O) bending vibration. Whereas the vibrational band located at 743 cm -1 could be attributed to the bending vibration mode of (C-H) bond. Additionally, the vibrational band positioned at 1213 cm -1 may be credited to the (C-O) bond stretching. Moreover, vibrational bands at 1713 cm -1 could be assigned to the stretching modes of carbonyl (C=O) groups [37]. Lastly, The broad band at 3020 cm −1 indicates the presence of the (C-H) and (O-H) stretching vibration. The increase and decrease in the peak intensities of the whole FTIR spectra of (PMMA-PVA) polymeric thin films is mainly due to the intermolecular bonding between the PMMA and PVA.
at 667 cm could be ascribed to the (C-O) bending vibration. Whereas the vibrational band located at 743 cm -1 could be attributed to the bending vibration mode of (C-H) bond. Additionally, the vibrational band positioned at 1213 cm -1 may be credited to the (C-O) bond stretching. Moreover, vibrational bands at 1713 cm -1 could be assigned to the stretching modes of carbonyl (C=O) groups [37]. Lastly, The broad band at 3020 cm −1 indicates the presence of the (C-H) and (O-H) stretching vibration. The increase and decrease in the peak intensities of the whole FTIR spectra of (PMMA-PVA) polymeric thin films is mainly due to the intermolecular bonding between the PMMA and PVA.

FTIR Spectra of (PMMA-PVA)/TiO2 Nanocomposite Thin Films
FTIR is performed to investigate the vibrational bands of polymerized thin films. The positions of the peaks of the FTIR patterns are found to shift due to the incorporation of TiO2-NPs into (PMMA-PVA) polymeric thin films. Figure 15 shows FTIR spectra of

FTIR Spectra of (PMMA-PVA)/TiO 2 Nanocomposite Thin Films
FTIR is performed to investigate the vibrational bands of polymerized thin films. The positions of the peaks of the FTIR patterns are found to shift due to the incorporation of TiO 2 -NPs into (PMMA-PVA) polymeric thin films. Figure 15 shows FTIR spectra of (PMMA-PVA)/TiO 2 nanocomposite thin films with (wt.% = 0, 2, 4, 8, and 16%) of TiO 2 -NPs incorporated for a wavenumber range (500-4000 cm -1 ). Figure 16a shows FTIR spectra of (PMMA-PVA)/TiO 2 nanocomposite thin films for a wavenumber range (500-1500 cm −1 ). Clearly, the FTIR spectra have three peaks at 1214, 745, and 667 cm -1 . The band at 667 cm −1 is assigned to the bending vibration mode of (C-O) bending [23]. Additionally, the band at 745 cm −1 corresponds to the vibration mode of (C-H) bond [23]. Furthermore, the band at 1214 cm −1 is associated with the strong stretch bending vibration mode of the (C-O) bond [38]. The striking observation of FTIR spectra of all (PMMA-PVA)/TiO 2 nanocomposite thin films is the broadness and shifting to a higher wavenumber as TiO 2 -NPs contents in (PMMA-PVA) polymeric thin films are increased. The new bound of (PMMA-PVA)/TiO 2 nanocomposite thin films located at 1150 cm −1 is due to stretching and symmetric bending vibration that may be assigned to the Ti-O bond. Figure 16b shows FTIR spectra of (PMMA-PVA)/TiO 2 nanocomposite thin films for a wavenumber range (1500-2500 cm −1 ). Clearly, the FTIR spectra has one peak at 1725 cm −1 . The broad band at 1725 cm −1 is attributed to the stretching modes of carbonyl (C=O) group [6,23]. Figure 16c shows FTIR spectra of (PMMA-PVA)/TiO 2 nanocomposite thin films for a wavenumber range (2500-4000 cm −1 ). Clearly, the FTIR spectra has two peaks at 3020 and 2952 cm −1 . The broad band at 3020 cm −1 indicates the presence of the free hydroxyl (OH) groups and the stretching vibration of (C-H) [23]. Therefore, disturbance of the bonds and the formation of new bonds leads to the broadening and shifting of the peaks. Theoretically it has been predicted that oxygen vacancies in rutile TiO 2 causes lattice deformation and effectively narrows down the band gap [34]. Furthermore, the new band at 2952 cm −1 is associated with the strong stretching mode of the (C-H) binding [6,23,38]. The intensity of the peaks at 1725 and 2952 cm −1 are observed to decrease upon increasing TiO 2 -NPs contents. The reduction of the intensities of the peaks in the entire FTIR spectra is expected and it is attributed to the intermolecular bonding between the constituents of (PMMA-PVA)/TiO 2 nanocomposite thin films. shows FTIR spectra of (PMMA-PVA)/TiO2 nanocomposite thin films for a wavenumber range (2500-4000 cm −1 ). Clearly, the FTIR spectra has two peaks at 3020 and 2952 cm −1 . The broad band at 3020 cm −1 indicates the presence of the free hydroxyl (OH) groups and the stretching vibration of (C-H) [23]. Therefore, disturbance of the bonds and the formation of new bonds leads to the broadening and shifting of the peaks. Theoretically it has been predicted that oxygen vacancies in rutile TiO2 causes lattice deformation and effectively narrows down the band gap [34]. Furthermore, the new band at 2952 cm −1 is associated with the strong stretching mode of the (C-H) binding [6,23,38]. The intensity of the peaks at 1725 and 2952 cm −1 are observed to decrease upon increasing TiO2-NPs contents. The reduction of the intensities of the peaks in the entire FTIR spectra is expected and it is attributed to the intermolecular bonding between the constituents of (PMMA-PVA)/TiO2 nanocomposite thin films.   3.5. Thermogravimetric (TGA) Analysis of (PMMA-PVA)/TiO 2 Nanocomposite Thin Films Figure 17 shows the thermogravimetric thermograms of (PMMA-PVA)/TiO 2 nanocomposites with different concentrations of TiO 2 -NPs. Thermal stability is investigated by employing TGA analysis at temperatures up to 400 • C. The TGA curves of (PMMA-PVA)/TiO 2 nanocomposites thin films show weight loss (WL) steps at different temperatures. The TGA profiles of nanocomposite has two WL steps at 110 and 250 • C regardless of the degree of incorporation of TiO 2 -NPs. First and second WL are insignificantly shifted toward lower and higher temperatures indicating the influence of the change of intermolecular and intramolecular bonding. Clearly, the weight loss of pure (PMMA-PVA) polymeric thin films is observed to be about 92% at 400 • C. This value decreases as TiO 2 -NPs contents in polymeric matrix is increased. It attains a minimum value of 17% as TiO 2 -NPs concetration in the polymeric thin film is increased to 16%. The WL of the nanocomposites is inversely proportional to their wt.% of TiO 2 -NPs content. Conveniently, (PMMAPVA)/TiO 2 nanocomposite materials are found to be thermally stable at temperatures below 110 • C. In spite of the slight and negligible slope in TGA curve below 110 • C which is mostly due to water or solvent adsorption and can be easily tackled, most of the practical optical applications can be performed below this temperature. Blending of PVA and PMMA reduces the thermal stabilities of both polymers. However, the presence of TiO 2 nanoparticles improves their thermal stabilities. Moreover, TiO 2 -NPs also influence the volatilization of the degradation products from the blend, acted as degradation catalyst and retarded the escape of volatile degradation products [39].

Scanning Electron Microscope (SEM)
The surface morphology of thin films is inspected using Scanning Electron Microscopy (SEM). Surface morphology of (PMMA-PVA)/TiO2 nanocomposite thin films at different concentrations of TiO2-NPs at a 100-μm magnification are presented in Figure 18. Figure 18a shows that the nanocomposite thin films of PMMA-PVA exhibit an amorphous nature with a smooth surface. Figure 18(b-e) show the TiO2-NPs immersed homogenously on the surface of the thin film matrix. The observed TiO2-NPs dimension is within the average particle size between (100-500) nm in diameter. Furthermore, SEM was used to examine the morphology and dispersion of TiO2-NPs on the surface of PMMA-PVA films. The SEM images indicate a good dispersion of TiO2-NPs on the surface of the PMMA-PVA polymeric matrix. This provides substantial evidence of the validity of our synthesis process of obtaining TiO2-NPs.

Scanning Electron Microscope (SEM)
The surface morphology of thin films is inspected using Scanning Electron Microscopy (SEM). Surface morphology of (PMMA-PVA)/TiO 2 nanocomposite thin films at different concentrations of TiO 2 -NPs at a 100-µm magnification are presented in Figure 18. Figure 18a shows that the nanocomposite thin films of PMMA-PVA exhibit an amorphous nature with a smooth surface. Figure 18b-e show the TiO 2 -NPs immersed homogenously on the surface of the thin film matrix. The observed TiO 2 -NPs dimension is within the average particle size between (100-500) nm in diameter. Furthermore, SEM was used to examine the morphology and dispersion of TiO 2 -NPs on the surface of PMMA-PVA films. The SEM images indicate a good dispersion of TiO 2 -NPs on the surface of the PMMA-PVA polymeric matrix. This provides substantial evidence of the validity of our synthesis process of obtaining TiO 2 -NPs.

Conclusion
In summary, (PMMA-PVA)/TiO2 nanocomposite thin films doped with different concentrations of TiO2-NPs and ranging from 0 to 16% are synthesized and deposited on glass substrates via a dip-coating technique. As-grown thin films are investigated to elucidate the spectral behavior of key optical parameters such as transmittance, reflectance, absorption coefficient, optical constants, and optical dielectric functions. Furthermore, a combination of classical models such as Tauc, Urbach, Spitzer-Fan, and Drude models are applied to calculate the optical band gap energy and optoelectronic parameters of the doped polymerized thin films. The transmittance decreases dramatically in the high-absorption region (UV region, λ ≤ 350 ). The transmittance values of undoped (PMMA-PVA) polymeric thin film at λ = 550 nm is found to be about 91.6%. Insertion (wt.% = 2, 4, 8, and 16%) of TiO2-NPs lead to a decrease in transmittance values to 90, 89, 87, and 81% at λ = 550 nm, respectively. Therefore, (PMMA-PVA)/TiO2 exhibit good optical transparency in the visible region. Furthermore, the calculated refractive index of pure (PMMA-PVA) polymeric thin film is found to exhibit values ranging between 1.5 and 1.85. Interestingly, increasing TiO2-NPs contents in PMMA-PVA polymeric thin films lead to the increase in refractive index values. The obtained high refractive indices of both as-grown thin films indicate that they could be key candidates for strong optical confinement applications and enhance the optical intensities of nonlinear interactions in optical components of modern devices. Moreover, the optical band gap energy of undoped (PMMA-PVA) polymeric thin film is found to be 4.101 eV. It slightly decreases as (TiO2-NPs) doping levels introduced in (PMMA-PVA) polymeric thin films are increased. The high transmittance, wide bandgap energy, and high refractive index indicate that these films could be employed in the fabrication of a wide range of optoelectronic devices. The thermal stability of both asprepared thin films is investigated by measuring the TGA thermograms. Providentially, the nanocomposite thin films are thermally stable at temperatures below 110 °C. Most of

Conclusions
In summary, (PMMA-PVA)/TiO 2 nanocomposite thin films doped with different concentrations of TiO 2 -NPs and ranging from 0 to 16% are synthesized and deposited on glass substrates via a dip-coating technique. As-grown thin films are investigated to elucidate the spectral behavior of key optical parameters such as transmittance, reflectance, absorption coefficient, optical constants, and optical dielectric functions. Furthermore, a combination of classical models such as Tauc, Urbach, Spitzer-Fan, and Drude models are applied to calculate the optical band gap energy and optoelectronic parameters of the doped polymerized thin films. The transmittance decreases dramatically in the high-absorption region (UV region, λ ≤ 350 nm). The transmittance values of undoped (PMMA-PVA) polymeric thin film at λ = 550 nm is found to be about 91.6%. Insertion (wt.% = 2, 4, 8, and 16%) of TiO 2 -NPs lead to a decrease in transmittance values to 90, 89, 87, and 81% at λ = 550 nm, respectively. Therefore, (PMMA-PVA)/TiO 2 exhibit good optical transparency in the visible region. Furthermore, the calculated refractive index of pure (PMMA-PVA) polymeric thin film is found to exhibit values ranging between 1.5 and 1.85. Interestingly, increasing TiO 2 -NPs contents in PMMA-PVA polymeric thin films lead to the increase in refractive index values. The obtained high refractive indices of both as-grown thin films indicate that they could be key candidates for strong optical confinement applications and enhance the optical intensities of nonlinear interactions in optical components of modern devices. Moreover, the optical band gap energy of undoped (PMMA-PVA) polymeric thin film is found to be 4.101 eV. It slightly decreases as (TiO 2 -NPs) doping levels introduced in (PMMA-PVA) polymeric thin films are increased. The high transmittance, wide bandgap energy, and high refractive index indicate that these films could be employed in the fabrication of a wide range of optoelectronic devices. The thermal stability of both asprepared thin films is investigated by measuring the TGA thermograms. Providentially, the nanocomposite thin films are thermally stable at temperatures below 110 • C. Most of the optical applications involving thin films can be performed at temperatures close to 110 • C. Our detailed and comprehensive investigations of the optical, lattice dynamical, and thermal properties of (PMMAPVA)/TiO 2 nanocomposite thin films reveal that they could be utilized in manufacturing realistic scaled optoelectronic and photonic devices. To elucidate a deeper understanding of the vibrational modes of (PMMA-PVA)/TiO 2 nanocomposite thin films, we carry out FTIR measurements. We identify and interpret all vibrational bands associated with formation, rotation, and twisting of different bonds involved in the investigated polymerized thin films.