<p>The X-ray diffraction patterns of vanadium pentoxide (V<sub>2</sub>O<sub>5</sub>) films, deposited by flash evaporation on glass slides upheld at 400 °C, reveal orthorhombic <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\alpha\)</EquationSource> </InlineEquation>-V<sub>2</sub>O<sub>5</sub>with a prominent (001)-peak. The normal-incidence transmittance-wavelength <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\((T_{\exp } (\lambda ) - \lambda )\)</EquationSource> </InlineEquation> spectra of the {air/flash-evaporated V<sub>2</sub>O<sub>5</sub> film/glass slide/air} samples had been collected in the <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\lambda\)</EquationSource> </InlineEquation>-range 400–1100 nm. There <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(T_{\exp } (\lambda ) - \lambda\)</EquationSource> </InlineEquation> spectra exhibit a steep drop at, <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\lambda \approx 550\,{\text{nm}}\)</EquationSource> </InlineEquation> above which few broad, maxima/minima are displayed. The point-wise unconstrained minimization approach (PUMA) was implemented to fit the <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\({T}_{\text{exp}}\left(\lambda \right)-\lambda\)</EquationSource> </InlineEquation> data to a theoretical transmittance formula, <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\({T}_{\text{theor}}\left(\lambda ,{n}_{s}\left(\lambda \right);n\left(\lambda \right), \kappa \left(\lambda \right), d\right)\)</EquationSource> </InlineEquation>. The analysis yielded a value for the thickness <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\((d\)</EquationSource> </InlineEquation>) of the <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\alpha\)</EquationSource> </InlineEquation>-V<sub>2</sub>O<sub>5</sub> films and for the spectral dispersion of its refractive index <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(n(\lambda )\)</EquationSource> </InlineEquation> and extinction coefficient <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\kappa \left(\lambda \right)\)</EquationSource> </InlineEquation>, with <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\({n}_{s}\left(\lambda \right)\)</EquationSource> </InlineEquation>, the refractive index of glass slides was pre-calculated at each <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(\lambda\)</EquationSource> </InlineEquation>. The extracted <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(n\left(\lambda \right)-\lambda\)</EquationSource> </InlineEquation> data fit well a two-constant Wemple-DiDomenico (WDD) equation in the film’s transparent and weak absorption regions. The <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(\alpha \left(h\nu \right)\)</EquationSource> </InlineEquation>, the absorption coefficient was calculated from <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(\alpha \left(h\nu \right)\equiv 4\pi \kappa \left(\lambda \right)/\lambda\)</EquationSource> </InlineEquation> at each photon energy (<InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(h\nu\)</EquationSource> </InlineEquation>). In this work, the <InlineEquation ID="IEq18"> <EquationSource Format="TEX">\(\alpha \left(h\nu \right)\)</EquationSource> </InlineEquation>-<InlineEquation ID="IEq19"> <EquationSource Format="TEX">\(h\nu\)</EquationSource> </InlineEquation> data covering the band-tail and strong absorption regions, together with their overlapped region, were analyzed by a three-parameter Dilogarithm function <InlineEquation ID="IEq20"> <EquationSource Format="TEX">\({\text{Li}}_{2} {\text{(h}}\nu {; }\alpha_{0} {,}\Gamma_{{\text{U}}} {\text{,E}}_{{\text{g}}} {)}\)</EquationSource> </InlineEquation> to determine simultaneously <InlineEquation ID="IEq21"> <EquationSource Format="TEX">\(\alpha_{0} ,\Gamma_{U}\)</EquationSource> </InlineEquation> (Urbach-tail energy), and <InlineEquation ID="IEq22"> <EquationSource Format="TEX">\({E}_{\text{g}}\)</EquationSource> </InlineEquation> (bandgap energy). For comparison, the <InlineEquation ID="IEq23"> <EquationSource Format="TEX">\(\alpha \left(h\nu \right)-h\nu\)</EquationSource> </InlineEquation> data were fitted to the Tauc and Urbach <InlineEquation ID="IEq24"> <EquationSource Format="TEX">\(\alpha \left(h\nu \right)\)</EquationSource> </InlineEquation>-formulas in their limited spectral regions to find <InlineEquation ID="IEq25"> <EquationSource Format="TEX">\({E}_{\text{g}}\)</EquationSource> </InlineEquation> and <InlineEquation ID="IEq26"> <EquationSource Format="TEX">\({\Gamma }_{\text{U}}\)</EquationSource> </InlineEquation> separately, a procedure that involves complexity in picking properly the individual spectral range. Such problematic features are overcome in the three-parameter <InlineEquation ID="IEq27"> <EquationSource Format="TEX">\(\alpha \left(h\nu \right)\)</EquationSource> </InlineEquation>-Dilogarithm model.</p>

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Validity of a three-parameter dilogarithm dispersion function for the description of the energy dependence of the absorption coefficient of flash-evaporated V2O5 films

  • Mahmoud H. Saleh,
  • Tariq M. Al-Daraghmeh,
  • Basim Bulos,
  • Bashar Lahlouh,
  • Omar S. Mansour,
  • Nidal M. Ershaidat,
  • Mousa M. Abdul-Gader Jafar

摘要

The X-ray diffraction patterns of vanadium pentoxide (V2O5) films, deposited by flash evaporation on glass slides upheld at 400 °C, reveal orthorhombic \(\alpha\) -V2O5with a prominent (001)-peak. The normal-incidence transmittance-wavelength \((T_{\exp } (\lambda ) - \lambda )\) spectra of the {air/flash-evaporated V2O5 film/glass slide/air} samples had been collected in the \(\lambda\) -range 400–1100 nm. There \(T_{\exp } (\lambda ) - \lambda\) spectra exhibit a steep drop at, \(\lambda \approx 550\,{\text{nm}}\) above which few broad, maxima/minima are displayed. The point-wise unconstrained minimization approach (PUMA) was implemented to fit the \({T}_{\text{exp}}\left(\lambda \right)-\lambda\) data to a theoretical transmittance formula, \({T}_{\text{theor}}\left(\lambda ,{n}_{s}\left(\lambda \right);n\left(\lambda \right), \kappa \left(\lambda \right), d\right)\) . The analysis yielded a value for the thickness \((d\) ) of the \(\alpha\) -V2O5 films and for the spectral dispersion of its refractive index \(n(\lambda )\) and extinction coefficient \(\kappa \left(\lambda \right)\) , with \({n}_{s}\left(\lambda \right)\) , the refractive index of glass slides was pre-calculated at each \(\lambda\) . The extracted \(n\left(\lambda \right)-\lambda\) data fit well a two-constant Wemple-DiDomenico (WDD) equation in the film’s transparent and weak absorption regions. The \(\alpha \left(h\nu \right)\) , the absorption coefficient was calculated from \(\alpha \left(h\nu \right)\equiv 4\pi \kappa \left(\lambda \right)/\lambda\) at each photon energy ( \(h\nu\) ). In this work, the \(\alpha \left(h\nu \right)\) - \(h\nu\) data covering the band-tail and strong absorption regions, together with their overlapped region, were analyzed by a three-parameter Dilogarithm function \({\text{Li}}_{2} {\text{(h}}\nu {; }\alpha_{0} {,}\Gamma_{{\text{U}}} {\text{,E}}_{{\text{g}}} {)}\) to determine simultaneously \(\alpha_{0} ,\Gamma_{U}\) (Urbach-tail energy), and \({E}_{\text{g}}\) (bandgap energy). For comparison, the \(\alpha \left(h\nu \right)-h\nu\) data were fitted to the Tauc and Urbach \(\alpha \left(h\nu \right)\) -formulas in their limited spectral regions to find \({E}_{\text{g}}\) and \({\Gamma }_{\text{U}}\) separately, a procedure that involves complexity in picking properly the individual spectral range. Such problematic features are overcome in the three-parameter \(\alpha \left(h\nu \right)\) -Dilogarithm model.