Physical review. B, Condensed matter · 1993 · 122 citations · 34 references
Natural SciencesChemistryMaterials ScienceMaterials ChemistryOptical MaterialsThin FilmsConducting PolymersInfrared SpectroscopyOptical Properties Of MaterialsOptical Thin FilmsSurface PhysicsThin Film Optical PropertiesConductivityDielectric FunctionOptical ConductivityOptical Dielectric FunctionOptical ReflectanceOptical Thin Film CharacterizationPolyanilineReflectance
Recent progress in the processing of conducting polyaniline (PANI) protonated with functionalized sulfonic acids [such as camphor sulfonic acid (CSA)] has enabled the fabrication of high-quality, homogeneous films with excellent surface quality. We present measurements of the reflectivity of such PANI-CSA films over a wide spectral range (0.006--6 eV) at temperatures from 10 to 300 K. The reflectance spectra of PANI-CSA are characterized by metal-like signatures in the infrared (IR), including high reflectance in far IR and a plasma resonance around 1.2 eV. However, the optical conductivity \ensuremath{\sigma}(\ensuremath{\omega}) and the real part of the dielectric function, ${\mathrm{\ensuremath{\varepsilon}}}_{1}$(\ensuremath{\omega}), are not typical of a Drude metal; \ensuremath{\sigma}(\ensuremath{\omega}) is suppressed below the Drude extrapolation as \ensuremath{\omega}\ensuremath{\rightarrow}0 with a peak around 0.2 eV, and ${\mathrm{\ensuremath{\varepsilon}}}_{1}$(\ensuremath{\omega})>0 below 0.2 eV. These features arise from disorder-induced localization (Anderson localization) in PANI-CSA. We present a quantitative analysis of \ensuremath{\sigma}(\ensuremath{\omega}) and ${\mathrm{\ensuremath{\varepsilon}}}_{1}$(\ensuremath{\omega}) in terms of the localization-modified Drude model. The analysis indicates that the mean free path is approximately 7 \AA{}, comparable to the structural repeat unit along the PANI chain, implying that PANI-CSA is a disordered metal on the metal-insulator boundary.
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Introduction to Solid State Physics
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