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Structure and properties of the pure and Pr-doped Ge25Ga5Se70 and Ge30Ga5Se65 glasses
Affiliation:

a Department of General and of Inorganic Chemistry, University of Pardubice, Legions Sq. 565, 53210, Pardubice, Czech Republic

b Joint Laboratory of Solid State Chemistry, Acad. Sci. of Czech Republic, University of Pardubice, 53210, Pardubice, Czech Republic

Abstract:The Ge25Ga5Se70 and Ge30Ga5Se65 pure and Pr3+-doped glasses were prepared by direct synthesis from elements and PrCl3. It was found that up to 1 mol% PrCl3 can be introduced in the Ge25Ga5Se70 and Ge30Ga5Se65 glasses. Both types of glasses with overstoichiometric and substoichiometric content of Se were homogeneous and of black color. The optical energy gap is Eoptg=2.10 eV, and the glass transition temperature is Tg=543 K for Ge25Ga5Se70 and Tg=633 K for Ge30Ga5Se65. The long-wavelength absorption edge is near 14 μm and it corresponds to multiphonon processes. Doping by Pr3+ ions creates absorption bands in transmission spectra, which can be assigned to the electron transitions from the ground 3H4 level to the higher energy levels of Pr3+ ions 3H5, 3H6, 3F2, 3F3 and 3F4, respectively. By excitation with YAG:Nd laser line (1064 nm), two intense luminescence bands (1343 and 1601 nm) were excited. The first band can be ascribed to electron transitions between 1G4 and 3H5 energy levels of Pr3+ ions. Full width at half of maximum (FWHM) of the intensity of luminescence was found to be not, vert, similar70 nm for (Ge25Ga5Se70)1 ? x(PrCl3)x and (Ge30Ga5Se65)1 ? x(PrCl3)x glasses. The FWHM in selenide glasses is lower than in halide and sulphide glasses. The second luminescence band (1601 nm) can be probably ascribed to the transitions between 3F3 and 3H4 energy levels of Pr3+ ions. The absorption and luminescence spectra of Pr3+ ions in studied glasses are slightly influenced by stoichiometry of glassy matrix. The Raman spectra of studied glasses were deconvoluted and assignment of Raman bands to individual vibration modes of basic structural units was suggested. The structure of studied glasses is mainly formed by corner-sharing and edge-sharing GeSe4 tetrahedra. The vibration modes of Ga-containing structural units were not found, they are apparently overlapping with Ge-containing structural units due to small difference between atomic weights of Ge and Ga. In the glasses with substoichiometry of Se, the Ge–Ge bonds of Ge2Se6 structural units were found. In Se-rich glasses the Se–Se vibration modes were found. In all studied glasses also ‘wrong' bonds between like atoms were found in small amounts. Maximum phonon energy of studied glasses is not, vert, similar320 cm?1.
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