“…Our results fall into two categories: the first focuses on the physical characteristics of the new glassy matrix (80 Sb 2 O 3 -10 ZnBr 2 -10 KCl), and the second shows the up-conversion emission of the matrix doped with trivalent lanthanides and the same spectrum of the Yb:Er co-doped glass. Main physical properties of this glass are gathered at tables 1a and 1b.They are close to those reported for other antimonite glasses [37][38][39][40][41][42][43][44][45][46]. The Yb 3+ / Er 3+ co-doping results in the population of two additional levels 2 H 11/2 and 4 F 9/2 and two additional emission lines, by comparison to the glass doped only with Er 3+ .…”
Section: Resultssupporting
confidence: 88%
“…There may be a possibility of existence of antimony ions in the Sb 5+ state and participate in the glass network forming with Sb 5+ O 4 structural units may enhance the nonlinear optical properties [48].Antimonite glasses are based on Sb 2 O 3 as a glass former. They belong to the group of HMOG and have been reported in a large number of vitreous systems [37][38][39][40][41][42][43][44][45][46]. They exhibit large linear and non-linear refractive index.…”
The up-conversion emission of Nd 3+ , Sm 3+ and Er 3+ has been studied in a new halogenoantimonite glass with the chemical composition 80 Sb 2 O 3 -10 ZnBr 2 -10 KCl. Doping concentration was 0.2 mol% of lanthanide (Ln) ions. Rare earths were introduced as fluorides LnF 3 that were further converted into oxides. Main physical properties of base glass were measured, including density, thermal expansion, characteristic temperatures, refractive index and optical transmission. The amount of residual hydroxyls was calculated from the OH absorption band around 3000 nm. The recorded up-conversion emission lines are λ em = 536 nm for Nd 3+ pumped at 805 nm; λ em = 563 nm, 600 nm, 631 nm and 645 nm for Sm 3+ pumped at 945 nm; λ em = 531 nm for Er 3+ pumped at 798 nm. Co-doped glass (0.1 Yb 3+ + 0.1 Er 3+ ) pumped at 980 nm has three emission lines at 524 nm, 545 nm and 650 nm. Corresponding transitions have been identified and the mechanisms ruling the up-conversion process is discussed. They include excited state absorption (ESA), energy transfer (ET) cooperative energy transfer (CET), emission assisted by phonon (EAP), multiphonon relaxation (MR) and cross-relaxation (CR).
“…Our results fall into two categories: the first focuses on the physical characteristics of the new glassy matrix (80 Sb 2 O 3 -10 ZnBr 2 -10 KCl), and the second shows the up-conversion emission of the matrix doped with trivalent lanthanides and the same spectrum of the Yb:Er co-doped glass. Main physical properties of this glass are gathered at tables 1a and 1b.They are close to those reported for other antimonite glasses [37][38][39][40][41][42][43][44][45][46]. The Yb 3+ / Er 3+ co-doping results in the population of two additional levels 2 H 11/2 and 4 F 9/2 and two additional emission lines, by comparison to the glass doped only with Er 3+ .…”
Section: Resultssupporting
confidence: 88%
“…There may be a possibility of existence of antimony ions in the Sb 5+ state and participate in the glass network forming with Sb 5+ O 4 structural units may enhance the nonlinear optical properties [48].Antimonite glasses are based on Sb 2 O 3 as a glass former. They belong to the group of HMOG and have been reported in a large number of vitreous systems [37][38][39][40][41][42][43][44][45][46]. They exhibit large linear and non-linear refractive index.…”
The up-conversion emission of Nd 3+ , Sm 3+ and Er 3+ has been studied in a new halogenoantimonite glass with the chemical composition 80 Sb 2 O 3 -10 ZnBr 2 -10 KCl. Doping concentration was 0.2 mol% of lanthanide (Ln) ions. Rare earths were introduced as fluorides LnF 3 that were further converted into oxides. Main physical properties of base glass were measured, including density, thermal expansion, characteristic temperatures, refractive index and optical transmission. The amount of residual hydroxyls was calculated from the OH absorption band around 3000 nm. The recorded up-conversion emission lines are λ em = 536 nm for Nd 3+ pumped at 805 nm; λ em = 563 nm, 600 nm, 631 nm and 645 nm for Sm 3+ pumped at 945 nm; λ em = 531 nm for Er 3+ pumped at 798 nm. Co-doped glass (0.1 Yb 3+ + 0.1 Er 3+ ) pumped at 980 nm has three emission lines at 524 nm, 545 nm and 650 nm. Corresponding transitions have been identified and the mechanisms ruling the up-conversion process is discussed. They include excited state absorption (ESA), energy transfer (ET) cooperative energy transfer (CET), emission assisted by phonon (EAP), multiphonon relaxation (MR) and cross-relaxation (CR).
“…Because of these qualities, GeO 2 based glasses are also being used to generate phase gratings directly in optical fibers by UV irradiation [9]. Addition of heavy metal oxides like PbO and Sb 2 O 3 to these glasses further strengthen their second harmonic generation [10] capability and makes the glasses useful for nonlinear optical devices like ultrafast optical switches, power limiters and broad band optical amplifiers operating around 1.5 μm [11,12]. GeO 2 glasses are also well-known glasses for solid electrolyte applications [13] since they exhibit high ionic conductivity.…”
“…In 1996, Hoell et al reported that a small quantity of chloride in 13Na 2 O-11CaO-76SiO 2 (mol%) glass system causes a dramatic change of kinetics and equilibrium conditions for the phase separation process in the glass [18]. Glass formation in the Sb 2 O 3 -CdCl 2 -SrCl 2 ternary system was reported by Iezid et al They exhibited low-phonon energy [19]. Recently, the properties of 70TeO 2 -10Sb 2 O 3 -20PbCl 2 composition are reported [20].…”
a b s t r a c tOxyfluoride glass-ceramics are extensively being investigated for their excellent optical properties and widespread use in photonic applications. But oxychloride systems are scarcely studied although they are potential candidates for those fields. Here we report chloroborosilicate glass system SiO 2 -B 2 O 3 -BaO-K 2 O-Al 2 O 3 -BaCl 2 (mol%) within which BaCl 2 nanocrystals have been generated by melt-quench technique followed by heat treatment. Samples were characterized by differential scanning calorimetry, X-ray diffraction, infrared and UV-vis spectroscopy, elastic constants measurement, etc. Micro-and nanostructures were analyzed by using FESEM, TEM and SAED. Formation and growth mechanism of BaCl 2 nanocrystals have been demonstrated with the help of schematic representations. Size (7-47 nm) and morphology of the nanocrystals were found to be controlled by temperature and heat-treatment time. Activation energy for crystallization was determined by non-isothermal method using DSC and found to be 510 kJ/mol. Chloroborosilicate glasses containing BaCl 2 nanocrystals having low-phonon energy (∼350 cm −1 ) are promising for different photonic applications.
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