Er^3+-doped tellurite glasses with molar compositions of xNb2O5 - (14.7 - x)Na2O-10ZnO-5K2O-10GeO260TeO2-0.3Er2O3 (x = 0, 3, 5, 7 and 9) have been investigated for developing 1.5 μm fibre and planar amplifiers. ...Er^3+-doped tellurite glasses with molar compositions of xNb2O5 - (14.7 - x)Na2O-10ZnO-5K2O-10GeO260TeO2-0.3Er2O3 (x = 0, 3, 5, 7 and 9) have been investigated for developing 1.5 μm fibre and planar amplifiers. The effects of Nb2O5 on the thermal stability and optical properties of Er^3+-doped tellurite glasses have been discussed. It is noted that the incorporation of Nb205 (x=5) increases the thermal stability of tellurite glasses significantly. Er^3+-doped niobium tellurite glasses exhibit a large stimulated emission cross-section (7.2×10^-21 - 10.7×10^-21 cm^2) and the gain bandwidth, FWHM×σ^peak (274 ×10^-28 - 480×10^-28 cm^3), which are significantly higher than that of silicate and phosphate glasses. In addition, the intensity of upconversion luminescence of the Er3+-doped niobium tellurite glasses decreases rapidly with increasing Nb2O5 content. As a result, Er^3+-doped niobium tellurite glasses might be a potential candidate for developing laser or optical amplifier devices.展开更多
The Cs_(2)NaInCl_(6) double perovskite is one of the most promising lead-free perovskites due to its exceptional stability and straightforward synthesis.However,it faces challenges related to inefficient photoluminesc...The Cs_(2)NaInCl_(6) double perovskite is one of the most promising lead-free perovskites due to its exceptional stability and straightforward synthesis.However,it faces challenges related to inefficient photoluminescence.Doping and high pressure are employed to tailor the optical properties of Cs_(2)NaInCl_(6).Herein,Sb^(3+)doped Cs_(2)NaInCl_(6)(Sb^(3+):Cs_(2)NaInCl_(6)) was synthesized and it exhibits blue emission with a photoluminescence quantum yield of up to 37.3%.Further,by employing pressure tuning,a blue stable emission under a very wide range from 2.7 GPa to 9.8 GPa is realized in Sb^(3+):Cs_(2)NaInCl_(6).Subsequently,the emission intensity of Sb^(3+):Cs_(2)NaInCl_(6) experiences a significant increase(3.3 times)at 19.0 GPa.It is revealed that the pressure-induced distinct emissions can be attributed to the carrier self-trapping and detrapping between Cs_(2)NaInCl_(6) and Sb^(3+).Notably,the lattice compression in the cubic phase inevitably modifies the band gap of Sb^(3+):Cs_(2)NaInCl_(6).Our findings provide valuable insights into effects of the high pressure in further boosting unique emission characteristics but also offer promising opportunities for development of doped double perovskites with enhanced optical functionalities.展开更多
基金Project supported by the National Natural Science Foundation of China (Grant No 50472053), New Century Excellent Talent Program in University of China (Grant Nos 04-0821 and 04-0823), Guangzhou Science and Technology Program of China (Grant No 2004Z2-D0131), and Youth Nature Science Foundation of South China University of Technology (Grant No 123-E5040900).
文摘Er^3+-doped tellurite glasses with molar compositions of xNb2O5 - (14.7 - x)Na2O-10ZnO-5K2O-10GeO260TeO2-0.3Er2O3 (x = 0, 3, 5, 7 and 9) have been investigated for developing 1.5 μm fibre and planar amplifiers. The effects of Nb2O5 on the thermal stability and optical properties of Er^3+-doped tellurite glasses have been discussed. It is noted that the incorporation of Nb205 (x=5) increases the thermal stability of tellurite glasses significantly. Er^3+-doped niobium tellurite glasses exhibit a large stimulated emission cross-section (7.2×10^-21 - 10.7×10^-21 cm^2) and the gain bandwidth, FWHM×σ^peak (274 ×10^-28 - 480×10^-28 cm^3), which are significantly higher than that of silicate and phosphate glasses. In addition, the intensity of upconversion luminescence of the Er3+-doped niobium tellurite glasses decreases rapidly with increasing Nb2O5 content. As a result, Er^3+-doped niobium tellurite glasses might be a potential candidate for developing laser or optical amplifier devices.
基金supported by the National Key Research and Development Program of China(Grant Nos.2021YFA1400200 and2021YFA0718701)the National Natural Science Foundation of China(Grant Nos.U2032127,11904322,12104411,12174347)+4 种基金the Natural Science Foundation of Henan province of China(Grant No.202300410356)the China Postdoctoral Science Foundation(Grant Nos.2019M652560 and 2020M682326)the CAS Interdisciplinary Innovation Team(Grant No.JCTD-2019-01)the Postdoctoral Research Grant in Henan Province(Grant No.1902013)the Science Foundation for Highlevel Talents of Wuyi University(Grant No.2021AL019)。
文摘The Cs_(2)NaInCl_(6) double perovskite is one of the most promising lead-free perovskites due to its exceptional stability and straightforward synthesis.However,it faces challenges related to inefficient photoluminescence.Doping and high pressure are employed to tailor the optical properties of Cs_(2)NaInCl_(6).Herein,Sb^(3+)doped Cs_(2)NaInCl_(6)(Sb^(3+):Cs_(2)NaInCl_(6)) was synthesized and it exhibits blue emission with a photoluminescence quantum yield of up to 37.3%.Further,by employing pressure tuning,a blue stable emission under a very wide range from 2.7 GPa to 9.8 GPa is realized in Sb^(3+):Cs_(2)NaInCl_(6).Subsequently,the emission intensity of Sb^(3+):Cs_(2)NaInCl_(6) experiences a significant increase(3.3 times)at 19.0 GPa.It is revealed that the pressure-induced distinct emissions can be attributed to the carrier self-trapping and detrapping between Cs_(2)NaInCl_(6) and Sb^(3+).Notably,the lattice compression in the cubic phase inevitably modifies the band gap of Sb^(3+):Cs_(2)NaInCl_(6).Our findings provide valuable insights into effects of the high pressure in further boosting unique emission characteristics but also offer promising opportunities for development of doped double perovskites with enhanced optical functionalities.