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The influence of cation additives on the NIR luminescence intensity of Er~(3+)-doped borate glasses 被引量:1
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作者 周永亮 张晓松 +4 位作者 徐建萍 张忠朋 张高峰 魏凤巍 李岚 《Chinese Physics B》 SCIE EI CAS CSCD 2012年第6期398-402,共页
Er3+-doped 25BaO-(25-x)SiO2-xAl2O3-25B2O3 transparent glasses are prepared with x = 0,12.5 and 25 by a solid-state reaction.The Er-related NIR luminescence intensity,which corresponds to the transition of 4I15/2-4I13/... Er3+-doped 25BaO-(25-x)SiO2-xAl2O3-25B2O3 transparent glasses are prepared with x = 0,12.5 and 25 by a solid-state reaction.The Er-related NIR luminescence intensity,which corresponds to the transition of 4I15/2-4I13/2,is obviously altered with different silicon/aluminum ratios.The Judd-Ofelt parameters of the Er3+ ions are adopted to explain the intensity change in the NIR fluorescence,and the Raman scattering intensity versus the amount of Al and/or Si components are discussed.The spectra of the three samples are quite similar in the peak positions,but different in intensity.The maximal phonon density of state for the samples is calculated from the Raman spectra and is correlated to the NIR luminescence efficiency. 展开更多
关键词 maximal phonon density of state Judd-Ofelt intensity parameter er3+-doped borate glasses
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掺Er^(3+)玻璃的光限幅特性研究 被引量:5
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作者 李玉琼 孙真荣 +2 位作者 康海峰 元以中 王祖赓 《光谱学与光谱分析》 SCIE EI CAS CSCD 北大核心 2007年第1期5-7,共3页
利用波长为532 nm的皮秒脉冲激光,研究了掺Er3+玻璃的光限幅特性和反饱和吸收。当入射功率不断增加且超过一定阈值时,透射功率不再随着入射功率快速增大,而是逐渐趋向于较稳定状态,从而实现了对强激光的光限幅效应。进一步利用布居速率... 利用波长为532 nm的皮秒脉冲激光,研究了掺Er3+玻璃的光限幅特性和反饱和吸收。当入射功率不断增加且超过一定阈值时,透射功率不再随着入射功率快速增大,而是逐渐趋向于较稳定状态,从而实现了对强激光的光限幅效应。进一步利用布居速率方程讨论了其机制并给出了激发态的吸收截面,结果表明激发态吸收是其主要的光限幅机理。 展开更多
关键词 非线性光学 光限幅 er^3+碲酸盐玻璃 激发态吸收
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980nm激光泵浦下掺Er^(3+)碲酸盐玻璃的光子雪崩上转换
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作者 李玉琼 孙真荣 王祖赓 《光谱学与光谱分析》 SCIE EI CAS CSCD 北大核心 2006年第6期977-979,共3页
在980 nm激光二极管的抽运下,掺Er3+碲酸盐玻璃辐射出很强的绿色上转换荧光,荧光强度与抽运功率呈非线性关系,发光强度和积累时间与激光抽运功率的关系研究表明存在雪崩阈值44 mW。发现光子的积累时间(几十毫秒量级)远大于荧光的寿命,... 在980 nm激光二极管的抽运下,掺Er3+碲酸盐玻璃辐射出很强的绿色上转换荧光,荧光强度与抽运功率呈非线性关系,发光强度和积累时间与激光抽运功率的关系研究表明存在雪崩阈值44 mW。发现光子的积累时间(几十毫秒量级)远大于荧光的寿命,且积累时间随抽运功率的增大而减小。与早先报道的690和579 nm抽运波长相比,980 nm是更加有效的抽运波长。 展开更多
关键词 上转换 光子雪崩 er^3+碲酸盐玻璃
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Er^3+ - Yb^3+共掺碲酸盐光纤上转换光谱研究
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作者 李尊 徐善辉 《功能材料》 EI CAS CSCD 北大核心 2007年第A01期220-222,共3页
采用波长为976nm的半导体激光器以透镜耦合方式抽运自制的掺Er^3+ - Yb^3+碲酸盐短光纤,实验中可直接裸眼观测到很强烈的上转换绿色荧光,3dB带宽为20nm,中心波长为546nm,所需光纤长度仅1.8cm,荧光平均波长以及3dB带宽具有不依赖... 采用波长为976nm的半导体激光器以透镜耦合方式抽运自制的掺Er^3+ - Yb^3+碲酸盐短光纤,实验中可直接裸眼观测到很强烈的上转换绿色荧光,3dB带宽为20nm,中心波长为546nm,所需光纤长度仅1.8cm,荧光平均波长以及3dB带宽具有不依赖抽运功率的稳定性,并且分析了上转换绿光的主要发光机理。 展开更多
关键词 上转换荧光 透镜耦合 er^3+ - YB^3+ 共掺碲酸盐光纤
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Growth,structure and spectral characteristics of KEr_(0.1)Yb_(0.9)(WO_4)_2 laser crystal 被引量:1
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作者 张莹 刘景和 +5 位作者 曾繁明 林海 李春 王成伟 张学建 秦杰明 《Journal of Rare Earths》 SCIE EI CAS CSCD 2010年第1期48-53,共6页
The 10 at.% Er3+-doped KYb(WO4)2(KEr0.1Yb0.9(WO4)2) laser crystal with dimensions up to 25 mm×15 mm×10 mm was grown by the Kyropoulos method.The crystal structure was identified as β-KEr0.1Yb0.9(WO4)2 by XR... The 10 at.% Er3+-doped KYb(WO4)2(KEr0.1Yb0.9(WO4)2) laser crystal with dimensions up to 25 mm×15 mm×10 mm was grown by the Kyropoulos method.The crystal structure was identified as β-KEr0.1Yb0.9(WO4)2 by XRD analysis.Through TG-DTA curves,the melting point and transition point of the crystal were determined to be 1058 and 1031 °C,respectively.Infrared spectrum and Raman spectrum were measured,and the vibration frequencies of infrared and Raman active modes for the crystal were assigned.The absorption cross ... 展开更多
关键词 er3+-doped potassium ytterbium tungstate Kyropoulos method STRUCTURE spectral characteristics rare earths
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Multiphoton process and optical amplification in Er^(3+)-Yb^(3+)-doped fiber pumped by Ti:Al_2O_3 tunable laser at 980-nm band
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作者 明海 孙晓泉 +5 位作者 刘宇 董晓鹏 杨宝 谢建平 张运生 耿玉珍 《Chinese Science Bulletin》 SCIE EI CAS 1995年第22期1883-1887,共5页
The .Er<sup>3+</sup>-Yb<sup>3+</sup>-doped fiber has a broadened absorption spectrum, which means the pumping sources can work efficiently from 810 to 1100nm. Among them 980nm is the maximum.ab... The .Er<sup>3+</sup>-Yb<sup>3+</sup>-doped fiber has a broadened absorption spectrum, which means the pumping sources can work efficiently from 810 to 1100nm. Among them 980nm is the maximum.absorption (10 dB/km) wavelength. By energy transferring and multiphoton process, the visible and ultraviolet radiation occurs when the Er<sup>3+</sup>-Yb<sup>3+</sup>-doped fiber is pumped by the laser at 980-nm band. Further researches on the mechanism of the fluorescence of Er<sup>3+</sup>-Yb<sup>3+</sup>-doped silica fiber pumped by Ti: A1<sub>2</sub>O<sub>3</sub> tunable laser at 980-nm band are helpful 展开更多
关键词 MULTIPHOTON process optical amplification Ti:AI2O3 laser er3+-Yb3+-doped fiber.
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Optical Properties of a Novel Trivalent Erbium Ions Doped into Phosphate Glass
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作者 张继森 秦伟平 +4 位作者 张立国 秦冠仕 吴崇锋 赵丹 林海洋 《Journal of Rare Earths》 SCIE EI CAS CSCD 2003年第S1期65-67,共3页
A novel Er (3+)-doped (ZnO)(P_2O_5)(B_2O_3) glass with excellent optical properties was prepared. The glasses were proved to have high stability by the investigation of the durability in boiling water. The properties ... A novel Er (3+)-doped (ZnO)(P_2O_5)(B_2O_3) glass with excellent optical properties was prepared. The glasses were proved to have high stability by the investigation of the durability in boiling water. The properties of their spectra at about 1.5 μm change a lot with the concentrations of both Er (3+) and B_2O_3. Compared with Er (3+)-doped into the borate glass and the zinc phosphate glass,the glass prepared in our laboratory shows a larger quenching concentration and a much broader emission band at 1.54 μm. 展开更多
关键词 OPTICS er3+-doped phosphate glass rare earths
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Multiband infrared luminescence of Er3+-Ho3+-Nd3+/Tm3+- codoped telluride glasses
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作者 Yaojing ZHANG Lu SUN +2 位作者 Ying CHANG Wenbin LI Chun JIANG 《Frontiers of Optoelectronics》 CSCD 2014年第1期74-76,共3页
This paper reports the simultaneous emissions around 1.53, 1.80, 2.10, 2.70 and 3.00 gm in Er3+-Ho3+ - Nd3+/Tm3+-codoped telluride glasses upon excitation of a conventional 808 nm laser diode. Both emission bands ... This paper reports the simultaneous emissions around 1.53, 1.80, 2.10, 2.70 and 3.00 gm in Er3+-Ho3+ - Nd3+/Tm3+-codoped telluride glasses upon excitation of a conventional 808 nm laser diode. Both emission bands of 1.53 and 2.70 gm were assigned to the transitions of 4113/2 -4115/2, 4111/2 -4113/2 of Er++ ions, respectively, the emission near 1.80 gm was assigned to the transition *F4 -4H6 of Tm3+ ions, and the emissions at 2.10 and 3.00 μm arose from the transitions of 5I7 -518, 5I6 -5I7 of Ho3+ ions. The materials are promising for ultra-broad band amplified spontaneous emission optical sources at near and middle infrared region. 展开更多
关键词 multiband luminescence er3+-Ho3+-Nd3+/Tm3+ telluride glass
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Nonlinear optical properties of Er_2O_3-doped 75Nb_2O_5-20TeO_2-5ZnO glasses
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作者 王宇飞 孙真荣 +5 位作者 张诗按 王祖庚 林健 黄文旵 徐至展 李儒新 《Chinese Optics Letters》 SCIE EI CAS CSCD 2004年第2期109-112,共4页
We have performed time-resolved degenerate four-wave mixing (DFWM) experiments in 75Nb2O5-20TeO2-5ZnO glasses doped by Er2O3 at different excitation intensities and lattice temperatures. DFWM signal exhibits three pea... We have performed time-resolved degenerate four-wave mixing (DFWM) experiments in 75Nb2O5-20TeO2-5ZnO glasses doped by Er2O3 at different excitation intensities and lattice temperatures. DFWM signal exhibits three peaks at high excitation intensities, where a main peak appears at zero time delay and two rather weak side peaks locate symmetrically at the negative and positive time delay, respectively. The main peak is attributed to local-field effect and two side peaks are attributed to Coulomb interaction (CI). 展开更多
关键词 DFWM In Nonlinear optical properties of er2O3-doped 75Nb2O5-20TeO2-5ZnO glasses ZnO
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碲化物发光玻璃中银纳米颗粒表面等离激元增强铒离子发光的研究(英文)
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作者 陈晓波 李崧 +9 位作者 赵国营 龙江迷 王水锋 郑东 吴正龙 孟少华 郭敬华 徐玲芝 于春雷 胡丽丽 《光谱学与光谱分析》 SCIE EI CAS CSCD 北大核心 2019年第7期2293-2298,共6页
有趣的贵金属表面等离激元的光学性质,尤其是在发光增强领域的表现,使得它已经成为全球的一个研究热点。表面等离激元就是光与贵金属中的自由电子相互作用时,自由电子和光波电磁场由于共振频率相同而形成的一种集体振荡态。该文研究了... 有趣的贵金属表面等离激元的光学性质,尤其是在发光增强领域的表现,使得它已经成为全球的一个研究热点。表面等离激元就是光与贵金属中的自由电子相互作用时,自由电子和光波电磁场由于共振频率相同而形成的一种集体振荡态。该文研究了碲化物玻璃中银纳米颗粒的表面等离激元共振增强铒离子的发光。我们测量了吸收谱、激发谱、发光谱以及荧光寿命。首先,我们挑选365.5和379.0nm吸收峰作为激发波长测量了385~780nm波长范围的可见发光光谱,发现有4个发光峰,依次位于408.0,525.0,546.0和658.5nm,容易指认出它们依次为铒离子的2H9/2→4I15/2,2H11/2→4I15/2,4S3/2→4I15/2和4F9/2→4I15/2的荧光跃迁;可以计算出[80nm平均粒径纳米银的Er^3+(0.5%)Ag(0.2%):碲化物玻璃的样品A]的上述4个可见发光的峰值强度是[Er^3+(0.5%):碲化物玻璃的样品C]的大约1.44~2.52倍。同时,[50nm平均粒径纳米银的Er^3+(0.5%)Ag(0.2%):碲化物玻璃的样品B]的上述4个可见发光的峰值强度是样品C的大约1.08~1.55倍。随后,我们挑选365.5和379.0nm吸收峰作为激发波长测量了928~1680nm波长范围的近红外发光光谱,发现近红外波段有两个发光峰,位于979.0和1530.0nm,容易指认出它们依次为铒离子的4I11/2→4I15/2和4I13/2→4I15/2的荧光跃迁;同样可以计算出样品A的上述2个近红外发光的峰值强度是样品C的大约1.43~2.14倍。同时,样品B的上述2个近红外发光的峰值强度是样品C的大约1.28~1.82倍。因此,发光的最大增强大约是2.52倍。从荧光寿命动力学实验,我们发现样品A的荧光寿命为τA(550)=43.5μs,样品B的荧光寿命为τB(550)=43.2μs,样品C的荧光寿命为τC(550)=48.6μs。这些实验结果证实了τA≈τB<τC。它意味着样品(B)相对于样品(C)的发光增强是源于自发辐射增强效应。然而,它也意味着样品(A)相对于样品(B)的发光增强是源于纳米银颗粒的粒径尺寸r效应。也就是说当粒径尺寸r增大的时候,散射截面Cs和r^6成正比,而吸收截面Ca和r^3成正比,因此散射截面Cs增大的速度会远大于吸收截面Ca增大的速度,而散射截面Cs是荧光增强的原因,吸收截面Ca是荧光减弱的原因,所以随着银纳米颗粒尺寸的增大,其散射截面占主要部分,当发光材料和金属表面等离子体SP发生耦合时,能量快速的转移到金属表面等离子体SP上,而后被散射到远场,这有利于增强荧光。其综合的结果就导致了发光强度会随r的增大而增强。上述实验的结果对太阳能电池的光伏发电和生物物理应用等领域都有着很好的应用前景。 展开更多
关键词 银纳米颗粒 发光增强 表面等离激元 碲化物的玻璃 铒离子
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