纳米单斜相Gd2O3：Bi3+,Nd3+的燃烧法制备和近红外发光

采用甘氨酸作为燃料,制备了单斜相Gd₂O₃：Bi³⁺,Nd³⁺纳米发光材料。使用X射线粉末衍射仪和TEM对样品的结构和形貌进行了表征,并研究了制备条件对样品的可见及近红外激发和发射光谱、发光强度、荧光寿命等的影响。结果表明,体系中存在高效的Bi³⁺→Nd³⁺能量传递过程,当Bi³⁺和Nd³⁺的掺杂摩尔分数分别为6%和2%时,单斜相Gd₂O₃：Bi³⁺,Nd³⁺荧光粉可以获得最强的近红外光发射。与单掺Nd³⁺的样品相比,单斜相Gd₂O₃中掺杂Bi³⁺和Nd³⁺后,样品的近红外发光增强近20倍。     

Ce3+∶BaF2多晶透明陶瓷的热压烧结法制备

采用沉淀法制备了Ce³⁺∶BaF₂纳米粉体,研究了反应顺序和F^－浓度对沉淀法制备Ce³⁺∶BaF₂粉体的影响,采用XRD、SEM、TEM、ICP等手段对粉体进行了分析。结果表明:采用阴离子滴入阳离子的反应顺序,在较高F^－浓度下制备的粉体保持了单一物相,粉体中稀土离子含量接近于初始掺入量。采用热压法于900 ℃温度同时在模具上施加30 MPa压力的条件下制备了Ce³⁺∶BaF₂多晶透明陶瓷,陶瓷断面SEM结果显示,晶粒内存在闭气孔,陶瓷表面腐蚀后晶界完整清晰。X射线发光谱测试结果显示,Ce³⁺的掺杂摩尔分数为0.1%时,陶瓷样品的发光强度最大,此时Ce³⁺的掺杂量小于单晶中发光最强时的掺杂量。     

Nd3+:GdScO3晶体场能级及拟合分析

采用提拉法生长出了钕掺杂钪酸钆晶体(Nd³⁺:GdScO₃),通过低温吸收光谱和室温发射光谱,对其中Nd³⁺的实验能级进行分析指认,确定了Nd³⁺:GdScO₃的66个实验Stark能级,拟合了其自由离子参数和晶体场参数,拟合均方根误差为13.17 cm^-1.与Nd³⁺:YAP和Nd³⁺:YAG相比, Nd³⁺:GdScO₃的晶场强度较弱.弱的晶体场强度有可能是Nd³⁺:GdScO₃晶体具有优良激光特性的原因之一.本文数据集可在https://www.doi.org/10.57760/sciencedb.15702中访问获取.     

CdSe:Nd纳米晶及CdSe:Nd@SiO2核壳结构的合成及发光性能

利用有机相法合成Nd³⁺掺杂CdSe纳米晶（CdSe∶Nd）,通过X射线粉末衍射（XRD）、透射电镜（TEM）、紫外吸收光光谱及荧光光谱表征,证明Nd³⁺已经成功掺入到CdSe的晶格中。与纯CdSe纳米晶相比,CdSe∶Nd纳米晶的结构仍为立方晶型,且形貌近似球形,均匀分散,粒径约为2~4 nm。紫外吸收峰和荧光发射峰都发生红移,而且掺杂后的CdSe∶Nd纳米晶量子产率也提高,这可能是由于掺杂Nd³⁺引入了新的杂质能级,带隙减小。为了实现CdSe∶Nd纳米晶的可加工性和功能性,通过微乳法合成SiO₂壳包覆的CdSe∶Nd纳米球（CdSe∶Nd@SiO₂纳米球）,CdSe∶Nd@SiO₂纳米球呈均匀球形,直径约为100~115 nm,并且包壳后的CdSe∶Nd@SiO₂纳米球发射峰（581 nm）与CdSe∶Nd纳米晶（598 nm）相比,发光强度提高且发射峰蓝移,蓝移约为17 nm,可能是因为SiO₂壳可以减少纳米晶表面的非辐射跃迁以及改善表面缺陷导致的。     

尺寸效应对Er3+掺杂纳米Y2O3的发光特性的影响

采用燃烧法制备了不同尺寸的Er³⁺掺杂Y₂O₃粉体材料,研究了尺寸效应对Er³⁺掺杂纳米Y₂O₃材料发光特性的影响.光声光谱显示,对于不同晶粒尺寸的样品,Er³⁺离子光声峰位置几乎保持不变.这表明小尺寸效应对稀土离子能级位置影响很小.对488nm激光激发下的发射谱的分析发现,随着样品颗粒尺寸的减小,4S_3/2能级和关键词： 3+离子')" href="#">Er³⁺离子 纳米 发光 能量传递     

发光二极管用SrWO4:Eu3+红光荧光粉激发谱强度的调控

采用化学共沉淀法制备了Eu³⁺掺杂摩尔分数不同、煅烧温度不同的SrWO₄:Eu³⁺系列发光粉体, 所制备的粉体均具有Eu³⁺特征的强室温红光荧光发射. 通过调节煅烧温度和掺杂摩尔分数来调控近紫外和蓝光吸收强度, 进而调控用395 nm的近紫外光和465 nm的蓝光激发样品所得红光发光强度. 研究结果表明, 所制备的SrWO₄:Eu³⁺红光荧光粉可以被紫外和蓝光发光二极管有效激 关键词： 稀土掺杂 4:Eu³⁺')" href="#">SrWO₄:Eu³⁺ 光致发光 白光发光二极管     

玻璃中的ZnS:Mn2+超微粒发光的量子尺寸效应

自从Bhargava等^[1]报道了化学反应合成的ZnS:Mn²⁺纳米微粒的光学性质,掺杂半导体纳米微粒发光性质的研究受到了极大的重视。掺杂纳米微粒有可能成为新的一类发光材料.本文报导用熔融法制备的ZnS:Mn²⁺玻璃在光学性质上的量子尺寸效应。     

不同助烧剂对Nd∶YAG激光陶瓷前驱粉体烧结活性的影响

采用氨水共沉淀法制备了Nd∶YAG激光陶瓷前驱粉体,并在其中分别加入助烧剂SiO2和CaCO3。利用XRD、SEM及荧光光谱分析了不同助烧剂对Nd∶YAG激光陶瓷前驱粉体烧结活性的影响。XRD测试结果表明,助烧剂SiO2和CaCO3不能促进Nd∶YAG激光陶瓷前驱粉体的结晶。SEM照片观察发现,SiO2的助烧效果较好,能促进Nd∶YAG激光陶瓷前驱粉体的烧结,增加了前驱粉体的烧结活性,并且通过荧光光谱分析发现,助烧剂不改变Nd3+的4F3/2—4I11/2荧光发射。     

Nd3+掺杂的氧化镧钇透明激光陶瓷的光谱性能研究

采用传统无压烧结工艺制备了Nd³⁺掺杂的Y_2-2xLa_2xO₃(x=0.08)透明陶瓷并对其光谱性能进行了研究. 结果表明：Nd³⁺:Y_1.84La_0.16O₃透明陶瓷在780—850 nm的波长范围内有较宽的吸收带. 当Nd³⁺掺杂量为1.5at%时，在820 nm和激光二极管抽运的808 nm处的吸收截面分别为σ_abs(820 nm)=1.81×10^-20 cm²，σ_abs(808 nm)=1.54×10^-20 cm². 最强的发射峰位于1078 nm处，并具有荧光寿命长、发射带宽宽、量子效率高等特点. 加入La₂O₃后，基质的光谱品质参数X_Nd由1.6减小到0.46，因此和⁴F_3/2—⁴I_11/2跃迁相对应的荧光分支比β_J,11/2增大为56.82%. Nd³⁺:Y_1.84La_0.16O₃透明陶瓷的这些性质有利于高效率的激光输出和超短锁模激光脉冲的实现. 关键词： 氧化镧钇透明陶瓷 光谱性能 3+')" href="#">Nd³⁺     

Nd:YAG陶瓷的烧结性能研究

采用注浆成型和真空烧结制备了Nd:YAG激光透明陶瓷,研究了烧结温度和时间对致密化过程的影响。研究结果表明:在1050~1300℃之间坯体发生明显的收缩生成YAM和YAP相;在1300~1420℃,生成YAG相。随着烧结温度的增加,陶瓷中气孔含量减少,晶粒尺寸长大。在1700~1800℃烧结20h能够获得完全致密的Nd:YAG陶瓷样品。     

Optical characteristics of Cr and Nd codoped Y3Al5O12 ceramics

The optical characteristics of Cr³⁺ and Nd³⁺ codoped Y₃Al₅O₁₂ (YAG) ceramics are measured. These measurements are done using two pumping sources, a 808 nm laser diode (LD) and a Xe short-arc lamp, to simulate solar radiation. The specimens used are 0.1%Cr³⁺/1.0%Nd³⁺ and 3.0%Cr³⁺/1.0%Nd³⁺ (atomic%) codoped YAG ceramics. A Nd:YAG crystal doped with 1.0%Nd³⁺ is used as a reference. The saturation intensities of the Cr/Nd:YAG ceramics pumped by the LD are the same as that of the Nd:YAG crystal, while they are higher when they are pumped by the Xe lamp. The saturation intensities are for the 0.1% Cr-doped ceramic and for the 3.0%Cr-doped ceramic. The small signal gains of the 0.1%Cr-doped and 3.0%Cr-doped ceramics are measured and found to be 1.8 times and 7.0 times higher than that of Nd:YAG for the same intensity of solar pumping, respectively. The quantum efficiency of energy transfer from Cr³⁺ to Nd³⁺ is estimated to be 0.88±0.09 for the 0.1%Cr-doped ceramic and 0.67±0.08 for the 3.0%Cr-doped ceramic.     

Characterization of Nd Doped Films Prepared by Femtosecond Pulsed Laser DepositionSCIEI北大核心CSCD

Thin films of Nd : YAG and Nd : Glass were prepared on Si (100) substrate by pulsed laser deposition technology. The morphology of film surface and cross section, composition, absorption spectrum and photoluminescence (PL) spectra of films were investigated by scanning electron microscope (SEM), energy disperse spectroscopy (EDS), Fourier transform infrared spectrometer(FTIR), optical parametric oscillator(OPO) and grating spectrometer. The results show that both Nd : YAG films and Nd : Glass films grown on the substrates at room temperature are amorphous. Nd : YAG films grown by PLD contain Nd element with 0. 15 at. % stoichiometric proportion. The absorption spectrum of bulk Nd : YAG target rather than deposited films exhibit two absorption peaks at 750 and 808 nm. There are no evident peaks in the photoluminescence spectra curve of Nd : YAG films. However, the photoluminescence spectra of Nd : Glass films with two sharp peaks at the wavelength of 877 and 1 064 nm are observed. It indicates that Nd is doped into glass host as optically active Nd3+ ions when Nd : Glass films grow at room temperature. But for Nd : YAG films, Nd don't incorporate into YAG host as Nd3+ ions.     

氟磷酸锶晶体Cr4+:YAG被动调Q激光特性研究

采用氙灯泵浦,实现了掺钕氟磷酸锶晶体以Ｃｒ＾４＋：ＹＡＧ作为被动调Ｑ元件的１．０５９μｍ激光运转,测量了Ｃｒ＾４＋：ＹＡＧ 同小爱过率及不同泵浦能量上激光单脉冲的输出能量、脉冲宽度、重复率,给出了Ｎｄ：Ｓ－ＦＡＰ晶体Ｃｒ＾４＋：ＹＡＧ调Ｑ工作原理的方程组,数值求解该方程组得的理论结果与实验值相符。     

Continuous-wave and passively Q-switched Nd:GdVO4 lasers at 1.06 μm end-pumped by laser-diode-array

We demonstrated a diode-end-pumped continuous-wave and passively Q-switched Nd:GdVO₄ laser operating at 1.06 μm wavelength with a three-mirror folded resonator. The maximum continuous-wave output power of 8.18 W was obtained at the incident pump power of 22.5 W, with the corresponding optical conversion efficiency of 36.4%. For Q-switched operation, the maximum average output power was measured to be 4.64 W with the corresponding optical conversion efficiency of 25.8%, when the initial transmission of Cr⁴⁺:YAG crystal was 90%. The shortest pulse width of 83 ns, the largest pulse energy of 20.7 μJ and the highest peak power of 246.7 W were obtained when the Cr⁴⁺:YAG crystal with an initial transmission of 85% was used.     

Passive Q-switching of Pulsed and CW Nd: YAG Lasers with Cr~(4 ): YAG

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Laser-diode pumped self-Q-switched microchip lasers

Optical properties of Cr,Yb:YAG, Cr,Nd:YAG crystals, and composite Yb:YAG/Cr:YAG ceramics self-Q-switched solid-state laser materials are presented. The merits of these self-Q-switched laser materials are given and the potentials of such lasers can be chosen by the applications. Cr,Yb:YAG and composite Yb:YAG/Cr:YAG ceramics self-Q-switched laser are conducted. Although several tens of kW peak power can be obtained with a monolithic microchip Cr,Yb:YAG laser, the experimental results show that the performance of this laser is limited by the absorption of Cr⁴⁺ ions at a pump wavelength of 940 nm and strong fluorescence quenching at high Cr concentration. Composite Yb:YAG/Cr:YAG ceramics are more suitable to realize high pulse energy and peak power (up to MW level) with optimized lasing and Q-switching parts. In addition, the instabilities induced by the multi-longitudinal mode competition in Cr,Nd:YAG and Cr,Yb:YAG microchip lasers are addressed. The different gain bandwidths of Yb:YAG and Nd:YAG play an important role in the instability of the output laser pulse trains. Stable laser pulses from the Cr,Yb:YAG microchip laser were obtained due to the antiphase dynamics. For the Cr,Nd:YAG microchip laser, the instability caused by the multi-longitudinal mode competition is an intrinsic property. Different transverse patterns were observed in Cr,Nd:YAG microchip lasers when a pump beam with larger diameter was used. Saturated inversion population distribution inside the gain medium plays an important role in the transverse pattern formation. Different transverse patterns were reconstructed by combining different sets of the Hermite-Gaussian modes.     

Experimental study of a high power and high efficiency CW diode-side-pumped Nd:YAG laser

This paper reports on the characterization of a diode-side-pumped CW Nd:YAG laser. A side-pumped configuration with 9 laser diodes is used for the laser. Pump light is directly coupled into the Nd:YAG rod without focusing lenses and the pump light distribution in the Nd:YAG rod was calculated. A maximum output power of 150 W in multimode operation is obtained for a pumping power of 400 W. The optical–optical efficiency is 37%. Output power of the laser under different output couplers, resonator lengths and temperatures of the cooling water have been studied.     

Electron Spin Resonance Study of Yttrium Aluminum Garnet Films Doped with Nd and Yb Ions

Yttrium aluminum garnet (YAG) thin films doped with optical active rare earth ions grown on YAG substrate can be used as wave-guide laser. Measured layers YAG:Yb, Nd (grown by the isothermal liquid phase epitaxy (LPE)) was additionally doped with Ga and Lu ions in order to increase film refractive index and decrease strains in layers, respectively. Electron spin resonance measurements have been performed on a number of YAG:Yb, Nd thin films with Yb concentrations ranging from 0at.% to 15at.% and Nd concentration equals to 1 at.% and 3 at.%. It was found that the measured angular dependence of the Yb^3? ion linewidth is typical for a mosaic structure. Moreover, it was shown that internal strains in the layers depend on the kind of dopant as well as on their concentration.     

飞秒脉冲激光沉积钕掺杂薄膜特性研究

采用脉冲激光沉积(PLD)技术在Si(100)衬底上生长了Nd∶YAG薄膜以及Nd∶Glass薄膜,利用扫描电子显微镜(SEM)、能谱仪(EDS)、傅里叶变换红外光谱仪(FTIR)、光学掺量振荡器(OPO)以及光栅光谱仪等测试装置分析了薄膜的表面和断面结构形貌、组成成分、光学吸收谱以及光致发光谱。结果表明：在室温衬底温度下生长的Nd∶YAG薄膜以及Nd∶Glass薄膜均呈无规则非定型结构,没有明显的取向性微晶生长;PLD生长的Nd∶YAG薄膜中存在0.15 at.%化学计量比的Nd元素;Nd∶YAG块体靶材在750和808 nm有两个明显的吸收峰,而薄膜没有明显的吸收峰;Nd∶YAG薄膜在808 nm波长泵浦光下没有明显的光致发光谱峰,而Nd∶Glass薄膜在877和1 064 nm波长处有明显的光致发光谱峰。说明在室温衬底温度下生长的Nd∶Glass薄膜中Nd元素以Nd3+光学活性离子形式掺杂进玻璃基质中,而Nd∶YAG薄膜中的Nd元素没有以Nd3+光学活性离子形式掺杂进YAG基质中。     

Investigation on the scattering effect of ceramic Nd:YAG

This paper investigates the scattering effect of domestic 0.5 at{\%} ceramic Nd:YAG. An effective method has been utilized to measure the scattering and absorption coefficients. An end-pumped continuous wave (CW) Nd:YAG ceramic laser was also demonstrated. A maximum output power of 6.7~W at 1064~nm was obtained at an 808-nm pump power of 32.9~W. Conversion efficiency and slope efficiency have been achieved. This indicates that scattering has an important effect on the optical performance of ceramic Nd:YAG.