Nd^3＋：Na3La9O（BO3）8晶体生长和光谱性能

采用顶部籽晶法生长Nd^3＋：Na3La9O3（BO3）8晶体。在室温下测试了吸收光谱、发射光谱和荧光寿命。应用Judd-Ofelt理论评价了Nd^3＋：Na3La9O3（BO3）8晶体的光谱性能。812nm处较宽的吸收峰适合AlGaAs LD泵浦的吸收。分别计算了Nd^3＋离子的唯象强度、谱线强度、辐射寿命、荧光分支比和荧光量子效率。     

Na3La9O3(BO3)8的晶体结构

以Na2CO3-H3BO3为助熔剂,用顶部籽晶法生长出Na3La9O3(BO3)8单晶.测定了Na3La9O3(BO3)8晶体结构,结果表明:该晶体属六方晶系,空间群:P62m,晶胞参数为a=b=0.89229(13)nm,c=O.87366(17)nm,α=β=90°,γ=120°,Z=1,V=0.60240(17)nm3,密度为5.066g/cm3.晶体结构中的硼氧基团是平面的BO3基团,BO3基团相互独立,通过与Na(1)O6、La(1)O9和La(2)O8的配位多面体连结形成层状结构,所有层平行于(001)面.描述了Na3La9O3(BO3)8晶体在非线性光学材料领域的应用前景.     

Na3La2(BO3)3:Nd3+的合成及其光谱特性

本文采用固相反应法合成了一系列掺Nd3+的Na3La2(BO3)3(Na3La2(BO3)3:Nd3+)多晶粉末,X-ray粉末衍射分析表明,它们属于正交晶系,Amm2空间群.测试了Na3La2(BO3)3:Nd3+的红外光谱、反射光谱和荧光光谱,观察到试样在590 nm、740 nm和800 nm附近存在显著吸收,以及在878 nm、1067 nm、1326 nm三个发射带.研究了发光强度与Nd3+离子浓度之间的关系,确定了Nd3+离子在Na3La2(BO3)3基质中发光的适宜浓度为10 ;摩尔分数.     

Na3La2(BO3)3的晶体结构

以Na2CO3-H3BO3-NaF为助熔剂,使用顶部籽晶法生长出Na3La2(BO3)3透明单晶.测定了Na3La2(BO3)3的晶体结构,该晶体属正交晶系,空间群:mm2(No.38),晶胞参数为a＝0.51580(10)nm,b=1.1350(2)nm,c=0.73230(15)nm,α＝β＝γ＝90°,V＝0.42871(15)nm3,密度:.053g/cm3.晶体结构中的硼氧基团是平面的BO3基团,BO3基团相互独立,且与Na(1)O6、Na(2)O8、Na(3)O6和La(1)O9配位多面体连结形成三维网络骨架结构.讨论了Na3La2(BO3)3的晶体结构与倍频效应的关系.     

非线性光学晶体Na3La9O3(BO3)8的生长研究

以Na3CO3和H3BO3为助熔剂,Na3CO3和H3BO3摩尔比为7/6,熔质Na3La9O3(BO3)8和助熔剂摩尔比为1/10～1/14,采用顶部籽晶生长方法,生长Na3La9O3(BO3)8晶体,晶体尺寸为30×18×8mm3.本文讨论了籽晶方向对Na3La9O3(BO3)8晶体生长的影响,(100)方向比(001)方向更有利于晶体生长.     

Yb3+: Sr3Gd(BO3)3激光晶体的生长和光谱特性

采用提拉法(Czochralski)生长出了掺Yb3+的Sr3Gd(BO3)3晶体,晶体尺寸达到:25 mm×30 mm.测量了Yb3+: Sr3Gd(BO3)3晶体的吸收谱、荧光谱以及荧光寿命.Yb3+: Sr3Gd(BO3)3晶体在975 nm有一半峰宽为7 nm的强吸收峰,π谱的吸收跃迁截面σa=7.28×10-21 cm2,在1040 nm的发射跃迁截面σe=1.43×10-21 cm2.辐射寿命为1.46 ms, Yb3+浓度为13 at;时的荧光寿命f=2.14 ms,Yb3+浓度为0.5 at;时的荧光寿命f=1.21 ms.     

GdAl3(BO3)4和Nd离子掺杂的倍频与自变频激光晶体研究

采用熔盐顶部籽晶法从K2Mo3O10-B2O3助熔剂中生长出尺寸为20 mm的优质GdAl3(BO3)4(简称GAB)和Nd3+激活的自变频激光晶体.确定了GAB晶体的透光波长范围、折射率和倍频系数随波长的变化,结果表明其在整个透光范围内均可实现相位匹配.测定了Nd3+∶GAB晶体在室温下的偏振吸收、荧光光谱和荧光寿命,进行了光谱计算,测试了晶体的自变频激光性能,实现了紫外-可见光-红外-中红外多波段激光输出.     

(K,Na)3La2(BO3)3固溶体系的晶体结构

本文合成了一系列的(K,Na)3La2(BO3)3硼酸盐,通过自发结晶得到了组分为K1.34,Na1.66La2(BO3)3的单晶.单晶X射线结构分析表明该晶体与Na3La2(BO3)3同构,并且当K+取代Na+的数量小于2/3时,晶体结构仍为Na3La2(BO3)3构型.该晶体的基本结构单元为孤立的(BO3)3-基团.一个单胞中含有6个BO3基团,其中两个沿c方向一致平行排列,而剩余的4个BO3基团的排列方向与c方向呈一定的角度,从而减小了BO3基团对非线性效应的贡献.粉末倍频测试该晶体的有效非线性系数约为KDP的2.4倍.此外,研究表明用适量的Rb+,Li+取代Na+时,固溶晶体结构也不发生改变.     

双掺Er~(3+)/Yb~(3+)∶Sr_3La_2(BO_3)_4晶体的生长与光谱特性

采用提拉法生长了尺寸为20mm×30mm的Er3+/Yb3+∶Sr3La2(BO3)4晶体,研究了Er3+/Yb3+∶Sr3La2(BO3)4晶体的吸收光谱和荧光光谱。根据Judd-Ofelt理论分析并计算了辐射跃迁几率、辐射寿命、荧光分支比等光谱参数,获得的唯象参数为:Ω2=15.59×10-20cm2,Ω4=2.25×10-20cm2,Ω6=1.49×10-20cm2。在Er3+/Yb3+∶Sr3La2(BO3)4晶体中Er3+在1533nm处发射跃迁截面为7.88×10-21cm2,Er3+的4I13/2→4I15/2能级跃迁的荧光寿命和辐射寿命分别为0.728ms和4.24ms,结果表明Yb3+对Er3+有敏化作用,提高了对泵浦光的吸收能力,Er3+/Yb3+∶Sr3La2(BO3)4晶体可望作为1.55μm波段的一种有潜力的激光材料。     

Nd~(3+)掺杂的Sr_3Y_2(BO_3)_4晶体光谱特性研究

采用提拉法生长出25mm×40mm的Nd3+∶Sr3Y2(BO3)4晶体,测试了该晶体的吸收光谱、荧光光谱及荧光寿命。结果表明:Nd3+∶Sr3Y2(BO3)4晶体在807nm附近有最强的吸收峰,其半峰宽(FWHM)为16nm,宽的吸收半峰宽适合于LD泵浦;从荧光光谱得到发射波长分别为910.8nm、1065.2nm和1399nm的荧光峰。根据吸收和荧光光谱,计算了晶体的吸收截面和发射截面。采用J-O理论计算了Nd3+在Sr3Y2(BO3)4中的强度参数、各能级的振子强度、自发辐射几率、荧光分支比等参数。计算结果表明,其强度参数Ω2=3.816×10-20cm2,Ω4=10.895×10-20cm2,Ω6=12.44×10-20cm2,辐射寿命为104μs,量子效率η=49.7%,荧光分支比β1(0.88μm)=0.429,β2(1.06μm)=0.461,β3(1.35μm)=0.107,β4(1.88μm)=0.003。     

Ho~(3+)∶La_2CaB_(10)O_(19)晶体生长和光谱性能(英文)

采用顶部籽晶法生长Ho3+∶La2CaB10O19晶体。测试了晶体的X射线衍射谱图以及晶体器件的摇摆曲线,半峰宽为21.6 arcsec,晶体结晶质量良好。在室温下测试了吸收光谱、发射光谱和荧光寿命。应用Judd-Ofelt理论评价了Ho3+∶La2CaB10O19晶体的光谱性能。分别计算了Ho3+的唯象强度、谱线强度、辐射寿命、荧光分支比等参数。     

Nd3+:LiLa(MoO4)2晶体生长、光谱和激光特性

本论文报道了Nd3+:LiLa(MoO4)2晶体生长、光谱和激光特性.采用提拉法生长出尺寸为φ20×34mm3的Nd+3+:LiLa(MoO4)2晶体.应用Judd-Ofelt理论计算了Nd3+离子在Nd3+:LiLa(MoO4)2晶体中唯象强度、自发发射跃迁几率、荧光分支比、辐射跃迁寿命和荧光量子效率.Nd3+:LiLa(MoO4)2晶体的偏振吸收跃迁截面分别为9.52×10-20cm2(π-偏振)和4.46×10-20cm2(σ-偏振).它的偏振发射跃迁截面分别为0.67×10-19cm2(σ-偏振)和1.02×10-19cm2(σ-偏振).在氙灯泵浦下,获得74.4mJ的1.06μm的激光输出,激光阈值为0.676J,激光总效率和斜率效率分别为0.39;和0.48;.     

Nd3+:d3Ga5O12晶体的室温吸收光谱和荧光光谱

用提拉法生长了掺钕的钆镓石榴石(Nd3+:GG)激光晶体.研究了室温下的吸收光谱和荧光光谱性质,分析了Nd3+:GG晶体4F3/2→4I11/2能级跃迁与1.06μm附近的荧光谱线之间的关系.吸收系数、发射系数、荧光寿命分别是4.32×10-20 cm-2,2.3×10-19cm-2, 240μs, 比较了Nd3+∶GGG 和 Nd3+∶YAG 的物理参数,实验表明:d3+∶GGG较Nd3+∶YAG有一系列的优点.     

Nd3+:α~NaYF4单晶体的生长与光谱特性

以KF为助熔剂,初始原料按照NaF:KF:YF3:NdF3=30:18:47:5的摩尔比例,采用助熔剂-坩埚下降法成功生长出了优质块体Nd3+掺杂α~NaYF4单晶体.XRD图谱表明,引入少量钕离子没有改变单晶体的立方相结构.测定了钕离子在晶体中的实际掺杂浓度为3.15mol;,相比初始掺杂浓度偏小,说明在单晶体中稀土离子存在着分凝现象.根据吸收图谱,在800nm处具有最强吸收峰,最大吸收系数α和吸收跃迁截面σabs分别为0.91cm-1和0.138×10-20cm2.在800nm激光激发下,发射光谱在800~1500nm范围内有三个峰,由4F3/2能级跃迁到4I11/2能级所产生位于1052nm处的峰值最强,测得荧光寿命为35μs.掺钕氟化钇钠晶体的光学特性表明它在中红外激光领域具有潜在的应用价值.     

Yb3+浓度对掺铥碲酸盐玻璃的热稳定性及光谱性能的影响

采用高温熔融冷淬法制备70.75TeO2-19ZnO-9.5La2O3-0.75Tm2O3-xYb2O3碲酸盐玻璃,使用差示扫描量热仪(DSC)分析了玻璃样品的热稳定性,表明样品均具有良好的热稳定性.根据紫外-可见-近红外分光光度计测量得到的玻璃吸收光谱,结合Judd-Ofelt理论,计算了Tm3+在玻璃中的Judd-Ofelt强度参数、自发辐射概率A、荧光分支比β和辐射寿命τR等光谱参数.结果表明,当Yb3+掺杂浓度为0.625mol;时,Tm3+在3H4处的荧光寿命最长,为0.443 ms,表明铥镱共掺杂碲酸盐玻璃有望成为一种理想的S波段光纤放大器用基质材料.     

Crystal growth and spectral properties of Nd:Ca5(BO3)3F

A neodymium doped Ca₅(BO₃)₃F single crystal with size up to 51×48×8 mm³ has been grown by the top seeded solution growth (TSSG) technique with a Li₂O‐B₂O₃‐LiF flux. The spectra of absorption and fluorescence were measured at room temperature. According to Judd‐Ofelt (J‐O) theory, the spectroscopic parameters were calculated and the J‐O parameters Ω₂, Ω₄, Ω₆ were obtained as follows: Ω₂ = 1.41×10⁻²⁰cm², Ω₄ = 3.18×10⁻²⁰cm², Ω₆ = 2.11×10⁻²⁰cm². The room temperature fluorescence lifetime of NCBF was measured to be 51.8 μs. According to the J‐O paramenters, the emission probabilities of transitions, branching ratios, the radiative lifetime and the quantum efficiency from the Nd^{3+ 4}F_3/2 metastable state to lower lying J manifolds were also obtained. In comparasion with other Nd‐doped borate crystals, the calculated and experimental parameters show that NCBF is a promising SFD crystal.     

Studies on the growth and optical characterization of dysprosium gadolinium oxalate single crystals

Preparation and optical characterization of dysprosium gadolinium oxalate (DGO) single crystal is reported. The crystals were grown using silica gel technique, by the controlled reaction of rare earth nitrates with oxalic acid. Crystals were characterized using X‐ray powder diffraction, optical absorption and fluorescence studies. Radiative transition probability, fluorescence branching ratio and radiative lifetime of Dy³⁺ in the crystal are evaluated by the parameterization of the absorption spectrum by the Judd‐Ofelt theory. The recorded fluorescence spectrum showed two well resolved peaks at 480 nm and 571 nm and are assigned to the transitions from ⁴F_9/2 → ⁶H_15/2 and ⁶H_13/2 of Dy³⁺. Stimulated emission crossection and optical gain of these transitions are also evaluated. (© 2004 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)     

Optical properties of Er3+-singly doped and Er3+/Yb3+-codoped novel oxyfluoride glasses

Novel oxyfluoride glasses SiO₂–Al₂O₃–Na₂O–ZnF₂ doped with Er³⁺ and Er³⁺/Yb³⁺ were fabricated. The optical properties of the synthesized glasses were experimentally and theoretically investigated in detail. The experimental and calculated oscillator strengths of Er³⁺ were determined by measurement of the absorption spectrum of Er³⁺-singly doped glass. According to the Judd–Ofelt theory, the experimental intensity parameters were calculated, from which the radiative transition probabilities, fluorescence branching ratios and radiative lifetimes were obtained. The fluorescence lifetime and quantum efficiency for the near-infrared emission of Er³⁺-singly doped glass were determined to be 3.0 ms, and 42%, respectively. Visible upconversion luminescence was observed under 980 nm diode laser excitation. The dependence of the upconversion emission intensity upon the excitation power was examined, and the upconversion mechanisms are discussed.     

Optical and laser properties of Nd:LuVO4 crystal

Polarized absorption spectra of Nd:LuVO₄ crystal were measured at room temperature. The optical parameters of π polarization and σ polarization were calculated by Judd‐Ofelt theory. Meanwhile, the phenomenological intensity parameters: Ω₂, Ω₄, and Ω₆ were obtained, then the parameters were used to calculate the luminescence parameters of Nd:LuVO₄ crystal, including oscillator strengths, fluorescence branching ratio, radiative lifetime and integrated emission cross‐sections. Experiments of a‐cut and c‐cut Nd:LuVO₄ lasers were also performed, and opt‐opt conversion efficiency and slope efficiency were 40.3%, 50.5% for a‐cut and 23.6%, 30.9% for c‐cut, respectively. (© 2007 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)     

Nd:NaY(WO4)2激光晶体光谱性能研究

Nd:NaY(WO4)2 是一种性能优良的激光晶体.本文采用提拉法生长了Nd:NaY(WO4)2晶体,测试了该晶体的吸收光谱和光荧光光谱.结果表明,该晶体在804nm、752nm、586nm附近有较强、较宽的吸收峰,适合于LD泵浦.从光荧光光谱得到发射波长分别为1064nm和1350nm,并计算了晶体的吸收截面和发射截面.