铒镱共掺钨酸钆钾激光晶体的光谱性能及光谱参数计算(英文)

采用顶部籽晶溶液法生长出铒镱共掺钨酸钆钾[Er3+:Yb3+:KGd(WO4)2,Er:Yb:KGW]激光晶体.测量了晶体的红外光谱、Raman光谱、吸收光谱和发射光谱,分析了晶体的振动模式,并对晶体振动光谱进行归属.利用Judd-Ofelt理论计算晶体的吸收及发射截面、强度参数、辐射跃迁几率、荧光分支比和荧光寿命等光谱参数.结果表明:Er:Yb:KGW晶体在380,523,935nm和981nm处存在较强的吸收峰,主峰981nm处的吸收截面为 3.35×10-20cm2.强度参数为Ω2=1.0729×10-20cm2,Ω4=1.2956×10-20cm2,:Ω6=0.933 5×10 20cm2.用488nm和980nm波长激发晶体,得到较强的1.53μm人眼安全波段激光,由于Yb3+对Er33+的敏化作用不级可以提高泵浦光的吸收效率,而且可以降低激光振荡阈值.     

铒镱共掺钨酸钆钾激光晶体生长、结构及光谱特性

采用顶部籽晶提拉法生长出铒镱共掺钨酸钆钾[Er3 :Yb3 :KGd(WO4)2,Er:Yb:KGW]激光晶体.这种晶体的最佳生长工艺参数为:转速为10～15 r/min,提拉速率为1～2mm/d,降温速率为0.05～0.1℃/h,生长周期为10～15d.X射线衍射分析表明,所生长的晶体为β-Er:Yb:KGW.经热重-差热分析确定:晶体的熔点为1 079℃,相转变温度为1 024℃.测量晶体的红外及Raman光谱,并对峰值及相应的原子基团振动进行了归属.晶体样品的吸收光谱显示:在380,523,935 nm和981 nm处存在较强的吸收峰,主峰981 nm处的吸收截面积为3.35×10-20 cm2.分别在488 nm和980 nm波长光激发下,均可以产生较强的1.53 μm对人眼安全的激光,表明Yb3 对Er3 具有敏化作用,既提高了对泵浦光的吸收效率,又降低了激光振荡阈值.     

Er:LiGdF_4晶体生长及光谱性能

采用提拉法生长出掺铒氟化钆锂(Er3+:LiGdF4,Er:LGF)激光晶体。晶体生长工艺参数为:提拉速率为0.16mm/h,晶体转速为3r/min,冷却速率为10℃/h。X射线粉末衍射分析表明:晶体属于四方晶系,白钨矿结构,空间群为I41/a,计算的晶胞参数:a=0.5196nm,c=1.10286nm。晶体的吸收光谱和荧光光谱表明:晶体在659,980nm和1540nm附近的吸收峰较强,其中在1540nm处的吸收截面为1.09×10-20cm2。在激光二极管的532nm波长泵浦下,发射峰分别位于995nm和1530nm附近,其中1530nm处的半高宽为52nm。     

In∶Yb∶Er∶LiNbO_3晶体的生长和光谱性能

采用提拉法生长了掺0.25%(摩尔分数,下同)Yb2O3,0.25%Er2O3和(0.5%、1.0%、1.5%)In2O3的3种同成分In∶Yb∶Er∶LiNbO3晶体。通过晶体的红外光谱,解释了In3+,Yb3+和Er3+在晶体中的占位,由于Yb3+和Er3+离子的掺入,在In∶Yb∶Er∶LiNbO3晶体中In3+既占据Li位又部分占据Nb位,使2%In∶Yb∶Er∶LiNbO3晶体达到阈值浓度。采用980nm二极管激光器测试了In∶Yb∶Er∶LiNbO3晶体上转换发射光谱。结果表明:晶体的绿光上转换发射中心波段位于525、550nm处,分别相应于Er3+的2 H11/2→4 I15/2跃迁和4 S3/2→4 I15/2跃迁;上转换红光发射中心波段在660nm处,对应Er3+的4 F9/2→4 I15/2辐射跃迁。In3+能提高Yb∶Er∶LiNbO3晶体的抗光损伤能力,改变Er3+和Yb3+的局部环境及Yb3+对Er3+的敏化作用,使得In∶Yb∶Er∶LiNbO3晶体发光性能改变。     

铒/镱共掺硼酸钙镧晶体的生长和光谱性质

在CaO-Li2O-B2O3助熔体系中,生长了掺铒和镱的硼酸钙镧(Er3 :Yb3 :La2CaB10O19,Er:Yb:LCB)晶体.Er:Yb:LCB晶体中Er3 ,Yb3 的分凝系数分别为0.50,0.25.X射线衍射分析表明:Er:Yb:LCB和LCB具有相同的晶体结构.Er:Yb:LCB晶体的熔点大约为1046℃.Er:Yb:LCB晶体的吸收光谱和荧光光谱的测试结果表明:与Er:LCB相比,Er:Yb:LCB晶体在970 nm的吸收系数显著提高,在1 531 nm的发射强度也显著增强,其荧光寿命为0.48 ms.     

Tm~(3+)掺杂KYb(WO_4)_2自激活激光晶体生长与光谱特性分析

以K2W2O7为助熔剂,Tm3+掺杂摩尔分数为8%,采用顶部籽晶提拉法生长出了单斜晶系的铥掺杂钨酸镱钾[Tm3+:KYb(WO4)2,Tm:KYbW]晶体.测试了晶体的红外光谱和Raman光谱,并对出现的峰值进行了振动归属.测量了晶体的吸收光谱和荧光光谱,计算了相应的光谱参数.吸收光谱显示:Yb3+在945,958nm处吸收峰最强,半峰宽为91 nm.荧光光谱表明:Tm:KYbW晶体在1 735nnl和1 759nm附近有较强的发射峰,主峰1 759nm处的发射线宽达146nm,因此,Tm:KYbW晶体可作为可调谐激光增益介质.晶体的上转换荧光谱表明:在481 nm和646nm处分别得到了上转换蓝光和红光,并分析了相应的上转换机制.     

Yb3+:Gd3Ga5O12激光晶体原料合成与生长的研究

采用溶胶-凝胶法合成了Yb：GGG多晶料.以XRD分析方法对合成料的前驱体及烧成的粉体的相结构进行了研究,XRD分析结果表明,950 ℃煅烧的粉体已是Yb:GGG纯相.采用提拉法,通过设计合理而稳定的温场、选择最佳工艺参数等生长了Yb:GGG晶体.荧光光谱测试结果表明,Yb:GGG晶体主要发射峰位于1030 nm,该荧光是由Yb3+激发态2F5/2向基态2F7/2能级跃迁产生的.     

Yb3+∶La2CaB10O19晶体的生长

以CaB4O7为助熔剂生长出尺寸为31 mm×32 mm×12 mm、质量较好的掺Yb3+的摩尔分数分别为10%,15%的Yb3+∶La2CaB10O19(Yb3+∶LCB)单晶,生长工艺参数是:降温速率＜0.5 ℃/d,转速＜12 r/min.测试了晶体的X射线粉末衍射谱、透射光谱和粉末倍频效应,结果表明:Yb3+∶LCB晶体的粉末衍射峰与LCB的衍射峰一致;Yb3+∶LCB晶体在925, 975 nm附近有明显的吸收峰,其中975 nm附近吸收很强;倍频效应与KDP同一量级.     

Yb^3＋：La2CaB10O19晶体的生长

以CaB4O7为助熔剂生长出尺寸为31 mm×32 mm×12 mm、质量较好的掺Yb3+的摩尔分数分别为10%,15%的Yb3+∶La2CaB10O19(Yb3+∶LCB)单晶,生长工艺参数是降温速率＜0.5 ℃/d,转速＜12 r/min.测试了晶体的X射线粉末衍射谱、透射光谱和粉末倍频效应,结果表明Yb3+∶LCB晶体的粉末衍射峰与LCB的衍射峰一致;Yb3+∶LCB晶体在925, 975 nm附近有明显的吸收峰,其中975 nm附近吸收很强;倍频效应与KDP同一量级.     

Er,Yb:(LaGd)_2O_3纳米粉体的制备与发光性质

以碳酸氢铵为沉淀剂,采用共沉淀法制备了Er,Yb:(La Gd)2O3纳米粉体。经1 000℃煅烧2 h得到的粉体颗粒呈规则球形,平均粒径约为90 nm,团聚低,分布均匀。研究了Er3+,Yb3+的掺杂量对样品发光强度的影响。结果表明:掺杂Er3+和Yb3+的摩尔分数分别为4%和5%时,所得样品的发光性能最优。样品的激发和发射光谱显示:在379 nm处激发峰最强,对应Er3+的4I15/2→4G11/2能级跃迁;最强发射峰位于562 nm处,对应于4S3/2/2H11/2→4I15/2能级跃迁。样品的上转换光谱表明:样品在548和662 nm有较强的发射峰,对应Er3+的4S3/2/2H11/2→4I15/2跃迁和4F9/2→4I15/2跃迁。并讨论了发光跃迁机制。     

Er3+ cross-section spectra of Er3+/Pr3+:Gd3Ga5O12 single-crystal: Pr3+-codoping effect

Fluorescence and absorption spectra at 530 nm (²H_11/2→⁴I_15/2), 560 nm (⁴S_3/2→⁴I_15/2), 660 nm (⁴F_9/2→⁴I_15/2), 980 nm (⁴I_11/2→⁴I_15/2), 1530 nm (⁴I_13/2→⁴I_15/2), and 2710 nm (⁴I_11/2→⁴I_13/2) of Er³⁺ in Gd₃Ga₅O₁₂ single-crystal codoped with Pr³⁺ have been measured. Judd-Ofelt analysis yields the intensity parameters Ω₂ = (0.68 ± 0.03) × 10⁻²⁰ cm², Ω₄ = (0.60 ± 0.07) × 10⁻²⁰ cm², and Ω₆ = (0.90 ± 0.17) × 10⁻²⁰ cm². A comparison with previously reported values of Er³⁺-only doping case shows that Pr³⁺-codoping causes slight change of both Ω₂ and Ω₄, while onefold increase of Ω₆. From calculated radiative rates and measured fluorescence spectra, Er³⁺ emission cross-section spectra were calibrated at first. Then, the absorption cross-section spectra were calculated using McCumber relation. In parallel, the absorption cross-section spectra were also obtained from the measured absorption spectrum, and compared with those obtained from the McCumber relation. The comparison shows that both methods give consistent result of absorption cross-section spectrum. Further comparison with Er³⁺-only doping case shows that Pr³⁺-codoping causes considerable change of Er³⁺ cross-section value. In spectrally mixing regions of Er³⁺ and Pr³⁺, Pr³⁺ emission affects little the determination of Er³⁺ emission cross-section as Pr³⁺ fluorescence is much weaker than Er³⁺ fluorescence due to low Pr³⁺ concentration.     

Er3+:Yb3+:Y3Al5O12单晶中Er3+离子光谱参数的计算

采用提拉法生长出光学质量的Er3 :Yb3 :Y3Al5O12(YAG)单晶,测定了晶体的吸收光谱和上转换荧光光谱,根据Judd-Ofelt理论,计算出Er3 在YAG晶体中的强度参数Ω2=1.074 1×10-20cm2,Ω4=1.295 3×1020cm2,Ω6=0.923 8×1020cm2.由此得到部分波段跃迁的荧光分支比、辐射寿命和积分发射截面积.提出将679 nm波段的4F9/2→4I15/2跃迁作为激光输出进一步研究的新通道.     

Eu^3＋、Dy^3＋对CaTiO3：Pr^3＋红色磷光体发光性能的影响

采用改进高温固相法合成了掺杂Eu3+和Dy3+作为共激活离子的红色长余辉磷光体,详细阐述了Eu3+、Dy3+对CaTiO3:Pr3+红色磷光体发光性能的影响.通过X-射线衍射仪和电子扫描显微镜对所得样品的晶相类型及表面形态进行了表征,结果发现,在一定灼烧温度下,Eu3+或/和Dy3+对晶相的作用是协同的,且Eu3+或/和Dy3+对CaTiO3:Pr3+红色磷光体的粒径也有影响.室温条件下采用荧光/磷光发光光度计对其发光性能进行测定,结果表明,一定量的Eu3+或/和Dy3+能显著改善CaTiO3:Pr3+红色磷光体的发光性能.     

Highly-doped YAG:Sm3+ transparent ceramics: Effect of Sm3+ ions concentration

YAG:Sm³⁺ (3–15 at.%) transparent ceramics, a promising cladding material for suppressors of parasitic oscillations at 1064 nm of YAG:Nd³⁺ lasers, have been prepared by solid-state reactive sintering at 1725 °C. The effect of samarium ions concentration on the microstructure and optical properties of YAG:Sm³⁺ sintered ceramics was studied for the first time. The solubility limit of samarium ions in the garnet matrix was found to lie within the range of 9–11 at.%. The spectroscopic characterization of YAG:Sm³⁺ (3–15 at.%) ceramic samples showed that the absorption coefficients corresponding to Sm³⁺ ions transitions increased linearly with increasing Sm³⁺ doping. Also, the increase in the concentration of Sm³⁺ ions contributes to the increase in the intensities of the satellites, leading to the broadening of the main spectral lines and implicitly to the increase of the absorption coefficient around 1064 nm. It was shown that YAG:Sm³⁺ ceramics doped with 9 at.% Sm³⁺ ions possess optical losses of 0.07 cm^?1 at 808 nm and an optical absorption coefficient of 4.45 cm^?1 at 1064 nm. The concentration dependence of the ⁴G_5/2 level decay confirmed that the luminescence extinction is due to the energy transfer between the Sm³⁺ ions through cross-relaxation processes. All these results show that highly-doped YAG:Sm³⁺ (9 at.%) ceramics could be the best candidate for parasitic oscillation suppression in high-power YAG:Nd³⁺ lasers at 1064 nm.     

GdF3∶Eu3+和NaGdF4∶Eu3+发光粉的可控合成与发光性质

采用聚乙烯吡咯烷酮(PVP)辅助水热法合成了GdF3∶Eu3+和NaGdF4∶Eu3+发光粉。利用X射线衍射(XRD)、扫描电子显微镜和荧光光谱对样品的结构、形貌和发光性能进行了研究。XRD分析表明:GdF3晶相到NaGdF4晶相的转换可以通过改变初始溶液pH值、PVP加入量和NaF与稀土离子(Gd3+和Eu3+)摩尔配比等合成条件实现。NaGdF4∶Eu3+发光粉的形貌受合成条件的影响。荧光光谱研究表明:GdF3∶Eu3+发光粉主发射峰位于593nm处,来自于Eu3+的5 D0→7 F1磁偶极跃迁;NaGdF4∶Eu3+发光粉主发射峰位于616nm,来自于Eu3+的5 D0→7 F2电偶极跃迁。2个样品中Gd3+与Eu3+离子之间存在较好的能量传递,而NaGdF4晶格更有利于2种离子的能量传递。     

InBO3:Eu3+荧光粉的制备及光谱特性

合成了InBO3:Eu3 红色荧光粉 ,测定了其发光光谱 ,讨论了其发光亮度与稀土离子Eu3 浓度的关系     

Ligand-Sensitised LaF3:Eu3+ and SrF2:Eu3+ Nanoparticles and in Vitro Haemocompatiblity Studies

Luminescent Ln³⁺-doped nanoparticles (NPs) functionalised with the desired organic ligand molecules for haemocompatibility studies were obtained in a one-pot synthesis. Chelated aromatic organic ligands such as isophthalic acid, terephthalic acid, ibuprofen, aspirin, 1,2,4,5-benzenetetracarboxylic acid, 2,6-pyridine dicarboxylic acid and adenosine were applied for surface functionalisation. The modification of the nanoparticles is based on the donor–acceptor character of the ligand–nanoparticle system, which is an alternative to covalent functionalisation by peptide bonding as presented in our recent report. The aromatic groups of selected ligands absorb UV light and transfer their excited-state energy to the dopant Eu³⁺ ions in LaF₃ and SrF₂ NPs. Herein, we discuss the structural and spectroscopic characterisation of the NPs and the results of haemocompatibility studies. Flow cytometry analysis of the nanoparticles’ membrane-binding is also presented.     

LaF3:Ce3+荧光特性的研究

LaF3：Ce多晶中Ce^3 的荧光发射谱由双峰带结构组成。Ce^3 与其他稀土粒子共掺杂，Ce^3 发射强度均降低，原因是一部分稀土离子(如Eu^3 等)与Ce^3 产生了电子转移；一部分稀土离子(如Er^3 等)与Ce^3 产生了能量传递。     

Abnormal upconversion luminescence induced by defects and Er3+–Yb3+ distance change in Cs3GdGe3O9:Er3+/Yb3+ phosphors

A series of Er³⁺/Yb³⁺ co-doped Cs₃GdGe₃O₉ (CGG) phosphors were prepared by solid-phase sintering method, and the microstructure and upconversion luminescence (UCL) properties were tested by variable-temperature X-ray diffractometry and variable-temperature spectrometer. Abnormal UCL phenomena were found, which include UCL intensity continuously increasing under 980 nm laser continuous irradiation and UCL thermal enhancement. After 10 min of continuous irradiation by 980 nm laser at 513 K, the UCL intensity increased 2.91 times compared with the initial UCL intensity. The phenomenon is due to the electron releasing of host defects. The green UCL intensity of CGG:0.1Er³⁺/0.2Yb³⁺ decreases at 303–423 K and increases at 423–723 K, which reaches 13.23 times compared with that at 423 K. The phenomenon is due to Er³⁺–Yb³⁺ distance change by temperature and phonon-assisted transitions. In addition, the absolute temperature sensitivities of samples are calculated by luminescence intensity ratio technology, the maximum absolute sensitivity of CGG:0.1Er³⁺/0.4Yb³⁺ is 0.00691 K⁻¹ at 546 K, and the maximum relative sensitivity of CGG:0.1Er³⁺/0.1Yb³⁺ is 0.01224 K⁻¹ at 303 K. These results indicate that CGG:Er³⁺/Yb³⁺ phosphors can be used as a high-temperature optical thermometer.     

Er3+,Er3+-Yb3+和Er3+-Na+掺杂CaF2透明陶瓷的光学性能

以Ca(NO3)2、Er(NO3)3、Yb(NO3)3、KF和NaF为原料,采用热压烧结方法制备出Er3+,Er3+-Yb3+和Er3+-Na+掺杂CaF2透明陶瓷。测试了样品室温吸收光谱和发射光谱。利用Judd-Ofelt理论分析了样品的光学性能,并对吸收光谱进行计算拟合,得到光谱参数?t (t=2,4,6),根据光谱参数?t计算出Er3+某些能级的的跃迁几率、荧光分支比、辐射寿命和品质因子,讨论并比较了Er3+-Yb3+和Er3+-Na+共掺对CaF2透明陶瓷光学性能的影响。结果表明：掺杂Yb3+和Na+改变了Er3+光谱参数;Er3+-Yb3+共掺有利于提高样品的荧光强度;Er3+-Na+共掺有利于提高荧光寿命。