ZnS:ErF3电致发光薄膜2H11/2,4S3/2→4I15/2发光的猝灭过程

本文通过ZnS:ErF3交流电致发光薄膜发光光谱和发光衰减特性研究了Er3+离子2H11/2,3S3/2发光的猝灭过程,实验结果表明由于Er3+离子间多极矩相互作用,一个激发的Er3+离子从2H11/2态无辐射弛豫到4F9/2态,同时另一个激发的Er3+离子从4F7/2或4F5/2+4F3/2态跃迁到2H9/2或4G11/2态的交叉弛豫过程是2H11/2,4S3/2发光浓度猝灭的一个主要机制,交叉弛豫几率随着掺杂浓度的增加而增大,根据在固定掺杂浓度下2H11/2,4S3/2、4F9/2发光衰减时间不随激发密度而改变的实验结果,排除了处于激发的Er3+离子之间直接能量传递的可能性,这结果与扩散限制的能量传递理论相符。     

Tm3+离子掺杂的钨酸钇钠晶体中浓度猝灭效应的研究

测量了Tm3+离子不同浓度(0.5at.%,3 at.%,5 at.%)掺杂的NaY(WO4)2晶体在800 nm激光二极管激发下的上转换发射光谱.结合吸收谱、荧光谱和由Judd-Ofelt理论计算的光谱参数,详细分析了Tm36:NaY(WO4),晶体中上转换能量传递机理和离子浓度对上转换发射的影响.讨论了四种影响上转换发光效率的离子间相互作用机理:3H5+1G4→3H6+1D2,3H5+3H5→3H6+3F3,1G4+3H6→3F4+3F3,1G4+3H6→3F3+3F4,并根据Miyakawa-Dexter理论定量计算了各过程的发生概率.论证了交叉弛豫和共协上转换等浓度猝灭效应是影响Tm3+离子蓝色上转换荧光发射效率的主要因素.     

Y2O3:Ho/Yb纳米晶的上转换发光性质

采用燃烧法制备了不同尺寸和不同掺杂浓度的Y2O3：Ho／Yb纳米晶,并系统地研究了颗粒尺寸对Y2O3：Ho／Yb纳米晶发光性质的影响。研究发现,随着尺寸的减小,发射强度和荧光分支比均发生了显著变化,Ho^3 的整体发射强度降低,但5^F5→^5I8的红光发射比^5S2(^5F4)→^5I8的绿光发射的荧光分支比增强。尺寸减小,表面原子更易吸附空气中的水和二氧化碳,引入一些较大的振动模式,从而增大了无辐射跃迁的速率,荧光分支比随尺寸的变化被归因于表面效应引起的无辐射弛豫过程^5S2(^5F4)→^5F5和^5I6→^5I7的增强。     

氟氧化物纳米相玻璃陶瓷Tb(0.7)Yb(5):FOV的合作下转换发光

报道了氟氧化物纳米相玻璃陶瓷Tb(0.7)Yb(5)∶FOV的红外量子剪裁研究,测量了从可见到红外的荧光发光光谱、激发谱、和荧光寿命,分析了{1([5 D4→7 F6](Tb3+),2([2 F7/2→2 F5/2](Yb3+)}的红外量子剪裁现象,发现了487.0nm光激发5 D4能级和378.0nm光激发(5 D3,5 G6)能级的理论量子剪裁效率ηx%Yb依次分别为121.35%和136.27%。首次发现了一种新颖的合作(共协)下转换发光现象{2([(5 D3,5 G6)→5 D4](Tb3+),1([2 F7/2→2 F5/2](Yb3+)},即首次发现施主Tb3+离子释放两个小能量光子[(5 D3,5 G6)→5 D4]的能量,导致出现一个受主Yb3+的[2 F5/2→2 F7/2]的中等能量的光子。     

氟氧化物纳米相玻璃陶瓷Tb(0.7)Yb(5)∶FOV的合作下转换发光

报道了氟氧化物纳米相玻璃陶瓷Tb(0.7)Yb(5)∶FOV的红外量子剪裁研究,测量了从可见到红外的荧光发光光谱、激发谱、和荧光寿命,分析了{1([5 D4→7 F6](Tb3+),2([2 F7/2→2 F5/2] (Yb3+)}的红外量子剪裁现象,发现了487.0nm光激发5 D4能级和378.0nm光激发(5 D3,5 G6)能级的理论量子剪裁效率ηx％Yb依次分别为121.35％和136.27％.首次发现了一种新颖的合作(共协)下转换发光现象{2([(5 D3,5 G6)→5 D4](Tb3+),1([2 F7/2→2 F/2](Yb+)},即首次发现施主Tb3+离子释放两个小能量光子[(5 D3,5 G6)→5 D4]的能量,导致出现一个受主Yb3+的[2 F5/2→2 F7/2]的中等能量的光子.     

Ce3+对Er3+/Yb3+共掺氟磷酸盐玻璃光谱性质的影响

研究了能量接受离子Ce3+对Er3+上转换发光强度以及Er3+在1.5 μm附近波段发光性能参数的影响,并从能量匹配及能级结构角度出发对Er3+/Ce3+间的能量转移机制进行了分析.分析认为,4 I11/2能级的Er3+通过无辐射能量转移把能量传递给2F5/2能级的Ce3+激发其跃迁至2F7/2能级,而4I11/2能级上的Er3+则无辐射弛豫至4I13/2能级,从而有效降低氟磷酸盐玻璃中Er3+的上转换发光.当Er3+浓度为1.11×1020 cm-3时,Ce3+的最佳掺杂浓度为2.22×1020 cm-3,此时Ce3+的引入不仅可以降低上转换发光,而且有助于提高Er3+在1.5 μm附近波段的荧光强度、发射截面以及4I13/2能级荧光寿命.     

Tm∶YVO4晶体中Tm3+的发光研究

测量了Tm∶YVO4 晶体的吸收光谱 ,以 34 6nm、36 3nm(1D2 )、475nm(1G4 )、6 98nm (3 F2 ,3 F3 )和 80 1nm(3 H4 )光激发时的发射光谱 ,以及位于 45 4nm (1D2 → 3 F4 )、475nm (1G4 → 3 H6)、6 46nm (1G4 → 3 F4 )、80 6nm(3 H4 →3 H6)的荧光谱线的激发光谱 ,对测量的结果进行了详细分析 ,解释了离子能级间的跃迁过程。提出了Tm∶YVO4 晶体基质与Tm3 + 之间的能量交换的概念和新的跃迁通道 ,证实了存在1D2 +3 H6→1G4 +3 F4 以及1G4 +3 H6→3 H4 +3 H5的能量传递过程 ,还可能存在交叉弛豫过程 1G4 +3 H6→3 F2 +3 F4 。这些过程使得Tm∶YVO4 晶体难以实现1D2 能级上转换发光 (4 5 4nm左右 ) ,但 475nm的上转换发光 (1G4 →3 H6)较强 ,3 F4 能级是潜在红外激光发射能级。     

钨酸钇钠晶体中Tm3+的光谱特性

测量了Tm3 :NaY(WO4 ) 2 晶体的吸收光谱、发射光谱和激发光谱 ,利用J_O理论计算了钨酸钇钠晶体的强度参数 :Ω2 =7 2 130 4× 10 - 2 0 cm2 ,Ω4 =0 5 0 4 76 6× 10 - 2 0 cm2 ,Ω6 =0 977784× 10 - 2 0 cm2 ,以及Tm3 的光学参数包括各能级的荧光寿命和荧光分支比、积分发射截面等 ,在计算了Tm3 的自发辐射概率时 ,同时考虑了电偶极跃迁和磁偶极跃迁 .研究了其发光特性和跃迁通道 ,发现存在1 D2 3H6 →1 G4 3F4 的交叉弛豫     

Ce3+对Er3+/Yb3+共掺TeO2-WO3-ZnO玻璃发光性能的影响

在Er3+/Yb3+共掺TeO2-WO3-ZnO玻璃中引入Ce3+,研究了Ce3+对Er3+1.5μm发射性能及其上转换发光性能的影响.结果表明,随Ce3+浓度的增加Er3+1.5μm波段的荧光强度先增强后降低,优化的Ce3+掺杂浓度在2.07×1020/cm3左右;1.5μm波段的荧光寿命则随Ce3+浓度的增加有轻微降低,从3.4ms降到3.0ms,但Ce3+浓度的增加对1.5μm波段的荧光半高宽基本无影响;Er3+/Ce3+间的交叉弛豫Er3+(4I11/2+Ce3+(2F5/2→Er3+(4I13/2+Ce3+(2F7/2使玻璃的上转换发光强度大大降低,但在过高的Ce3+浓度下,Er3+/Ce3+间的另一交叉弛豫Er3+(4I13/2+Ge3+(2F5/2→Er3+(4I15/2+Ce3+(2F7/2则使Er3+4I13/2能级粒子数减少,导致1.5μm波段荧光强度和荧光寿命降低.     

Tm：YVO4晶体中Tm^3＋的发光研究

测量了Tm:YVO4晶体的吸收光谱,以346nm,363nm(^1D2),475nm(^1G4),698nm(^3F2,^3F3)和801nm(^3H4)光激发时的发射光谱,以及位于454nm(^1D2→^3F4),475nm(^1G4→^3H6),646nm(^1G4→^3F4),806nm(^3H4→^3H6)的荧光谱线的激发光谱,对测量的结果进行了详细分析,解释了离子能级间的跃迁过程,提出了Tm:YVO4晶体基质与Tm^3 之间的能量交换的概念和新的跃迁通道,证实了存在^1D2 ^3H6→^1G4 ^3F4以及^1G4 ^3H6→^3H4 ^3H5的能量传递过程,还可能存在交叉弛豫过程^1G4 ^H6→^3F2 ^3F4. 这些过程使得Tm:YVO4晶体难以实现^1D2能级上转换发光（454nm左右）,但475nm的上转换发光（^1G4→^3H6)较强,^3F4能级是潜在红外激光发射能级。     

Cs 5D_(5/2)-6F 728 nm Laser Spectroscopy with Single Pumping Laser

The sub-Doppler absorption laser spectroscopy at 728 nm transition from the 5D5/2 state to the 6 F state of cesium with linewidth near 10 MHz is first experimentally performed with indirect pumping from the ground state 6S_(1/2)to the state 7P_(3/2)by a 455.5 nm diode laser.Using a 455.5 nm diode laser as an indirect pump laser,several excited states will be populated due to spontaneous decay from the 7P state.We first implement the sub-Doppler absorption laser spectroscopy at 728 nm from the 5D_(5/2)state to the 6F state when Cs atoms within thermal glass cell decay to the 5D_(5/2) state.Due to velocity transfer effect,the hyperfine structure of 5D_(5/2)shows a mixed and complicated pattern but very clear structure when the 455.5 nm pumping laser is counter-propagating(or co-propagating)with the 728 nm probing laser.     

聚(9,9-二辛基芴)和聚(9,9-二辛基芴-共-苯并噻二唑)的光物理特性的理论和实验研究

通过比较分析聚(9,9-二辛基芴)(PFO)和聚(9,9-二辛基芴-共-苯并噻二唑)(F8BT),对半导体聚合物的光物理特性进行了系统研究. 量子化学计算显示,苯并噻二唑单元的引入促进了链内电荷转移(ICT),调节了聚合物的电子跃迁机制. 瞬态吸收测定表明,在单分散系统中的受激PFO衰减时主要表现为链内激子弛豫.在F8BT溶液中,ICT状态出现,并参与到激发态的弛豫过程中. 凝聚相中PFO和F8BT的弛豫过程加速和显示了在高激发强度下具有显著的激子湮灭行为. 在相同的激发强度下,F8BT的平均寿命长于PFO,有助于实现良好的电荷离域.     

DMSO溶剂中All-trans-astaxanthin激发态的飞秒时间分辨光谱

基于飞秒时间分辨瞬态吸收和多元瞬态光栅光谱技术对全反式Astaxanthin(AXT)在DMSO溶剂中的超快激发态弛豫动力学进行了观测.结果表明,光激发后AXT/DMSO体系直接发生S_0→S_2跃迁,基态漂白对应光谱范围为420~550nm.由S_2→S_1的内转换过程发生的时间常数为120~160fs.S_1态激发态吸收对应的光谱范围为550~740nm,基态漂白恢复过程对应的是S_1→S_0的内转换过程,其时间尺度为4.50~5.50ps.     

紫外激发Ba_2SiO_4∶Gd~(3+),Tb~(3+)的发光性能

采用高温固相法合成了可被紫外光激发的Ba_2SiO_4∶Gd~(3+),Tb~(3+)荧光粉。考察了激活离子掺杂量等因素对发光性能的影响。通过X射线衍射(XRD)、荧光(FL)光谱和荧光寿命曲线对所合成样品的结构和发光性能进行表征,研究了Gd~(3+)和Tb~(3+)的特征吸收波长激发Ba_2SiO_4∶Gd~(3+),Tb~(3+)的发光性能。在275 nm(Gd~(3+):8S7/2→6IJ)激发下,检测到了Tb~(3+)的特征发射。通过对比不同Tb~(3+)掺杂量下Gd~(3+):~6P_(7/2)能级的衰减曲线,发现随着Tb~(3+)掺杂浓度的增加,该能级的荧光寿命不断缩短,表明样品中存在Gd~(3+)→Tb~(3+)的能量传递,传递方式为无辐射共振能量传递。在244 nm(Tb~(3+):4f~8→4f~75d~1)激发下,Gd~(3+)的掺入使得Tb~(3+)的~5D_3能级的发射逐渐减弱,5D4能级的发射增强。Gd~(3+)的掺入使得544 nm(~5D_4→~7F_5)处的特征发射增强了59%~128%,结合荧光衰减曲线得出Gd~(3+)的掺入对Tb~(3+)能级中~5D_3→~5D_4与~7F_6→~7F_0交叉驰豫有促进作用。     

Intra-acceptor hole relaxation in Be δ-doped GaAs/AlAs multiple quantum wells

This paper studies the dynamics of intra-acceptor hole relaxation in Be δ -doped GaAs/AlAs multiple quantum wells (MQW) with doping at the centre by time-resolved pump-probe spectroscopy using a picosecond free electron laser for infrared experiments. Low temperature far-infrared absorption measurements clearly show three principal absorption lines due to transitions of the Be acceptor from the ground state to the first three odd-parity excited states respectively. The pump-probe experiments are performed at different temperatures and different pump pulse wavelengths. The hole relaxation time from 2p excited state to 1s ground state in MQW is found to be much shorter than that in bulk GaAs, and shown to be independent of temperature but strongly dependent on wavelength. The zone-folded acoustic phonon emission and slower decay of the wavefunctions of impurity states are suggested to account for the reduction of the 2p excited state lifetime in MQW. The wavelength dependence of the 2p lifetime is attributed to the diffusion of the Be atom δ -layer in quantum wells.     

Time resolved excited state absorption of Mn

Excited state absorption (ESA) of Mn²⁺ in spinel MgAl₂O₄ is investigated in detail. For excitation ps-pulses of 351 nm wavelength from a tripled Nd phosphate glass laser are used. During relaxation down to the lowest excited state ESA is measured for various delay times between exciting pulse and probe pulse. The resulting absorption spectra are interpreted in terms of the Mn²⁺ configurational model.     

香豆素C1F和C2F在醇类溶剂中的激发态溶剂效应

本文在Grabowski模型基础上,提出了一种描述TICT态生成动力学的理论模型,并采用时间相关单光予计数荧光光谱方法,测量了香豆素C1F和C2F在醇类溶剂中的荧光寿命,考察了各种溶剂效应(极性、粘度和温度)对TICT态生成速率的影响,并将结果与DSE关系比较,指出在醇类溶剂中,氢链效应的影响是十分重要的.     

Ultrafast proton transfer dynamics of 2-(2'-hydroxyphenyl)benzoxazole dye in different solvents

The excited-state intramolecular proton transfer of 2-(2-hydroxyphenyl)benzoxazole dye in different solvents is investigated using ultrafast femtosecond transient absorption spectroscopy combined with quantum chemical calculations.Conformational conversion from the syn-enol configuration to the keto configuration is proposed as the mechanism of excited-state intramolecular proton transfer.The duration of excited-state intramolecular proton transfer is measured to range from 50 fs to 200 fs in different solvents.This time is strongly dependent on the calculated energy gap between the N-S;and T-S;structures in the S;state.Along the proton transfer reaction coordinate,the vibrational relaxation process on the S;state potential surface is observed.The duration of the vibrational relaxation process is determined to be from8.7 ps to 35 ps dependent on the excess vibrational energy.     

铯原子nP_(3/2)(n=70—94)里德伯态的紫外单光子激发及量子亏损测量

基于成熟的光纤激光器、光纤放大器及高效激光频率转换技术,我们在实验中研制了一套瓦级输出的窄线宽连续波单频可调谐318.6 nm紫外激光系统,并在室温铯原子气室中实现了6S_(1/2)—nP_(3/2)(n=70—94)单光子跃迁里德伯激发.借助由铯原子6S_(1/2)(F=4)基态、6P_(3/2)(F′=5)激发态和nP_(3/2)(n=70—94)里德伯态构成的V型三能级系统,通过频率锁定于铯原子6S_(1/2)(F=4)—6P_(3/2)(F′=5)超精细跃迁的852.3 nm探测光束的吸收减弱信号获得了里德伯态的信息,并利用高精度波长计测量了铯原子nP_(3/2)(n=70—94)里德伯态的量子亏损值.经过与理论计算值的变化趋势进行对比,我们认为由于原子气室的里德伯屏蔽效应并不能完全屏蔽外部直流电场,铯原子气室内存在残余的直流电场,影响了对里德伯态的量子亏损值的实验测量.利用残余直流电场的Stark效应理论模型及其与有效主量子数n*的依赖关系,对铯原子里德伯态的量子亏损实验测量值进行了修正.修正后的铯原子nP_(3/2)(n=70—94)态量子亏损测量值为3.5591±0.0007,与理论计算值相吻合.     

Study of amorphous thin films of (Ti, Nb)O2 solid solutions by X-ray absorption at the Ti K edge

As the (Ti, Nb)O₂ amorphous thin films cannot be prepared under a self-supported form, we have recorded the X-ray reflectivity. A new program which allows extraction of the X-ray absorption from the reflectivity is briefly described. The correction of the anomalous dispersion effect is effective, particularly near the edge within 200 eV. Hence, it has allowed a comparison between the amorphous layers and the crystalline analogues for which the X-ray absorption has been recorded by transmission. In the amorphous state, the TiO₆ group is smaller than in the crystalline state because of the relaxation of the crystallographic constraints. The oxygen coordination octahedron is almost regular in the films. On the other hand, in both cases, an electron transfer takes place from Nb to Ti.