准波导结构染料薄膜中荧光和放大自发辐射的泄漏模特性

通过理论分析和实验测量,研究准波导结构染料薄膜中荧光和放大自发辐射（ASE）的泄漏模特性。理论上,考虑薄膜传输损耗及染料吸收损耗对准波导结构中泄漏模特性的影响,通过计算准波导结构中泄漏模的光强分布,给出了相应的物理机制分析;实验上,以棱镜为衬底制备染料薄膜,根据棱镜耦合法测量不同出射角对应的泄漏模的荧光与ASE光谱,验证理论的正确性。此外,采用光束分析仪探测各泄漏模式对应的荧光及ASE的光强分布,研究了准波导结构中ASE的激励特性。结果证明,荧光峰及ASE峰的红移以及泄漏模的激发是界面反射率、薄膜传输损耗及染料吸收损耗等共同作用的结果,而界面反射率对ASE泄漏模激发特性有重要影响,染料的自吸收是荧光峰及ASE峰产生红移的主要因素。     

有机染料TMQ掺杂的SiO2薄膜的光谱特性

采用溶胶 -凝胶法合成了紫外波段有机染料 TMQ掺杂的 Si O2 薄膜和块体材料。薄膜中掺杂的染料浓度高达 1.2 4× 10 -2 mol/ L,块体材料中染料浓度可掺至 1.5× 10 -3 mol/ L。由于Si O2 “笼”的束缚作用 ,在吸收光谱中未观察到二聚体的特征谱带 ,在荧光光谱中未观察到荧光猝灭现象 ;同时由于 Si O2 “笼”的极化作用 ,其吸收峰和发射峰的位置相对于其在环己烷溶液中的吸收峰和发射峰位置发生了 10 nm左右的红移。     

染料掺杂聚合物光纤的荧光及其光谱下转换性质

为了拓展染料掺杂聚合物光纤的应用范围,利用甲基丙烯酸甲酯(MMA)单体合成了掺有Coumarin540和Rhodamine 6G两种激光染料的聚甲基丙烯酸甲酯(PMMA)聚合物玻璃棒,并将其拉制成直径约1 000μm的聚合物光纤。以市售LED灯为光源,在侧向照明和前端照明两种条件下分别研究了染料掺杂的聚合物光纤中染料的荧光、荧光传输损耗以及光纤的光谱下转换等性质。两种染料的Stokes波长红移幅度分别达到70 nm和50 nm。在掺杂浓度分别为0.01 mg/g和0.04 mg/g时,侧向照明条件下测得两种光纤分别对520nm和577 nm的荧光的传输损耗为0.336 cm-1和0.343 cm-1。在前端照明条件下,在光纤输出端获得了较高下转换效率的光谱输出,其转换效率与染料掺杂浓度和光纤长度有关。这种染料掺杂的聚合物光纤有可能与石英玻璃光纤耦合,对其所传输的光进行光谱下转换的光频调控以更好地满足不同的应用需求。     

掺杂偶氮化合物的PMMA光折变聚合物的拉曼光谱分析

光折变聚合物具有良好的光折变效应,采用以惰性聚合物PMMA为基体,掺杂偶氮化合物染料的光折变聚合物具有较好的光学非线性和稳定性。文章主要介绍使用激光拉曼光谱仪对合成聚合物的各单体和聚合物薄膜进行拉曼光谱扫描,对比分析各个单体成分的特征谱峰与聚合物薄膜特征谱峰,肯定了实验中得到的光折变聚合物薄膜与理论上要求得到的一致性。     

利用谐波光谱的伴线结构测量自生磁场

在飞秒激光与固体靶相互作用中,利用OMA光学多道分析谱仪,在靶前表面激光镜反方向测量了激光的二次谐波(2ω₀)光谱和三次谐波(3ω₀)光谱,观测到了红移的2ω₀光谱和3ω₀光谱的伴线结构。在激光功率密度为～1018 W·cm-2的条件下,通过2ω₀和3ω₀谐波光谱的伴线结构,回推出激光与等离子体相互作用中产生的自生磁场均小于1 MGs。随着激光功率密度的增大,谐波谱红移峰向长波方向移动,光谱同时发生展宽。分析认为,等离子体临界面的迅速膨胀是导致二次谐波和三次谐波红移的主要原因。随着预脉冲功率密度的增大,临界面膨胀速度增大,导致了谐波光谱峰更大的红移。自生磁场的测量为诊断临界面的运动方向和速度提供了新的依据。     

宽带输出PM580掺杂聚甲基丙烯酸甲酯固体染料激光器研究

采用高效激光染料PM580作为掺杂物质,聚甲基丙烯酸甲酯(PMMA)作为基质,在对固体染料光谱特性研究的基础上,重点研究了调Q倍频Nd:YAG抽运下不同染料掺杂浓度的固体染料激光输出特性.研究结果表明掺杂浓度对输出激光波长影响明显,随着掺杂浓度的增加,激光输出波长红移,从激光增益出发,对该现象给出了理论解释.掺杂浓度对激光转化效率也有影响,当掺杂浓度为2×10^－4mol/L时,获得染料激光输出斜率效率最高达53.8%,抽运能量410mJ时,获得染料激光输出220mJ,激光带宽～8nm 关键词： 固体染料 宽带染料激光 PM580 聚甲基丙烯酸甲酯     

染料掺杂聚合物薄膜的光谱下转换研究

在玻璃基片表面制作了Coumarin 500、Coumarin 540和Rhodamine 6G 3种染料掺杂的聚合物薄膜,并以市售LED灯和氙灯为光源,实验研究了单一染料掺杂和混合染料掺杂的聚合物薄膜的吸收光谱、荧光光谱及其光谱下转换的特征。研究结果表明：这种多染料掺杂的聚合物薄膜能够吸收350~550 nm波长范围内的光子并将其转换至波长为580 nm左右的光子。在一定的浓度范围内,较高的染料浓度能够获得较高的下转换光子输出。由于Nd³⁺/Yb³⁺共掺玻璃中Nd³⁺离子在 580 nm 附近有一个较强的吸收峰,这种染料掺杂聚合物薄膜的光谱下转换有助于提高Nd³⁺/Yb³⁺共掺玻璃对太阳光中蓝绿光的吸收并通过共振能量转移激发Yb³⁺离子的近红外发光,对提高单晶硅太阳能电池的综合光伏转换效率有潜在的应用价值。     

基于有机半导体激光材料的高灵敏度溶液检测传感器件

采用光抽运有机激光增益材料产生的放大自发辐射(amplified spontaneous emission ASE), 实现了不同浓度液体的实时检测. 以两种聚合物poly(9, 9-dioctylfluorene-co-benzothiadiazole)和poly(3-hexylthiophene)共混的激光增益介质薄膜作为平面光波导, 观察在滴加少量溶液前后以及不同溶液浓度下, 由于光波导的相对折射率变化导致的放大自发辐射阈值及峰位的变化, 实现对溶液检测. 实验结果显示, 在常温常压下对25 wt.% NaCl溶液检测可得与纯水相比, 放大自发辐射光谱红移了4.5 nm, ASE阈值从0.579 μJ/pulse上升到1.447 μJ/pulse, 约2.5倍, 溶液检测灵敏度达到97.8 nm/RIU(refractive index unit), 精度达到141.9 nm/RIU, 充分说明上述方法能实现高灵敏度溶液检测.     

Zn1-x-yNaxCoyO薄膜的脉冲激光沉积制备及表征

采用脉冲激光沉积技术,在Si(111)衬底上成功制备出不同含量Na,Co共掺的ZnO薄膜.利用X射线衍射仪、原子力显微镜、荧光光谱仪以及四探针电阻率测试台对薄膜的结构、表面形貌和光电性质进行了表征.重点讨论了不同掺杂浓度对薄膜光电性质的影响.结果表明:Na,Co共掺没有改变ZnO的六角纤锌矿结构且掺杂导致薄膜仅有的的紫外发光峰出现红移.当Na,Co掺杂浓度分别为10%时,峰值最强且红移最明显,发光峰波长为397 nm,薄膜的电阻率最低,达到了8.34×10^-1 Ω ·cm.深入讨论了 关键词： 脉冲激光沉积 1-x-yNa_xCo_yO薄膜')" href="#">Zn_1-x-yNa_xCo_yO薄膜 光电性质 红移     

Rh6G/氧化多孔硅复合膜的荧光光谱

为了发展性能良好的固体染料激光器,多孔介质中镶嵌激光染料是一种可行的途径。将氧化多孔硅作为基质材料,通过浸泡的方式将激光染料Rh6G嵌入其中,形成Rh6G/氧化多孔硅复合膜,对比研究了Rh6G在无水乙醇、多孔硅、多孔氧化硅中的荧光特性。结果表明,经高温氧化后,氧化多孔硅透明度提高,其荧光强度明显变弱,在复合膜中已检测不到其荧光行为。相比于在无水乙醇溶液中,在氧化多孔硅中Rh6G发射光谱的半峰全宽有所展宽,峰值波长略有红移,对称性大为提高,具有类似单体发光特性,这种现象与纳米孔对Rh6G的聚集程度的限制有关。     

The stimulated Raman scattering competition between solute and solvent in Rhodamine B solution

The competition between the stimulated resonance Raman scattering(SRRS) of Rhodamine B(RhB) and the stimulated Raman scattering(SRS) of ethanol(C2H5OH) is observed at the RhB in C2H5OH solution.For different concentrations of the solution,the peak wavelengths of the SRRS,the amplified spontaneous emission(ASE),the fluorescence and the absorption of RhB are different.The SRRS of RhB and the SRS of C2H5OH are simultaneously generated when the concentration of the solution is 10 5 mol/L and the energy of the excitation laser is 20.4 mJ.Otherwise,only either the SRRS of RhB or the SRS of C2H5OH is generated.The SRRS can be amplified by the ASE gain when the SRRS is near the peak of the ASE,and the peak wavelength of the SRRS coincides with the wavelength of the maximal intensity ASE.     

Stimulated resonance Raman scattering of Rhodamine B

Stimulated resonance Raman scattering (SRRS) of the Rhodamine B (RhB) in the methanol (CH₃OH) or ethanol (C₂H₅OH) solutions have been observed. SRRS from RhB can be distinguished from the amplified spontaneous emission (ASE) of RhB with increasing the input laser energy. When the RhB is dissolved in the methanol or ethanol (10^?3 mol/L), the RhB have the different peak wavelengths of SRRS, ASE, fluorescence and absorption, respectively. SRRS can be amplified by the ASE gain when the SRRS is near the peak of the ASE, and the peak wavelength of SRRS coincides with the maximal intensity wavelength of ASE.     

Two-photon-pumped amplified spontaneous emission and cavity lasing of an organic dye HEASPS in PHEMA polymer

Two-photon-absorption (TPA)-induced upconverted amplified spontaneous emission (ASE) and cavity lasing of a styrylpyridinium dye: trans-4-[p-(N-hydroxyethyl-N-ethylamino)styryl]-N-methylpyridinium p-toluene sulfonate (abbreviated as HEASPS) in poly(2-hydroxyethyl methacrylate) (abbreviated as PHEMA) polymer were observed under a picosecond pump condition. The spectral and temporal behaviors of TPA-induced fluorescence, ASE and cavity lasing were studied. The cavity lasing with a total oscillation time of more than 200 ps was achieved when pumped with 1064-nm, 50-ps laser irradiation. The population inversion could persist for three times longer than the duration of the pump pulse. The gain coefficients of the dye-doped polymer at various wavelengths were calculated based on cavity lasing spectra and one-photon fluorescence spectra. PACS 78.20.Ek; 42.65.Ky; 42.65.Re; 78.47.+p     

The stimulated Raman scattering competition between solute and solvent in Rhodamine B solution

The competition between the stimulated resonance Raman scattering (SRRS) of Rhodamine B (RhB) and the stimulated Raman scattering (SRS) of ethanol (C₂H₅OH) is observed at the RhB in C₂H₅OH solution. For different concentrations of the solution, the peak wavelengths of the SRRS, the amplified spontaneous emission (ASE), the fluorescence and the absorption of RhB are different. The SRRS of RhB and the SRS of C₂H₅OH are simultaneously generated when the concentration of the solution is 10^-5 mol/L and the energy of the excitation laser is 20.4 mJ. Otherwise, only either the SRRS of RhB or the SRS of C₂H₅OH is generated. The SRRS can be amplified by the ASE gain when the SRRS is near the peak of the ASE, and the peak wavelength of the SRRS coincides with the wavelength of the maximal intensity ASE.     

Two-dimensional DFB laser fabricated on dye-doped hybrid zirconia film by soft lithography

A two-dimensional(2D) distributed feedback(DFB) structure is fabricated on dye-doped sol-gel derived hybrid zirconia films by soft lithography.The Q-switched Nd:YAG laser(λ = 532 nm) is used to pump these structures.The lasing emissions of the gain medium doped with Rhodamine 6G(Rh6G) in two perpendicular directions are shown,and the threshold pump energy is measured.     

固溶态染料激光物质的研究

本文从不同改进的掺Rh6G聚甲基丙烯酸甲脂(PMMA)固溶态物质获得了有效的激光.热稳定性得到改善以及工作寿命得到延长.研究了它们的激射和光谱特性.     

紫外新激光染料IBOP的研究

本文介绍一种新合成的化合物IBOP.经在多种染料激光器上测试表明,其激光转换效率高,光化学稳定性好,能溶于多种溶剂.性能优于DPS等相同波段的常用激光染料.IBOP在各种溶剂中的激光调谐范围为388～428nm,激光峰值波长在400nm左右.本文给出了IBOP的荧光光谱、吸收光谱、激光特性、溶剂效应和浓度效应等数据,并作了讨论.     

芴类荧光染料掺杂DNA-CTMA薄膜的放大自发辐射特性

钯催化Suzuki反应合成得到一种9,9-二乙基-2,7-二-(4-吡啶)芴（DPFP）荧光染料,研究了该染料的吸收和荧光光学特性,以及DPFP掺杂DNA-CTMA薄膜的荧光光谱特性和放大自发辐射特性。实验结果表明:DPFP的吸收峰位于333 nm,DPFP的荧光光谱在370 nm和386 nm出现荧光峰,在408 nm出现肩峰,存在从激发态S1能级到基态S0能级的S10-S00,S10-S01和S10-S02三种振动带的电子跃迁;同时,在Nd:YAG纳秒激光器355 nm输出光的泵浦下,DPFP掺杂DNA-CTMA薄膜在波长390 nm和406 nm处实现了放大自发辐射,其阈值能量密度分别为3.24和3.40 mJ/cm2;此外,通过调节DPFP掺杂DNA-CTMA的质量比可以实现特定波长的放大自发辐射。