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1.
采用5 W激光二极管端面抽运Nd∶YAG晶体,通过设计合理的谐振腔膜系,再分别利用双折射滤波器和标准具获得单一谱线基频光,采用长度为10 mm的Ⅰ类临界相位匹配LBO晶体进行倍频,获得稳定的561 nm单谱线输出。理论分析了双折射滤波器和标准具抑制其他竞争谱线的过程,发现使用双折射滤波器可以获得更窄线宽的输出,而使用标准具获得的输出功率更高,理论与实验相符。在泵浦功率为4.8 W时,分别获得227 mW和254 mW的561 nm单谱线输出。斜效率分别为6%和6.68%。  相似文献   

2.
实验采用激光二极管阵列(LDA)端面抽运Nd∶YVO4晶体,腔内产生1064 nm和1342 nm双波长振荡,通过非线性晶体LBO的I类相位匹配产生连续输出的593.5 nm和频光。在不同的实验条件下,测量并分析了噪声特性,并用法布里-珀罗干涉仪和光束轮廓仪分别测量了593.5 nm激光在低噪声与高噪声状态下的纵模结构与横模模式。结果表明:I类相位匹配的和频光噪声情况与其纵模结构密切相关,而抽运功率和谐振腔微调对和频光的纵模结构有很大影响。激光输出在多纵模结构不稳定时的噪声要高于多纵模结构稳定时的噪声。并且激光输出为高阶横模模式时,也会引起激光噪声的增大。  相似文献   

3.
报道了利用激光二极管端面抽运Nd∶YAG晶体,通过LBO非线性晶体腔内倍频实现的561nm激光输出。LBO晶体尺寸为2mm×2mm×10mm,采用Ⅰ类相位匹配切割。抽运功率为5W时,561nm的最大输出功率为123mW,此时的光-光转换效率为2.46%。实验中发现激光器很容易同时出现556nm及558nm倍频光。从非线性转换效率对基频光振荡的影响角度出发,分析了1112nm与1116nm谱线起振的原因。作为对比,利用允许角范围小的KTP作为倍频晶体进行了同样的实验,KTP晶体的尺寸为2mm×2mm×8mm,采用Ⅱ类相位匹配切割。实验结果显示,在KTP晶体倍频情况下,激光器很容易实现561nm单谱线激光输出。实验结果与理论分析相一致。  相似文献   

4.
设计了一种结构紧凑、性能稳定、成本低的腔内和频单纵模593.5 nm黄光激光器。采用线性平凹腔结构,LD端面泵浦Nd:YVO_4晶体产生1064 nm和1342 nm双波长激光束;通过KTP(KTiOPO_4)Ⅱ类临界相位匹配在腔内和频产生593.5 nm连续黄光激光输出。利用由单个布氏片(BP)与和频晶体KTP构成的双折射滤波片进行选频,在泵浦功率为5.0 W时,593.5 nm和频光单纵模输出功率为30 mW,方均根噪声为0.8%,线宽为150 MHz。此时,检测到1064 nm和1342 nm基频光均为单纵模状态。实验结果表明,在和频激光器中,利用双折射滤波片技术使得基频光次振荡纵模损耗≥1.5%,即可以实现单纵模和频激光输出。  相似文献   

5.
付林  李斌 《激光与红外》2012,42(6):642-645
介绍了一种在腔内插入全波片实现671 nm激光低噪声稳定运转的方法。该方法利用全波片和Nd∶YVO4激光器的偏振特性构成双折射滤光片,使用I类临界相位匹配LBO作为倍频晶体,在注入泵浦功率2.7 W的情况下获得149 mW的671 nm低噪声红光输出,光-光转换率为5.6%。使用该方法研制的激光器结构简单、紧凑,适用于中低功率激光器。  相似文献   

6.
报道了一种激光二极管抽运Nd∶YVO4晶体、腔内Ⅰ类临界相位匹配LBO和频、连续波输出的全固态橙黄色激光器的设计和实验结果。橙黄色激光由Nd∶YVO4晶体的1064nm和1342nm谱线腔内和频产生,输出波长为593.5nm。实验采用了双镜谐振腔结构,在1.6W的808nm注入抽运功率下,获得了最高功率为84mW连续波TEM00的橙黄色低噪声激光输出,光-光转换效率为5.3%,光束质量因子M2<1.2。实验和分析表明,采用激光二极管抽运Nd∶YVO4晶体、LBOⅠ类临界相位匹配腔内和频是获得橙黄色激光的实用方法,并可以应用到Nd∶YVO4晶体的其它谱线或具有多条谱线的其它激光增益介质,获得更多不同颜色的单谱线激光输出。  相似文献   

7.
8 W高功率全固态LD双端抽运连续波绿光激光器   总被引:2,自引:0,他引:2  
高功率全固态绿光激光器在激光抽运、激光精密加工、激光医学、激光展示、光存储、信息处理、检测等方面有许多应用。Nd∶YVO4 LBO是目前用于产生 5 32nm绿色激光辐射的一组理想晶体组合。本实验小组以 3mm× 3mm× 10mm @0 .5wt . %的Nd∶YVO4晶体为增益介质 ,4mm× 4mm× 15mm ,Ⅰ类非临界相位匹配的LBO为二倍频晶体 ,当抽运功率为 2 8 9W时 ,获得了 8W (已滤除掉 1 0 6 4μm的基频光 )的稳定绿光输出 ,光 光转换效率高达约2 8%。图 1实验装置Fig .1Experimentalsetup  实验装置采用Z型折叠腔 (见图 1) ,通过数值计算与优化得…  相似文献   

8.
报道了一种激光二极管抽运Nd:YVO4晶体、腔内Ⅰ类临界相位匹配LBO和频、连续波输出的全固态橙黄色激光器的设计和实验结果。橙黄色激光由Nd:YVO4晶体的1064nm和1342nm谱线腔内和频产生,输出波长为593.5nm。实验采用了双镜谐振腔结构,在1.6W的808nm注入抽运功率下,获得了最高功率为84mW连续波TEM00的橙黄色低噪声激光输出,光-光转换效率为5.3%,光束质量因子M21.2。实验和分析表明,采用激光二极管抽运Nd:YVO4晶体、LBOⅠ类临界相位匹配腔内和频是获得橙黄色激光的实用方法,并可以应用到Nd:YVO4晶体的其它谱线或具有多条谱线的其它激光增益介质,获得更多不同颜色的单谱线激光输出。  相似文献   

9.
报道了LD 端面泵浦Nd∶YVO4 晶体产生1064nm 和1342nm 双波长激光束,采用一个线性平凹腔结构,利用LBO Ⅰ类临界相位匹配在腔内和频产生593. 5nm连续黄光激光输出的全固体激光器的实验研究。在泵浦功率为10W时得到593. 5nm的黄光激光输出功率为260mW。光束远场发散角θ< 1mrad。593. 5nm激光输出为低噪声输出。24h 功率不稳定度小于±2 %。  相似文献   

10.
红光低噪声激光器在很多方面有着重要的应用,实现低噪声的方法很多,如环形腔法、扭摆模腔法、标准具法等等,以上方法要么结构复杂要么损耗很大,不适合小型化,产品化.研究报道了一种利用Nd1YVO4激光器的偏振特性和Ⅱ类临界相位匹配LBO作为倍频晶体构成双折射滤光片的方法实现低噪声红光激光输出,在注入泵浦功率2W的情况下获得61mw的671nm低噪声红光输出,光-光转换率3%,该结构简单、紧凑,适合用于中低功率激光器.  相似文献   

11.
Waveguide multilayer optical card (WMOC) is a novel storage device of three-dimensional optical information. An advanced readout system fitting for the WMOC is introduced in this paper. The hardware mainly consists of the light source for reading, WMOC, motorized stages addressing unit, microscope imaging unit, CCD detecting unit and PC controlling & processing unit. The movement of the precision motorized stage is controlled by the computer through Visual Basic (VB) language in software. A control panel is also designed to get the layer address and the page address through which the position of the motorized stages can be changed. The WMOC readout system is easy to manage and the readout result is directly displayed on computer monitor.  相似文献   

12.
IntroductionNanoimprint Lithography is a well-acknowl-edged low cost, high resolution, large area pattern-ing process. It includes the most promising methods,high-pressure hot embossing lithography (HEL) [2],UV-cured imprinting (UV-NIL) [3] and micro contactprinting (m-CP, MCP) [4]. Curing of the imprintedstructures is either done by subsequent UV-lightexposure in the case of UV-NIL or by cooling downbelow the glass transition temperature of the ther-moplastic material in case of HEL…  相似文献   

13.
The collinearly phase-matching condition of terahertz-wave generation via difference frequency mixed in GaAs and InP is theoretically studied. In collinear phase-matching, the optimum phase-matching wave hands of these two crystals are calculated. The optimum phase-matching wave bands in GaAs and lnP are 0.95-1.38μm and 0.7-0.96μm respectively. The influence of the wavelength choice of the pump wave on the coherent length in THz-wave tuning is also discussed. The influence of the temperature alteration on the phase-matching and the temperature tuning properties in GaAs crystal are calculated and analyzed. It can serve for the following experiments as a theoretical evidence and a reference as well.  相似文献   

14.
Composition dependence of bulk and surface phonon-polaritons in ternary mixed crystals are studied in the framework of the modified random-element-isodisplacement model and the Bom-Huang approximation. The numerical results for Several Ⅱ - Ⅵ and Ⅲ- Ⅴ compound systems are performed, and the polariton frequencies as functions of the compositions for ternary mixed crystals AlxGa1-xAs, GaPxAS1-x, ZnSxSe1-x, GaAsxSb1-x, GaxIn1-xP, and ZnxCd1-xS as examples are given and discussed. The results show that the dependence of the energies of two branches of bulk phonon-polaritons which have phonon-like characteristics, and surface phonon-polaritons on the compositions of ternary mixed crystals are nonlinear and different from those of the corresponding binary systems.  相似文献   

15.
A doping system consisting of NPB and PVK is employed as a composite hole transporting layer (CHTL). By adjusting the component ratio of the doping system, a series of devices with different concentration proportion of PVK : NPB are constracted. The result shows that doping concentration of NPB enhances the competence of hole transporting ability, and modifies the recombination region of charge as well as affects the surface morphology of doped film. Optimum device with a maximum brightness of 7852 cd/m^2 and a power efficiency of 1.75 lm/W has been obtained by choosing a concentration proportion of PVK : NPB at 1:3.  相似文献   

16.
An insert layer structure organic electroluminescent device(OLED) based on a new luminescent material (Zn(salen)) is fabricated. The configuration of the device is ITO/CuPc/NPD/Zn(salen)/Liq/LiF/A1/CuPc/NPD/Zn(salen)/Liq/LiF/A1. Effective insert electrode layers comprising LiF(1nm)/Al(5 nm) are used as a single semitransparent mirror, and bilayer cathode LiF(1 nm)/A1(100 nm) is used as a reflecting mirror. The two mirrors form a Fabry-Perot microcavity and two emissive units. The maximum brightness and luminous efficiency reach 674 cd/m^2 and 2.652 cd/A, respectively, which are 2.1 and 3.7 times higher than the conventional device, respectively. The superior brightness and luminous efficiency over conventional single-unit devices are attributed to microcavity effect.  相似文献   

17.
Due to variable symbol length of digital pulse interval modulation(DPIM), it is difficult to analyze the error performances of Turbo coded DPIM. To solve this problem, a fixed-length digital pulse interval modulation(FDPIM) method is provided. The FDPIM modulation structure is introduced. The packet error rates of uncoded FDPIM are analyzed and compared with that of DPIM. Bit error rates of Turbo coded FDPIM are simulated based on three kinds of analytical models under weak turbulence channel. The results show that packet error rate of uncoded FDPIM is inferior to that of uncoded DPIM. However, FDPIM is easy to be implemented and easy to be combined, with Turbo code for soft-decision because of its fixed length. Besides, the introduction of Turbo code in this modulation can decrease the average power about 10 dBm, which means that it can improve the error performance of the system effectively.  相似文献   

18.
It is a key problem to accurately calculate beam spots' center of measuring the warp by using a collimated laser. A new method, named double geometrical center method (DGCM), is put forward for the first time. In this method, a plane wave perpendicularly irradiates an aperture stop, and a charge couple device (CCD) is employed to receive the diffraction-beam spots, then the geometrical centers of the fast and the second diffraction-beam spots are calculated respectively, and their mean value is regarded as the center of datum beam. In face of such adverse instances as laser intension distributing defectively, part of the image being saturated, this method can still work well. What's more, this method can detect whether an unacceptable error exits in the courses of image receiving, processing and calculating. The experimental results indicate the precision of this method is high.  相似文献   

19.
High purity organic-tantalum precursors for thin film ALD TaN were synthesized and characterized.Vapor pressure and thermal stability of these precursors were studied.From the vapor pressure analysis,it was found that TBTEMT has a higher vapor pressure than any other published liquid TaN precursor,including TBTDET,TAITMATA,and IPTDET.Thermal stability of the alkyl groups on the precursors was investigated using a 1H NMR technique.The results indicated that the tertbutylimino group is the most stable group on TBTDET and TBTEMT as compared to the dialkylamido groups.Thermal stability of TaN precursors decreased in the following order:TBTDET > PDMAT > TBTEMT.In conclusion,precursor vapor pressure and thermal stability were tuned by making slight variations in the ligand sphere around the metal center.  相似文献   

20.
In order to diagnose the laser-produced plasmas, a focusing curved crystal spectrometer has been developed for measuring the X-ray lines radiated from a laser-produced plasmas. The design is based on the fact that the ray emitted from a source located at one focus of an ellipse will converge on the other focus by the reflection of the elliptical surface. The focal length and the eccentricity of the ellipse are 1350 mm and 0.9586, respectively. The spectrometer can be used to measure the X- ray lines in the wavelength range of 0.2-0.37 nm, and a LiF crystal (200) (2d = 0.4027 nm) is used as dispersive element covering Bragg angle from 30° to 67.5°. The spectrometer was tested on Shengnang- Ⅱ which can deliver laser energy of 60-80 J/pulse and the laser wavelength is 0.35 μm. Photographs of spectra including the 1 s2p ^1P1-1s^2 ^1S0 resonance line(w), the 1s2p ^3P2-1s^2 1S0 magnetic quadrupole line(x), the 1s2p ^3P1-1 s^2 ^1S0 intercombination lines(y), the 1 s2p ^3S~1-1 s^2 ^1S0 forbidden line(z) in helium-like Ti Ⅹ Ⅺ and the 1 s2s2p ^2P3/2-1 s622s ^2S1/2 line(q) in lithium-like Ti Ⅹ Ⅹhave been recorded with a X-ray CCD camera. The experimental result shows that the wavelength resolution(λ/△ 2) is above 1000 and the elliptical crystal spectrometer is suitable for X-ray spectroscopy.  相似文献   

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