共查询到20条相似文献,搜索用时 140 毫秒
1.
2.
采用经典的光学传输矩阵法和微腔理论计算具有不同厚度的功能有机薄膜和电极形式的顶发射有机发光二极管光学的耦合出光效率。根据仿真计算结果,制备了绿色荧光Alq3顶发射器件并进行了相关测试。研究发现,采用银作为半透明阴极并蒸镀NPB有机覆盖层,相对于无覆盖层的器件来说,出光效率大大增强,该增强效应采用近场光学理论的偶极子辐射与银电极相互作用理论,即耦合表面等离子体激元理论,解释为是金属Ag薄膜阴极增强的透射、变化的微腔增益以及最主要的出光银阴极上的耦合表面等离子体激元效应三个因素的综合作用。 相似文献
3.
微片固体激光器具有体积小、寿命长等优点,是精密测量仪器的重要光源。构建了平-平、半外腔的Nd:YAG和Nd:YVO4微片激光器,通过控制压电陶瓷伸缩改变激光器的谐振腔长,同时使用F-P扫描干涉仪和波长计观察纵模和波长。研究了这2种微片固体激光器的腔调谐特性,包括腔长与光功率的关系,激光纵模扫过出光带宽过程的光功率和单、双纵模变化的规律。实验结果表明:腔调谐过程中单、双纵模交替出现,腔长和泵浦电流共同影响激光器的输出模式和光功率。 相似文献
4.
采用新型有机吡啶盐trans-4-[p-(N-hydroxyethyl-N-methylamino)styryl]-N-methylpyridinium iodide (ASPI)与有机小分子8-羟基喹啉铝(Alq3)组成能量传递体系,掺杂于惰性聚合物聚甲基丙烯酸脂(PMMA)薄膜中作为增益介质,利用分布布拉格反射镜(DBR)和金属Ag层作为反射镜,制备了垂直微腔结构的有机半导体固体激光器.在纳秒脉冲激光抽运下研究了该有机微腔的受激发射特性,观测到峰值位于600 nm处谱半高全宽为243 nm的单模激光出射;同时观察到明显的激光能量阈值特性,单脉冲的受激发射能量阈值为8?μJ.-----------------2009年《物理学报》第58卷第4期第2781-2784页一文,由于作者的责任,故撤销该文。
关键词:
有机盐
能量转移
微腔
受激发射 相似文献
5.
结合微腔面发射器件辐射/发光亮度的空间分布以及相对光谱功率分布给出了器件外量子效率的计算模型. 该模型可以计算工作于不同波段的微腔面发射器件的外量子效率,如红外波段的垂直腔面发射激光器,可见光波段的微腔有机发光二极管和谐振腔发光二极管以及太赫兹波段的平面微腔结构等. 制备了结构为玻璃/DBR /ITO /NPB /Alq ∶C545T/Alq/LiF/Al的微腔有机电致发光器件,测试其不同观察角度下器件的发光亮度以及发光光谱. 当电流密度和发光亮度分别为14 A/m2和100 cd/
关键词:
外量子效率
平面微腔器件
辐射/发光亮度空间分布 相似文献
6.
报道了一种利用激光二极管(LD)双端面泵浦的Nd:YAG激光晶体,Cr4+:YAG晶体被动调Q,LBO临界相位匹配腔内倍频的高转换效率的绿光激光器。分析了双端面泵浦YAG激光器的热效应,实验中LD双端面泵浦,采用U型平行平面腔结构对Nd:YAG进行传导冷却。当总泵浦光为33.8 W时,得到被动调Q频率10 KHz、功率8.21 W的线偏振基频光输出。6.72 W的绿光输出的倍频效率为86%,输出光束为基模,M2为1.4。实验表明双端面泵浦YAG倍频激光器具有很高的转换效率。 相似文献
7.
耦合光学微腔(Coupled optical microcavity,CMC)是一种特殊结构的微腔,在耦合微腔中,两个独立的微腔相邻耦合在一起.通常一个腔是无源的,另一个腔是有源的.首次研究了有机材料在耦合微腔中的自发发射特性.实验采用的有机发光材料为八羟基喹啉铝Tris(8-quinolinolato)aluminium(Alq3),器件的结构为Glass/DBRA/Filler/DBRB/Alq3/DBRC.底部腔是无源的,组成为DBRA/Filler/DBRB.顶部腔是有源的,由DBRB/Alq3/DBRC构成.其中反射镜DBRA、DBRB、DBRC以及填充层(Filler)均由光学介质材料构成.通过结构设计使两个腔的谐振波长均位于530nm.耦合微腔器件与单层Alq3薄膜相比较,Alq3薄膜的光致发光光谱是峰值位于511nm的宽谱带,而在耦合微腔器件中观察到的是具有两个腔模式,峰值波长分别位于518,553nm的增强并窄化的光谱.这是由于两个腔的光场耦合引起了腔模式分裂.结果表明耦合微腔能极大地改变有机材料的自发发射特性,可以用来提高器件的发光效率. 相似文献
8.
研制了一台高效率全固态平均功率7.13 W的1 319 nm宏微脉冲激光器。激光器采用热稳Z形折叠腔,增益模块采用自行研制的准连续15个二极管芯片环形泵浦的Nd:YAG模块,采用主动声光锁模器作为锁模元件,并在腔内插入倍频KTP晶体对激光器的输出尖峰进行抑制。为了获得稳定的锁模状态,对激光器腔长进行了精确设计和调节。当激光器腔长与锁模器驱动频率匹配时,获取了宏脉冲重复频率400 Hz、脉宽约190 μs,微脉冲重复频率95.6 MHz、脉宽小于1.0 ns的1 319 nm激光脉冲。 相似文献
9.
分析在纵向泵浦微片激光器中Fox-Li迭代法适用条件,通过数值计算,得出在不同泵浦参数下平平F-P有源腔微片激光器的横模结构。 相似文献
10.
中国科学院上海光学精密机械研究所“激光技术开放研究实验室”于1991年7月8日采用本所“半导体光电子学实验室”研制的一维锁相列阵半导体激光器泵浦外腔YAG激光器获得1.064μm激光输出。外腔结构的实验成功为进一步研究和发展半导体激光泵浦的固体激光器打下了基础。 对于半导体激光泵浦的YAG激光器,为了减少激光腔内的损耗,从而降低激光阈值,国内外在研究初期都采用全内腔的单块(monothic)YAG激光器,随着腔内倍频和增大激光输出等研究的发展和需要,又发展为外腔方式。 相似文献
11.
12.
采用多晶LaB6材料制成平板二极管阴极,阳极采用钼材料,阴极采用热传导与热辐射加热,加热体为石墨。实验研究了不同阴极温度、不同真空度下的脉冲发射特性,并对热发射稳定性进行了分析。结果表明: 在动态真空系统中, 阴极发射面积为0.012 1 cm2, 工作真空度为2×10-4 Pa, 阴极温度分别为1 600, 1 650和1 700 ℃,在脉冲宽度为40 ms、重复频率为107 Hz的条件下,最大脉冲发射电流密度分别为34.0,44.0和53.8 A/cm2; 2×10-4,5×10-4和2×10-3 Pa压强下的发射能力没有明显的差异;脉冲宽度的变化不影响发射电流密度的变化。 相似文献
13.
Anders A. Anders S. Juttner B. Botticher W. Luck H. Schroder G. 《IEEE transactions on plasma science. IEEE Nuclear and Plasma Sciences Society》1992,20(4):466-472
The ignition and arc phases of vacuum arcs were investigated using differential dye laser absorption photography with simultaneous high spatial (micrometer) and temporal (nanosecond) resolution. The discharge duration was 800 ns, the current 50-150 A, the electrode material copper, and the cathode-anode distance less than 50 μm. A 0.4 ns laser pulse (tunable, γ=480-530 nm) was used to obtain momentary absorption photographs of the cathode region. During ignition, an optically thick anode plasma expanded toward the cathode, decaying within 25 ns after bridging the electrode gap. In the arc phase, a fragmentary structure of the cathode spots was observed in situ for the first time. The microspots have a characteristic size of 5-10 μm. They appear and disappear on a nanosecond time scale. The plasma density of the microspots was estimated to be greater than (3-6)×1026 m-3 相似文献
14.
M. Yang 《Applied physics. B, Lasers and optics》1983,32(3):127-135
A cw uv copper hollow cathode laser is described, which could be operated for a longer time duration with an output power of 7 mW in the 260 nm region. A double-cathode configuration with a protection for the mirrors from metal-vapour deposition is presented. Characteristics of the laser output power, the spontaneous emission, and the ion densities in the negative glow were measured as depending on the discharge current, the neon gas pressure, and the size of the cathode slit. The observed saturation of the laser output power at high discharge current (1 A/cm2) and the optimum slot size are discussed. 相似文献
15.
H. J. Eichler H. Koch R. Molt J. L. Qiu W. Martin 《Applied physics. B, Lasers and optics》1981,26(1):49-56
The cw output power of the uv CuII laser has been optimized with respect to the hollow cathode geometry, the discharge current, the fill gas pressure and the resonator mirror parameters. A maximum laser output power of 900 mW for multiline operation at 248.6, 259.1, 260.0, and 270.3 nm was achieved with 100 A discharge current, 260 V voltage and 16 mbar fillgas pressure, when a hollow cathode of 1.2 m length and 2×6 mm2 cross section was employed. The single-pass pain gl has been estimated to 7%. A hollow cathode cross section of 1.5×4.5 mm2 is suggested as an optimum geometry. In addition, some investigations on the mechanism of the laser power decay in Ne–Cu-discharges are presented. 相似文献
16.
Vogel N. Heinzinger J. Cichos F. 《IEEE transactions on plasma science. IEEE Nuclear and Plasma Sciences Society》1995,23(6):926-931
The cathode spot formation in air within the first 170 ns was investigated by laser absorption photography and ps-pulse interferometry. The discharge was initiated between electrodes made from Ag or Pd with cathode-anode distance below 300 μm, the arc duration was some milliseconds, and the arc current 5-10 A. Picosecond holographic interferometry and momentary absorption photography yielded spatial-temporal density distributions in the ignition phase of the cathode spot. An absolute electron density value on the order of 4×1026 m-3 has been found. In contrast to vacuum, the cathode spot plasmas broaden little with increasing distance from the cathode, thus narrow plasma channels are observed in the vicinity of the cathode surface having diameters <20 μm 相似文献
17.
基于透射式阴极发射模型和平响应XRD原理,设计了透射式阴极,并制作550nm CH+50nm Au的阴极,并在神光Ⅲ原型装置上开展了初步验证实验。首先利用反射式XRD施加负偏压的实验开展直穿光影响评估,施加偏压为-1500V时,没有观测到探测信号,表明直穿光产生光电子得到了有效抑制。利用原型主激光与第九路激光打靶实验,施加负偏压的透射式XRD获得探测信号显示第二个峰值信号延后第一个信号3.01ns,该结果与第九路激光延迟时间一致,时间分辨能力满足实验要求。 相似文献
18.
A theoretical and experimental study of Ne - H2 Penning Recombination Laser operating on the Nel 585.3 nm line in the negative glow of a helical hollow cathode discharge is presented. A detailed kinetic model of the plasma-chemical reactions determining the inversion population on the Nel (2p1-1s2) transition is developed. The time dependent behaviour of the main plasma and laser parameters is numerically calculated. The behaviour of the plasma and laser parameters as a function of the discharge conditions is investigated and compared with the experimental results. 相似文献
19.
Lebedev VF Tenyakov SY Gaister AV Podstavkin AS Shestakov AV Sorokin VN 《Optics letters》2006,31(10):1438-1440
Room-temperature tunable cw laser oscillation of Cr3+ ions in forsterite crystals (Mg2SiO4) codoped with chromium and lithium has been demonstrated, for the first time to the authors' knowledge, in pumping a crystal with a Ti:sapphire laser into the first excited level of Cr3+ ions (4A2-4T2 transition). The laser is smoothly tunable in the region of 1095-1170 nm. A slope efficiency as great as 4.4% has been achieved. 相似文献