共查询到20条相似文献,搜索用时 171 毫秒
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根据光增益与载流子密度的对数关系,在受激发射速率中分别引入了增益饱和项和载流子复合项,通过适应于多量子阱激光器的速率方程,从理论上证明了短腔结构存在与阈值电流最小值对应的最佳阱数。给出了多量子阱激光器的瞬态呼应特性的直接仿真结果及相图,分析了注入电流、阱数和腔长对其激射阈值、开关延误时间、弛豫振荡频率和光输出等能量的影响。 相似文献
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热效应是限制外腔面发射激光器(VECSEL)输出功率和光束质量的主要原因。为了优化VECSEL增益芯片有源区量子阱的设计,降低激光器的热效应,提高斜效率和输出功率,采用光致荧光谱方法,对设计波长980nm VECSEL自发辐射谱的热特性进行了实验研究。取得了不同热沉温度下边发射和面发射谱随温度的变化数据。结果表明,反映有源区量子阱自身特性的边发射谱峰值波长随温度升高的红移速率是0.5nm/K,而受到增益芯片多层结构调制的面发射谱峰值波长随温度升高的红移速率只有0.1nm/K;由于受到VECSEL增益芯片中微腔的限制,面发射谱分离为多个模式,分别与微腔的腔模对应。可见对量子阱的发射波长及微腔腔长做预偏置优化处理,可以显著改善激光器的输出性能。 相似文献
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采用光增益与载流子浓度的对数关系,考虑到非辐射复合的影响,从理论上推导出多量子阱垂直腔面发射半导体激光器(VCSELs)的速率方程。讨论了阈值电流密度、最佳阱数等与器件参数(腔长和端面反射率)之间的依赖关系。为改善VCSELs阈值特性和优化器件结构提供了理论依据。 相似文献
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采用光增益与载流子浓度的对数关系,考虑到非辐射复合的影响,从理论上推导出多量子阱垂直腔面发射半导体激光器(VCSELs)的速率方程。讨论了阈值电流密度、最佳阱数等与器件参数(腔长和端面反射率)之间的依赖关系。为改善VCSELs阈值特性和优化器件结构提供了理论依据。 相似文献
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光学微腔中偶极子自发辐射受到空间和频谱调制,能实现自发辐射增强或抑制效应,而且其有源区体积可以非常小,有利于极低阈值工作和极高的调制速率.在过去的二十多年来,垂直腔面发射激光器、回音壁模式(whispering-gallery mode)微腔激光器以及光子晶体微腔激光器三类光学微腔激光器的研究取得了很大的进展.回音擘模式微腔中,模式光线由于其在微腔界面的入射角大于全反射临界角而受到限制,是一种结构非常简单的光学微腔.微盘激光器作为典型的回音壁模式微腔激光器,可利用普通的边发射激光器外延片材料,采用半导体平面工艺制作,引起了人们很大的重视.但圆对称结构的微盘激光器易于实现回音壁模式的全反射限制,却难以得到定向的激光输出,限制了它的应用.人们往往采用局部破坏圆盘的对称性、整体变形以及消逝波耦合的输出波导实现微盘激光器的定向激光输出.在圆对称的微盘结构中,模式光线在微腔与空气界面上的入射角是恒定的,而在整体变形的圆盘中,如椭圆形微腔中,模式光线在界面的入射角则不断变化,并在某些位置上小于全反射临界角而折射出光学微腔,从而实现定向输出.这种变形微盘中模式光线往往具有混沌现象,因而吸引了人们的注意. 相似文献
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为了确定激光晶体在不同温度下的自发辐射光谱 (荧光谱),实验研究了阈值附近微片激光器的输出 光谱特性。当抽运功率略小于阈值时,微片激光器输出经干涉的自发辐射光;当抽运功率大 于阈值时,微 片激光器输出激光。测量了激光阈值与晶体温控的关系,结果表明激光阈值随晶体温度的升 高而增加,其 变化率为0.017W/℃。在不同温控条件下,对阈值以下的自发辐射光 谱包络进行了拟合测量,结果表明随 着晶体温度的升高自发辐射光谱包络峰值降低,下降率为0.681%/℃ ;光谱包络中心波长发生红移,漂移率为3.1pm/℃。 相似文献
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Analysis Expression of Rate Equation for Vertical Cavity Lasers 总被引:1,自引:0,他引:1
An analysis solution of rate equation is derived for vertical cavity surface-emitting lasers.Based on the enhanced spontaneous emission caused by VCSELs and influence of nonradiative recombination, the relation between output properties and structural parametersof multi-quantum wells(MQWs) is obtanined.It was found that the characteristic curve of a “thresholdless“ laser is strongly nonradiative depopulation-dependent.When the nonradiative depopulation is no zero,the light-current characteristic is not linearly even for an ideal closed microcavity.The light output is increased by the enhanced well number and by the reduced width.In particular, a lower threshold current density for MQWs structure in the short cavity is realized by us, meanwhile the sharpness of the variation depends on spontaneous emission factor. 相似文献
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We report here our experimental observations on the temperature dependence of threshold current, carrier lifetime at threshold, external differential quantum efficiency, and gain of both the 1.3 μm InGaAsP-InP and GaAs-AlGaAs double heterostructure (DH) lasers. We find that the gain decreases much faster with increasing temperature for a 1.3 μm InGaAsP DH laser than for a GaAs DH laser. Measurements of the spontaneous emission observed through the substrate shows that the emission is sublinear with injection current at high temperatures for the 1.3 μm InGaAsP DH laser. Such sublinearity is not observed for GaAs DH lasers in the entire temperature range 115-350 K. The experimental results are discussed with reference to the various mechanisms that have been proposed to explain the observed temperature dependence of threshold of InGaAsP DH lasers. We find that inclusion of a calculated nonradiative Auger recombination rate can explain the observed temperature dependence of threshold current, carder lifetime at threshold, gain, and also the sublinearity of the spontaneous emission with injection current of the 1.3 μm InGaAsP-InP DH laser. Measurement of the nonradiative component of the carrier lifetime (τA ) as a function of injected carrier density (n ) shows thattau_{A}^{-1} sim n^{2.1} which is characteristic of an Auger process. 相似文献
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The saturation behavior of the spontaneous light-current characteristic of InGaAsP (lambda = 1.3 mu m) lasers and light emitting diodes are investigated as a function of injection level and temperature. For carrier injection levels below that at which optical gain is observed, it is shown that a nonradiative Auger recombination mechanism is consistent with the observed saturation behavior of the spontaneous emission intensity of lasers. Further evidence of the importance of Auger recombination at these low injection levels is provided by the dependence of the nonradiative component of the measured carrier lifetime (τA ) on injection level (n ) where it is found thattau_{A}^{-1} propto n^{2.1} . For injection levels above that required to achieve optical gain we report the direct observation of superlinear emission due to single pass gain in edge emitting LED's. The onset of this superluminescence at low temperatures (T < 200 K) is found to correspond with the onset of saturation of the spontaneous emission from the sides. These results show that both Auger recombination and superluminescence should be taken into account when the electrooptical characteristics of InGaAsP LED's are calculated. 相似文献
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半导体微腔中电偶极子的自发发射 总被引:1,自引:0,他引:1
由于反射电场的影响,电偶极子在微腔中的自发发射速度不同于自由空间中的自发发射速度。本文采用镜像法计算了理想平面微腔、金属平面镜组成的半导体微腔和由分布布喇格反射镜(DBR)作为谐振腔的垂直发射激光器(VCSEL)中电偶极子的自发发射速率。计算结果表明:由于微腔的调制作用,在某些情况下电偶极子自发发射速率增加,在一定腔长下电偶极子自发发射速度被抑制。 相似文献
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Spontaneous emission factor in post microcavity lasers 总被引:1,自引:0,他引:1
R.J. Ram E. Goobar M.G. Peters L.A. Coldren J.E. Bowers 《Photonics Technology Letters, IEEE》1996,8(5):599-601
The first measurements of the spontaneous emission coupling efficiency (/spl beta/) for electrically pumped microcavity lasers with transverse photon confinement are reported. The influence of scattering losses and carrier diffusion on microcavity lasers is investigated, A /spl beta/ of 0.01 is measured at 126 K in a 3-/spl mu/m diameter device with optimal gain-cavity detuning. 相似文献
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Wei Dong Zhou Sabarinathan J. Bhattacharya P. Kochman B. Berg E.W. Pei-Chen Yu Pang S.W. 《Quantum Electronics, IEEE Journal of》2001,37(9):1153-1160
A microcavity surface-emitting coherent electroluminescent device operating at room temperature under pulsed current injection is described. The microcavity is formed by a single defect in the center of a 2-D photonic crystal consisting of a GaAs-based heterostructure. The gain region consists of two 70-Å compressively strained In0.15Ga0.85As quantum wells, which exhibit a spontaneous emission peak at 940 nm. The maximum measured output power from a single device is 14.4 μW. The near-field image of the output resembles the calculated TE mode distribution in a single defect microcavity. The measured far-field pattern indicates the predicted directionality of a microcavity light source. The light-current characteristics of the device exhibit a gradual turn-on, or a soft threshold, typical of single- or few-mode microcavity devices. Analysis of the characteristics with the carrier and photon rate equations yields a spontaneous emission factor β≈0.06 相似文献
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The intensity noise level and the spectral line-width of semiconductor injection lasers are theoretically analyzed. Approximated but simple forms representing these characteristics are found to give criteria for various types and sizes of cavity, including microcavity lasers. The noise and the line-width are reduced by operation with high injection current or high optical power in general. For operation at a low-power level in the microcavity laser, increase of the spontaneous emission factor as well as reduction of the threshold current level and the threshold gain level are important to get a low noise level and narrow line-width 相似文献
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Deppe D.G. Huffaker D.L. Zou Z. Park G. Shchekin O.B. 《Quantum Electronics, IEEE Journal of》1999,35(8):1238-1246
The spontaneous emission spectra and lasing characteristics of long-wavelength (1.3-μm) quantum-dot lasers are studied. It is found experimentally that nonradiative recombination can dominate the room-temperature efficiency and limit threshold, By describing the quantum-dot spectral emission as due to energy levels of a two-dimensional harmonic oscillator, rate equations are developed to account for the temperature-dependent spontaneous and lasing characteristics 相似文献