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1.
解析式表示外腔半导体激光器的特征参量   总被引:1,自引:1,他引:0  
用射线法研究了强反馈可调谐外腔式半导体激光器的阈值行为,导出了ECLD被财在不同波长振荡所需的阈值载流子数密度外腔长度及阈值电流的解析表达式,也得到了不同电流ECLD的调谐输出功率及载流子密度的表达式。  相似文献   

2.
周小红  陈建国 《半导体光电》1997,18(6):400-404,413
由于镀了减反射膜的半导体激光二极管端面的反射曲线的谱宽有限,而且,增益峰值波长随载流子密度的变化,因而实际上起作用的反射率通常都比能测到的最低反射率高,在腔内可建立的载流子密度的上限比预期的低。在考虑了这些因素后,计算了用这种管子作外腔半导体激光器(ECLD)的增益介质时,ECLD的调谐范围。  相似文献   

3.
本文提出了一种将回波抵消器(EC)作为LD-CELP编解码器的部分工作的方法,将EC功能融入LD-CELP编解码器之中,文中讨论了用两片TMS320C30实时实现LD-CELP与EC于一个系统中的可能性。  相似文献   

4.
直接耦合场效应逻辑(DCFL)具有简单的结构、良好的速度/功耗性能,是GaAsFETLSI电路中一种重要的逻辑形式。传统E/D型DCFL电路具有较低的成品率和较差的温度特性,本文研究了改进的E/E型DCFL电路。对E/D、E/E型DCFL电路的直流、瞬态及温度特性进行了分析、模拟和比较,E/E逻辑具有良好的高温性能。经优化设计,最后制作出单门延迟约100ps、单门功耗约1mW的E/D和E/E型DCFL电路,且E/E型电路较E/D型电路具有更高的成品率。  相似文献   

5.
余山  黄敞 《电子学报》1994,22(5):94-97
对溶亚微米器件,由于工作电压下降,要求重新确定LDD和常规MOSFET在VLSI中的作用。本文从基本器件数理方程发出,对深亚微米常规及LDD MOSFET的器件特性、热载流子效应及短沟道效应进行了二维稳态数值模拟,指出了常规和LDD MOSFET各自的局限性,明确了在深亚微米VLSI中,LDD仍然起主要作用。  相似文献   

6.
本文介绍一种采用载流子总量方法分析SOI MOSFET器件特性及热载流子效应的数值模型。使用专用模拟程序LADES7联解器件内部二维泊松方程、电子和空穴的连续性方案。LADES7可用于设计和预测不同工艺条件、几何结构对器件性能的影响。该模型直接将端点电流、端点电压与内部载流子的输运过程联系在一起,可准确地模拟SOI MOSFET器件的特性并给出清晰的内部物理图象。本文给出了LADES7软件模拟的部  相似文献   

7.
文章通过对PROTEL和CorelDraw两个软件包的分析,提出了利用CorelDraw作为工具,打印PROTEL图形,以及插入WORD文档中的方法。同时介绍了使用CorelDraw处理PROTEL图形的进一步应用,以及将PROTEL图形插入WORD文档中的实用技巧  相似文献   

8.
江剑平 《半导体光电》1995,16(4):302-312
文章综述CLEO’94及IQEC’94会议报道的有关光电子器件的发展状况,叙述了大功率LD、蓝绿光LD、垂直腔面发射半导体激光器、可调谐LD及OEIC的最新研究进展。  相似文献   

9.
本文较详细介绍了 EL7512C DC/DC 升压转换器的性能以及在DSL用户端(CPE)电源设计与布线中要考 虑的要素。  相似文献   

10.
阐述了ADSL中EOC的功能,EOC帧结构,EOC命令,以及EOC协议,对在ADSL数据帧中插入EOC帧这一问题也进行了讨论。  相似文献   

11.
Small-signal admittance and phasor diagrams for metal-semiconductor-metal microwave oscillator diodes (BARITT diodes) were calculated by taking previously neglected carrier diffusion and field dependence of carrier velocity into account. It was shown that the microwave performance greatly degrades with an increase of dc current density and of oscillation frequency.  相似文献   

12.
The large-signal behavior of DFB lasers is analyzed, including lateral as well as longitudinal variations in carrier density, photon density, and refractive index. The effective index method and other approximations are used to reduce the complex three-dimensional problem to one dimension. The coupled wave and carrier rate equations are then solved in a self-consistent manner. Lateral spatial carrier hole burning and lateral diffusion are found to affect the relaxation oscillation frequency and damping rate of DFB lasers, depending on their detailed structure. The effective time-averaged linewidth enhancement factor is also affected. In symmetric AR-coated λ/4 phase-shifted lasers the side mode suppression ratio can be deteriorated significantly by lateral spatial hole burning when kL is large  相似文献   

13.
A study was made of the behavior of external cavity semiconductor lasers with tilted external cavity mirrors providing variable feedback. The appearance of intermittent breakdowns of the light intensity induced by the tilting of the external mirror is demonstrated. The rate of the breakdowns of the light intensity is directly related to the relaxation oscillation frequency of the external cavity semiconductor laser. The authors describe the experimental observations theoretically by the coupled rate equations for the electric field density and the carrier density  相似文献   

14.
The dependence of the (low-frequency) resonance of light intensity noise in an external-cavity GaAs laser on cavity length and bias current, combined with the dependence of the threshold current on the magnitude of the light feedback, is used to determine simultaneously the carrier recombination lifetime, the carrier injection at transparency, and the optical loss. The key to this technique is understanding the correction term to the relaxation oscillation frequency due to finite carrier density at transparency and the influence of the long external cavity transit time on the photon lifetime in the three-mirror cavity. The technique uses commercial lasers without modifying them and does not require fast electronics  相似文献   

15.
利用由射线法导出的广义两段式半导体激光器的输出光谱的表达式,讨论了外腔式半导体激光器(ECLD)的调谐范围,当ECLD调谐到半导体激光二极管的共振波长附近振荡时,可以重到ECLD的最大调谐范围;当激光器调谐到半导体激光二极管的反共振波长附近振荡时,可以获得ECLD的准连续调谐范围;同时,还求得了实现准连续调谐所需的面向外腔的半导体二极管端面的反射率。  相似文献   

16.
Metal-semiconductor contact injection on the junction side of diffused-mesa avalanche diodes has been found to have a significant effect on the performance of these diodes as oscillators. A minority carrier injection ratio of 6 percent reduces the efficiency of what would be 9 percent efficient diodes to less than 1 percent and increases the FM noise by a factor of 2 as tested in a 6-GHz oscillator circuit. The dependence of the minority carrier injection ratio of the metal-semiconductor barrier upon current density has been measured and quantitatively modeled. Calculated values of diode admittance, including the effects of injection at the contact, are shown to be in agreement with measured values of both small-signal diode admittance versus frequency and large-signal diode admittance versus RF voltage. Germanium avalanche diodes with low-minority carrier injection contacts have demonstrated CW oscillation efficiencies greater than 9 percent at 6 GHz. The realization of low-injection contacts is shown to be a requirement for achievement of high-efficiency avalanche oscillation.  相似文献   

17.
The DC and microwave properties of strained In0.65Ga 0.35As/In052Al0.48As HEMTs (high electron-mobility transistors) with double-heterojunction design are presented. The high sheet carrier density and good carrier confinement give rise to excellent device performance with very low output conductance. For 1×150-μm2 long-gate HEMTs, the measured cutoff frequency fT and maximum frequency of oscillation fmax are as high as 37 and 66 GHz, respectively  相似文献   

18.
A model, based on the transfer matrix method, and extended to above-threshold conditions in order to be used in the analysis and design of distributed feedback (DFB) structures, is presented. It provides the oscillation parameters as lasing frequency and net material gain, the linewidth estimation and output power, the photon density, carrier density, and effective refractive index profiles. This model can be used with or without facet reflectivities and with a number of symmetric or asymmetric phase shifts. It takes into account nonuniform envelope material gain and nonuniform index saturation. It is easily adaptable to any structure modifications  相似文献   

19.
The performance of an innovative delta-doped AlGaN/AlN/GaN heterojunction field-effect transistor (HFET) structure is reported. The epitaxial heterostructures were grown on semi-insulating SiC substrates by low-pressure metalorganic chemical vapour deposition. These structures exhibit a maximum carrier mobility of 1058 cm2/V s and a sheet carrier density of 2.35×1013 cm-2 at room temperature, corresponding to a large ns μn product of 2.49×1016 V s. HFET devices with 0.25 μm gate length were fabricated and exhibited a maximum current density as high as 1.5 A/mm (at VG=+1 V) and a peak transconductance of gm=240 mS/mm. High-frequency device measurements yielded a cutoff frequency of ft≃50 GHz and maximum oscillation frequency fmax≃130 GHz  相似文献   

20.
Using the Foreman effective mass Hamiltonian for strained In/sub x/Ga/sub 1-x/As--In/sub y/Ga/sub 1-y/As/sub z/P/sub 1-z/ quantum wells, the propagation of subpicosecond pulses in a 1.55-/spl mu/m optical amplifier was calculated. The multisubband carrier dynamics as well as the polarization dynamics were taken into account. Carrier heating and coherent light-carrier interactions as well as the interplay of these nonlinear processes and the amplifier dispersion are studied. Strong Rabi oscillations occur in the optical field of a propagated pulse, its frequency chirp, as well as in the carrier density and temperature. While the Rabi oscillation imposes negative frequency chirp and hence red-shifts the pulse spectrum, positive frequency chirp can occur due to the local gain dispersion, where the higher frequency components of the pulse have larger gain. Due to the Rabi oscillation, the spectrum of the amplified pulse is considerably distorted and sidebands emerge. For a linearly chirped input pulse, the spectrum of the output pulse can be either red-shifted or blue-shifted with respect to its center frequency, depending on its initial chirp. For strong pulse propagation, a pronounced pulse break up occurs when a 175-fs pulse propagates in the gain regime, while a significant pulse compression occurs when the pulse propagates at the transparency point.  相似文献   

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