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1.
本文报导利用真空镀膜技术在BK7玻璃波导上,制备成ZnS/ZnSe迭层光栅滤波器,在室温下,用Ar^=脉冲激光,通过棱镜与波导耦合,实现了光栅滤波器的光控开关调制。  相似文献   

2.
分层优化电致发光器件加速层的研究   总被引:1,自引:0,他引:1  
徐征  王向军 《光电子.激光》1996,7(6):370-372,317
在本文的工作,对于加速层我们研究了SiO2和ZnS两种材料的加速八月主采用这两种材料作为加速层的器件的传导电荷情况。实验结果表明ZnS作加速层的电荷注入能力优于SiO2作加速层;但是后者对热电子的加速作用明显优于前者,而且在同等条件下,以SIO2作加层的器件亮度明显高天ZnS的作加速层的器件。  相似文献   

3.
我们首次利用Z-扫描技术在室温下研究了ZnCdSe-ZnSe/CaF2多量子了进中的三阶非线性,得到非线性系数n2为-4.46×10^-8esu。其主要非线性机理归结为ZnCdSe-ZnSe/CaF2多量子阱中的带填充效应。  相似文献   

4.
用光助低压MOCVD进行ZnSe及ZnSe:N外延层生长,由发光光谱表明,在光助下生长的本征ZnSe外延膜具有高质量:ZnSe:N外延层中与N有关的深中心发射得到有效抑止,其p-ZnSe受主载流子深度达3×10^17cm^-3。在制备n-ZnSe/ZnCdSe-ZnSeQW/p-ZnSe结构中,在室温下观测到该二极管电脉冲下的蓝色电致发光(EL)。  相似文献   

5.
采用基于LMTO-ASA的平均结合能计算方法,研究了在ZnSxSe1-x衬底上沿(001)方向外延生长的应变层异质结ZnS/ZnSe的价带带阶值。研究表明,应变的结果使价带带阶随衬底组分(x)的变化呈非线性且单调的关系;与其他理论计算和实验结果比较,本文的计算结果比较理想。  相似文献   

6.
在静压和液氮温度下观察到(CdSe)m/(ZnSe)n短周期超晶格中重空穴激子的复合发光和多达4阶的类ZnSeLO多声子喇曼散射,并观察到厚ZnSe势垒层的带边发光和限制在厚势垒层中的类ZnSeLO声子散射.结果表明,加压后(CdSe)m/(ZnSe)n短周期超晶格中的类ZnSe的1LO和2LO声子模频率分别以3.76和7.11cm-1/GPa的速率向高频方向移动,超晶格阱层光致发光峰的压力系数为59.8meV/GPa.与(CdSe)m/(ZnSe)n短周期超晶格共振时的类ZnSe1LO声子模频率比与ZnSe势垒层共振时的类ZnSe1LO声子模频率低2.0cm-1,反映了(CdSe)m/(ZnSe)n短周期超晶格中LO声子的限制效应  相似文献   

7.
本文采用泵浦-探测技术研究了ZnSe/ZnCdSe多量子阱室温激子饱和吸收,并根据K-K关系计算得到521.6nm至544nm的光学非线性折射率的变化.观测到由折射率变化引起的ZnSe/CdZnSe多量子阱光双稳器件的室温激子光双稳.根据ZnSe/ZnCdSe多量子阱的激子吸收谱及激子的非线性理论,归结其主要非线性机制为激子态的相空间填充和激子带展宽.  相似文献   

8.
在静压和液氮温度下观察到(CdSe)m/(ZnSe)n短周期超晶格中重空穴激子的复合发光和多达4阶的类ZnSeLO多声子喇曼散射,并观察到厚ZnSe势垒层的带边发光和限制在厚势垒层中的类ZnSeLO声子散射。结果表明,加压后(CdSe)m/(ZnSe)n短周期超晶格中的类ZnSe的1LO和2LO声子模频率分别以3.76和7.11cm^-1/GPa的速率向高频方向移动,超晶格阱层光致发光峰的压力系数  相似文献   

9.
测量了ZnSe,Zn0.84Mn0.16Se合金和ZnSe/Zn0.84Mn0.16Se超晶格的10~300K的变温光致发光谱.发现ZnSe的带隙在10K时比Zn0.84Mn0.16Se合金的带隙小,而在300K时比合金的带隙大.预计ZnSe/Zn0.84Mn0.16Se超晶格中在130K附近会发生势阱层和势垒层的反转.在ZnSe/Zn0.84Mn0.16Se超晶格中观测到了这种反转但发生在80K附近.超晶格中Zn0.84Mn0.16Se层的应变可能是反转温度变低的原因.  相似文献   

10.
本文报道了分子束外延生长的应变层超晶格Zn0.77Cd0.23Se/ZnSe和ZnSe/ZnS0.12Se0.88的光致发光谱.分析了影响激子线型展宽的主要因素.定量表征了4.4K下合金涨落和阱厚涨落对线型展宽的贡献.理论分析表明,在低温(4.4K)下,合金涨落和阱宽涨落对线型展宽起主导作用.对比结果显示,Zn0.77Cd0.23Se/ZnSe超晶格的合金涨落和阱宽涨落对线型展宽的贡献大于ZnSe/ZnS0.12Se0.88超晶格  相似文献   

11.
李福利 《中国激光》1982,9(8):496-497
将双光子光学双稳态理论推广到包含全部交流斯塔克项,首次表明存在双光子作用的光学双双稳态以及两种不同类型的双光子光学三稳态。  相似文献   

12.
Effect of oblique incidence on bistability of nonlinear microcavity   总被引:1,自引:0,他引:1  
Based on the nonlinear medium transfer theory, optical bistability of nonlinear microcavity is investigated at oblique incidence. It is found that the critical frequency of incident light inducing bistability phenomenon is related to the polarization and incident angle. The critical frequency increases with the incident angle. Increasing the incident angle can make bistability happen easier for focusing Kerr medium, but will hinder bistability for defocusing Kerr medium. The bistability switch threshold of TE mode is significantly lower than that of TM mode at a large incident angle.  相似文献   

13.
庞叔鸣  顾宁 《电子器件》1997,20(3):36-39
本文第一次报导了Ag-TCNQ薄膜的双稳态现象。双稳F-P腔是由Ag-AgTCNQ-Ag膜系组成。并观察了Ag-TCNQ薄膜典型的双稳回线。  相似文献   

14.
Two different types of bistability in proton-implanted GaAs quantum-well (QW) vertical-cavity surface-emitting lasers (VCSELs) have been observed. The first type of bistability has a small hysteresis width (~50 μA) in the light versus current and voltage versus current characteristics. Light-induced large negative differential resistance, random fluctuations, and self-pulsations are observed at the switching point. The emission patterns show that the bistability occurs at a spatially localized area under the output facet that covers only a small fraction of the N1S-μm-diameter aperture. The bistability stems from spatially localized saturable absorption. The second type of bistability has a large hysteresis width (~1 μA) in the L-1 characteristics and is observed well above the threshold current. In this case, no observable bistable loop exists in the voltage versus current characteristics, and the bistability is associated with transverse mode-hopping  相似文献   

15.
Dynamic responses of optical polarization bistability and self-sustained pulsation in transverse-magnetic (TM) wave injected semiconductor lasers are analyzed. Due to the TM wave injection, laser amplification of TM wave and laser oscillation in the transverse-electric (TE) mode simultaneously occurs in the laser. The calculated dynamic responses of optical polarization bistability are compared with measured responses. The upper limit of the switching time and the repetition frequency are clarified from calculations. The self-sustained pulsation triggered by a change of TM input power is found in the course of the calculation. The conditions needed for the pulsation are discussed  相似文献   

16.
The phenomenon of purely absorptive bistability is examined using a self-consistent multibeam interference method. A state equation is derived and shown to be identical to that derived from mean-field theory (MFT) in the limit of small absorption length products and high saturation. Using the theory given, we are able to examine the time evolution of the system analytically. The results show a critical slowing behavior near the bistable points of the system and are used to examine switching times. In addition, we give a different condition for bistability which results in a larger range of admissibleCvalues.  相似文献   

17.
We present a theoretical study of multiple bistability in an optical-fiber double-ring resonator. The multiple bistability is caused by the optical Kerr effect, which modulates the refractive index of the fiber. The dependence of the multiple bistability on various parameters of the fibers and the couplers is investigated  相似文献   

18.
Optical bistability (OB) in semiconductors is of increasing interest in both basic and applied research. Much is known about optical nonlineari-ties and OB in CdS crystals. This paper reports, for the first time, about the optical bistability in CdS single crystal film grown on a CaF2 transparent substrate. High quality of the film has been identified by photolumines- cence and absorption. The OB is measured by 514.5nm line of Ar+ laser modulated into 6ms square light pules at room temperature. Two spikes appear at the front and back edges of transmitted light pulses. The switchins time is about 200μs at 200mW power level, smaller than the time in CdS bulk crystal at the same condition. The mechanism of the OB is due to the increasing absorption and thermal red shift of the absorption edge.  相似文献   

19.
Pitchfork bifurcation polarisation bistability has been observed experimentally in a vertical-cavity surface-emitting laser for the first time. All-optical flipflop operation has been successfully demonstrated by injecting the trigger light inputs having the two orthogonal polarisations  相似文献   

20.
The effect of light fluctuations on the light-induced bistability of the photocarrier distribution is studied. The bistability can be explained by the threshold character of interband transitions and narrowing of the band gap of the semiconductor with increasing photocarrier density. The stationary probability density of the states and the mathematical expectation of the transition time between states are calculated. It is shown that external noise induces a strongly absorbing state of the semiconductor below the critical intensity of the incident radiation and suppresses stationary states above this value. Fiz. Tekh. Poluprovodn. 32, 296–298 (March 1998)  相似文献   

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