共查询到20条相似文献,搜索用时 93 毫秒
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本文提出了一类在非线性偏置条件下,由N-型负阻器件构成的具有三个奇点(其中有两个奇点在负阻区)的触发振荡电路。借助于点变换方法研究了该电路的工作特性。分析表明,所提出的电路具有足够宽的触发振荡工作区。用隧道二极管进行了实验,实验结果与理论有较好的符合。 相似文献
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提出了一种利用串联谐振腔来抑制光电振荡器边模的方案. 此方案中, 在传统光电振荡器结构中加入无源微波谐振腔结构来提高滤波器的Q值. 分析了该结构的基本原理, 并与传统光电振荡器结构进行对比, 此结构能有效提高边模抑制比. 实验中产生了10 GHz的微波信号, 所测得的边模抑制比达72 dB, 单边带相位噪声为-122 dBc/Hz@10 kHz. 同时, 利用锁相技术, 振荡频率的稳定性得到了很大的改善, 在3 h内漂移小于± 4 Hz. 该方案无需增加有源器件, 保留了传统光电振荡器低相位噪声的优势, 又有效抑制了边模, 为光电振荡器的应用提供了一种新的方法. 相似文献
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一种新型双环路光电振荡器 总被引:3,自引:0,他引:3
利用偏振分束器(PBS)和合束器(PBC)在不增加有源器件的基础上设计了一种双环路光电振荡器。该振荡器可以同时产生光、电两种输出。由于没有增加有源器件,可以避免附加电噪声的引入。此外,光载波在光域中是正交耦合,消除了随机干涉和拍噪声对振荡频率的影响。通过理论分析,双环结构的光电振荡器可以有效抑制每一单环路中起振的边模。经过实验对比,采用双环结构可以把边模抑制比提高30~70 dB。最后,利用该方案和普通商用器件得到了中心频率为12 GHz的振荡,测得边模抑制比为50~70 dB,相位噪声为-93 dBc/Hz at10kHz,Q值达到1010。 相似文献
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有机薄膜器件负电阻特性的影响因素 总被引:1,自引:1,他引:0
研究了影响有机染料掺杂聚合物薄膜器件负电阻特性的因素,为探索有机负电阻的机理提供实验依据。实验中制备了多种有机染料掺杂聚合物薄膜器件,研究了有机小分子染料、聚合物基体、薄膜组成及厚度、ITO和聚苯胺阳极等对有机染料掺杂聚合物薄膜器件负电阻特性的影响。在室温、大气环境下,所制备的多种有机染料掺杂聚合物器件在所加电压为3~4V时,观察到明显的负电阻特性,电流峰谷比最大约为8。负电阻现象及峰谷比的大小受膜厚和器件的结构、制备工艺等影响。提出用负电阻和二极管并联组成的等效电路模型解释影响负电阻特性的因素,认为负电阻特性与载流子的不平衡注入有关。在此基础上设计、合成了主链含唔二唑电子传输基团的可溶性聚对苯撑乙烯衍生物,该聚合物兼具空穴和电子传输功能,在空气中具有较稳定的N型负电阻特性。进一步控制相关材料和工艺条件,有可能得到易于控制的负阻效应,开发出新型的有机负电阻器件。 相似文献
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硅基MIS隧道发光二极管为制造用于超大规模集成电路的硅基光器件提供了可能性,报道了MIS隧道发光二极管的制作 过程,电流电压和发射光谱特性,讨论了负阻现象和发光机理。 相似文献
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用高阻硅制作的光学元件是太赫兹系统里常用的器件, 但是其高达3.42的相对折射率所引起的阻抗失配严重影响了太赫兹系统的功率, 因此研究人员尝试了各种各样的方式在高阻硅表面镀上有效的增透膜. 在太赫兹波段, 缺乏合适的材料是增透研究中亟需解决的一个重要问题. 介绍一种结构新颖的硅材料增透器件----- 三维光子倒置光栅. 与普通高阻硅片相比, 当结构周期为15 μm时, 该器件在0.2---7.3 THz范围内对太赫兹波具有明显的增透作用, 且覆盖了大部分太赫兹波段. 此外, 该器件的使用不受太赫兹偏振方向限制, 适用于大入射角情形, 并具有高达116.3%的相对3 dB带宽. 相似文献
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Plasmon-induced transparency effect in hybrid terahertz metamaterials with active control and multi-dark modes 下载免费PDF全文
Yuting Zhang 《中国物理 B》2022,31(6):68702-068702
We numerically demonstrate a photo-excited plasmon-induced transparency (PIT) effect in hybrid terahertz (THz) metamaterials. The proposed metamaterials are regular arrays of hybrid unit cells composed of a metallic cut wire and four metallic split-ring resonators (SRRs) whose gaps are filled with photosensitive semiconductor gallium arsenide (GaAs) patches. We simulate the PIT effect controlled by external infrared light intensity to change the conductivity of GaAs. In the absence of photo excitation, the conductivity of GaAs is 0, thus the SRR gaps are disconnected, and the PIT effect is not observed since the dark resonator (supported by the hybrid SRRs) cannot be stimulated. When the conductivity of GaAs is increased via photo excitation, the conductivity of GaAs can increase rapidly from 0 S/m to 1×106 S/m and GaAs can connect the metal aluminum SRR gaps, and the dark resonator is excited through coupling with the bright resonator (supported by the cut wire), which leads to the PIT effect. Therefore, the PIT effect can be dynamically tuned between the on and off states by controlling the intensity of the external infrared light. We also discuss couplings between one bright mode (CW) and several dark modes (SRRs) with different sizes. The interference analytically described by the coupled Lorentz oscillator model elucidates the coupling mechanism between one bright mode and two dark modes. The phenomenon can be considered the result of linear superposition of the coupling between the bright mode and each dark mode. The proposed metamaterials are promising for application in the fields of THz communications, optical storage, optical display, and imaging. 相似文献
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Xiaowei Zhu Xiaohong Jiang Wei Hong Yiyuan Chen 《International Journal of Infrared and Millimeter Waves》1993,14(2):347-354
There is a growing interest in optically controlled millimeter wave oscillators. In this paper, we have investigated the external-circuit impedances of an optically controlled millimeter wave subharmonic Gunn diode oscillator, which is illuminated by GaAs/GaAlAs laser beam. The variation of the external-circuit impedances looking outward from the Gunn diode with respect to the optical injection plasma density are calculated based on a field analysis method. The results give some useful conclusions for optically controlled millimeter wave Gunn diode oscillator design. Experimentally an optical tuning frequency shift of 7MHz is achieved at W-band. 相似文献
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提出了一种基于平面光波导谐振腔的可调谐光电振荡器.该振荡器中,相位调制器串联光波导谐振腔,取代了传统系统中的强度调制器、长光纤和滤波器.由于光学谐振腔对光子频率和相位敏感,调节激光器改变输出光的波长,不仅可以调制光的强度,还可以对微波光子进行选频输出.当光子在波导腔中发生谐振时,产生很强的延时特性,可以取代传统系统中的长光纤.整个光电振荡器系统体积为长29.5cm、宽21cm、高7cm.实验中,改变0.1pm的光子波长,能够产生步长为12.535.5 MHz的调谐,调谐范围达2 GHz,且系统能够产生10 GHz的微波信号,在中心频率为10 GHz处其相位噪声为-109.7dBc/Hz@10kHz.该研究为光电振荡器的小型化和实用化提供了一种新的思路. 相似文献
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A method of measurement of anomalous dispersion near spectral lines of absorption from interference fringe shifts is described. The sensitivity and accuracy of the method is analyzed and its advantage over the hook method is demonstrated. The system consists of Rozhdestvenskii's interferometer and a diffraction grating spectrometer. The device is adapted both to photo and photoelectric recording of the interference fringes.The technique is tested on the first resonance doublet of sodium with the wave lenghts 5890, 5896 Å. For the oscillator strengths ratio ?5890/?5896 we get 2.05±0.03. 相似文献
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High-power, continuous-wave, singly resonant optical parametric oscillator based on MgO:sPPLT 总被引:1,自引:0,他引:1
We report a high-power, widely tunable, cw singly resonant optical parametric oscillator (OPO) based on MgO:sPPLT. The OPO is pumped in the green by a cw diode-pumped Nd:YVO(4) laser at 532 nm and can provide continuously tunable output across 848-1430 nm. Using a 30 mm crystal and double-pass pumping, an oscillation threshold of 2.88 W has been obtained, and single-pass idler powers in excess of 1.51 W have been generated over 1104-1430 nm for 6W of pump power at an extraction efficiency of 25.2% and photon conversion efficiency of 56.7%. 相似文献
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《Chinese Journal of Physics (Taipei)》2018,56(5):2560-2573
In this paper, a three-dimensional autonomous Van der Pol-Duffing (VdPD) type oscillator is proposed. The three-dimensional autonomous VdPD oscillator is obtained by replacing the external periodic drive source of two-dimensional chaotic nonautonomous VdPD type oscillator by a direct positive feedback loop. By analyzing the stability of the equilibrium points, the existence of Hopf bifurcation is established. The dynamical properties of proposed three-dimensional autonomous VdPD type oscillator is investigated showing that for a suitable choice of the parameters, it can exhibit periodic behaviors, chaotic behaviors and coexistence between periodic and chaotic attractors. Moreover, the physical existence of the chaotic behavior and coexisting attractors found in three-dimensional proposed autonomous VdPD type oscillator is verified by using Orcard-PSpice software. A good qualitative agreement is shown between the numerical simulations and Orcard-PSpice results. In addition, fractional-order chaotic three-dimensional proposed autonomous VdPD type oscillator is studied. The lowest order of the commensurate form of this oscillator to exhibit chaotic behavior is found to be 2.979. The stability analysis of the controlled fractional-order-form of proposed three-dimensional autonomous VdPD type oscillator at its equilibria is undertaken using Routh–Hurwitz conditions for fractional-order systems. Finally, an example of observer-based synchronization applied to unidirectional coupled identical proposed chaotic fractional-order oscillator is illustrated. It is shown that synchronization can be achieved for appropriate coupling strength. 相似文献
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Gauge covariant construction of the coherent states for a time-dependent harmonic oscillator by algebraic dynamical method 总被引:5,自引:0,他引:5
Lian-Fu Wei Shun-Jin Wang Quan-Lin Jie 《Zeitschrift für Physik B Condensed Matter》1997,102(4):541-543
Time-dependent coherent states for a time-dependent harmonic oscillator are constructed in the framework of algebraic dynamics. These coherent states are gauge-covariant, and its time evolution is governed only by the solutions of a linear differential equation which describes the motion of the corresponding classical timedependent harmonic oscillator. Its non-classical and quantum statistical properties can thus be controlled by a proper choice of the frequency of the harmonic oscillator. Our coherent states reduce to Glauber coherent states in the case as the frequency is independent of time. 相似文献