高效多信道光子晶体滤波器的设计与仿真

利用二维光子晶体仿真设计了四信道光滤波器.首先根据时域耦合模理论导出了实现100％信道耦合的条件;然后根据该条件设计了四信道滤波器,并利用时域有限差分法进行了仿真.仿真结果显示,四信道耦合效率均超过96％,当晶格常量取570 nm时,四信道的中心频率在1 520 nm到1 580 nm之间,信道间隔均小于20 nm,信道间窜扰很小.     

一维可调谐非磁化等离子体光子晶体的滤波特性

用时域有限差分(Finite-Different Time-Domain,FDTD)的分段线形电流密度卷积(Piecewise Linear Cur-rent Density Recursive Convolution,PLCDRC)算法研究了含单一介质缺陷层的一维非磁化等离子体光子晶体的滤波特性.从频域角度分析得到微...     

时变磁化等离子体光子晶体的禁带特性

采用磁化等离子体的分段线形电流密度卷积(Piecewise Linear Current Density Recursive Convolution,PLCDRC)时域有限差分(Finite-Different Time-Domain, FDTD)算法研究了一维时变磁化等离子体光子晶体的禁带特性。以高斯脉冲为激励源,用算法公式所得的电磁波透射系数来讨论了等离子体上升时间、密度、周期常数对其禁带特性的影响。结果表明,改变等离子体上升时间和密度可以实现对禁带的控制。     

光子晶体四信道波分复用器的研究

提出了一种由2-D光子晶体构成的四信道波分复用系统。该系统包括利用光子晶体的线缺陷实现的波导部分和利用光子晶体微腔实现的频率选择部分。采用时域有限差分(FDTD)方法,研究了光在含点缺陷(即微腔)和线缺陷(即波导)的光子晶体中的传输特性,并给出了仿真结果。计算结果表明,该结构可以实现波长为λ=1550nm附近的四信道波分复用。     

光子晶体微腔温度响应特性研究

利用平面波展开法对由硅(Si)介质柱构成的二维正方晶格光子晶体在TM模式下的能带进行计算。构造了光子晶体微腔,利用时域有限差分法对该光子晶体微腔的谐振特性进行了数值模拟,得到了缺陷态模场分布。考虑硅的热膨胀效应和热光效应对硅性质的影响,引入到光子晶体微腔谐振模式的计算中,模拟计算了微腔谐振波长随温度的变化关系。结果表明,随着温度的升高光子晶体微腔的谐振波长增大,温度每升高1℃,波长向长波漂移6.7pm,而且具有良好的线性。光子晶体微腔的这种特性可以用于温度传感,具有一定的实用意义。     

带有环形谐振器的1×2光子晶体功率分配器传输性能

 利用正方格2维光子晶体设计了带有环形谐振器的1×2光子晶体功率分配器结构,该结构具有1个输入端口和2个输出端口。采用时域有限差分法研究了该功率分配器对电磁波的传输性能,结果表明：其结构在第三通信窗口(1 550 nm波长)实现了电磁波的高效传输,同时具有优良的电磁波通频带功率二等均分性,以及电磁波传输转向设计灵活、损耗低、结构紧凑等优点。     

平行光子晶体波导的传输特性及应用

采用时域有限差分法研究两平行光子晶体波导的传输特性及模场分布,利用耦合模理论计算光子晶体波导的耦合系数。计算结果表明,在不同的频率范围内两平行光子晶体波导之间表现出不同的耦合特性:在高频段(0.32~0.44)(ωa/2πc)的范围内两直波导表现出相互的能量交换,实现光耦合,耦合系数随入射波 频率增加而减小;而在低频段(0.29~0.32)(ωa/2πc)的范围内,两波导的传输谱图几乎重合。最后,提出一种采用固定波导耦合长度同时实现光分束及光均分器的方案,当耦合长度取34a时,可将频率为0.333 (ωa/2πc)和 0.357(ωa/2πc)的两入射波分束传播,同时将低频段中的任意频率波进行能量均分。     

含单缺陷层的一维可调谐磁化等离子体光子晶体滤波特性研究

采用在等温近似的条件下,以等离子体的上升时间、温度和密度为可调谐参量,用磁化等离子体的分段线形电流密度卷积时域有限差分算法研究了含单一缺陷层的一维磁化等离子体光子晶体的滤波特性.以高斯脉冲为激励源,用算法公式得到的电磁波透射系数来讨论了等离子体上升时间、温度、等离子体层密度对其滤波特性的影响.结果表明,改变等离子体上升时间和等离子体层密度可以实现对滤波通道的调整.谐振频率不能通过改变温度进行调整.     

含单缺陷层的一维可调谐磁化等离子体光子晶体滤波特性研究

采用在等温近似的条件下,以等离子体的上升时间、温度和密度为可调谐参量,用磁化等离子体的分段线形电流密度卷积时域有限差分算法研究了含单一缺陷层的一维磁化等离子体光子晶体的滤波特性.以高斯脉冲为激励源,用算法公式得到的电磁波透射系数来讨论了等离子体上升时间、温度、等离子体层密度对其滤波特性的影响.结果表明,改变等离子体上升时间和等离子体层密度可以实现对滤波通道的调整.谐振频率不能通过改变温度进行调整.     

1×4光子晶体波导分束器的特性

在完整的二维光子晶体中引入线缺陷,形成了光子晶体波导,光子晶体波导分束器是集成化光学电路的重要组成元件。我们设计了一种线缺陷1×4光子晶体分束器,并且用有限时域差分法研究了它的特性。研究表明,输出端的透射传输特性与入射光的波长和分支的几何形状有关,并且入射波分别相等地流入四个输出端口。为了减少1×4分束器在三个Y型分支区的反射,可以通过调节在分支区的可调介质柱的半径R,使每个输出端口具有很高的透射率。     

Wavelength division demultiplexing by photonic crystal waveguides with asymmetric corrugated surfaces

<正>We propose a new type of wavelength division demultiplexer composed of a photonic crystal waveguide with asymmetric corrugated exit surface.The focus displacement for different symmetric corrugated surfaces is relative to the intensity of the excited surface mode.By systematically investigating the effects of the parameters of the corrugated surface on the focus shift,we demonstrate an on-axis focus by a photonic crystal waveguide with an asymmetric corrugated exit surface at a specific wavelength.The precise equivalences of surface modes at each side of the exit surface are broken.Thus,for the light source with other wavelengths,the emerging beams are off-axis focused at different directions,similar to the function of a wavelength division demultiplexer.     

Dense wavelength division demultiplexing using photonic crystal waveguides based on cavity resonance

We demonstrated a photonic crystal waveguide based dense wavelength division multiplexing device using the resonances in the cavities. The demultiplexing is achieved through filtering. This filtering is achieved by varying the radii of the surrounding holes of the cavity, which in turn changes the resonant wavelength of the cavity. The four wavelengths demultiplexed in the design are 0.8 nm apart in the optical region centered on 1.55 and 1.56 μm. The device designed and simulated has easy to realize structure as well as high quality factor. Two-dimensional Finite Difference Time Domain (FDTD) is chosen to do the simulation of this work.     

Theoretical study on biosensing characteristics of heterostructure photonic crystal ring resonator

In this paper, we investigate the biosensing characteristics of two-dimensional heterostructure photonic crystals (PCs) ring resonator theoretically by using the finite difference time domain (FDTD). The coupling air holes and inner air holes of ring resonator are treated as coupled sensing area and internal sensing area. When both of the sensing areas are filled with the same biological samples solution, the resonant peak wavelength shift of the ring resonance is different. Both the resonant peak center wavelength and peak intensity are related to the positions of sensing holes. With the same refractive index change of the biological sample, the sensing sensitivity of the coupling sensing area is much higher than that of the inner sensing area. Meanwhile, through the analysis of resonant peak wavelength shift, the refractive index change of the sample filled in the sensor area can be derived, which can be monitored real-time.     

Coupling length variation and multi-wavelength demultiplexing in photonic crystal waveguides

In this Letter, the effects of material/structure parameters of photonic crystal(Ph C) parallel waveguides on the coupling length are investigated. The results show that, increasing the effective relative permittivity of the Ph C leads to a downward shift of the photonic bandgap and a variation of the coupling length. A compact Ph C 1.31/1.55 μm wavelength division multiplexer(WDM)/demultiplexer with simple structure is proposed,where the output power ratios are more than 24 d B. This WDM can multiplex/demultiplex other light waves efficiently.     

光子晶体环形腔的四波长THz滤波器

提出一种基于光子晶体环形腔的四波长THz滤波器,该滤波器在光子晶体结构中引入两个环形腔,且环形腔内部各增加一个正方形介质柱,四周各引入一个散射介质柱。应用基于时域有限差分法(FDTD)的Rsoft软件进行仿真分析,结果表明通过对内部正方形介质柱的边长、散射介质柱半径以及耦合介质柱半径等结构参数的调节,可以滤出74.813,76.98,78.168和78.883 m四个太赫兹波长。该滤波器性能优良,透过率高、Q值高、信道隔离度大,对于THz技术应用具有重要意义。     

Nonlinear Fabry-Perot resonator with a silicon photonic crystal waveguide

We derive an equation that describes the nonlinear operation of a Fabry-Perot resonator with a large group index waveguide. Specifically, a silicon photonic crystal microcavity with two-photon-excited free carrier nonlinearity and Kerr nonlinearity is assumed. The equation clearly explains the bistability of the device and the reduction of the required pump energy for a specific nonlinear phase shift at an appropriate phase detuning from the resonance. We present a simple procedure to predict the required optical pump energy for the modulation and the resulting modulation depth by use of the equation and the device parameters.     

一种新型可调制的光子晶体环形腔滤波器

在光子晶体环形腔中增加两个散射介质柱,构成一个新型的环形腔滤波器,该滤波器能有效选择光波透过,光波的透射率可以达到90%以上,带宽较小.可通过这两种不同的调节方式使滤波器中波长的带宽和数值进行任意的改变:1)减小散射介质柱半径,从负载波导输出波长的带宽变大,主波导中波长的带宽减小;增大其半径时,它们的变化正好相反.2)改变耦合区域介质柱半径的大小,滤波器中波长的数值也会相应地变化,它与介质柱半径的变化呈正比,并且透射率也会发生明显的变化.这就为其在制备集成光子器件的应用中奠定了基础. 关键词： 环形腔 滤波器 散射介质柱 透射率     

T-shaped channel drop filter based on photonic crystal ring resonator

Photonic crystal ring resonators are promising candidates for realizing all optical filters with acceptable transmission efficiency and quality factor values. In this paper, by putting a12-fold quasi crystal at the middle of on 7 × 7 square cavity we created a ring resonator structure and designed a T-shaped channel drop filter. The drop wavelength of our filter is at 1551 nm, with transmission efficiency and quality factor equal to 90% and 387. Our structure is composed of dielectric rods immersed in air. Because in this kind of structures the dominant band gap is in TM mode, all of our simulations have been done in TM mode. The total footprint of our filter is 242.4 μm², which makes it suitable for all optical integrated circuits.     

Optical properties and photonic bands of GaAs photonic crystal waveguides with tilted square lattice

Reflectance measurements at variable angle of incidence are performed on GaAs photonic crystal waveguides with unconventional square lattices. The technique yields the dispersion of photonic bands for the investigated lattices, as first shown by Astratov et al. [Phys. Rev. B 60, R16225 (1999)]. A sample with a square lattice of air rings and small air fraction yields narrow resonant structures and a dispersion of photonic modes close to that of free photons. Another sample with a square lattice of dielectric squares and large air fraction leads to broader structures and to a dispersion of photonic modes which differs strongly for the two polarizations of light: this sample has a pseudo-gap around 1 micron wavelength. The experimental results are in good agreement with theoretical calculations of the reflectance and of the photonic mode dispersion in the photonic crystal slabs. Received 16 January 2002