硅基竖直耦合三环谐振波分复用器的特性

对1×N信道硅基竖直耦合三环谐振波分复用器的传输特性进行了分析,给出了光学传递函数的公式.在中心波长1550.918nm、波长间隔1.6nm的情况下,对其振幅耦合比率、波谱响应、分光光谱、插入损耗、信道间的串扰进行了数值模拟.计算结果表明,该器件具有以下良好性能:若取小环与信道间的振幅耦合比率为0.27,小环与大环间的振幅耦合比率为0.06,该器件具有箱形波谱响应,输出光谱中的次峰值已被抑制到-25dB,谐振峰平坦且陡峭,3dB带宽约为0.28nm,每条输出信道的插入损耗及串扰较小,插入损耗小于0.71dB,串扰可降至-53dB以下.     

基于Interleave和微谐振环的32信道波分复用器特性

对结合interleave滤波器的1×32信道垂直耦合双环谐振波分复用器件的传输特性进行了研究,得到了器件的光学传递函数公式,对器件的参数、光谱响应、分波光谱、插入损耗以及信道间的串扰进行了数值模拟和优化.分析结果表明,通过在微环谐振波分复用器件的前端增加interleave滤波器,使信道间的串扰降低了14 dB,并且改善了器件的输出光谱形状,提高了器件的信道复用密度;同时,由于采用了在同一基片上集成,保证了器件的低插入损耗.通过参数优化,得到了中心波长为1 550 nm、波长间隔为0.4 nm、3 dB带宽为0.21 nm、插入损耗低于1.1 dB和串扰低于-32 dB的32信道密集波分复用器(DWDM).     

平行信道串联多环谐振滤波器的箱形波谱响应

对平行信道串联多环谐振滤波器的传输特性进行了理论分析,给出了其光学传递函数公式。在谐振波长为1．55μm情况下,对其滤波特性进行了数值模拟。计算结果表明,选取串联微环数为4、信道与微环间的振幅耦合比率为0．25以及相邻微环间的振幅耦合比率为0．022时,箱形波谱响应即可形成,其3dB带宽约为0．2nm,谐振光的插入损耗约为1．5dB,非谐振光的最小值已接近-150dB。     

17×17信道光谱响应平坦化的聚合物阵列波导光栅的研制

选用氟化聚芳醚FPE聚合物材料,设计并制备出了17×17信道光谱响应平坦化阵列波导光栅（AWG）波分复用器. 实验测试结果表明,器件的中心波长为1550.83nm,波长间隔为0.8nm, 3dB带宽约为0.476nm,插入损耗为13~15dB,串扰低于-21dB.     

17×17信道光谱响应平坦化的聚合物阵列波导光栅的研制

选用氟化聚芳醚FPE聚合物材料,设计并制备出了17×17信道光谱响应平坦化阵列波导光栅(AWG)波分复用器.实验测试结果表明,器件的中心波长为1550.83nm,波长间隔为0.8nm,3dB带宽约为0.476nm,插入损耗为13～15dB,串扰低于-21dB.     

17×17信道光谱响应平坦化的聚合物阵列波导光栅的研制

选用氟化聚芳醚FPE聚合物材料,设计并制备出了17×17信道光谱响应平坦化阵列波导光栅（AWG）波分复用器.实验测试结果表明,器件的中心波长为1550.83nm,波长间隔为0.8nm,3dB带宽约为0.476nm,插入损耗为13-15dB,串扰低于-21dB.     

箱型光谱响应聚合物阵列波导光栅的研制

通过减少奇数阵列波导的芯宽度,同时增加偶数阵列波导的芯宽度的技术,构造了箱型光谱-选用氟化聚芳醚FPE聚合物材料,设计并制备了17×17信道箱型光谱响应阵列波导光栅(AWG)波分复用器.测试结果表明,器件的中心波长为1550.87nm,波长间隔为0.8nm,3dB带宽约为0.476nm,串扰低于-21dB,插入损耗为13～15dB.     

箱型光谱响应聚合物阵列波导光栅的研制

通过减少奇数阵列波导的芯宽度,同时增加偶数阵列波导的芯宽度的技术,构造了箱型光谱. 选用氟化聚芳醚FPE聚合物材料,设计并制备了17×17信道箱型光谱响应阵列波导光栅（AWG）波分复用器. 测试结果表明,器件的中心波长为1550.87nm,波长间隔为0.8nm, 3dB带宽约为0.476nm,串扰低于-21dB,插入损耗为13~15dB.     

热光可调谐Si基聚合物列阵波导光栅

报道了用五氟苯乙烯共聚甲基丙烯酸环氧丙酯(PFS-co-GMA)的聚合物材料制备的33×33信道热光(TO)可调谐的阵列波导光栅(AWG)。给出了器件的制作工艺流程和测试结果。测得器件的波长间隔为0.81nm,3dB带宽为0.35nm,串扰约为-20dB,中心输出信道和边缘输出信道的插入损耗分别为10.4dB和11.9dB,TO可调谐值为-0.12nm/K,在温度为10~65℃时的器件工作中心波长为1545.21~1551.81nm,调谐范围为6.6nm。     

50/100GHz AWG型光学梳状滤波器的设计与制备

以Si基SiO2平面光波导为基础,设计并制备了50/100GHz AWG型光学梳状滤波器.制备得到的AWG型光学梳状滤波器可以覆盖1520～1585nm的波长范围,共有160个信道.功率输出不均匀度＜0.5dB,插入损耗＜8dB,相邻通道的串扰＞13dB,在距离中心频率最远的信道,输出频率偏离ITU标准15GHz.分析了影响器件串扰和信道频率偏移的原因,并提出了相应的解决办法.     

An all-fiber dense wavelength-division multiplexer/demultiplexerusing photoimprinted Bragg gratings

A wavelength multiplexing/demultiplexing device is fabricated and used to drop/insert a single wavelength channel from/into a multiple wavelength transmission link with 100 GHz channel-spacing at 1550 nm. The device consists of an all-fiber Mach-Zehnder interferometer with photoinduced Bragg gratings. The following performances were measured: extraction/coupling efficiency =99.4%, excess loss <0.5 dB, adjacent channel-isolation >20 dB, and return loss >23 dB     

基于定向耦合的可见光三波长合波器

本文提出了一种基于定向耦合的可见光三波长合波器,该器件由两级定向耦合器级联而成,实现可见光波段中三波长合成。以常见的635nm,532nm以及488nm三波长为例,提出具体的设计方案与结构参数,整个器件的长度为2500um,用BeamPROP软件对该器件进行模拟,各个波长的插入损耗小于0.15dB。     

Tunable sampled-grating DBR lasers with integrated wavelengthmonitors

We report on the design and development of a wavelength monitor for use with tunable semiconductor lasers. The device is based on two-mode interference in an asymmetrically excited waveguide that is coupled to a Y-branch splitter. The monitoring range of the device is 30 nm. The wavelength monitor is capable of operating over an input power range of 34 dB, and the waveguide detectors do not saturate at photocurrents as high as 1.2 mA. The sensitivity of the monitor is only 1.24 nm for an isolated device, but improves to 0.44 nm when it is integrated on chip with the laser     

Short Polarization Filter in Pillar-Based Photonic Crystals

The strong polarization dependence of two- dimensional photonic crystals is exploited for polarization filtering. The device with a length of 3.9 mum is integrated in a photonic integrated circuit based on InP waveguide technology. The average transmissions in the wavelength range from 1530 to 1570 nm are -8.7 dB for transverse-magnetic polarization and -26.5 dB for transverse-electric polarization.     

Wavelength-tunable single-mode fibre grating reflector

An optical fibre grating filter is demonstrated that has broad wavelength tuning capability for the back-reflected guided wave. A novel ?fan?-shaped diffraction grating is used for this device in which the period varies continuously with position along its length. A 3 dB reflection bandpass of 0.8 nm that is tunable over a wavelength range from 1.46 to 1.54 ?m has been observed.     

Four-channel integrated-optic wavelength demultiplexer with weakpolarization dependence

A planar four-channel wavelength demultiplexer with weak polarization dependence is proposed and demonstrated. This demultiplexer is based on an optical-phased array. An experimental device with dimensions 4.5×3.2 mm² was designed and fabricated, using conventional (high-quality) optical lithography. The demultiplexer operates in the wavelength range 776.5-781.2 nm, with a channel spacing of 1.55 nm. Insertion loss was 0.6 dB for the central channels and 1.2 dB for the outer channels for transverse-electric (TE) polarization, excluding 1.3-dB waveguide propagation loss. Crosstalk values measured 15.4-29.7 dB for the TE and 13.4-22.2 dB for the transverse-magnetic (TM) polarization     

17×17 硅基聚合物信道箱形光谱阵列波导光栅的制备

Arrayed waveguide grating (AWG) is a key device in wavelength-division multiplexing (WDM) system, and the flat spectral response of the AWG device is required. In this paper, the RIE process has been improved. By using the steam- redissolution technique, the insertion loss and the crosstalk have been reduced. Experimental results show that the central wavelength is 1550.86nm, and 3-dB bandwidth is about 0.478 nm, insertion loss is 10.5 dB, crosstalk is about –22 dB. The insertion loss of an AWG device is reduced by about 3 dB for the central channel and 4.5 dB for the edge channels, and the crosstalk is reduced by 2.5 dB after the steam- redissolution.     

A unidirectional output optical frequency conversion device with anasymmetric-κ DBR structure

A novel optical frequency conversion device that successfully demonstrates optical frequency conversion and unidirectional transmission of optical signals has been designed and fabricated. The device is composed of a gain region and saturable absorber region with monolithically integrated distributed Bragg reflector (DBR) mirrors with different coupling coefficients. The device structure is optimized to achieve three functions: 1) unidirectional light output, 2) converted-light wavelength tuning, and 3) optically triggered optical frequency conversion. The output power of converted light from the light input-end facet of the device is 30 dB smaller than that from the output-end facet, and the converted light wavelength can be scanned over 4 nm without a bias current to the input-end DBR region, and it is widened to 7.8 nm by injecting current to that region. The device emits converted light only when light input is injected and optical signals are unidirectionally transmitted, and its response frequency is estimated to be 0.8 GHz     

光子晶体电光调制和粗波分复用集成器件研究

提出了一种用于电光调制和粗波分复用的片上集成器件。该集成器件的电光调制器模块和粗波分复用器模块都是由硅基光子晶体波导和L3型谐振腔组成,两个模块间采用硅基光子晶体波导连接。该器件根据等离子体色散效应,采用L3型谐振腔和PN结实现了对波长的调制;根据微腔与波导的直接耦合理论,采用L3型谐振腔结构实现了滤波。利用基于三维时域有限差分法(3D-FDTD)的Lumerical软件对其进行仿真分析,结果表明该集成器件在工作波长1530 nm和1550 nm下均可以先完成各自的电光调制再进行双通道波长的复用。该器件在工作波长1530 nm和1550 nm下的插入损耗分别为0.70 dB和0.95 dB,消光比分别为20.97 dB和22.05 dB,调制深度均为0.99,信道串扰分别为-29.05 dB和-27.59 dB,器件尺寸仅为17.83μm×17.3μm×0.22μm。该集成器件结构紧凑,易于集成,可应用于高速大容量波分复用光通信系统。