基于固体腔F-P 标准具的可调谐自适应光滤波器

对F—P干涉滤波器的原理特性进行了分析。提出了通过改变入射角度来实现波长调谐的可调谐滤波器结构。采用了一种新的降低斜入射F—P标准具偏振相关损耗的结构。采用位置敏感探测器成功实现了关键约定位工作。采用了一种简单易行的波长跟踪方案。本系统实现了32通道0．8nm间隔DWDM系统精确滤波。     

GaAs基MOEMS波长可调谐滤波器的设计和理论模拟

采用传输矩阵理论和结合悬臂梁的电学一机械模型对GaAs基1.55 μm微光电机械系统(MOEMS)波长可调谐滤波器的光学和电学特性进行了深入的对比分析和研究.结果表明,采用800 nm厚的空气腔可以实现滤波器波长的调谐范围为100 nm,所需最大反向偏压为4 V,波长的调谐速率可以达到1.83 MHZ.     

具有90nm调谐范围的1.3μm Si基MOEMS可调谐光滤波器

利用表面微机械技术,成功制作了1.3μm Si基MOEMS可调谐光滤波器.原型器件在50V的调谐电压下,调谐范围为90nm.该技术可以用于制作1.3μm Si基可调谐光探测器.     

具有90nm调谐范围的1.3μm Si基MOEMS可调谐光滤波器

利用表面微机械技术,成功制作了1.3μm Si基MOEMS可调谐光滤波器.原型器件在5 0 V的调谐电压下,调谐范围为90 nm.该技术可以用于制作1.3μm Si基可调谐光探测器.     

基于Mach-Zehnder滤波的可调谐光纤激光器

() ()基金项目: 。摘要:为了实现高稳定性的可调谐激光输出,提出并设计了一种基于Mach-Zehnder(M-Z)滤波结构,结合Fabry-Perot(F-P)滤波器的可调谐掺铒光纤激光器,并对激光器的原理及实现方案进行理论分析和实验验证。所设计激光器系统的泵浦源工作波长为976 nm;长度5 m的掺铒光纤作为增益介质;采用全光纤M-Z结构进行滤波,并结合F-P滤波器实现单波长激光可调谐输出。实验中,通过调节F-P滤波器,在泵浦功率为60 mW时,实现了1547～1568 nm范围内单波长激光的稳定可调谐输出,波长调谐间隔小于1.7 nm,每个输出波长的边模抑制比均大于55 dB,线宽均小于0.1 nm。     

基于低温缓冲层的单片集成长波长可调谐光探测器

实现了一种单片集成的长波长可调谐光探测器.通过外延实验,摸索出低温缓冲层的最佳生长条件,成功地在GaAs衬底上生长出晶格失配度约4%的高质量的InP基材料.基于此低温缓冲层,在GaAs衬底上首先生长GaAs/AlAs材料的F-P腔滤波器,然后异质外延InP-In0.53 Ga0.47 As-InP材料的PIN结构.制作出的器件通过热调谐,峰值波长从1533.1nm红移到1543.1nm,实现了10.0nm的调谐范围,同时响应线宽维持在0.8nm以下,量子效率保持在23%以上,响应速率达到6.2GHz.     

基于低温缓冲层的单片集成长波长可调谐光探测器

实现了一种单片集成的长波长可调谐光探测器.通过外延实验,摸索出低温缓冲层的最佳生长条件,成功地在GaAs衬底上生长出晶格失配度约4%的高质量的InP基材料.基于此低温缓冲层,在GaAs衬底上首先生长GaAs/AlAs材料的F-P腔滤波器,然后异质外延InP-In0.53 Ga0.47 As-InP材料的PIN结构.制作出的器件通过热调谐,峰值波长从1533.1nm红移到1543.1nm,实现了10.0nm的调谐范围,同时响应线宽维持在0.8nm以下,量子效率保持在23%以上,响应速率达到6.2GHz.     

MEMS可调谐平顶窄带光学滤波器

设计了一种基于MEMS技术的可调谐光学滤波器,它通过光栅将输入的宽带光信号色散展开,以一个MEMS扭镜选择将对应滤波器通带的光信号反射至输出端,从而实现光学滤波和波长调谐功能。滤波器的输入端采用单模光纤,输出端采用多模或者少模光纤,可以实现窄带且平顶的通带特性。经过参数优化,仿真分析得结果显示,采用多模/少摸光纤输出的两种滤波器,其0.5 dB和25 dB带宽分别为0.95 nm/0.29 nm和1.39 nm/0.69 nm,分别满足100 GHz和50 GHz信道间隔的DWDM系统要求。由于输出端采用多模或者少摸光纤,从该滤波器输出的光信号不能继续在单模光纤中传输,只能由光探测器接收,因此该滤波器一般应用于全光网络节点中的下载端口。     

基于F-P干涉技术的通信波段可调谐激光器

根据F-P干涉原理设计制作了楔型F-P滤波器,使用这种滤波器进行可调谐掺铒光纤激光器实验,980nmLD泵浦功率为25mW时获得了稳定的单纵模激光输出,输出功率约0．6mW,线宽低于0．06nm,在34．2nm波长调谐范围内功率变化不超过0．5dB,边模抑制比大于35dB。     

一种新颖的宽带可调光纤光栅滤波器

分析了光纤光栅（FBG）调谐的基本原理,进而采用新颖的调谐结构,设计并实现了一种宽带可调谐的FBG滤波器。该滤波器仅用1支FBG制做而成,其波长调谐范围最高可达40nm。实验结果表明,该FBG滤波器的调谐波长与调谐步进位移量之间具有良好的二次曲线关系。     

可调微型环阵列加强马赫-曾德尔滤波性能分析

提出并分析了一种将微型环谐振腔阵列耦合集成在马赫-曾德尔干涉仪(MZI)的一臂上实现的集成波导型滤波器结构。利用微型环阵列可在MZI的谱特性上引入多个零点和极点,从而对输出频谱进行优化,使其在中心波长1550nm处具有矩形系数为0．4的门状响应,并且保持比较大的自由谱宽(28nm)。使用新型电光聚合物作为波导材料可以对器件进行快速调谐,在折射率变化0．001时中心波长调谐1nm。     

应力作用下光纤光栅Bragg波长调谐特性的研究

本文对１５５０ｎｍ光纤光栅在纵向拉伸应力和侧向拉伸应力作用下Ｂｒａｇｇ波长的偏移特性进行了实验研究。当纵向拉伸应力加至３．６０Ｎ（３６７．６０ｇ）时,得到了５．０２ｎｍ的调谐范围。这可能是在相同应力作用下,目前所报道的最好结果。此外,还对光纤光栅弯曲所导致的其Ｂｒａｇｇ波长的迁移特性进行了实验研究,并比较了对光纤光栅段添加涂覆层前后的调谐情况,得到了最大为３．０２ｎｍ的皮长调谐范围。     

Tuning Bragg wavelength by writing gratings on prestrained fibers

Bragg gratings at a specific wavelength are made using an excimer KrF laser and a phase mask. The wavelength can be varied for fine tuning and multiplexing applications by straining the optical fiber during UV illumination. When the strain is removed, the grating formed is at a smaller wavelength than that dictated by the phase mask for the unstrained fiber. This technique was demonstrated by writing two gratings located at the same point in the optical fiber. The transmission from the first grating was used as a means for in situ absolute wavelength tuning. The second grating made with approximately 0.2% axial strain was at 1534.54 nm. Once the grating was made, the strain was removed from the fiber leaving the second grating tuned to 1532.04 nm, a wavelength shift of 2.5 nm     

Transparent wavelength conversion in fibre with 24 nm pump tuningrange

A transparent continuous wave-pumped highly nonlinear fibre wavelength converter (WC) with a conversion bandwidth of 61 nm and a pump wavelength tuning range of 24 nm, the largest ever reported for fibre-based WCs, is demonstrated. The conversion quality is confirmed by bit error rate measurements showing < 1.4 dB power penalty at 10 Gbit/s data transmission     

A Tunable-MMI-Coupler-Based Wavelength Adjustable Laser

This paper introduces a novel integrated widely tunable laser, the tunable multimode interference (T-MMI) laser, with as tunable component an MMI coupler with a wavelength adjustable transmission spectrum. Experiments demonstrate up to 150 nm of tuning range for the T-MMI component and operation of a widely tunable T-MMI laser is demonstrated over a wavelength range of 38 nm.     

Optical N×N demultiplexer with continuous wavelength tuningby thin film heater

A continuous wavelength tuning of 2.1 nm for a waveguide grating array demultiplexer by means of a thin film heater is demonstrated. Low transmission losses of 6 dB and a crosstalk suppression of >20 dB are maintained over the entire tuning range     

Tunable filters based on an SOI nano-wire waveguide micro ring resonator

Micro ring resonator(MRR) filters based on a silicon on insulator(SOI) nanowire waveguide are fabricated by electron beam photolithography(EBL) and inductive coupled plasma(ICP) etching technology.The cross-section size of the strip waveguides is 450×220 nm2,and the bending radius of the micro ring is around 5μm.The test results from the tunable filter based on a single ring show that the free spectral range(FSR) is 16.8 nm and the extinction ratio(ER) around the wavelength 1550 nm is 18.1 dB.After thermal tuning,the filter’s tuning bandwidth reaches 4.8 nm with a tuning efficiency of 0.12 nm/℃Meanwhile,we fabricated and studied multi-channel filters based on a single ring and a double ring.After measurement,we drew the following conclusions: during the signal transmission of multi-channel filters,crosstalk exists mainly among different transmission channels and are fairly distinct when there are signals input to add ports.     

Bragg grating fast tunable filter for wavelength divisionmultiplexing

A Bragg grating fast tunable filter prototype working over a linear tuning range of 45 nm with a maximum tuning speed of 21 nm/ms has been realized. The tunable filter system is based on two piezoelectric stack actuators moving a mechanical device thus compressing an apodized fiber Bragg grating. The filter allows both traction and compression and can work in transmission and in reflection. It is designed to work with a channel spacing of 100 GHz according to the ITU specifications for wavelength division multiplexing systems     

Resonant cavity-enhanced InGaAs-AlGaAs heterojunctionphototransistors with an optical design for high uniformity and yield

We present uniformity data on resonant cavity-enhanced InGaAs-AlGaAs heterojunction phototransistors (HPT's) with an optical design that promotes high uniformity and yield. The HPT's operate in the wavelength region where the GaAs substrate is transparent and the data show the HPT's to be suitable for vertical integration with optical emitters or modulators to form two-dimensional arrays of smart pixels operating in transmission mode. The absorbing region of the HPT consists of an InGaAs multiple-quantum-well structure where the quantum wells (QW's) have been distributed to make the total absorption in the cavity insensitive to growth variations as well as the spatial matching of the standing wave and absorbing QW's. Theoretically, we estimate the absorption to be 39%±1% of the incident optical power, even at wafer nonuniformities of 12.5%. With these nonuniformities, the resonant wavelength moves ±25 nm, making postgrowth tuning of the wavelength necessary. Experimentally, we show postgrowth tuning of the resonance wavelength without loss in uniformity. The arrays have good uniformity as well as very high responsivities. The average responsivity is 160 A/W ±15% from 927-955 nm. The standard deviation of a typical array is 0.5 nm in resonant wavelength and about 5% of the average responsivity. The difference between maximum and minimum values for an array is typically 3 nm in resonant wavelength and ±10% of the average responsivity     

宽带可调谐光纤光栅色散补偿器系统设计

文章提出一种在光纤光栅自身热膨胀效应产生啁啾的基础上,利用铝片热膨胀系数比较高的特点产生应力来增强光纤光栅啁啾,从而实现了宽带、大范围色散调谐的新型光纤光栅色散补偿器。该色散补偿器能够分别对群速度色散及中心波长独立调谐。实验结果表明,在中心波长为1 551.25nm处,能够实现>1.5nm的色散补偿带宽,-350～-690ps/nm的群时延色散调谐范围;在色散为-660ps/nm情况下,能够实现中心波长1nm的偏移。