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.     

1×8阵列波导光栅型波分复用/解复用器设计的一种简单方法

用有效折射率法,采用近轴近似和波导模场分布的高斯近似,简化了阵列波导光栅 (AWG)器件的设计过程中繁杂的计算,且保证了器件的性能指标.给出了设计思路,并给出了1×8路、中心波长为1550.9nm,波长间隔为1.6nm的AWG波分复用/解复用器的设计实例.     

1×8阵列波导光栅型波分复用/解复用器设计的一种简单方法

用有效折射率法 ,采用近轴近似和波导模场分布的高斯近似 ,简化了阵列波导光栅( AWG)器件的设计过程中繁杂的计算 ,且保证了器件的性能指标 .给出了设计思路 ,并给出了 1× 8路、中心波长为 1 550 .9nm,波长间隔为 1 .6nm的 AWG波分复用 /解复用器的设计实例     

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.     

离子束辅助沉积真空镀膜技术制备阵列波导光栅波导材料

采用离子束辅助沉积(IBAD)真空镀膜技术制备阵列波导光栅(AWG)波导材料。以固体石英玻璃材料作为衬底,采用离子束辅助沉积真空镀膜制备SiO2膜层,以实现偏振不敏感的阵列波导光栅。实验表明器件的偏振相关性大大改善,其双折射B约为1.4077×10-5,远小于二氧化硅-硅基波导结构阵列波导光栅的双折射B=2×10-4。器件的热稳定性也得以改善,当工作环境的温度变化范围为-10~70℃时,采用此方法研制的阵列波导光栅最大波长漂移为1.144 nm,小于普通的二氧化硅-硅基波导结构阵列波导光栅的波长漂移1.368 nm。     

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.     

相位误差对阵列波导光栅传输特性的影响

研究了阵列波导光栅 (AWG)制作过程中产生的误差所引起的相位误差对AWG传输特性的影响。非随机误差引起的相位误差使信道的中心波长产生漂移 ,研究表明波导宽度 0 0 2 μm的变化将引起中心波长漂移 0 1nm。随机误差所产生的随机相位误差将恶化AWG的串扰特性 ,计算表明 ,最大随机误差为 0 0 0 0 0 4rad μm时 ,串扰将增加 4 2dB。     

基于SOI的16通道200GHz阵列波导光栅

设计并制作了基于绝缘体上硅(SOI)材料的1×16阵列波导光栅(AWG).该AWG器件的中心波长为1 550 nm,信道间隔为200 GHz,采用了脊型波导结构.首先确定了波导的结构尺寸以保证单模传输,并利用束传播法(BPM)模拟了波导间隔、弯曲半径和锥形波导长度等参数对器件性能的影响,对器件结构进行了优化,同时也利用BPM方法模拟了器件的传输谱.模拟结果显示:器件的最小信道损耗为4.64 dB,串扰小于-30 dB.根据优化的器件结构,通过光刻等半导体工艺制作了AWG,经测试得到AWG器件的损耗为4.52～8.1 dB,串扰为17～20 dB,能够实现良好的波分复用/解复用功能.     

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.     

Fabrication of 17 × 17 polymer/Si arrayed waveguide grating with flat spectral response using steam-redissolution technique

Arrayed waveguide grating (AWG) is a key device in the 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 1550.86 nm, the channel spectral response flatness is about 1.5 dB, 3-dB bandwidth is about 0.478 nm, insertion loss is 10.5 dB, and 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.     

Fabrication of 17×17 polymer/Si arrayed waveguide grating with flat spectral response using steam-redissolution technique

Arrayed waveguide grating(AWG) is a key device in the 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 1550.86 nm,the channel spectral response flatness is about 1.5 dB,3-dB bandwidth is about 0.478 nm,insertion loss is 10.5 dB,and crosstalk is abo...     

Dye-doped step-index polymer optical fiber for broadband opticalamplification

We report the development of a novel and simple technique for fabricating polymer optical fibers of good optical quality for special device applications. This technique aims at polymer fibers doped with various functional organic materials. On the basis of the technique, step-index polymer optical fibers doped with laser dyes have been fabricated. High-gain and high-efficiency optical amplification has been achieved in a Rhodamine B-doped polymer fiber with a low pump power of less 1 kW and pulse width 5 ns. Because a high dye concentration is used, the optimal wavelength range of optical amplification in this fiber is significantly red-shifted toward the center of the communication window (at 650 nm wavelength) of methyl methacrylate-based polymer optical fiber. The shift is from the originally 560 and 590 nm to presently 610 to 640 nm. We also present experimental results that show good photostability of the Rhodamine B-doped polymer fiber, compared with those recently reported in the improved polymer material systems. From the experimental observation, we identified the thermally induced bleach of dye molecules as the major contributing factor to the lifetime of our material system     

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.     

Five-channel polymer waveguide wavelength division demultiplexerfor the near infrared

A five-channel wavelength division demultiplexer (WDDM) fabricated in polymer gelatin waveguides and operating over a 100-nm bandwidth centered at 770 nm in the near infrared is discussed. The device has a maximum diffraction efficiency of 80% at 730 nm, has a spectral bandwidth of 17±3 nm per channel, and effectively utilizes a portion of the large optical transparency bandwidth (~2400 nm) of the photo-lime gelatin polymer material at laser diode wavelengths. High-channel-density WDDM devices at longer infrared wavelengths should be possible     

基于场景的热红外高光谱数据光谱定标

传感器每个波段的中心波长和半高全宽（Full Width at Half Maximum，FWHM）随成像环境变化会发生较大的系统性漂移。这种漂移最终会影响发射率和温度的反演精度，尤其是在大气吸收波段附近的发射率反演精度。选择水汽在11.73 m处的吸收通道作为参考波段，提出了适用于热红外高光谱数据的光谱定标技术流程。模拟实验表明:光谱分辨率为50 nm，中心波长偏移在-50~50 nm、FWHM变化在-25~25 nm时，大气水汽含量对光谱定标误差的影响最大。同时，对误差分布曲面进行拟合得到描述误差分布模型，用于误差的估计。当大气水汽含量足够大时，光谱中心波长偏移估算误差可达到1 nm以内。最后，将所提方法应用于机载热红外高光谱数据光谱定标。结果显示，热红外高光谱成像仪中心波长偏移为28.4 nm，FWHM变化为-18.5 nm。     

Silicon-based Fano resonance devices based on photonic crystal nanobeams

To address the driving power and density of wavelength-division-multiplexing (WDM) computing architectures, a Fano resonator based on a photonic crystal nanobeam is proposed. The Fano resonator comprises a T-shaped waveguide, introducing an additional phase shift in the continuous propagation mode, and a photonic crystal nanobeam with a discrete mode. The device has one resonance peak within wavelength ranging from 1 500 nm to 1 600 nm, with a maximum extinction ratio of 8.7 dB and a transmission spectrum slope of up to 11.30 dB/nm. The device has good reusability, extinction ratio, and spectral resolution. It is expected to provide essential photonic components for low-energy consumption and high-density photonic computing to meet the requirements of future convolutional neural network (CNN) acceleration computing.     

基于全息聚合物液晶光栅的动态增益均衡器的设计与模拟

介绍了聚合物分散液晶(PDLC)材料及体全息光栅的特性,提出了基于全息聚合物液晶(H-PDLC)电控光栅多极串联式动态增益均衡器的设计。根据光栅的衍射特性计算公式,对全息聚合物液晶光栅在中心波长为1550 nm的波长选择特性进行模拟,并且进一步利用遗传算法模拟实现全息聚合物液晶动态光强增益均衡器的功能。计算模拟表明,选择合适的全息聚合物液晶光栅参量,能够使光栅在1550 nm为中心波长的衍射谱线半宽度达到10 nm。同时,采用基于全息聚合物液晶的动态光强增益均衡器,能够使掺饵光纤放大器在1530~1560 nm内,其自发辐射谱的不平坦度从3.3 dB降到0.1 dBp-p(峰-峰值)。     

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。