Optically controlled tunable dispersion compensators based on pumped fiber gratings

We demonstrate optically tunable dispersion compensators based on pumping fiber Bragg gratings made in Er/Yb codoped fiber. The tunable dispersion for a chirped grating and also a uniform-period grating was successfully demonstrated in the experiment. The dispersion of the chirped grating was tuned from 900 to 1990 ps/nm and also from -600 to -950 ps/nm in the experiment.     

Wideband multichannel dispersion compensation based on a strongly chirped sampled Bragg grating and phase shifts

A novel multichannel dispersion compensator based on a strongly chirped sampled Bragg grating with phase shifts is demonstrated experimentally. With a single phase mask, various channel spacings and dispersion can be achieved by proper control of the sampling period and the phase shifts. A 100 GHz channel-spacing compensator with a dispersion of -1000 ps/nm and another 200 GHz channel-spacing compensator with a dispersion of -500 ps/nm are designed. As an example, a 40 channel, 100 GHz channel-spacing compensator with a dispersion of approximately -560 ps/nm is fabricated. All the designs are based on one phase mask, thus showing the flexibility of our method.     

Wide-field-angle behavior of blazed-binary gratings in the resonance domain

Blazed-binary gratings for which a blazed effect with binary etches is achieved under normal incidence offer first-order diffraction efficiencies larger than those of blazed-échelette gratings in the resonance domain [Opt. Lett. 23 1081 (1998)]. We provide further insight into the behavior of blazed-binary gratings and show that they operate efficiently under symmetrical mounting and over a wide field-angle interval. These properties are illustrated with theoretical and experimental results obtained for an approximately 1000-line/mm grating at 633 nm.     

Light scanner based on a viscoelastic stretchable grating

We present a new technique for light scanning by use of viscoelastic-based deformable phase diffraction gratings. Mechanical stretching of the grating permits control of its spatial period, and thus the orders of diffraction can be spatially deflected. In the experiments the viscoelastic gratings with triangular and rectangular profiles have been characterized at lambda = 633 nm. It is demonstrated that the reversible elongation can exceed 20% of the initial length. For the triangular profile grating, the diffraction angle of the first order changed from 6.6 degrees to 5.4 degrees while the diffraction efficiency remained almost constant at approximately 17%. Dynamic scanning of a laser beam at frequencies of approximately 1 kHz is demonstrated by use of electromechanically driven viscoelastic gratings.     

Electro-optic properties of switchable gratings made of polymer and nematic liquid-crystal slices

We report the diffraction properties at wavelengths of 632.8 and 1550 nm for volume transmission gratings made of a sequence of continuously aligned nematic liquid-crystal layers separated by isotropic polymer slices. The gratings are generated by holographically curing a solution of liquid crystal diluted in an isotropic prepolymer by means of a laser beam at a wavelength of 352 nm with a total intensity of approximately 10 mW/cm2. A diffraction efficiency of 98% was measured, and an electric field as low as 5 V/microm switches off the phase grating. Measured angular spectra are fitted by use of the modified coupled-mode theory including the effects of grating birefringence.     

啁啾光纤光栅在光纤通信系统中的色散补偿

报道一个简单而新颖的、能将均匀光栅改变为线性啁啾光栅的方法,此方法可对光纤光栅的喃啾度和中心波长进行独立调节,实验表明,一长为１０ｃｍ的均匀光栅其啁啾度可增加至０．５ｎｍ／ｃｍ,而中心波长独立可调量达０．７ｎｍ利用这样的可调啁啾光栅在标准单模光纤（Ｇ６５２）中对一脉宽为２５ｐｓ的输入信号在１５５０ｎｍ窗口传输,成功地实现１００ｋｍ的色散补偿。     

Fiber Bragg gratings for pure dispersion-slope compensation

Single-fiber Bragg gratings designed to compensate for pure third-order dispersion are demonstrated. The devices are designed by use of a layer-peeling inverse-scattering technique and exhibit dispersion profiles across their reflection bandwidths of -20, +/- 40, and -225 ps/nm2 over bandwidths of 4.5, 6, and 3 nm, respectively. Furthermore, they have almost constant peak reflectivities of approximately 75% and are, respectively, only 8, 23, and 40 mm long.     

Fiber-based tunable dispersion compensation

Tunable dispersion has been implemented in various technology platforms, including fiber gratings, planar waveguides, thin film etalons, and bulk optic technologies. This paper will focus on fiber grating based tunable dispersion compensation, because fiber gratings are at present one of the best developed TDC technologies available. The paper is divided into three parts. In the first part we describe grating based TDC technologies and discuss their advantages and disadvantages. We focus on thermally tuned linearly chirped fiber gratings, as these have to date been the most successful grating technology for 40 Gbit/s. We also compare grating TDCs to two other prominent tunable dispersion technologies: thin film etalons and planar waveguide ring resonators. In the second section we describe the techniques used to fabricate high performance dispersion compensation gratings as well as the theory of the primary defect of fiber grating dispersion compensation: group delay ripple (GDR). In the third section we describe the telecom system related issues for tunable gratings, including characterization of grating performance, tunability requirements and results from actual system trials using tunable FBGs.     

双光栅切换微型平场全息凹面光栅光谱仪

基于CCD的微型平场全息凹面光栅光谱仪,以其简单紧凑的结构和快速高效的工作方式在光谱分析领域获得了广泛的应用。但是,由于受限于色散距离,单纯依靠优化光栅像差很难进一步使光谱分辨率获得大幅提高。提出一种双光栅切换微型平场全息凹面光栅光谱仪的设计方法,用两个使用结构相同的光栅代替传统的单光栅设计,给出一个光谱范围为400～1000nm光谱仪的具体设计,计算显示光谱分辨率最大可提高为原来的2.5倍。通过对光栅衍射效率的计算分析,说明此方法能够显著改善仪器的通光效率。设计制作了原理样机,进行了装调测试,实验结果与理论计算相吻合。     

短腔Er/Yb光纤光栅激光器

报道采用光敏Ｅｒ／Ｙｂ 光纤制作短腔Ｅｒ／Ｙｂ 光纤光栅激光器的实验结果。激光谐振腔由一对直接写在３０ ｍ ｍ 长的Ｅｒ／Ｙｂ 光纤上、长度分别为６ ｍ ｍ 及１０ ｍ ｍ 、反射率分别为９０％ 及９８．６％ 、３ ｄＢ带宽分别为０．２８ ｎｍ 及０．２６ ｎｍ 的光纤布拉格光栅组成, 激光器的泵浦阈值为８ｍ Ｗ, 斜效率约１４％ , 输出光的信噪比为６１ ｄＢ, 偏振模抑制比为３０ ｄＢ。     

变迹啁啾Bragg光纤光栅的矩阵分析

本文用传输矩阵法分析了各种变迹与线性啁啾Bragg光纤光栅的响应特性,构造了各种变迹函数,进行了比较.分析了变迹函数、啁啾系数、折射率变化量以及光栅长度对反射带宽、最大反射率的影响.找到了最佳变迹函数和量佳啁啾系数.特例中的数值分析表明,补偿100km光纤色散带宽为1nm的最佳光栅长度是140mm,最佳啁啾系数为0.048nm/cm.     

光折变多重体光栅的制作及应用

根据光折变多重体光栅的滤波原理,在10×10×10 mm3的LiNbO3∶Fe晶体中利用循环曝光法写入了光栅波矢夹角为0.037°且衍射效率均衡的8重体光栅,实验上证实了光写入多重光折变体光栅应用于波分复用系统的可行性.利用LiNbO3∶Fe晶体制作了一个原理性双通道波分复用器,成功地实现了对相同方向入射的波长分别为635 nm和650 nm的两束光的有效分离,并根据布喇格条件,将光折变体光栅应用于光波波长的测量,测量精度可达10 pm量级.     

Magneto-Optic Fiber Gratings Useful for Dynamic Dispersion Management and Tunable Comb Filtering

Intelligent control of dispersion management and tunable comb filtering in optical network appfications can be performed by using magneto-optic fiber Bragg gratings （MFBGs）. When a nonuniform magnetic field is applied to the MFBG with a constant grating period, the resulting grating response is equivalent to that of a conventional chirped grating. Under a linearly nonuniform magnetic field along the grating, a linear dispersion is achieved in the grating bandgap and the maximal dispersion slope can come to 1260ps/nm2 for a l0-mm-long fiber grating at 1550nm window. Similarly, a Gaussian-apodizing sarnpled MFBG is also useful for magnetically tunable comb filtering, with potential application to clock recovery from return-to-zero optical signals and optical carrier tracking.     

Photoerasure of ultraviolet-induced birefringence and polarization-mode dispersion of chirped fiber Bragg gratings

The first, to my knowledge, experimental demonstration of photoerasure of UV-induced birefringence and polarization-mode dispersion (PMD) in chirped fiber Bragg gratings is presented here. The photoerasure process carried out by launching high-peak-power (approximately 0.6-kW) pulsed (10-Hz, 5-ns) circularly polarized laser light in the visible wavelength (532 nm) through the core of a fiber with the grating was found to reduce its PMD by more than 85% to 0.12 ps. Possible reasons for the photoerasure process, including photobleaching of UV-induced absorption and randomization of dipole orientation of UV-induced defects, are discussed.     

Broadband Terahertz Polarization Converter and Asymmetric Transmission Based on Coupled Dielectric‐Metal Grating

Coupled dielectric‐metal gratings are investigated for broadband terahertz (THz) wave polarization conversion and asymmetric transmission by the experiments and numerical simulations, which are composed of the subwavelength Si grating and metallic wire grating layers. The dielectric grating layer with a large artificial birefringence and low dispersion is employed as a phase engineered waveplate, and the metal wire grating arranged with a 45° angle to the dielectric grating is utilized as a high‐efficiency polarizer. Due to the subwavelength integration, this coupled grating presents a local resonance coupling mechanism between dielectric and metal gratings, which greatly enhances the polarization rotation and expands the bandwidth, not a simple combination with dielectric and metallic gratings. The results demonstrate that a broadband asymmetric transmission with an extinction ratio of 30dB from 0.2 to 1.2 THz is achieved and the highest transmission of 90% can be obtained. It provides a simple way towards practical applications for THz artificial dispersion materials, polarization control and asymmetric transmission.     

Optical filter based on subtractive dispersion planar reflective gratings

We have successfully designed, fabricated, and tested an optical filter based on cascaded planar reflective gratings. The device uses a combination of two grating elements arranged in a subtractive dispersion configuration. The first grating demultiplexes a 300 nm wide band and drops optical channels at 1490 and 1550 nm, commonly used in passive optical networks. The second grating completely counter-balances the dispersion properties of the first grating and ultimately yields zero dispersion in the output waveguide. Such a configuration allows the transmission of optical signals though the device in an ultra-wide band spanning 1250-1410 nm. The filter was manufactured using an industry standard silica-on-silicon process which was augmented with grating facet formation and metallization. In spite of using low refractive index contrast waveguides (0.82%), the device had a remarkably low footprint of only 0.21 cm². Applications of the device in passive optical networks are discussed.     

光纤布喇格光栅的金属管封装与电调谐

本文用薄金属套管对光纤光栅进行了封装,并利用其进行了光纤布喇格光栅的电调谐实验.这种调谐方法保持了光纤光栅体积小的优点,操作简便,可远距离实现,光纤光栅的波长变化与电流的平方或电功率成正比.实验中用3.2A的电流获得了3nm的波长调谐,调谐速率约为0.59nm/W.     

3333lp/mm X射线透射光栅的研制

针对X射线透射光栅摄谱仪中的高线密度光栅,研究了采用电子束曝光和X射线曝光技术结合制作高线密度X射线透射光栅的工艺技术.首先利用电子束曝光和微电镀技术在镂空的薄膜上制备母光栅X射线掩模版,然后利用X射线曝光和微电镀技术小批量复制光栅.在国内首次完成了3333lp/mm X射线透射光栅的研制,栅线宽度为150nm,周期为300nm,金吸收体厚度为500nm.衍射效率标定的结果表明,该光栅的占空比合理、侧壁陡直,具有良好的色散特性,能够满足空间探测、同步辐射和变等离子诊断等多个领域的应用.     

复合金属光栅模式分离与高性能气体传感器应用

为实现近红外波段表面等离子体共振(SPR)模式的分裂和移动, 同时提高光栅基SPR传感器的品质因数, 提出了一种由双金属光栅构成的新型复合结构光栅, 并研究了其气体传感特性. 运用有限时域差分算法对该结构进行了数值模拟, 发现由复合金属光栅激发的SPR出现模式分裂的现象. 通过增大双金属光栅阵列间的相对位移改变原结构的对称性, 导致复合金属光栅分裂的SPR模式朝相反方向移动. 当相对位移量进一步增大到双光栅合并成新的单一光栅时, 随光栅结构对称性的恢复, 分裂的两共振模式最后又重新合并为一个模式. 如果待测物的折射率为1.01≤n_a≤1.05, 当相对位移量为0时, 基于复合光栅结构气体传感器的折射率灵敏度为1207.5 nm/RIU, 且品质因数达到1290.7; 当相对位移量为100 nm时, 与双共振模式对应的折射率灵敏度分别为1205.0 nm/RIU和1210.0 nm/RIU, 品质因数分别为1295.4和762.3. 因此, 复合光栅SPR传感器具有超高品质因数的性能, 使得它在生物化学传感领域中有巨大的应用潜力.     

Highly efficient tunable fiber Bragg grating filters using multilayer piezoelectric transducers

We realized a wavelength tunable optical filter based on a fiber Bragg grating using multilayer piezoelectric transducers (MLP). The Bragg wavelength of the filter can be easily tuned in proportion to an applied low DC voltage. The tuning range efficiency was as high as 0.2 nm/V. We realized a 10 nm Bragg wavelength shift by applying as low as 50 V to the MLP. The MLP was also used in a higher order dispersion equalizer which consists of a pair of nonlinearly chirped gratings. A zero dispersion wavelength shift of 7 nm was successfully realized for the equalizer.