高双折射低色散光子晶体光纤设计

为了高效传输太赫兹(Terahertz,THz)波并促进太赫兹的实际应用.提出了一种具有高双折射,低色散特性的太赫兹光子晶体光纤(Photonic Crystal Fiber,PCF).利用全矢量有限元法对所提出的PCF 结构进行数值仿真,分析了结构参数与双折射以及色散的关系.仿真结果表明,该光纤在0.9～1.3 TH...     

八角晶格光子晶体光纤的损耗特性分析

应用多极法对O-PCF的损耗进行了计算和分析,并与H-PCF进行了比较,发现相同空气填充率下,O-PCF的损耗小于H-PCF的损耗,O-PCF在能获得更大有效模式面积的同时,在损耗特性方面也更具优势;研究了包层空气孔层数、孔直径和孔间距等在1.33 μm和1.55μm处对损耗的影响,得到了损耗随各结构参数变化的规律,并总结了获得低损耗大模面积O-PCF的一般方法.     

新型光子晶体光纤近零平坦色散的研究

文章作者设计了一种新型的光子晶体光纤(PCF),在纤芯引入了一个小空气孔形成缺陷,并改变第一层空气孔的直径.采用平面波法研究了该PCF的色散特性,结果表明,该光纤能够得到比传统的PCF更低、更平坦的色散曲线;通过优化该光纤的结构参数,可以设计在1 350～2 010 nm波长范围内近于零的平坦色散PCF,其色散变化△D＜0.5 ps/(km·nm),在1 320～2 040 nm波长范围内色散斜率变化△D<,slope>＜0.02 ps/(km·nm<'2>).     

Design for photonic crystal fibers with high nonlinearity and flattened dispersion for self-frequency shift of Raman soliton

A new concept of photonic crystal fiber (PCF) with high nonlinearity and flattened dispersion was designed. The PCF structure is indeed a hexagon lattice. The bigger air holes in the outer rings are used to confine the light field into the core region for enhancing the nonlinearity. The flattened dispersion can be achieved by adjusting the diameters of six smaller air holes in the first ring, and six micro air holes are inserted between smaller air holes for higher nonlinearity and the better flattened dispersion. By optimizing the size of the smaller and micro holes, the PCF can reach to high nonlinearity of 23.3 W⁻¹ · km⁻¹ and the low dispersion of 51.32 ps/(nm·km) with the fluctuation range of 0.98 ps/(nm·km), which is within the wavelength range of 1 400 nm to 1 900 nm. The designed PCF can be used in important applications in realizing the Raman soliton self-frequency shift (RSSFS).     

Anomalous dispersion in photonic crystal fiber

We describe the measured group-velocity dispersion characteristics of several air-silica photonic crystal fibers with anomalous group-velocity dispersion at visible and near-infrared wavelengths. The values measured over a broad spectral range are compared to those predicted for an isolated strand of silica surrounded by air. We demonstrate a strictly single-mode fiber which has zero dispersion at a wavelength of 700 mm. These fibers are significant for the generation of solitons and supercontinua using ultrashort pulse sources     

模间色散为零的双芯光子晶体光纤

设计一种在短波长处可以实现零模间色散的双芯光子晶体光纤,该光纤的包层气孔直径具有渐变结构。利用全矢量有限元法进行分析,得到光纤耦合系数、模间色散及走离距离特性随传输频率和结构参数的变化曲线。数值分析结果表明,可以通过调节双芯间小孔的直径,灵活控制耦合系数的变化。在特定的传输频率处,模间色散存在过零点。且双芯间小孔的直径越大,模间色散过零点所在的传输频率越低。当模间色散为零时,可以完全消除模式间相位不匹配导致的脉冲失真,从而实现能量的完全交换。     

八角格子光子晶体光纤模式和色散特性研究

文章基于带有各向异性完全匹配层(PML)吸收边界条件的紧凑二维频域有限差分法对八角格子光子晶体光纤(O-PCF)的模式和色散特性进行了研究.利用有效面积法分析了八角格子和六角格子光子晶体光纤(H-PCF)的基模和多模截止特性,得到非限制模、基模及多模的相图,比较发现,填充率和空气孔间距相同时,O-PCF的单模运转区域宽于H-PCF,更易用于色散补偿.     

A novel design for dispersion compensating photonic crystal fiber Raman amplifier

This letter presents a novel design for dispersion compensating photonic crystal fiber (DCPCF) which shows inherently flattened high Raman gain of 19 dB (/spl plusmn/1.2-dB gain ripple) over 30-nm bandwidth. The proposed design module has been simulated through an efficient full-vectorial finite element method. The designed DCPCF has a high negative dispersion coefficient (-200 to -250 ps/nm/km) over C-band wavelength (1530-1568 nm). The proposed fiber module of 5.2-km length not only compensates the accumulated dispersion in conventional single-mode fiber (SMF-28) but also compensates for the dispersion slope. Hence, the designed DCPCF module acts as the gain-flattened Raman amplifier and dispersion compensator.     

非对称光子晶体光纤中的双折射和色散

采用矢量电磁波多极子方法,对两种类型的非对称光子晶体光纤——小微孔对称性破缺光纤和大微孔对称性破缺光纤,进行数值计算和模拟研究,得出了非对称光子晶体光纤能实现较高双折射,其拍长可达1mm量级的结论。此外还分析了小微孔对称性破缺光纤的色散,并和实验结果进行了比较,两者较为一致。     

Photonic crystal fiber with novel dispersion properties

Our recent research on designing microstruc-tured fiber with novel dispersion properties is reported in this paper. Two kinds ofphotonic crystal fibers (PCFs) are introduced first. One is the highly nonlinear PCF with broadband nearly zero flatten dispersion. With introducing the germanium-doped (Ge-doped) core into highly non-linear PCF and optimizing the diameters of the first two inner rings of air holes, a new structure of highly non-linear PCF was designed with the nonlinear coefficient up to 47 W-1·km-1 at the wavelength 1.55 μm and nearly zero flattened dispersion of ±0.5 ps/(km·nm) in telecom-munication window (1460-1625nm). Another is the highly negative PCF with a ring of fluorin-doped (F-doped) rods to form its outer ring core while pure silica rods to form its inner core. The peak dispersion - 1064 ps/(km·nm) in 8 nm full width at half maximum (FWHM) wavelength range and -365ps/(km·nm) in 20nm (FWHM) wavelength range can be reached by adjusting the structure parameters. Then, our recent research on the fabrication of PCFs is reported. Effects of draw parameters such as drawing temperature, feed speed, and furnace temperature on the geometry of the final photonic crystal fiber are investigated.     

光子晶体光纤色散补偿研究

从光脉冲在光纤中的传输过程分析着手,在理论和数值模拟两方面研究了光子晶体光纤的色散补偿特性作用。结果表明,利用光子晶体光纤进行色散补偿时,光子晶体光纤要选择合适的二阶色散系数,同时脉冲的输入峰值功率对其色散补偿也有影响,为保证补偿后脉冲的质量,补偿用光纤的长度尽量小。     

高双折射类椭圆纤芯光子晶体光纤设计与分析

为了改善传统光纤灵敏度低、损耗高和非线性效应不易控制的问题,设计一种新型高双折射、低损耗和高非线性的类椭圆纤芯光子晶体光纤(PCF)结构。基于全矢量有限元法,通过COMSOL分析研究了光纤端面的空气孔直径和位置对双折射、限制损耗、模场特性和非线性等特性的影响。仿真结果表明:所设计的PCF结构在波长为1.550μm处的双折射率达1.918×10^-3,x和y极化偏振方向的限制损耗分别为Lcx=1.6×10^-3dB/km和Lcy=8.0×10^-4dB/km,非线性系数达到9.4 km^-1W^-1,且满足单模传输,实现了高质量、高精度的光信号传输与传感。     

A single mode ultra flat high negative residual dispersion compensating photonic crystal fiber

In this paper, a single mode photonic crystal fiber based on hexagonal architecture is numerically demonstrated for the purpose of residual dispersion compensation in the wavelength range of 980–1580 nm. The designed fiber offers ultraflattened negative dispersion in the near-infrared to most widely used S to L wavelength bands and average dispersion of about −138 ps/(nm km) with an absolute dispersion variation of 12 ps/(nm km). Besides, the proposed fiber successfully operates as a single mode in the entire band of interest. Moreover, to check the dispersion accuracy, sensitivity of the fiber dispersion properties to a ±1–5% variation in the optimum parameters is studied for practical conditions.     

微结构芯光子晶体光纤色散特性的研究

在双包层近零色散平坦光子晶体光纤中引入微结构后,利用多极法对新的光子晶体光纤结构进行了数值模拟.其中在包层结构参数不变的前提下,研究了纤芯中微结构的结构参数变化对色散特性的影响.研究结果表明:通过优化纤芯结构参数,在不改变色散平坦度和色散平坦带宽的情况下,实现了色散曲线的整体下移,进而达到正常色散.     

Analysis of a realistic and idealized dispersion compensating photonic crystal fiber Raman amplifier

In the present paper, the highly efficient Raman amplification properties of a realistic and idealized dispersion compensating photonic crystal fiber (DCPCF) are described numerically. We have used an accurate full-vectorial finite element modal solver with hybrid curvilinear edge/nodal elements and anisotropic perfectly matched layers for an accurate modal characterization of the realistic as well as idealized DCPCF. A good agreement is observed between numerically evaluated and experimentally [P.J. Roberts, B.J. Mangan, H. Sabert, F. Couny, et al., J. Opt. Fiber Commun. Rep. 2 (2005) 435–461] measured dispersion values. A high peak Raman gain efficiency of 10.5 W⁻¹ km⁻¹ is obtained at 13.1 THz frequency shift for a 1455 nm depolarized pump. A DCPCF module of 1-km length can compensate for the dispersion accumulated over 70-km of conventional single mode fiber link with a residual dispersion of ±50 ps/nm and can provide an average gain of 7.6 dB with ±0.9 dB gain ripples over C-band.     

六角芯光子晶体光纤色散补偿特性研究

利用多极法的软件包对六角芯光子晶体光纤的色散补偿进行了数值模拟与分析,研究发现通过改变第一包层空气孔直径dO和空气孔间距A,可以灵活设计波长在1.55μm附近具有高色散值、负色散斜率和在短波长内单模传输的色散补偿型光纤.数值模拟和分析表明该光子晶体光纤在色散补偿型光纤方面具有广泛的应用前景.     

一种双包层低损耗色散平坦光子晶体光纤

借助多极法对具有双包层、双孔间距结构光子晶体光纤的色散特性,限制损耗,模场面积进行数值模拟,研究调整内外包层参数对色散和损耗的影响.通过优化结构参数,设计了可以在1.29～1.82μm的波长范围内实现±0.5ps/(km·nm)低色散值的色散平坦光子晶体光纤,其在λ=1.55μm处,限制损耗为2.2×10-3dB/km...     

低损耗平坦零色散光子晶体光纤的研究

设计了一种波长在800nm处具有低损耗平坦零色散特性的光子晶体光纤结构,应用多极法研究了结构参量空气孔直径d、孔距A对色散特性的影响和最外层空气孔直径对损耗的影响.该结构光纤在771 ～831nm波长范围内色散绝对值小于2ps/(nm·km),800nm处损耗为0.72dB/km.     

光子晶体光纤色散特性与结构关系的研究

利用基于多极法的数值模拟软件包对光子晶体光纤色散特性进行数值模拟和分析,发现通过改变包层空气孔直径d和空气孔间距A可以有效地调节光子晶体光纤的色散特性,即短波长零色散、近零超平坦色散和大负色散,得到了三种色散特性随光纤结构变化而变化的规律.