基于级联光纤光栅的双模外腔半导体激光器的实验研究

实现了使用两个级联的光纤Bragg光栅的外腔半导体激光器的双模运转.两个模的峰值波长取决于光纤Bragg光栅的峰值反射波长,分别为1531.5nm与1549.4nm.注入电流为53mA时,两模峰值功率达到均衡为0.5mW,边模抑制比为27dB.     

用布拉格光纤光栅制作啁啾光纤光栅

介绍了一种用布拉格光纤光栅制作啁啾光纤光栅的方法。采用氢氟酸腐蚀布拉格光纤光栅, 使光栅的横截面沿光栅轴向逐渐变小, 然后对光栅施加１．５０ Ｎ的拉力, 在光栅轴向建立应变梯度, 制作出长１５ ｍ ｍ 、峰值反射率达９２％ 、反射半高宽为５ ｎｍ 的啁啾光纤光栅。     

含耐高温涂覆层长周期光纤光栅的温度特性研究

利用逐点写入法在耐高温光纤中用红外飞秒激光直接写入了长周期光纤光栅,研究了光栅的高温温度特性,并做了理论分析.通过对含耐高温涂覆层的长周期光纤光栅进行20 ℃~300 ℃的温度传感实验,结果表明：在高温段光栅的谐振波长漂移量与温度之间仍能保持大的灵敏度（0.060 5 nm/℃）和好的线性度,且光纤耐高温涂覆层不受破坏,光纤耐高温涂覆在高温下不会出现碳化现象,光栅传感性能良好.实验证明该方法制作的光栅适合于长期在高温环境下使用,应用价值巨大.     

基于级联光纤Bragg光栅的外腔半导体激光器三波长同时激射

实现了使用3个级联的光纤Bragg光栅外腔半导体激光器3波长同时激射.3条谱线的峰值波长取决于光纤Bragg光栅的峰值反射波长,分别为1 531.5 nm、1 549.4 nm与1 554.8 nm.注入电流为52 mA时,激光器总输出功率为1 mW.该激光器的主要优点包括,由于输出波长被锁定在光纤Bragg光栅的Bragg波长上,因此输出波长稳定,谱线窄,成本低.可应用于多波长干涉测量以及全光通信等领域中.     

多模光纤光栅温度传感特性的实验研究

利用氢敏化处理的多模光纤制作了多模光纤光栅,并对多模光纤光栅的温度传感特性进行了实验研究与理论分析,表明这种光栅三个反射峰的布拉格波长随温度变化均呈现出良好的线性关系,并且重复性相当好,同一光栅的各反射峰的理论温度灵敏度系数都等于0．01nm／℃,实验测得的温度灵敏度系数为0．0098nm／℃或0．0099nm／℃,与理论分析相当吻合,这些特性与单模光纤光栅的温度传感特性接近相同。因此可以用多模光纤光栅代替单模光纤光栅开发光纤光栅传感器,以降低成本;这一实验结果还可以作为对多模光纤光栅进一步深入研究的参考。     

Grating-Outcoupled Radiation in Second-Order Fiber Bragg Gratings

Abstract

The experimental results of the radiation for second-order fiber Bragg gratings, which are made of a single-mode photosensitive fiber (PS-1500; Fiber-Core Corp.) and a single-mode fiber (SMF-28; Corning Inc.), by a phase mask writing fabrication technique are explored. For PS-1500 fiber Bragg gratings, the maximum radiation efficiency of ?23.5 dB at resonance λ = 1,539.34 nm with a very narrow bandwidth (about 0.02 nm) are measured from a 10-mm-diameter photo-detector, while for SMF-28 fiber Bragg gratings, the maximum radiation efficiency is ?34.6 dB (λ = 1,538.03 nm) with a bandwidth of 0.06 nm. The total efficiencies of the radiation are about ?16.8 dB for PS-1500 fiber Bragg gratings and ?28.1 dB for SMF-28 fiber Bragg gratings.     

三角形大带宽反射光谱光纤光栅的设计和制备

反射谱具有三角形形状的光纤光栅在光纤传感等领域中具有重要的应用前景。利用遗传算法设计出了产生三角形光谱分布的光纤光栅的耦合系数沿光纤的分布。计算表明,三角形光谱光纤光栅是可以实现的,其反射带宽可以通过光栅的啁啾量进行调节,常周期的三角光栅反射带宽小,变周期的三角光栅反射带宽大,其带宽同其啁啾量大致相等。实验中,采用光束扫描法制备了反射底宽为0．77nm三角形光谱的光纤光栅。     

用于光纤光栅解调的波长敏感光纤耦合器

为了拓宽光纤耦合器的使用范围,开发光纤耦合器的新功能,采用熔锥技术制作波长敏感耦合器,该耦合器在分光的同时对波长敏感。通过耦合理论验证实验结果,实验数据与理论值相符合。实验中得到波长灵敏度最大值为17.86%/nm的耦合器。采用拉锥工艺制作波长敏感耦合器工艺简单,耦合比峰值对应波长控制易于实现。该耦合器可用于光纤光栅布拉格波长漂移解调。令待解调光纤光栅布拉格波长与耦合器波长灵敏度最大值对应的波长一致,当波长发生漂移时,耦合器输出耦合比发生变化。自制的波长敏感耦合器实现了对布拉格波长为1566.71 nm光纤光栅波长漂移的解调,波长漂移1.80 nm,耦合比变化20.34%。此种解调方式具有光路简单,易于与光纤匹配的优点,可以应用在大型建筑中光纤光栅的健康监测。     

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。     

Dispersion Compensators Based on Overlaped Linearly Chirped Fiber Gratings for DWDM Systems

1　Ｉｎｔｒｏｄｕｃｔｉｏｎ　　ＴｈｅｒｅｉｓａｇｒｅａｔｄｅａｌｏｆｉｎｔｅｒｅｓｔｉｎｆｉｂｅｒＢｒａｇｇｇｒａｔｉｎｇｓｄｕｅｔｏｔｈｅｉｒｍａｎｙｉｍｐｏｒｔａｎｔａｐｐｌｉｃａｔｉｏｎｓｉｎｔｈｅｆｉｅｌｄｏｆｔｅｌｅｃｏｍｍｕｎｉｃａｔｉｏｎｓａｎｄｆｉｂｅｒｓｅｎｓｏｒｓ .ＢｅｃａｕｓｅｆｉｂｅｒＢｒａｇｇｇｒａｔｉｎｇｓｅｘｈｉｂｉｔｄｉｓｐｅｒｓｉｏｎｂｏｔｈｉｎｒｅｆｌｅｃｔｉｏｎ ,ｅｓｐｅｃｉａｌｌｙｗｈｅｎｔｈｅ ｇｒａｔｉｎｇｉｓｃｈｉｒｐｅｄ[1] ,ａｎｄｉｎｔｒａｎｓｍ…     

Dispersion Compensators Based on Overlaped Linearly Chirped Fiber Gratings for DWDM Systems

By introducing a convergent lens in the phase mask setup and by tilting appropriately the fiber from the phase mask, a linearly chirped fiber grating with an appropriate chirp can be obtained conveniently. Using this method, two groups of fiber gratings, each of them is composed of 8 overlaped linearly chirped fiber gratings but with different center reflection wavelength separations (～0.8 nm and ～1.6 nm, respectively) are fabricated. Experimental results show that, the compensators based on the two groups of fiber gratings can be used to compensate for the dispersion of 8×2.5 Gb/s transmission over 100 km of standard single-mode fiber for multiple channels in optical time-division multiplexing (OTDM) and densed wavelength division multiplexing (DWDM).     

双带通啁啾光纤光栅光谱特性仿真及分析

针对啁啾光纤光栅的带通滤波特性,设计了纤芯/包层复合结构的啁啾光纤光栅滤波器.基于光纤耦合模和传输矩阵理论及坐标变换方法,对其光谱特性进行仿真分析,验证了该光栅的双带通滤波特性;对周期为536、537、538nm,长度为8、10、12mm,折射率调试深度为0.0002、0.0003、0.0004,啁啾系数为0.05、0...     

光致折变布拉格光栅实验研究

本文介绍了 2 48nm、Kr F准分子激光经过石英相位掩膜版的空间调制 ,在载氢增敏处理过的通信光纤与 B/Ge光纤上分别写入光致折变布拉格光栅的实验研究。经实验测定 ,在光栅布拉格波长上 (λH2 =15 46 .45 5 4nm ,λB/Ge=15 45 .15 5 nm) ,两种光栅反射率均大于 99% ,3d B带宽分别为 0 .12 9nm和 0 .182 nm。经比较 ,B/ Ge光纤比氢载光纤具有更好的光敏性和热稳定性     

基于偏振保持掺Er3+光纤的高稳定性单波长光纤激光器

研制出光敏偏振保持掺Er³⁺光纤,通过在这种光纤上紫外写入三个光纤光栅,形成对抽运激光高转化效率的谐振腔.在输出功率为23.617dBm、工作波长为976nm的激光抽运下,得到均值功率为9.20dBm、均值中心波长为1554.554nm的单波长激光输出.在室温下800min（约13.3h）的测量时间内,其输出功率的波动为±0.05dB,中心工作波长的波动为±0.0015nm. 关键词： 光纤激光器 3+光纤')" href="#">偏振保持掺Er³⁺光纤 光纤Bragg光栅     

大功率多波长可转换双包层光纤激光器

在多模掺镱双包层光纤上,利用相位掩模法直接写制Bragg光栅作为激光器后腔镜,得到多波长激光输出.在室温下,通过调节偏振控制器可以得到稳定的单波长及多波长的激光输出,输出波长范围在1 056～1 061 nm,线宽均小于0.02 nm.在25 W的976 nm激光泵浦下,激光器得到功率为6 W的多波长输出.     

Highly sensitive cladding-etched arc-induced long-period fiber gratings for refractive index sensing

We have investigated the effects of cladding etching in arc-induced long-period fiber gratings. Comparing the position of the resonant wavelengths at each diameter with the corresponding theoretical dispersion curves of effective refractive index, it is found that some of the resonances show a better match with anti-symmetrical cladding modes, while others with symmetrical cladding modes. Etching the cladding diameter to ∼39 μm, results in coupling to a high-order cladding mode that is very sensitive to changes in the ambient refractive index. The resonant peak shifts remarkably (∼230 nm) toward shorter wavelengths as the external refractive index increases. This sensitivity is higher than any previously reported in arc-induced long-period fiber gratings.     

多波长啁啾叠栅的矩阵分析

在分析多波长啁啾叠栅特征的基础上,提出了多波长啁啾叠栅的矩阵分析模型,采用矩阵分析模型对4波长和8波长啁啾叠栅的反射谱特性进行了理论分析,数值分析结果与实验结果非常一致.还首次数值模拟了波长间隔0.8 nm的16波长啁啾叠栅.此方法对多波长啁啾叠栅的设计和制作具有参考价值.     

Pump-Induced Lasing Wavelength Shift in Er/Yb Codoped Fiber Grating Lasers

１ＩｎｔｒｏｄｕｃｔｉｏｎＥｒｂｉｕｍ／Ｙｔｅｒｂｉｕｍｃｏｄｏｐｅｄｆｉｂｅｒｓａｒｅｉｄｅａｌｇａｉｎｍｅｄｉａｆｏｒｃｏｎｓｔｒｕｃｔｉｎｇｓｉｎｇｌｅｆｒｅｑｕｅｎｃｙｆｉｂｅｒｌａｓｅｒｓ．Ｔｈｅｉｒｂｒｏａｄａｂｓｏｒｐｔｉｏｎｂａｎｄ...     

Birefringent azopolymer long period fiber gratings induced by 532 nm polarized laser

Based on the photoinduced birefringence in azo materials, the model of the birefringent long period fiber gratings (BLPFGs) has been proposed and the transmission of such birefringent fiber gratings was further simulated by the coupled mode theory. In order to obtain the optimum condition for making birefringent azopolymer optical fiber (APOF) gratings the photoinduced birefringence of azo dye and methyl methacrylate (MMA) copolymers was systematically studied. After photosensitivity study of azo samples, using Teflon technique, azo dye containing single mode polymer optical fiber (POF) was fabricated. Finally, BLPFGs can be fabricated in azopolymer fiber using polarized 532 nm laser. A 120 μm LPFG with a 50% duty cycle has been successfully written within the core of the fiber with 532 nm laser by an amplitude mask method. Under polarized microphotography, the grating was observed when the optical axis was set at 45° with the direction of the first polarizing lens of the polarization microscope.     

光纤耦合模理论及其在光纤布拉格光栅上的应用

将正确的光纤中的正交关系应用于微扰耦合模理论得到了光纤中的微扰耦合模方程；并将其应用于光纤布拉格光栅，得到了一种新耦合模方程。该方程中作为标志性特性的耦合系数与其它理论中的耦合系数都不相同。讨论了方程的解，得到了峰值反射率与布拉格波长、光栅长度之间的简单关系式。用光纤布拉格光栅进行了实验，理论和实验结果符合得很好。