共查询到19条相似文献,搜索用时 62 毫秒
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提出了一种光纤横截面折射率变化呈旋转非对称变化的长周期光纤光栅(R-LPFG) 结构,并利用多层圆波导理论和横截面折射率离散分析方法,结合模式耦合方程组和数值求解方法理论分析了这种光栅的模式耦合特征.理论分析表明R-LPFG纤芯基模主要与一阶非对称包层模发生耦合,当光栅旋转度逐渐变大时,R-LPFG基模会与一阶非对称包层模的奇模和偶模同时发生耦合,这就会使原来单一的谐振峰逐渐分裂成双峰,这是常规光栅类型所不具有的透射谱特征.由于R-LPFG的双峰来自同一对耦合模式,它们对温度的响应很相似,因此可利用双峰间距来进行无需温度补偿的扭曲、应变等物理量的测量.最后利用高频CO2激光脉冲写入法制作了这种光栅,并实验研究了这类光栅的传输谱演变特征,实验结果和理论分析一致.可以预见,这类光栅在光纤传感或通信中将具有较大的潜在应用价值. 相似文献
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提出了一种光纤横截面折射率变化呈旋转非对称变化的长周期光纤光栅(R-LPFG) 结构,并利用多层圆波导理论和横截面折射率离散分析方法,结合模式耦合方程组和数值求解方法理论分析了这种光栅的模式耦合特征.理论分析表明R-LPFG纤芯基模主要与一阶非对称包层模发生耦合,当光栅旋转度逐渐变大时,R-LPFG基模会与一阶非对称包层模的奇模和偶模同时发生耦合,这就会使原来单一的谐振峰逐渐分裂成双峰,这是常规光栅类型所不具有的透射谱特征.由于R-LPFG的双峰来自同一对耦合模式,它们对温度的响应很相似,因此可利用双峰间
关键词:
光纤传感
光纤光栅
2激光')" href="#">CO2激光
旋转折变 相似文献
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长周期光纤光栅的折射率敏感特性 总被引:1,自引:0,他引:1
利用光波导的耦合模理论分析了长周期光纤光栅(LPFG)的折射率传感特性,给出了LPFG 的谐振波长相对于环境折射率变化时的漂移量解析表达式.对 LPFG 的折射率传感特性进行了数值模拟.结果表明:在光栅周期不变的情况下,当包层折射率小于且接近外界环境折射率时,波长的漂移量增大,且对应的模次越高、包层半径越小、包层折射率越小,波长漂移量越大,即 LPFG 对应于外界折射率传感灵敏度得到显著提高;当外界环境折射率大于包层折射率时,光栅的谐振波长将近似不变. 相似文献
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提出一种具有温度自校准功能的光纤折射率(RI)传感器,传感头结构由2段很短的多模光纤(MMF)之间夹熔一段对折射率不敏感的光纤布拉格光栅(FBG)构成,传感头总长度为14 mm,FBG可以为折射率测量提供良好的温度校准功能。实验结果证明,该传感器的折射率灵敏度为126 nm。其干涉光谱共振波长的温度灵敏度为35.09 pm/℃,用于温度校准的FBG的温度灵敏度为11.14 pm/℃。相比于普通的折射率传感器,这种具有温度自校准功能的折射率传感器具有良好的实用前景。 相似文献
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理论分析了利用高频CO2激光脉冲在不同类型光纤中写入长周期光纤光栅(LPFG)时光纤包层和纤芯发生折射率改变的机理和计算方法.结果表明,残余应力释放、快速固化、光纤致密化和熔融变形是高频CO2激光能成栅的主要原因,但采用不同的写入方法、不同的激光写入能量在不同的光纤类型上制作光栅时各种机理的重要性不同.利用长周期光纤光栅对构成的M-Z干涉仪实验测量了高频CO2激光以不同辐射能量在光纤不同作用位置所引起的光纤纤芯或包层的折射率平均变化量,并通过实际制作光栅的过程来初步验证光纤折射率的变化情况.CO2激光与光纤相互作用机理的分析和实验研究为利用这种方法制作折变型全光纤器件提供了实验制作的基础和完善工艺的方法.
关键词:
光纤器件
长周期光纤光栅
2激光脉冲')" href="#">CO2激光脉冲
折变 相似文献
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We demonstrate a scheme for coherently induced grating based on a mixture of two three-level atomic species interacting with two standing-wave fields. As a result of interaction between the absorptive and amplified Raman resonances, the refractive index of the medium can be enhanced and modulated periodically. Then a sinusoidal grating, which can diffract the probe field into high-order directions, is coherently formed in the medium. The proposed scheme is theoretically investigated in a mixture of atomic isotopes of rubidium. The results show that the diffraction efficiency depends strongly on the two two-photon detunings of the two Raman transitions and the intensities of the two driving standing-wave fields.The proposed electromagnetically induced grating scheme may be applied to the all-optical switching and beam splitting in optical networking and communication. 相似文献
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By introducing a four-layer step-index waveguide modeling, the characteristics of long-period fiber grating (LPFG) with an nm-thick film overlay, which has higher refractive index than that of fiber cladding are investigated in detail. The influence of both the overlay thickness and refractive index on the tuning ability of LPFG is analyzed. The numerical results demonstrate that spectral response of LPFG is divided into three distinct regions as the overlay deposition increases and the shift of resonant wavelength is drastic in some special thickness range. In conjunction with higher-order cladding mode coupling and fiber cladding etching, the sensitivity of LPFG to the overlay refractive index is enhanced significantly and over 120 nm resonant wavelength tunable range is achieved. 相似文献
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Design of a coated thinly clad chalcogenide long-period fiber grating refractive index sensor based on dual-peak resonance near the phase matching turning point 下载免费PDF全文
A novel method for designing chalcogenide long-period fiber grating (LPFG) sensors based on the dual-peak resonance effect of the LPFG near the phase matching turning point (PMTP) is presented. Refractive index sensing in a high-refractive-index chalcogenide fiber is achieved with a coated thinly clad film. The dual-peak resonant characteristics near the PMTP and the refractive index sensing properties of the LPFG are analyzed first by the phase-matching condition of the LPFG. The effects of film parameters and cladding radius on the sensitivity of refractive index sensing are further discussed. The sensor is optimized by selecting the appropriate film parameters and cladding radius. Simulation results show that the ambient refractive index sensitivity of a dual-peak coated thinly clad chalcogenide LPFG at the PMTP can be 2400 nm/RIU, which is significantly higher than that of non-optimized gratings. It has great application potential in the field of chemical sensing and biosensors. 相似文献
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本文设计了一种单端面长周期光栅透射模式折射率传感器。首先,将2×2单模光纤耦合器输入端的一个光纤接头与光源相连接、输出端的两个光纤接头分别与光谱分析仪和长周期光栅的一个光纤接头相连接。然后,在包含长周期光栅的光纤另一个端面溅射反射银膜。最后,以一系列不同折射率的甘油水溶液为待测液体介质研究了直接透射模式与单端面镀银膜模式下长周期光栅的响应光谱的异同。实验结果表明:单端面镀银膜的长周期光栅的响应光谱仍然以透射谱的形式出现。对于同一种液体,单端面镀银膜的长周期光栅与直接透射模式的长周期光栅的响应光谱有着近乎相同的谐振波长值,但它们的光损耗存在一定的差异。在0~80%的甘油溶液中,直接透射模式下的光损耗从-12.92 dB变为-16.28 dB,再逐渐变到-13.22 dB;单端面镀银膜模式下的光损耗从-13.13 dB变为-13.74 dB,再逐渐变到-11.45dB。与直接透射模式相比,单端面镀银膜的长周期光栅的相对光损耗与甘油浓度的线性关系更加良好。本研究设计的长周期光栅测量系统采用单端面探头的方式检测环境介质,因而在测量中操作更加灵活方便,非常适合于远距离、恶劣环境或深层液体环境中的折射率测量。 相似文献
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亚波长直径微纳光纤强倏逝场传输的光学特性,使其对周围介质折射率的变化具有极高的灵敏度.本文提出一种基于微纳尺度光纤布拉格光栅(MNFBG)的折射率传感器,结合微纳光纤倏逝场传输和光纤布拉格光栅(FBG)强波长选择的特性来实现高精度折射率传感,对其制备可行性进行了讨论.论文中对MNFBG折射率传感机理进行了深入的理论分析,并使用OptiGrating软件进行了数值模拟,模拟数据显示MNFBG折射率测量的灵敏度随着光纤半径的减小而增加,其中光纤半径为400 nm的MNFBG灵敏度可达到993 nm/RIU,相比于包层蚀刻的FBG灵敏度增加了170倍,说明MNFBG对发展微型化、高灵敏度折射率传感器具有良好的应用前景.
关键词:
微纳光纤
光纤布拉格光栅
折射率传感 相似文献
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R. Zawisza T. Eftimov P. Mikulic Y. Chinifooroshan A. Celebańska W.J. Bock L.R. Jaroszewicz 《Opto-Electronics Review》2018,26(1):24-28
An interferometric structure based on a Dual-Resonance Long-Period Grating (DRLPG) within a Fiber Loop Mirror (FLM) is presented in this paper. Its purpose is to measure the refractive index (RI) of liquid analytes. The grating is the RI sensing probe, while the FLM serves as a band-pass filter. Due to the high extinction ratio of the FLM, amplitude measurements can be obtained, allowing implementation of the differential interrogation method to establish the sensitivity of the device. The use of a polarization controller makes it possible to fine-tune the interferometric peaks with respect to the two notches of the DRLPG. Precisely aligned configuration produces a maximum sensitivity of 3871.5?dB/RIU within the RI range of 1.3333 up to 1.3419 with linear sensor response. 相似文献