共查询到19条相似文献,搜索用时 187 毫秒
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以碲玻璃为基质材料,设计了八边形双芯光子晶体光纤.应用全矢量有限元法和模式耦合基本理论分析了八边形双芯光子晶体光纤中结构参数对耦合长度特性的影响.计算结果表明:在波长1.55μm处,减小孔间距可明显减小耦合长度,但只略微改变相对耦合长度;增大空气孔及椭圆率可略微增大耦合长度,但可明显增大相对耦合长度.当相对耦合长度为1时,设计的偏振分束器性能较理想.在此基础上,通过调节结构参数,设计了一种较短传输长度、高带宽、高消光比的偏振分束器,当光纤长度为139μm时,X、Y方向偏振光即可实现分离,消光比达到最小值-53.46dB,且在波长1.49μm~1.61μm,即带宽为120nm范围内,消光比小于-20dB,与同类型的高消光比和极短长度双芯偏振分束器相比,其综合性能比较突出. 相似文献
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将五光子晶体单模波导平行、邻近放置构成定向耦合器,依据自映像原理,数值分析了输入光场对称入射时,该系统中光的传播行为.基于此结构,设计了1×3光分束器,其器件长度可短至14.26μm.仅仅通过对称地改变耦合区中两个介质柱的有效折射率,使光场在横向发生重新分布,便可实现输出能量的均分或自由分配.通过非对称地改变耦合区中的一个介质柱,可实现3个输出端的输出能量的自由分配.该光分束器具有微小尺寸和各输出端输出能量的比例可自由调制的特点,在未来集成光回路中具有广泛的应用价值. 相似文献
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太赫兹波技术和光子晶体技术相结合为设计太赫兹波功能器件提供了新的思路和方法.本文提出了一种基于二维光子晶体的双波长太赫兹波功分器.在光子晶体中引入由三个相互平行的单模波导形成的定向耦合型分束器和Y型结构的1×2型分束器,同时,在Y型结构的分支处分别引入两个介质柱.利用平面波展开法和定向耦合原理计算了在不同入射波频率下,耦合波导的耦合长度,并采用时域有限差分法对功分器的传输特性进行了模拟仿真分析.结果表明,在频率f1=1.0THz时,实现了端口1和端口2的能量均分输出;在频率f2=0.893THz时,通过非对称改变两个介质柱的折射率,可以实现端口3和端口4输出能量的自由分配. 相似文献
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光纤的能量传输特性及应用 总被引:5,自引:0,他引:5
着重分析了影响光纤传输能量以及光纤传输中造成能量损耗的因素。这些因素主要包括光纤材料、构造、光纤的折射率分布、光纤的长度和芯径、光纤的数值孔径和热效应以及耦合等。同时 ,结合激光二极管点火的实例 ,分析探讨了其背景和应用价值。结论是 :为了尽可能减少能量损耗、提高光纤输出的激光功率和激光功率密度 ,应当选取合适的激光工作波长、较小的光纤长度、较小的芯径和较小的数值孔径 ,应采用渐变折射率分布光纤 ,应减少弯曲与耦合 相似文献
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提出了一种基于ZnTe碲酸盐玻璃的单芯光子晶体光纤偏振分束器.在外侧包层纤芯对称位置引入缺陷孔,使缺陷模和纤芯基模发生耦合以实现光束分离.采用全矢量有限元法对所提出的单芯光子晶体光纤偏振分束器的特性进行研究,结果表明:该分束器可以实现1.3μm和1.55μm波长光的分离,并使光束沿X和Y偏振方向同时传播;当光纤长度为15mm时,1.3μm和1.55μm处的串扰值分别低至-45.1dB和-40.2dB,小于-20dB的带宽分别为44.2nm和67.1nm;在传输波长1.3μm和1.55μm处的损耗值为0.063dB和0.048dB;偏振分束器在具有低串扰值的同时,具有较低的限制损耗. 相似文献
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The power imbalance between different waveguide outputs is compensated by manipulating the dispersion of the guided propagation in the multimode interference (MMI) region. This is attainable using a tapered region at the beginning of the MMI region that has been verified through simulation and experiment. From this, the fabrication tolerance for the diameters of holes in a tapered 1×3 photonic crystal waveguide (PhCW) splitter is relaxed up to a range of at least 27 nm. The output power is well-balanced to within 1 dB. The effective bandwidth of the splitters shifts only around 13 nm, for a reduction of 10 nm in the diameter of the PhCW holes. The optimized component is an outstanding ultracompact 1×3 splitter for the photonic integrated circuit (PIC). 相似文献
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通过等频图分析并结合时域有限差分法模拟,在一个与偏振态无关的自准直光子晶体环形谐振腔中,研究发现当环形谐振腔内的光传输距离改变时,横电波(TE)和横磁波(TM)两种偏振态的光在通过环形谐振腔之后的输出将会随之变化并呈现出不同的周期性.通过选择适合的传输距离,实现了TE,TM自准直的情况下同时分束50%的结果,构成了一种基于光子晶体自准直环形谐振腔的全光均分束器.全光均分束器扩大了分束器的运用范围,也会在高密度集成光路中发挥重要的作用.
关键词:
光子晶体
环形谐振腔
自准直
分束器 相似文献
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光学谐振腔由于其高Q值特性,作为谐振式陀螺的核心元件,有望实现谐振式陀螺的小型化、集成化,但是非互易性噪声成为制约其精度提高的不利因素. 介绍了采用传统半导体工艺制备的盘型腔与熔融法拉制的锥形光纤组成的耦合系统. 当盘型腔在光纤锥区的不同位置进行耦合谐振时,将输入输出正/反对调,观察到输出透射谱发生偏差,谐振频率、耦合效率以及Q值均发生变化,即存在非互易性现象. 用Rsoft软件对锥形光纤倏逝场分布特性进行仿真,理论分析了非互易性产生的原因. 以此可抑制谐振式光学陀螺应用中由锥形光纤与谐振腔组成的耦合系统产生的非互易性噪声.
关键词:
光学谐振腔
锥形光纤
非互易性
谐振式陀螺 相似文献
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将多光子晶体单模波导平行、邻近放置构成定向耦合器. 依据自映像原理,数值分析了输入光场对称入射时,该系统中光的传播行为. 基于此结构,以三、四通道为例,设计了超微多路光分束器,并仅通过对称地改变耦合区中两个介质柱的有效折射率,使光场在横向发生重新分布,实现了输出能量的均分或自由分配. 和已报道结果相比,此调制方法更为简单易行而且效率更高,并可以推广到具有更多输出通道的光分束器中,在未来的集成光回路中具有广泛的应用价值.
关键词:
光子晶体波导
定向耦合器
分束器
能量均分 相似文献
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Somnath Ghosh R. K. Varshney Bishnu P. Pal Gérard Monnom 《Optical and Quantum Electronics》2010,42(1):1-14
Chirped cladding is proposed as a novel tailoring tool to simultaneously attain wider transmission window and reduced temporal
dispersion in an all-solid Bragg-like microstructured optical fiber as compared to its perfectly periodic cladding counterpart.
This design route for photonic bandgap microstructured fibers could be exploited as an additional degree of freedom for bandgap
engineering. A suitably chirped clad fiber could be gainfully exploited to deliver femto-second pulse with ultra wide bandwidth.
Further, generation of self-similar parabolic profile pulse is demonstrated by simulating propagation of an input Gaussian
pulse through a 2 m long sample of such a linearly tapered Bragg like fiber. 相似文献
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A literal model using geometric examination was formulated to calculate the optimum width and length of multimode interference structure used in the 1 × 2 power splitter and plot electric field intensity for input and each output signal. Designing and simulation of the wavelength response of 1 × 2 splitter using Tapered and MMI assisted structure. Mechanism on the critical geographical parameters like length and width of MMI structure, separation distance between output ports ‘S’, arm angle ‘α’ which give the optimum power and electric field intensity for the considered necessary wavelength. Finite difference beam propagation methods have been used to simulate the conventional and tapered MMI device behaviour. 相似文献
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We report the possibility of using tapered microstructured fibers to improve the coupling efficiency from a standard single-mode fiber to a photonic crystal waveguide. The tapered microstructured fiber allows for the reduction of the mode mismatch between the output of the standard fiber and the input of the waveguide while maintaining single-mode guidance, which results in an enhanced coupling efficiency. Numerical simulations are conducted in order to optimize the cross section of the microstructured fiber as well as the taper profile. An improvement of more than 4 dB is obtained compared to non-tapered fibers. For further improvement, an elliptical-core tapered microstructured fiber is analyzed. The effect of misalignment between the tapered microstructured fiber and the waveguide is also studied. 相似文献