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We have proposed a novel kind of photonic crystal fiber which contains two asymmetric cores. The bireti'ingence and the dispersion are numerically analyzed based on finite element method when the size of the air holes and the pitch of two adjacent air holes are changed. It is shown that the proposed photonic crystal fiber has high birefringence up to the order of 10-2 and double-zero dispersion points are at the wavelengths of 1310 nm and 800 rim, simultaneously. At the same time, the normalized power and the extinction ratios of the proposed photonic crystal fiber have been simulated. It is demonstrated that, at the wavelength of 1310 rim, the x-polarized mode and the y-polarized mode are separated when the propagation distance is 2.481 ram.  相似文献   
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李建设  李曙光  赵原源  刘强  范振凯  王光耀 《物理学报》2016,65(21):214201-214201
采用可以减小纤芯面积的小气孔设计方案巧妙设计并成功拉制了一根高非线性的单零色散微结构光纤.利用有限元法模拟并计算得到了该光纤的基模有效折射率、色散系数和非线性系数等基本属性随波长的变化关系,然后利用四波混频的有效相位失配方程模拟了其相位失配曲线.模拟表明,在该光纤中可以同时发生两组四波混频.在位于微结构光纤的正常色散区的0.800,0.810和0.820μm三个波长处,分别采用不同的功率抽运,在实验上都非常明显地观察到了分列于抽运波长两侧的四个增益波带的产生.经与相位失配曲线比较,发现它们满足相位匹配条件,从而证明了两组四波混频过程的同时发生.实验结果与理论预言符合得很好.发生在正常色散区的四波混频效应的产生可归结于负的四阶色散对相位匹配过程的贡献.本文研究可对微结构光纤的结构设计和基于四波混频的多波长转移技术的发展提供经验与借鉴,同时也对非常见波段激光器和宽带光源的开发具有参考意义.  相似文献   
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由于InGaN材料的禁带宽度调节范围大,热稳定性好,化学性质稳定,因此在微电子、光电子和热电领域的高温区有良好的应用前景.基于Callaway导热系数模型从理论上计算了体材料和薄膜材料InGaN的导热系数,分析了温度、In组分和边界尺寸对InGaN导热系数的影响.研究结果表明,温度大于100 K时,不同组分的InGaN材料导热系数随温度的上升而下降,300 K时,体材料In0.1Ga09N的热导系数为90.15 W·m-1·K-1,比相同温度下GaN的导热系数小一半,200 nm的In01Ga0.9N热导系数为30.68 W·m-1·K-1.InGaN合金的热导系数随着In组分先变小再变大,理论计算结果表明In0.6Ga04N的导热系数最小,300 K时,体材料的导热系数为14.52 W·m-1·K-1,200 nm的薄膜材料导热系数为4.02 W·m-1·K-1,理论计算结果与文献报道的实验结果是合理一致的.  相似文献   
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We design a novel kind of polarization beam splitter based on a gold-filled dual-core photonic crystal fiber (DC-PCF). Owing to filling with two gold wires in this DC-PCF, its coupling characteristics can be changed greatly by the second-order surface plasmon polariton (SPP) and the resonant coupling between the surface plasmon modes and the fiber-core guided modes can enhance the directional power transfer in the two fiber-cores. Numerical results by using the finite element method show the extinction ratio at the wavethlengths of 1.327 μm and 1.55 μm can reach -58 dB and -60 dB and the bandwidths as the extinction ratio better than -12 dB are about 54 nm and 47 nm, respectively. Compared with the gold-unfilled DC-PCF, a 1.746-mm-long gold-filled DC-PCF is better applied to the polarization beam splitter in the two communication bands of λ = 1.327 μm and 1.55 μm.  相似文献   
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