共查询到19条相似文献,搜索用时 359 毫秒
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《光子学报》2017,(4)
利用Cu~(2+)离子注入的方式在熔融石英和石英晶体上分别制备了平面光波导结构.通过棱镜耦合实验测试了两种光波导的导模特性,结果表明:在同样的注入条件下熔融石英上形成了增加型的光波导结构,而石英晶体上形成了位垒型的光波导结构.研究了退火温度对两种光波导导模折射率的影响,熔融石英光波导中导模的折射率随着退火温度的升高而降低,而石英晶体光波导中导模的折射率随着退火温度的升高先增加后降低.为了进一步分析离子注入两种材料形成光波导的微观机理,利用SRIM模拟了Cu~(2+)离子注入两种材料的电子能量损失和核能量损失,并且模拟了两种光波导结构的折射率分布.模拟结果表明:熔融石英光波导的主要形成原因是离子注入表面的折射率大于其体材料的折射率,而石英晶体光波导的主要形成原因是离子射程末端的折射率小于其体材料的折射率.因此,在熔融石英光波导的形成中电子能量损失起主要作用,而在石英晶体光波导的形成中核能量损失起主要作用. 相似文献
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报道了液氮温度下He^+离子注入LiNbO3波导的制备,采用棱镜耦合法测量了波导退火前后导模的有效折射率,计算了波导层折射率的分布和晶体中He^+离子的射程分布和损伤分布,两者吻合得较好。 相似文献
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利用数值模拟对扩散非线性机制下由光折变表面波诱导的薄层波导中导模的形成和特点进行了研究。采用分布傅里叶法对导模的传输特性进行了模拟。通过求解本征方程,对光折变表面波诱导的薄层波导中存在的导波模式进行了数值求解。通过调节传播常数和波导参数的方法,可以控制导模的阶数和传播波形。随着阶数的增加,导模轮廓的对称性越来越差;随着波导参数的增加,导模的峰值振幅单调递增。导模的能量主要聚集在晶体薄层波导中靠近-c轴的一侧,随着传播常数的增大,导模能量先减小后增大,且导模可以稳定传播。 相似文献
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基于混合导光型光子晶体光纤的波分解复用器研究 总被引:2,自引:1,他引:1
设计了一种基于混合导光型光子晶体光纤的波分解复用器,该波分解复用器同时具有折射率导光型光子晶体光纤和带隙导光型光子晶体光纤的特点,可用于稀疏型波分复用系统中.设计的稀疏型波分解复用器由一段三芯光子晶体光纤组成,通过填充不同折射率的材料.形成了混合导光型光子晶体光纤.根据耦合模原理,在临近的波导中,当传播常数相等时,模式之间发生强烈耦合.能量在波导之间交替.由于填充的材料折射率不同,使得光功率在两个小同的波长上发生耦合,构成了两个不同响应波长的光滤波器.通过选择合适的光纤长度,使得在光纤的输出端,不同波长的光从不同的波导输出,实现波分解复用的功能.采用全矢量有限元法分析了光纤传输特性,计算了不同波长光的耦合长度.采用光束传播法仿真发现,长度为4.3 mm的光纤能实现波长为1.31μm和1.55μm光的解复用. 相似文献
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提出一种在光子晶体十字波导中加入点阵缺陷的特殊结构波导.采用时域有限差分法(FDTD)对该结构的导波特性进行数值模拟,计算结果表明:含缺陷结构的光子晶体波导的透射光谱较不含缺陷结构光子晶体波导的透射光谱带宽变得更窄,此结构具有窄带滤波作用.当改变波导中缺陷结构折射率取值时,该波导透射光的中心频率随缺陷介质折射率的增大而线性减小.改变中心缺陷介质柱直径时,该波导透射光波中心频率随介质柱直径的增大也呈逐渐减小趋势.这种光子晶体十字波导可作为一种窄带滤波器、分光器和可调式选频器等器件,具有一定的应用前景. 相似文献
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转移矩阵法在负折射率介质材料平板波导中的应用研究 总被引:3,自引:3,他引:0
利用严格电磁理论,推导出了适用于负折射率介质材料光波导的转移矩阵,分析讨论了转移矩阵的性质和应用.利用转移矩阵方法,推导出导波层为负折射率介质材料、覆盖层和衬底为右手材料的三层对称介质光波导的本征色散方程.用图解法研究了负折射率介质波导中TE波的异常色散特性.在负折射材料介质波导中没有零阶模,最低阶为1阶模,并且有截止频率,只有波导参量满足一定条件的时候才会存在,导模的横向波数可以为实数和纯虚数,而正折射率介质波导导模的横向波数只能为实数. 相似文献
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Results obtained in the fabrication of slab and strip waveguides by ion implantation into fused quartz are discussed. Using a step-index waveguide model the increase in refractive index is calculated. The optical loss is smaller than 1 dB/cm at λ = 568 nm without annealing. The properties of strip waveguides fabricated by ion implantation through photoresist masks of thicknesses from 0.4 μm to 0.8 μm are described. A bright fluorescence is observed with emission at 530 nm and 640 nm and its dependence on ion fluence and ion energy is measured. 相似文献
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P. L. F. Hemment 《辐射效应与固体损伤》2013,168(1-4):31-45
The formation and annealing of defects in ion implanted silicon dioxide layers and in connection with them the refractive index change are of high interest for the production of electronic and integrated optical devices. Several studies have shown that the ion implantation in fused silica leads to a compaction of the material and in consequence to an increasing of the refractive index.1–6 On the other hand the defect formation in crystalline quartz is connected with a decreasing of the refractive index up to nearly the same value for ion implanted quartz and fused silica layers in the high dose region.1,5 On the base of this effects optical waveguides had been produced by ion implantation in both material.2,7–12 However, the nature of the mechanisms responsible for the defect formation and for the changes of the optical properties are not well understood. This paper reports on the ion dose and annealing temperature dependence of several defects in connection with the refractive index change. 相似文献
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It is well known that the refractive indices of lots of materials can be modified by ion implantation, which is important for waveguide fabrication. In this work the effect of Ar and Zn ion implantation on silica layers was investigated by Rutherford Backscattering Spectrometry (RBS) and Spectroscopic Ellipsometry (SE). Silica layers produced by chemical vapour deposition technique on single crystal silicon wafers were implanted by Ar and Zn ions with a fluence of 1–2?×1016 Ar/cm2 and 2.5?×1016 Zn/cm2, respectively. The refractive indices of the implanted silica layers before and after annealing at 300°C and 600°C were determined by SE. The migration of the implanted element was studied by real-time RBS up to 500°C. It was found that the implanted Ar escapes from the sample at 300°C. Although the refractive indices of the Ar-implanted silica layers were increased compared to the as-grown samples, after the annealing this increase in the refractive indices vanished. In case of the Zn-implanted silica layer both the distribution of the Zn and the change in the refractive indices were found to be stable. Zn implantation seems to be an ideal choice for producing waveguides. 相似文献
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Chuan-Lei Jia Xue-Lin Wang Lei Wang Ke-Ming Wang Hong-Ji Ma Rui Nie 《Applied Surface Science》2008,254(16):5095-5099
We report on the optical planar waveguides formation and modal characterization in β-BaB2O4 crystals by Ni2+ ion implantation at energy of 3.0 MeV and doses of 1014 ions/cm2. The prism coupling method was used to investigate the dark-mode property at wavelengths of 633 nm and 1539 nm, respectively. The refractive index profiles of the waveguides with different doses were reconstructed by an effective refractive index method based on the reflectivity calculation method (RCM). The modal analysis indicates that the fields of TM modes can be well restricted in the guiding region, which means the formation of non-leaky waveguide in the crystal. 相似文献
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在熔融石英玻璃衬底上,通过注入氮离子和硼离子,制成了低损耗、单模平面光波导.波导的最大折射率和离子浓度分布的半宽度分别是1.48和0.5μm,波导损耗<0.1dB/cm. 相似文献
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We report on Nd:CNGG active planar waveguides produced by 6.0 MeV carbon ion implantation at fluence from 1 × 1014 ions/cm2 to 8 × 1014 ions/cm2. The refractive index profiles, which were reconstructed according to the measured dark mode spectroscopy, showed that the refractive indices had negative changes in the surface region, forming typical barrier waveguide. The width of waveguide structure induced by carbon ion implantation is ∼3.8 μm. The typical barrier-shaped distribution may be mainly due to the nuclear energy deposition of the incident ions into the substrate. By performing a modal analysis on the observed TE modes, it was found that the TE0 and TE1 modes can be well-confined inside the waveguide. 相似文献
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The first planar optical waveguide to the authors' knowledge has been formed in Cu-doped potassium sodium strontium barium niobate crystal by mega-electron-volt He(+) implantation. Both TE and TM modes are observed. The profiles of the ordinary and the extraordinary refractive indices are deduced from dark-line mode spectroscopy. The results show that the mega-electron-volt He implantation results in a decrease in refractive index in barriers for both n(o) and n(e), but for n(e) there is an obvious increase in the waveguide region. From an experiment in photorefractive two-wave mixing, it is found that the erasure time for two-wave mixing is prolonged by ion implantation. 相似文献
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We report on the fabrication and characterization of planar and channel waveguides in KTiOPO4 crystals by 6.0 MeV C3+ ion implantation with the dose of 1×1014 ions/cm2. The dark mode spectroscopy of the planar waveguide was measured using a prism coupling arrangement. An increase of the both
n
x
and n
y
refractive indices induced by the annealing after implantation is believed to be responsible for waveguide formation. The
bright near-field intensity distribution of the transverse-electric and transverse-magnetic modes in the annealed channel
waveguide was collected and studied by end-coupling method. 相似文献
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We report on the optical planar waveguide formation and modal characterization in Nd: GdVO4 crystals by triple oxygen ion implantation at energies of (2.4, 3.0, and 3.6 MeV) and fluences of (1.4, 1.4, and 3.1) × 1014ions/cm2. The prism-coupling method is used to investigate the dark-mode property at wavelength of 632.8 nm. The refractive index profiles of the waveguide are reconstructed by an effective refractive index, neff method. The modal analysis shows that the fields of TE modes are well restricted in the guiding region, which means the formation of nonleaky waveguide in the crystal. 相似文献