Compton散射下强激光PPCs光子带隙构新模型

应用光流线量子理论和多光子非线性Compton散射模型,研究了强激光等离子体光子晶体中光子带隙产生的机制,提出了将入射光和Compton散射光形成的耦合光流线作为在强激光等离子体光子晶体中形成光子带隙结构的新模型,给出了耦合光流线满足的基本方程.结果表明,Compton散射使强激光等离子体光子晶体中产生了较深的折射率势阱,改变了在这个势阱中运动的耦合光能量的量子化分布几率,从而改变了光子带隙的位置和结构.     

Compton散射对非均匀等离子体光子晶体光子带隙的影响

应用多光子非线性Compton散射模型和时域有限差分法,对多光子非线性Compton散射对非均匀等离子体光子晶体光子带隙特性的影响进行了研究,提出将入射和散射光作为形成光子带隙的新机制,对电磁波方程进行了修正.结果表明:与Compton散射前相比,散射使电磁波幅值衰减更快;随等离子体密度增加,透射谱禁带宽度几乎无变化,...     

Compton散射对非均匀等离子体光子晶体光子带隙的影响

应用多光子非线性Compton散射模型和时域有限差分法,对多光子非线性Compton散射对非均匀等离子体光子晶体光子带隙特性的影响进行了研究,提出将入射和散射光作为形成光子带隙的新机制,对电磁波方程进行了修正.结果表明:与Compton散射前相比,散射使电磁波幅值衰减更快|随等离子体密度增加,透射谱禁带宽度几乎无变化,其中心频率向高频方向有明显移动,向上的峰值有较大增加,反射谱向下的峰值有明显减小|随温度增加,透射谱禁带宽明显减小,向上的峰值略有减小,透射能量有所降低|随两种介质介电系数比增加,光子禁带数增加,且带隙间距显著减小.     

多光子非线性Compton散射对等离子体中电子运动的影响

应用多光子非线性Compton散射模型,研究了多光子非线性Compton散射对激光等离子体中电子运动的影响,提出了将入射激光和Compton散射光形成的耦合光、耦合光与等离子体产生的自生磁场形成的混合场作为加速电子的新机制,对电子动量和能量方程进行了修正和数值模拟。结果表明,当混合场的电场振幅与磁场振幅相等时,回旋共振电子在与混合场作用时间内能被加速到很高的能量;电子加速能量随耦合光幅值的增大而增大,随电子耦合初始角度的增大而周期变小,随电子横向耦合归一化初始速度的增大,开始时较快增加,之后缓慢增加,最后趋于稳定。     

光子带隙结构理论的新方法

本文应用光流线量子论的基本思想，把介质中传输的光看作是能量流线而非电磁披，认为当光在介质中传输时，光同介质并非是彼此独立的，而是要发生相互作用，这种相互作用使光能量在介质中呈量子化的几率分布。将构成光子晶体的周期性介质模拟为周期性折射率势阱，通过求解光流线量子论的基本方程，讨论光子晶体中带隙产生的物理机制。     

基于横向磁光效应磁化等离子体光子晶体的光子带隙特性

通过外加与电磁波传播方向垂直的磁场来调控等离子体光子晶体的光子带隙结构。采用时域有限差分方法数值分析了由本征层为等离子体层和其他电介质材料层交替堆叠而成的磁化等离子体光子晶体的光子带隙结构和频谱特性。数值结果表明,光子晶体中等离子体的介电常数随着外磁场大小的变化而改变,从而使磁化等离子体光子晶体的带隙特性在一定的频率范围相应地得到调节。     

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应用电子与多光子集团非线性Compton散射模型,将入射和散射光作为离子的传输机制,研究了Compton散射下多束相干强耦合激光等离子体中离子的运动,给出了相对论离子动力学方程,并进行了数值模拟。研究发现,散射使光的传播速度减小,系统的矢势和标势增大,由入射和散射光形成的多束相干强耦合激光能使质子加速到5.40GeV的能量,而耦合轴向电场在其中起着关键作用。     

Compton散射对短脉冲强激光在次临界等离子体中自聚焦的影响

应用相对论理论和多光子非线性Compton散射模型,研究了Compton散射对短脉冲强激光在次临界等离子体中自聚焦的影响,提出了将入射光和Compton散射光作为形成激光自聚焦的新机制,给出了三级电流密度满足的修正方程,并进行了数值模拟。结果表明,相对论效应使等离子体中的短脉冲强激光自聚焦趋势减缓,而散射则加速了自聚焦的发展,总自聚焦趋势比无相对论时来得快一些,主要原因是由于散射光和入射光形成的耦合光频率较入射光频率增大,散射效应补偿了因相对论效应引起的自聚焦减缓效应的缘故。     

Compton散射下等离子体中的离子加速

应用电子与多光子集团非线性Compton散射模型,将入射和散射光作为离子的传输机制,研究了Compton散射下多束相干强耦合激光等离子体中离子的运动,给出了相对论离子动力学方程,并进行了数值模拟。研究发现,散射使光的传播速度减小,系统的矢势和标势增大,由入射和散射光形成的多束相干强耦合激光能使质子加速到5.40GeV的能量,而耦合轴向电场在其中起着关键作用。     

Compton散射对短脉冲强激光在次临界等离子体中自聚焦的影响

应用相对论理论和多光子非线性Compton散射模型,研究了Compton散射对短脉冲强激光在次临界等离子体中自聚焦的影响,提出了将入射光和Compton散射光作为形成激光自聚焦的新机制,给出了三级电流密度满足的修正方程,并进行了数值模拟。结果表明,相对论效应使等离子体中的短脉冲强激光自聚焦趋势减缓,而散射则加速了自聚焦的发展,总自聚焦趋势比无相对论时来得快一些,主要原因是由于散射光和入射光形成的耦合光频率较入射光频率增大,散射效应补偿了因相对论效应引起的自聚焦减缓效应的缘故。     

光子晶体中的磁控光子开关线路

提出了一个光子晶体中的磁控光子开关线路的理论模型,并利用平面波展开加超原胞方法计算了它的光学性质.这个模型由设置在空气中的介电柱子光子晶体构成,其中一排柱子被具有同样介电常数的铁氧体柱子替换.当外加磁场时,铁氧体柱子产生了不等于一的磁导率,这就会在光子带隙中产生波导模.当撤去外场,整个体系还原为完美光子晶体.由此便可形成磁控光子开关线路.具体选择了正方形柱子设置在正方形格点上,计算结果证明这种设想是可行的,并给出一些有价值的结果. 关键词： 光子晶体 传导模 磁导率     

Localized photonic modes in photonic crystal heterostructures

In this work, interface modes of two-dimensional photonic crystal heterostructures have been investigated by usage of the supercell method. The photonic crystal heterostructure is made of two photonic crystals with square symmetry in which one of them is composed of circular dielectric rods in air background and the other one is constructed by drilled square holes in dielectric. It is shown that using of a proper supercell plays an important role in obtaining the correct interface modes. We have also showed that the guided interface modes and single mode which is different from those reported in some published works are nearly dispersionless.     

Design of photonic bands for opal-based photonic crystals

To make a device from an opal—or otherwise—the photonic bands and the optical properties derived from them are needed. Knowing the effects of different parameters defining the opal geometry and different possible modifications of its structure are needed, too. An accurate definition of the device will be required to obtain a good performance. With this aim, the optics of light with a wavevector in the vicinity of the L point in the Brillouin zone and its coupling to bare opals band structure are presented. An important aspect is the transition from finite to infinite crystal and the study of size effects on the bands. It is possible to substantially alter the photonic band structure of an opal-based system, while maintaining the lattice structure, simply by growing layers of other materials with an appropriate refractive index. Here, it is shown how, by the growth of accurately controlled thin layers of silicon and germanium, and further processing, one can induce the opening of two complete photonic band gaps (PBGs) in an opal structure. Finally, the possibility to fabricate a simple device consisting in a planar waveguide will be shown. By means of a very simple and inexpensive procedure, engineered planar defects acting as microcavities have been realized. These can be viewed as a particular case of a much more general class of heterostructures that can be grown by combining opal vertical deposition and chemical vapour deposition of oxides. A further step is made by applying electron beam lithography to provide lateral definition and facilitate three-dimensional structuring.     

Isotropic photonic gaps in a circular photonic crystal

We investigated the optical properties of a circular photonic crystal (CPC) for which the distance between lattices was systematically distributed. The transmission spectra of CPC composed of alumina cylinders were examined in the frequency region from 0 to 20 GHz. We show that photonic gaps are obtained not only in CPCs but also in phase-shifted CPCs. The isotropic photonic gaps are evidenced by changes in the incident angle of a millimeter wave.     

Extension of photonic band gaps in one-dimensional photonic crystals

A method is proposed for extending photonic band gaps by constructing periodic structures from two or more consecutively located photonic crystals with different lattice constants or filling factors. The photonic band gaps with a maximum extension are predicted by superposing the photonic band gap maps on one another. It is demonstrated that both the lowest and higher order band gaps can be merged in photonic crystals with a high refractive index contrast.     

Nonreciprocal photonic band structure of low-symmetry magnetic photonic crystals

We propose multicomponent magnetic photonic crystals as a basis component for nonreciprocal optical elements. It is shown that introduction of three or more components may provide violation of mirror reflection symmetry, which is a necessary condition for obtaining nonreciprocity in the dispersion of the structure's eigenmodes. Numerical simulations confirm that nonreciprocity indeed develops in the form of nonreciprocal photonic band structure of three-component low-symmetry photonic crystal. We find that symmetry constraints produce fine structure in the nonreciprocity at high-symmetry points of the Brillouin zone.     

Tunable photonic Bloch oscillations in electrically modulated photonic crystals

We exploit theoretically the occurrence and tunability of photonic Bloch oscillations (PBOs) in one-dimensional photonic crystals (PCs) containing nonlinear composites. Because of the enhanced third-order nonlinearity (Kerr-type nonlinearity) of composites, photons undergo oscillations inside tilted photonic bands, which are achieved by the application of graded external-pump electric fields on such PCs, varying along the direction perpendicular to the surface of layers. The tunability of PBOs (including amplitude and period) is readily achieved by changing the field gradient. With an appropriate graded pump ac or dc electric field, terahertz PBOs can appear and cover a terahertz band in an electromagnetic spectrum.     

Larger complete photonic bandgaps in two-dimensional photonic crystal heterostructure

A two-dimensional photonic crystal heterostructure with a large complete photonic bandgap is presented. It consists of two photonic crystals, whose dielectric configurations are reverse, with triangular lattice of circular columns. The structure retains the ease of fabrication while increasing the maximum quality factor of the gap 2–3 times after optimization. Photonic bandgap properties are calculated using a plane-wave method and the transmission spectra are obtained.     

Control of photonic band gaps in one-dimensional photonic crystals

The photonic band gaps in one-dimensional photonic crystals (PCs) are theoretically investigated. A new method to broaden the photonic band gaps is introduced. Based on the similar method, a kind of photonic crystals is constructed to generate photonic band gaps with proportioned central frequencies. This technology can be used for designing nonlinear PCs for harmonic generation.