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1.
用流体理论研究了带wiggler场圆柱型填充介质的自由电子激光器(FEL)。结果表明:本系统超辐射放大的工作主模式为横电(TE)模,并具有所有慢波FEL的特点。 关键词:  相似文献   

2.
本文利用自由电子激光(FEL)纵模统一理论讨论了光学速调管自由电子激光相干谐波的输出情况。从物理上分析了非对称光学速调管的设计,得出了采用非对称的光学速调管可使FEL的相干谐波输出提高近30%。  相似文献   

3.
 利用自由电子激光(FEL)纵模统一理论,系统地分析了光速调管FEL的小信号增益理论,并对色散参数Nd、束流能散度和发射度的影响进行了讨论。  相似文献   

4.
曙光一号自由电子激光装置的设计研究   总被引:1,自引:0,他引:1  
曙光一号自由电子激光装置(SG-1 FEL)是一台高功率毫米波段自由电子激光放大器,它由3.5MeV直线感应加速器、电子束调制系统、变参数摇摆器和微波种子源等部件组成。本文扼要叙述了SG-1 FEL的物理设计和主要技术参数,并重点分析了各主要部件的实验研究、计算模拟,以及物理设计和结构的特点。  相似文献   

5.
提出基于束流相空间拍频产生锁模多色自由电子激光的方案,利用带有能量啁啾的电子束流和上海软X射线自由电子激光装置(SXFEL)上的两个调制段-色散段结构,在束流中通过拍频形成多个流强脉冲串,并在此基础上进行高次谐波辐射,产生锁模多色自由电子激光辐射脉冲。模拟结果表明,利用264 nm的种子激光,可在束流中形成18次谐波的群聚分量,并能最终产生中心波长约14.58 nm的锁模多色FEL辐射。  相似文献   

6.
<正>高增益自由电子激光原理自由电子激光(Free Electron Laser,简写为FEL)是以相对论性电子束为放大介质、基于电磁辐射机制的相干光源。自由电子激光原理是20世纪70年代中期发展起来的,1976年,美国的梅迪(J.M.J.Madey)博士等人首次在实验上证实了振荡器型低增益FEL的原理,引起科技界极大的兴趣。20世纪80年代,科学家们提出了SASE(Self Amplified Spontaneous Emission,自放大自发辐射)高增益自由  相似文献   

7.
为了对自由电子激光(FEL)进行基本物理研究,中国工程物理研究院设计建造了曙光一号自由电子激光装置(SFLE),并于1991年9月17日首次出光。  相似文献   

8.
 孔耦合输出对自由电子激光(FEL)振荡器腔内光场的横向结构有很大的影响, 在输出镜上横模之间发生很复杂的耦合转换。基于中物院远红外自由电子激光振荡器, 研究了 孔输出波导 FEL的数值模拟, 对孔耦合及其引起的腔内光场的变化给以特别的注意, 依据数 值结果, 分析了孔耦合FEL光场横向结构的特性。  相似文献   

9.
根据于敏教授的自由电子激光纵模统一理论,推导了磁场含有随机误差影响时光场的小信号增益和指数增益。并且结合曙光一号FEL装置,给出了指数增益区磁场随机误差σ与增益参数g_0的定标关系。同时利用三维WAGFEL程序详细地模拟计算了磁场随机误差对自由电子激光增益和饱和增益的影响。线性理论的结果得到了模拟计算的证实。  相似文献   

10.
自由电子激光辐射频谱测量   总被引:1,自引:0,他引:1  
文章描述了在环形电子束和实心电子束自由电子激光(FEL)研究中,测量辐射频谱使用的两种方法——波导色散线和带通滤波器谱仪。介绍了测量系统的组成和特点,给出了测量结果:环形束FEL试验。辐射频率在27—38GHz内可调:实心束FEL试验,辐射频谱带宽~1.2GHz。  相似文献   

11.
Cherenkov free electron laser(CFEL) is simulated numerically by using the single particle method to optimize the electron beam. The electron beam is assumed to be moving near the surface of a flat dielectric slab along a growing radiation. The set of coupled nonlinear differential equations of motion is solved to study the electron dynamics. For three sets of parameters, in high power CFEL, it is found that an axial magnetic field is always necessary to keep the electron beam in the interaction region and its optimal strength is reported for each case. At the injection point, the electron beam's distance above the dielectric surface is kept at a minimum value so that the electrons neither hit the dielectric nor move away from it to the weaker radiation fields and out of the interaction region. The optimal electron beam radius and current are thereby calculated. This analysis is in agreement with two previous numerical studies for a cylindrical waveguide but is at odds with analytical treatments of a flat dielectric that does not use an axial magnetic field. This is backed by an interesting physical reasoning.  相似文献   

12.
未磁化等离子体介质切连科夫脉塞的线性理论   总被引:1,自引:0,他引:1       下载免费PDF全文
利用线性自洽场理论,讨论了电子在扰动场作用下的三维扰动.在此基础上,对常用的薄环形相对论电子环束在填充未磁化等离子体的介质筒慢波波导中激励的切连科夫辐射进行了详细的分析,导出了此电子环束与慢波系统中任意波导模互作用的色散方程和波增长率,并对其进行了详细的分析和讨论.分析表明切连科夫辐射是由其波导模与电子注模耦合所致.最后详细计算和分析了等离子体密度对色散特性和波增长率的影响 关键词:  相似文献   

13.
In this article, we propose a quantum regime for Cherenkov free-electron laser (CFEL) and surface plasmon polaritons (SPPs) excited in dielectric and multilayer graphene waveguides, respectively. This quantum regime is realized when the momentum spread induced in the interaction is smaller than the photon recoil. The discrete momentum exchange characterizing this interaction yields a significantly narrow single emission line. To determine the condition of the quantum regime, we derive an expression for the gain in the Cherenkov effect using a quantum mechanical treatment. It is assumed that the effective spread in momentum is due to the finite interaction length L (or the propagation length in the case of SPPs). For both cases, CFEL and SPPs, the effects of electron beam and waveguide parameters on the possibility of the quantum regime are studied. We conclude that the quantum regime can be basically verified at low electron beam energy (<40 keV) and at emission wavelengths in the near infrared range (<5 μm) when L is in the order of millimeters. In the case of SPPs, we also show that the feasibility to realize quantum SPPs is enhanced by increasing the chemical potential and number of graphene layers.  相似文献   

14.
The radiation characteristics of the double dielectric grating leaky-wave antenna are analyzed by the improved perturbation method. The results indicate that under the condition of the same radiation intensity, the double dielectric grating antenna has relatively smaller dimensions than that of the single one. It is undoubtly of great importance in the case that the limitation of the weight and volume of system is strictly required. The results obtained from this paper are compared with the exact solution based on the mode matching method. It is justified that the present perturbation procedure yields as highly results as the rigorous approach with extremely simplicity of the analysis and calculations.  相似文献   

15.
Angular dependences of electromagnetic radiation scattered by separate finite dielectric cylinders and their ordered assemblies have been numerically simulated using a volume integral equation formalism. Dependences of directional diagrams on optical-geometric parameters of both the separate finite cylinders and their spatial ordering were studied. It is shown that collective effects of a coherent nature in the assembly of spatially ordered cylinders result in a scattered radiation angular distribution that differs strongly from that obtained for a system of cylinders that are not electrodynamically coupled.  相似文献   

16.
The elements of the scattering matrix of the junction between two circular monomode dielectric waveguides with different diameters and/or different refractive indices are calculated using the mode matching method. The theory is evaluated numerically for a wide range of parameters and simplified considerably for two important cases of weakly guiding waveguides.The radiation pattern of the junction is calculated using the Huygens-Kirchhoff theory of diffraction and shown to be reducible to the weighted difference of the radiation patterns of the ends of the primary and secondary waveguide. Simple approximations are derived for weakly guided waves.The theory is verified experimentally by measuring the scattering parameters, the far-field radiation pattern and the near-field distribution of abrupt changes in diameter of microwave dielectric rod transmission lines.  相似文献   

17.
The effects of left-handed materials (LHM) on frequency selective reflection and transmission characteristics of dielectric periodic structures are carefully investigated using a method which combines the multimode network theory with the rigorous mode matching method. In addition, the effects of LHM dielectric loss on the selective properties are also given. It has been shown that the selective behavior of periodic structures can be modified by adding LHM layers above and below the periodic layer. Supported by the National Natural Science Foundation of China (No. 60171037) (No. 60371010) and (No. 63531020)  相似文献   

18.
Zhao C  Cai Y 《Optics letters》2011,36(12):2251-2253
The radiation forces on a Rayleigh dielectric sphere induced by a focused partially coherent elegant Laguerre-Gaussian (ELG) beam are investigated by using the Rayleigh scattering theory. It is found that a focused partially coherent ELG beam with suitable mode orders can be used to trap a Rayleigh particle whose refractive index is larger or smaller than that of the ambient by varying its initial spatial coherence width. Therefore, one can use one optical-trap system to trap two types of particles with different refractive indices.  相似文献   

19.
We have studied absorption and thermal radiation for a three dimensional lossy photonic crystal of dielectric spheres by using a multiple scattering method. It is shown that such simple structures have excellent selective thermal radiative characteristics in different photonic bands. There is stronger thermal radiation at high frequency than that at low frequency. In comparison with the uniform slab without photonic crystal structure, in the photonic band gap, the thermal emission intensity is greatly suppressed and very weak, but not zero due to the penetration depth. Under the same lattice structure, the thermal emission of photonic crystal varies with the change of the radius of the spheres.  相似文献   

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