自聚焦透镜组合光学系统的光线传输分析

本文导出了自聚焦透镜组合光学系统的光线传输方程,讨论了光线传输与自聚焦透焦透镜参数关系。对几种典型自聚焦透镜组合进行了计算、从而估计自聚焦透镜参数选择。     

大芯径石英光纤中皮秒脉冲激光的自聚焦

本文报道了对大芯径石英光纤中皮秒脉冲激光自聚焦现象的实验研究和理论分析.文中测量了自聚焦先场的近场光强轮廓,研究了自聚焦光场的时域和频域性质,并对环形自聚焦光场的成因进行了解释.     

一维自聚焦透镜及其应用

利用平板自聚焦透镜材料进行离子交换,制成一维自聚焦透镜.分析了平板自聚焦透镜的离子交换原理和折射率分布形成过程,测量了不同厚度时,折射率分布常量A的值.介绍了透镜的应用,并用一维自聚焦透镜制成小型半导体激光器耦合器件.     

耦合半导体光源和光纤的平凸自聚焦透镜

本文介绍了将半导体激光器耦合到光纤维的平凸自聚焦透镜的性质,并且给出了一些计算透镜参数的公式。通过分析指出,当需要使用大数值孔径的自聚焦透镜或自聚焦透镜不能充分靠近光源时,采用平凸自聚焦透镜是有益的。     

自聚焦透镜列阵重叠度的研究

本文讨论了自聚焦透镜列阵重叠度,分析了重叠度对分辨率及照度分布的影响,并对一系列单根自聚焦透镜和两列自聚焦透镜列阵作了测量,得到了制造自聚焦透镜列阵的一个重要依据.实验中总结出照度分布不均匀规律的经验公式.     

自聚焦透镜离轴耦合损耗理论研究

利用光线光学的原理分析了自聚焦透镜的光学性能,提出了求解自聚焦透镜离轴耦合损耗的数学模型,利用这一模型计算出了单模光纤与自聚焦透镜离轴耦合时的耦合损耗与模向距离的关系曲线,为自聚焦透镜离轴耦合的设计提供理论依据.     

采用GRIN透镜之光纤加速度计原理分析

根据近轴子午光线方程,研究了自聚焦透镜光纤加速度计的工作原理。据光功率耦合,分析了光纤和自聚焦透镜物理参数之选择。同时,对自聚焦透镜倾斜的影响给出了定量分析。本文从理论上证明了这种结构新颖,体积极小,精度高,成本低之自聚焦透镜光纤加速度计是合理可行的。     

自聚焦排透镜参数分析及制作

自聚焦排透镜(SLR)是利用自聚焦透镜(SELFOC LENS)制作的一成象器件。本文就SLR的工作原理,及各参数对成象的影响进行了分析。并实际制作了几种不同规格的自聚焦排透镜为研制自聚焦排透镜提供了极好的基础。     

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。     

An analysis of undulator optimization in self-seeding free electron lasers

A simple analysis is given for the optimum length of undulator in a self-seeding free electron laser(FEL).The obtained relations show the correlation between the undulator length and the system parameters.The power required for the seeding in the second part of the undulator and the overall efficiency of monochromatizating the seeding determine the length of the first part of the undulator;the magnitude of seeding power dominates the length of the second part of the undulator;the whole length of the undulator in a self-seeding FEL is determined by the overall efficiency for getting coherent seed,and is about half as long again as that of SASE,not including the dispersion section.The requirement of the dispersion section strength is also analyzed.     

Analysis of undulator radiation with an electromagnet undulator

In this paper we discuss the theory of undulator radiation in an electromagnet undulator. We discuss the spectral properties of undulator radiation when electrons are injected off the undulator axis. This paper highlights the distinctive features of the radiation spectrum from electromagnet undulators, as compared to PPM undulators.     

Choice of the parameters of a magnetic undulator

The total output power of undulator radiation is investigated as a function of the constructional parameters of the undulator and its supply current. Calculations are presented of the magnetic field in the undulator, and the optimum undulator dimensions for maximum magnetic field intensity per unit length of the system are calculated. It is shown that the total radiated power of the charged particles depends on the undulator periodicity.     

Calculation and analysis of the magnetic field of a linearly tapered undulator

There is an empirical formula describing the relationship between the peak magnetic field and the undulator structure parameters for a uniform-parameter hybrid undulator.In this paper, we investigate the relationship for a linearly tapered undulator through numerical calculation by using the code RADIA, and check it with the empirical formula.The results imply that this empirical formula is also effective for linearly tapered undulators at a big enough scope for the requirements of normal FEL experiments.Therefore, for a linearly tapered undulator,we can use the empirical formula to design the variation of the undulator gap.For the tapering rate demanded by normal FEL experiments, the gap of a linearly tapered undulator increases almost linearly, and the tapering rate will keep constant while adjusting the undulator gap with the same variation for each undulator period.     

用于THz源的混合型波荡器数值模拟

波荡器是基于自由电子激光的小型THz源关键器件, 其可调节的周期性磁场结构与两端的光腔配合, 使得穿越的电子束产生带增益的相干辐射, 最终达到THz源所需要的功率. 同纯永磁结构相比, 混合型波荡器通过软铁材料调节由永磁块磁化方向性差异导致的磁场分布误差, 同时可提供更高的场强. 本文针对小型THz源需求, 对混合型波荡器进行了相关物理设计. 在解析方法分析的基础上, 采用OPERA3D/TOSCA有限元分析软件, 对波荡器进行了三维磁场数值模拟和积分场优化. 通过对波荡器端部结构的调整, 优化后模型的一次场积分(导向误差)小于0.01Gs﹒m, 电子轨迹偏移小于0.02mm.     

纯永磁波荡器基波与谐波磁场的三维计算与测试

 对标淮的纯永磁波荡器进行了三维磁场的有限元计算,给出了纯永磁波荡器的基波与谐波磁场的幅值与相位,并与测试结果进行对比,结果表明,标准的纯永磁波荡器谐波磁场幅值比基波幅值低两个数量级。     

Theoretical and numerical analysis of electron motion in a three-dimensional undulator field

The results of numerical calculations of electron trajectories in the three-dimensional ideal magnetic field of an undulator are given. These trajectories can be regarded as exact results in our case. It is shown that, in a series of cases, results of the calculation of trajectories using approximate analytical formulas significantly differ from those obtained using numerical methods. The obtained numerical results show that the influence of the undulator on the dynamics of the electron beam is very complicated and cannot be reduced only to the focusing properties of the undulator magnetic field or wiggler.     

Effects of energy spread on brightness and coherence of undulator sources

The (spectral) brightness for partially transverse coherent sources such as synchrotron radiation and free‐electron laser sources can be defined as the maximum of the Wigner distribution. Then, the brightness includes information on both coherence and wavefront characteristics of the radiation field. For undulator sources, it is customary to approximate the single‐electron electric field at resonance with a Gaussian beam, leading to great simplifications. Attempts to account for the modified spatial and angular profile of the undulator radiation in the presence of detuning due to energy spread, currently build on the simplified brightness expression derived under the assumption of Gaussian beams. The influence of energy spread on undulator radiation properties is becoming important in view of diffraction‐limited rings with ultralow emittance coming on‐line. Here the effects of energy spread on the brightness of undulator radiation at resonance are discussed, as well as relevant relations with coherence properties.     

The prototype of new variable period undulator for Novosibirsk free electron laser

To improve the parameters of the second stage Novosibirsk free electron laser we plan to replace the existing electromagnetic undulator by permanent-magnet variable-period undulator (VPU). The VPUs have several advantages compared to conventional undulators, which include wider radiation wavelength tuning range and an option to increase the number of poles. Both these advantages will be realized in the new undulator under development in Budker INP. There are some technical problems, which have to be solved before this idea can be implemented in practice. To check the solution of these problems we designed and manufactured a small undulator prototype, which has just several periods. In this paper, the results of mechanical and magnetic measurements of this undulator prototype are presented and compared with simulations.     

Field integral measurement of a six period undulator in a pulsed wire set up

A pulsed wire method is described for undulator field measurement. The results of the second field integral are compared with Hall probe results. The pulsed wire data are taken at different locations of the sensor along the length of the wire and with different gap of the undulator. A planar undulator with six periods is used in the pulsed wire set up. The total length of the undulator is 30 cm. The pulsed wire result shows good agreement with the Hall probe data.