共查询到19条相似文献,搜索用时 359 毫秒
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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
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赵振堂 王东 殷立新 方国平 顾强 谷鸣 冷用斌 刘波 周巧根 沈立人 张猛 邓海啸 陈家华 陈建辉 陈志豪 丁建国 方文程 冯超 谷端 胡晓 黄大章 黄毛毛 蒋志强 李宾 林国强 刘以勇 孙森 王光宏 王兴涛 王震 吴衍青 俞路阳 袁启兵 张伟 钟少鹏 夏晓彬 唐传祥 黄文会 杜应超 颜立新 《光学学报》2021,41(1):245-256
X射线自由电子激光试验装置(以下简称"SXFEL试验装置")是中国第一台X射线相干光源,其输出波长小于9 nm。这台基于0.84 GeV直线加速器、以掌握装置相关技术和实验演示种子型自由电子激光(FEL)级联与短波长回声型FEL为主要目标的自由电子激光装置,于2020年11月通过国家验收。本文将介绍SXFEL试验装置的基本情况和主要进展。 相似文献
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FEL振荡器的一维模拟计算 总被引:1,自引:0,他引:1
利用基于自由电子激光经典理论的一维模型的两个程序(MFEL1和FEL0),数值模拟了1.06μm自由电子激光振荡器的各物理参数的演化。MFEL1是考虑了Slippage效应的短脉冲多模计算程序,FEL0是没考虑Slippage效应的长脉冲单模计算程序。前者更能反映实际情况,后者能更细致地模拟光场与电子束在一次放大过程中的演化。计算表明,在短脉冲情况下,激光强度、品质、增益和能量抽取效率强烈依赖于电子束流强度,对一定范围的能散变化却不敏感;但在长脉冲情况下,上述物理量对能散在同样范围内的变化较为敏感。光强度的增益谱清楚地再现了小信号放大的Madey定理。在信号接近饱和时,增益谱的非零部分出现在远离共振频率的区域,这正是FEL中的边带不稳定性。 相似文献
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在对中国工程物理研究院高功率太赫兹(THz)自由电子激光(FEL)装置理论分析和设计的基础上,针对目前THz FEL光腔设计面临的主要难点,提出了椭圆型耦合输出光腔的设计方案,并对椭圆型耦合输出光腔代替传统FEL光腔的优势、光腔品质、耦合效率等进行了分析研究。研究表明,椭圆型耦合光腔的设计更适合目前THz FEL波导光腔的光斑特点,可使光腔输出功率提高33%以上,输出耦合效率即光腔品质可提高30%~70%;随着辐射频率的提高,椭圆孔耦合输出光腔的优势提高更为明显。 相似文献
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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
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北京自由电子激光装置的设计研究 总被引:4,自引:2,他引:2
北京自由电子激光装置(BFEL)是一台工作在中红外区的康普顿型FEL振荡器。由一台30MeV的射频电子直线加速器提供电子束。特点之一是用微波电子枪作为高亮度注入器。本文首先概述了BFEL的一般情形和物理参数.接着用解析公式和模拟的方法论证了电子束的设计目标和激光器的运转特征。最后阐述了BFEL各部分采取的技术路线的特点,内容包括微波枪、加速器和微波系统、调制器、输运系统、摇摆磁铁、光学腔、电子束诊断、准直、自发辐射和激光实验。 相似文献
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利用已获得的大信号自由电子激光增益公式,导出了激光平均增长率表达式,分析了自由电子激光中电子与辐射波相互作用的有效时间,讨论了其主要物理参量对相互作用有效时间的影响
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《中国物理C(英文版)》2017,(1)
An infrared oscillator FEL user facility will be built at the National Synchrotron Radiation Laboratory at in Hefei, China. In this paper, the parameter design of the oscillator FEL is discussed, and some original relevant approaches and expressions are presented. Analytic formulae are used to estimate the optical field gain and saturation power for the preliminary design. By considering both physical and technical constraints, the relation of the deflection parameter K to the undulator period is analyzed. This helps us to determine the ranges of the magnetic pole gap,the electron energy and the radiation wavelength. The relations and design of the optical resonator parameters are analyzed. Using dimensionless quantities, the interdependences between the radii of curvature of the resonator mirror and the various parameters of the optical resonator are clearly demonstrated. The effect of the parallel-plate waveguide is analyzed for the far-infrared oscillator FEL. The condition of the necessity of using a waveguide and the modified filling factor in the case of the waveguide are given, respectively. 相似文献
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This Letter reports the first experimental results from the world's first distributed optical-klystron (DOK) free-electron laser (FEL), the DOK-1 FEL, at Duke University. The DOK-1 FEL is a hybrid system, comprised of four wigglers: two horizontal and two helical. With the DOK-1 FEL, we have obtained the highest FEL gain among all storage ring based FELs at 47.8% (+/-2.7%) per pass. We have also demonstrated that the FEL gain can be enhanced by increasing electron bunching using wigglers with a different polarization. Furthermore, we have realized controlled polarization switches of the FEL beam by a nonoptical means through the manipulation of a buncher magnet. 相似文献
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基于自由电子激光(FEL)的太赫兹源具有高功率、高效率、波谱范围宽且连续可调、波束质量好等显著优点,目前是获得最高输出功率的方法。紧凑型太赫兹源使整体装置小型化,减少了装置成本和占用空间,但依然可以提供高功率、高品质的太赫兹波束,是一种便利可靠的用户装置。由于空间限制,FEL上的磁铁要尽可能地减小其尺寸,并仍能满足束流参数设计要求。本文设计的四极磁铁磁轭孔径与有效长度,其中2块是64 mm100 mm,另外3块是45 mm100 mm。这些四极磁铁的磁场梯度可以达到0.6~1.9 Tm-1。采用Poisson和Oprra-3D软件进行四极磁铁的二维和三维仿真计算,设计优化四极磁铁的结构,并测量了加工完成后的四极磁铁的磁场。 相似文献
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J. Feldhaus E. L. Saldin J. R. Schneider E. A. Schneidmiller M. V. Yurkov 《Optics Communications》1997,140(4-6):341-352
A new design for a single pass X-ray Self-Amplified Spontaneous Emission (SASE) FEL is proposed. The scheme consists of two undulators and an X-ray monochromator located between them. The first stage of the FEL amplifier operates in the SASE linear regime. After the exit of the first undulator the electron bunch is guided through a non-isochronous bypass and the X-ray beam enters the monochromator. The main function of the bypass is to suppress the modulation of the electron beam induced in the first undulator. This is possible because of the finite value of the natural energy spread in the beam. At the entrance to the second undulator the radiation power from the monochromator dominates significantly over the shot noise and the residual electron bunching. As a result the second stage of the FEL amplifier operates in the steady-state regime when the input signal bandwidth is small with respect to that of the FEL amplifier. Integral losses of the radiation power in the monochromator are relatively small because grazing incidence optics can be used. The proposed scheme is illustrated for the example of the 6 nm option SASE FEL at the TESLA Test Facility under construction at DESY. As shown in this paper the spectral bandwidth of such a two-stage SASE FEL (Δλ/λ 5 × 10−5) is close to the limit defined by the finite duration of the radiation pulse. The average brilliance is equal to 7 × 1024 photons/(s × mrad2 × mm2 × 0.1% bandw.) which is by two orders of magnitude higher than the value which could be reached by the conventional SASE FEL. The monochromatization of the radiation is performed at a low level of radiation power (about 500 times less than the saturation level) which allows one to use conventional X-ray optical elements (grazing incidence grating and mirrors) for the monochromator design. 相似文献