共查询到19条相似文献,搜索用时 156 毫秒
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波荡器是同步辐射光源中产生X射线的关键设备,低温型Delta波荡器可明显提高镨铁硼永磁铁的峰值场强和内禀矫顽力,进而有效抵抗辐照环境下的磁场退化。为了使永磁阵列进入液氮温区,提出了磁铁干式传导冷却方案,设计了干式低温恒温器结构,利用数值模拟完成了热力学分析优化,并搭建实验台进行了降温测试。结果表明,Delta波荡器可通过单台小型低温制冷机传导冷却进入低温状态,并突破常压饱和液氮温度,最低达到40 K,四个梁的最大温差约1 K,达到温度均匀性要求,并将磁场强度提高20%以上。低温型Delta波荡器模组达到设计指标,验证了波荡器干式传导冷却方案的可行性,对低温型波荡器的研发设计具有重要意义。 相似文献
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同步辐射是本世纪70年代发展起来的一种新型光源,具有亮度高、波长(从红外到X光波段)连续可调、准直性好、完全确定的偏振度、洁净的工作环境(优于10-9的真空度)、快速而精确的光脉冲时间结构等一系列优点,在物理、化学、生物、医学、农业、材料科学、冶金、能源、地矿、微电子、化工等多学科领域有着广泛的应用.然而,早年用于高能物理实验研究的正、负电子对撞机所产生的同步辐射虽然远远优于其它辐射光源,但从其本身的条件考虑,仍然是不大理想的.因为这样产生的同步辐射是由储存环中的弯转磁铁产生的,利用弯铁作为同步辐射光源具有一定的局限性首先,对弯转磁铁来说,其主要作用是维持储存环中电子束流在封闭的真空管道内循环,应满足储存环上的物理要求,因而同步辐射仅是其一种副产品.由下式可知:B[T]ρ[m]=3.336E[GeV].式中B为弯铁磁场,ρ为弯转半径. 相似文献
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《中国光学与应用光学文摘》2004,(4)
介绍了用于NSRL的X射线衍射和散射光束线中环面聚焦镜的成像原理和基本结构.分析计算了各种像差和面形精度对成像质量的影响,重点描述了镜子因受力弯曲在子午方向的曲率变化与理论值的误差以及反射表面受同步辐射光照射而产生的热载变形,进而求得实验样品上束斑成像的高度。最后用CCD探测实际光斑的尺寸. 相似文献
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介绍了中国高能同步辐射光源验证装置(HEPS-TF)中超导3W1扭摆磁铁控制系统的设计。该控制系统主要包括电源控制系统和低温信号监测系统。整个控制系统基于实验物理及工业控制系统(EPICS),其硬件结构以串口服务器为核心,将接口转换为标准的RS232/485接口。软件方面,通过应用StreamDevice设备驱动模块开发了基于Modbus协议的EPICS驱动,缩短了设备驱动的开发周期。上层控制界面采用嵌入了EPICS Qt框架的Qt Creator开发,增强了其灵活性。目前控制系统的离线测试已完成。 相似文献
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曙光一号自由电子激光器的理论计算 总被引:1,自引:0,他引:1
系统总结曙光一号自由电子激光器理论计算的主要结果:包括曙光一号装置主要参数的选取和理解;磁场失谐曲线的计算;常参数摇摆器和变参数摇摆器的主要结果;高阶波导模的贡献;电子束参数扰动对激光性能的影响;空间电荷效应等。计算结果表明,常参数摇摆器激光输出功率可达80MW,效率约50%;变参数摇摆器激光输出功率可达250MW左右,效率约16%。 相似文献
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A. M. Batrakov P. V. Vagin P. D. Vobly D. S. Gurov N. I. Zubkov I. V. Ilyin A. B. Ogurtsov M. Tischer A. V. Utkin N. G. Khavin M. A. Kholopov D. S. Shichkov 《Journal of Surface Investigation: X-ray, Synchrotron and Neutron Techniques》2011,5(6):1038-1044
The Petra III synchrotron radiation source was developed based on the Petra-II 6-GeV electron accelerator (DESY). After installing the system for radiation damping, the horizontal emittance of the electron beam of Petra III decreased from 5 nm rad to 1 nm rad, which is a record parameter for this class of installations. The system of radiation damping includes 20 permanent magnet wigglers installed in two straight sections, 50 m each. The total radiation power of the wigglers reaches 800 kW. The wigglers used in the radiation damping system of Petra III were developed in collaboration with DESY (Hamburg) and fabricated by the Budker Institute of Nuclear Physics. The wiggler length is 4.04 m, the gap between the poles is 24 mm, the maximum magnetic field is B = 1.52?1.56 T, and the period is λ = 20 cm. This paper describes the design features of the permanent magnet wigglers and the methods and results of adjustment of the wiggler operating parameters. 相似文献
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Periodic magnetic structures (wigglers) have been successfully used for a long time for controlling beam parameters in charged-particle storage rings for various purposes (including the reduction of emittance). In this work, we optimize the optical functions of the storage ring gap into which a wiggler is installed for a more effective reduction of the emittance. Optimal solutions are obtained for the first time for FODOtype and theoretical minimum emittance (TME) structures. An original method is proposed for suppressing the contribution of the wiggler fields to the radiation excitation of the phase volume of the beam by modulating the field period along the wiggler axis. 相似文献
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Freund H.P. Ganguly A.K. 《IEEE transactions on plasma science. IEEE Nuclear and Plasma Sciences Society》1992,20(3):245-255
Results obtained with the three-dimensional nonlinear analysis and simulation code, ARACHNE, and a recent 33.4-GHz, collective, free-electron laser (FEL) amplifier experiment are compared. The experiment has demonstrated power levels of 61 MW (≈27% efficiency) without recourse to tapered magnetic fields, using a 750-keV/300-A electron beam with a nominal axial energy spread of 1.5% propagating through a cylindrical drift tube in the presence of a helical wiggler and an axial guide magnetic field. Significant differences in the character of the emission were found, depending on the direction of the guide magnetic field. When the wiggler and guide fields were parallel, observed power levels reached approximately 4 MW for both the strong and weak guide field regimes, but vanished in the neighborhood of the magnetic resonance. However, the maximum power was observed in the reversed field case when the wiggler and guide fields were antiparallel. In this case, no resonant enhancement in the transverse velocity is expected to occur; however, a significant reduction in the output power occurred in the neighborhood of the antiresonance. The ARACHNE simulation is in substantial agreement with the experiment 相似文献
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毫米波自由电子激光的数值模拟和实验的比较 总被引:2,自引:0,他引:2
从波导管毫米波自由电子激光器的设计要求出发,根据Livermore实验室FRED程序的物理思想,编制了空间三维的数值模拟程序(WAGFEL)。为了检验程序的可靠程度,结合ELF装置的实际参数,进行了数值模拟并和实验结果进行了比较。结果表明,把Wiggler磁场B_w增大300 Gs后,WAGFEL程序的模拟结果和Livermore实验室的实验结果基本符合。模拟使用的全部参数,除B_w增大300Gs外,都是ELF的实际参数。模拟时峰值磁场B_w=4050Gs,实验测量峰值磁场B_w=3720Gs,相差在8%左右。WAGFEL程序可以用来从事毫米波自由电子激光器的设计以及基本物理问题的研究。 相似文献
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