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渡越辐射在强流电子束诊断中的应用 总被引:2,自引:0,他引:2
文中描述了渡越辐射用于束流诊断的理论依据,介绍了利用渡越辐射对18MeV,2.7kA的强流脉冲电子束进行诊断的实验方案,介绍了在强流束测量中遇到的困难和解决方法.实验中获得了渡越辐射的特征图案,并对特征图案进行了分析,得到了测量时应该使用偏振片的结论.据此,利用渡越辐射测量了强流脉冲束的剖面、能量、发散角.并采用渡越辐射与切伦科夫辐射相结合的方法,用切伦科夫辐射测量束剖面,用渡越辐射测量能量和发散角,在同一次实验中获得了强流脉冲束的归一化发射度. 相似文献
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为了快速获得直线感应加速器电子束束剖面信息以便能加速加速器的调试,研制了一套基于切伦科夫辐射的束斑测量装置,如图1所示。切伦科夫辐射体采用φ80,厚度0.5mm的石英玻璃。石英玻璃背面经过磨砂处理,安装在真空传动装置上,可以随传动杆上下移动和左右转动。切伦科夫光经滤光片和焦距为25mm的佳能TV-16镜头成像在CCD摄像头上。由摄像头拍摄的图像信号经CA-MPE-1000F(H)型黑白图像采集卡读入计算机进行处理。图象采集卡具有外触发接口。通过从注入器控制系统的同步机中输出同步信号,经过单稳态电路,对采集卡进行外触发。 相似文献
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切伦科夫辐射“双成像法”测量电子束发射度 总被引:5,自引:0,他引:5
利用切伦科夫辐射,OTR或荧光靶等光学诊断方法进行发射度测量,国内外绝大部分实验是用CCD相机观测电子束打靶产生的光斑,变化四极透镜的磁场梯度,应用“三梯度法”计算出发射度.文中提出了一种新的“双成像法”测量方法,使切伦科夫辐射光通过一长焦距的消色差薄透镜,分别在焦平面和像平面获取图像.通过图像处理,前者可分析出电子束散角分布,后者可分析出电子束径向分布,从而直接得到均方根发射度.该方法对束流相空间和电荷密度分布无需假设,无需借助“三梯度法”,较其他常规测量方法具有实验装置更简便、测量精度更高和适用性更广等优点.文中给出了该测量方法对北京大学DC?SC光阴极注入器的发射度测量进行计算机模拟实验的结果和分析. 相似文献
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针对切伦科夫辐射特点,采用厚度尽量小的石英薄片作为转换靶,并将电子束以切伦科夫辐射角入射转换靶的形式构成一种电子束发散角分布的测量布局,并基于焦平面成像原理,研制了相应的电子束发散角光学测量系统。在强流脉冲直线感应加速器上完成了装置研制和测试工作,显示了电子束发散角分布测量系统可以获得电子束一定方向上的散角分布概况,测量结果具有一定的可信度,具有装置结构简单、数据处理难度低及速度快等特点。 相似文献
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针对直接测量16.7 MeV进行烧氚历史诊断所需聚变产额高的情况,模拟研究了利用14 MeV中子与副靶作用产生的非弹伽马进行烧氚历史诊断的情况,计算了几种材料14 MeV中子作用产生的次级伽马能谱以及切伦科夫辐射阈能之上的非弹伽马数目,对副靶材料和厚度进行了选择。计算了14 MeV中子产生的切伦科夫光子时间谱,分析了光电转换器件处伽马、电子以及正电子等噪声信号,分析了气体切伦科夫系统测量统计涨落与聚变中子产额之间的关系,确定了气体切伦科夫系统所适用的最低聚变中子产额,通过测量14 MeV中子与副靶产生的非弹伽马进行烧氚历史诊断较直接测量16.7 MeV伽马可将测量所需聚变中子产额降低2个量级。 相似文献
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聚变反应随时间变化诊断装置是惯性约束聚变(ICF)研究中的一项重要诊断设备, 使用蒙特卡罗程序Geant4研究了基于气体切伦科夫探测器的聚变反应随时间变化诊断装置的时间分辨和辐射转换效率,给出了优化后的辐射转换体材料厚度,以及CO2气室压力与长度。模拟计算表明,优化后的系统时间分辨可达22 ps左右,伽马-切伦科夫光子转换效率可达4.710-3 Cherenkov photons/gamma。 相似文献
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A New Measurement of Electron Beam Emittance with Cerenkov Radiation “Double Imaging” Method 下载免费PDF全文
GU An-Jia DING Yuan-Tao ZHAO Kui ZHANG Bao-Cheng QUAN Sheng-Wen LU Xiang-Yang CHEN Jia-Er 《中国物理C(英文版)》2003,27(2):163-168
A new way in electron beam emittance measurement with Cerenkov radiation "double imaging" method is proposed in this paper. In the standard emittance measurements with optical diagnostics such as Cerenkov radiation, OTR (Optical Transition Radiation), fluorescence screen or BMP (beam profile monitor) etc., the emittance is indirectly calculated through quadrupole-scanning technique, with the prior ssumption that the beam phase space density distribution is ellipse, which will certainly induce systematic error when the beam profile is quite irregular or the space-charge effects can not be omitted. In proposed method, the Cerenkov radiation pass through a 1-meter focal-length thin convex lens, and a CCD camera is used to capture two images of Cerenkov radiation at the focal plane and at the image plane of the lens respectively. Then, with image processing technique, we acquire the angular divergence information of the electron beam from the image of the focal plane and the radial distribution information from the image of the image plane, which we call Cerenkov radiation "double imaging" method. Therefore, the emittance can be directly attained according to the definition of the RMS emittance. By this method, we can measure the actual phase space distributions without making any prior assumptions about the density distributions. Compared with other general measurements, this "double imaging" method has advantages of simpler equipment, higher precision and wider application. This paper also presents the computer simulation results of emittance measurement on the DC-SC (DC-Superconducting) photocathode injector of PKU-SCAF (Peking University Superconducting Accelerator Facility) being built at Peking University. 相似文献
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给出双介质片平面波导契伦科夫自由电子激光波导模式的色散关系,求出器件的单程增益并证明存在一组新的波导模式__奇模。讨论了器件的工作频率和单程增益随介质片厚度、电子束能量和电子束通道宽度的变化关系。还研究了这组奇模对器件的影响。 相似文献
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为探索激光在束流截面测量上的应用,在北京正负电子对撞机二期工程(BEPCⅡ)的负电子传输线上建立了激光扫描系统。研究了激光扫描测量束流截面的相关计算方法。对激光和电子束相互作用、光子在介质中的切伦科夫辐射等过程进行了GEANT4模拟。对脉冲激光器进行了调试,测量了激光的脉宽、尺寸、功率等各项参数。设计并搭建了激光扫描系统的光路,编写了激光系统的机械扫描部件的控制软件。搭建了用于探测康普顿光子的契伦科夫探测器系统。激光的扫描、控制、以及激光参数的在线监测等系统工作正常,能满足激光扫描实验需要。 相似文献
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Soln J. 《IEEE transactions on plasma science. IEEE Nuclear and Plasma Sciences Society》1994,22(5):526-529
The observability of the helical Cerenkov effect as a novel radiation source is discussed. Depending on the value of the index of refraction of the medium, the strength of the uniform magnetic field, and the electron beam energy, helical Cerenkov radiation can occur in the same spectral regions as the ordinary Cerenkov effect, that is, from microwave to visible wavelengths. From the kinematics point of view, I argue that for a microwave wavelength of 10-1cm this effect should be observable in a medium with an index of refraction of 1.4, with a beam energy of 3 MeV, and a uniform magnetic field of 4 T. On the specific level, however, for the sake of simplicity, I discuss the observability of this effect for visible light with the central wavelength of 5×10-5 cm which can be achieved with 2 MeV in beam energy, silica aerogel as a medium (with an index of refraction of 1.075), and uniform magnetic fields from 5 to 10 T. For a 10-T magnetic field, I calculate that in the visible region of 250 to 750 nm an electron will produce a photon per 10 cm of traveled length. As to the stimulated helical Cerenkov emission, I estimate that respectable gains are possible even if the beam passes close to the dielectric rather than through it. In addition to being potentially a new radiation source, the helical Cerenkov effect could possibly be used as a detector of radiation by energetic electrons that are trapped in a medium by strong magnetic fields 相似文献
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A. Bodek W. Marsh M. V. Purohit P. S. Auchincloss R. Blair M. A. Ruiz F. J. Sciulli M. H. Shaevitz H. E. Fisk T. Kondo S. Pordes P. A. Rapidis D. D. Yovanovitch M. Abolins R. Brock D. Owen K. A. Jenkins O. Fackler 《Zeitschrift fur Physik C Particles and Fields》1983,18(4):289-299
We have observed Cerenkov light, well below threshold, in an integrating Cerenkov counter used to determine particle composition of the secondary hadron beam, which is the source of Fermilab narrow-band neutrinos. The phenomenon can be understood in terms of diffraction effects in a finite length counter caused by radiation emitted by particles traversing the counter even when it is evacuated. At zero pressure, the light can be considered as transition radiation produced when particles enter and leave the counter. A standard Cerenkov diffraction formula describes both the normal Cerenkov radiation and the light emitted below Cerenkov threshold. 相似文献