首页> 外文期刊>Nuclear Instruments & Methods in Physics Research. Section A, Accelerators, Spectrometers, Detectors and Associated Equipment >Spatial and temporal beam profile monitor with nanosecond resolution for CERN's Linac4 and Superconducting Proton Linac
【24h】

Spatial and temporal beam profile monitor with nanosecond resolution for CERN's Linac4 and Superconducting Proton Linac

机译:纳秒级分辨率的时空光束轮廓监测器,用于CERN的Linac4和超导质子直线加速器

获取原文
获取原文并翻译 | 示例

摘要

The Linac4, now being developed at CERN, will provide 160-MeV H beams of high intensity N = 2 × 10~(14) ions s~(-1). Before this beam can be injected into the CERN Proton Synchrotron Booster or future Superconducting Proton Linac for further acceleration, some sequences of 500-ps-long micro-bunches must be removed from it, using a beam chopper. These bunches, if left in the beam, would fall outside the longitudinal acceptance of the accelerators and make them radioactive. We developed a monitor to measure the time structure and spatial profile of this chopped beam, with respective resolutions △t~l ns and △x~2mm. Its large active area 40 mm × 40 mm and dynamic range also allows investigations of beam halos. The ion beam first struck a carbon foil, and secondary electrons emerging from the foil were accelerated by a series of parallel grid electrodes. These electrons struck a phosphor screen, and the resulting image of the scintillation light was guided to a thermoelectrically cooled, charge-coupled device camera. The time resolution was attained by applying high-voltage pulses of sub-nanosecond rise and fall times to the grids. The monitor has been tested with 700-ps-long UV laser pulses, and a 3-MeV proton beam. Its response over a wide range of beam intensities between N_e~5 and 4 × 10~8 electrons emitted from the foil per pulse was studied. The monitor can also be used to measure the profiles of antiproton beams in the future facilities of Facility for Low-energy Antiproton Ion Research (FLAIR) or Extra Low Energy Antiproton Ring (ELENA).
机译:目前正在欧洲核子研究组织(CERN)开发的Linac4将提供高强度N = 2×10〜(14)离子s〜(-1)的160MeV H光束。在将该光束注入CERN质子同步加速器或未来的超导质子直线加速器以进一步加速之前,必须使用光束斩波器从中去除一些500 ps长的微束序列。这些束如果留在光束中,将落在加速器的纵向接受范围之外,并使它们具有放射性。我们开发了一种监视器,用于测量该切碎光束的时间结构和空间轮廓,其分辨率分别为△t〜l ns和△x〜2mm。其较大的有效面积为40 mm×40 mm,动态范围也允许研究光束晕。离子束首先撞击碳箔,然后从箔中出来的二次电子被一系列平行的栅电极加速。这些电子撞击荧光屏,然后将闪烁光的图像引导至热电冷却的电荷耦合器件照相机。通过将亚纳秒上升和下降时间的高压脉冲施加到电网,可以达到时间分辨率。该监视器已经过700 ps长的UV激光脉冲和3-MeV质子束的测试。研究了它在N_e〜5和每个脉冲从箔片发射的4×10〜8电子之间的宽电子束强度范围内的响应。该监视器还可用于在低能反质子离子研究设施(FLAIR)或超低能反质子环(ELENA)设施的未来设施中测量反质子束的轮廓。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号