Volume 33 Issue 7
Jul.  2021
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Fang Jianwei, Hong Yuanzhi, Wang Yigang, et al. Design and establishment of cryogenic secondary electron yield measurement system[J]. High Power Laser and Particle Beams, 2021, 33: 074003. doi: 10.11884/HPLPB202133.210035
Citation: Fang Jianwei, Hong Yuanzhi, Wang Yigang, et al. Design and establishment of cryogenic secondary electron yield measurement system[J]. High Power Laser and Particle Beams, 2021, 33: 074003. doi: 10.11884/HPLPB202133.210035

Design and establishment of cryogenic secondary electron yield measurement system

doi: 10.11884/HPLPB202133.210035
  • Received Date: 2021-01-29
  • Rev Recd Date: 2021-06-15
  • Available Online: 2021-06-30
  • Publish Date: 2021-07-15
  • In the construction of Hefei advanced light facility (HALF), vacuum components of superconducting materials are widely used, especially superconducting radio frequency cavity. The superconducting cavity with the characteristics of high accelerating gradient, low beam impedance, high unloaded quality factor and low operating cost has become the first choice for large accelerators in the 21st century. However, electron cloud (EC) phenomenon is generated by the secondary electron emission on the surface of the superconducting cavity and cryogenic vacuum chamber. Deposition of extra dose secondary electron multiplicative power can induce thermal load increase in the cryogenic zone, superconducting cavity quench and so on. Therefore, reduction of the secondary electron emission in the superconducting radio frequency cavity is a great challenge for the design of HALF. On the basis of secondary electron yield (SEY) measurement system for room temperature materials, the authors independently designed the cryogenic sample rack to allow liquid helium to flow through the sample stage and cool sample by heat conduction. It was significant to calculate heat leakage for deciding refrigerating capacity and liquid helium consumption rate. After the system integration and debugging, the cooling performance test was carried out. The results show that cryogenic SEY measurement system was established.
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  • [1]
    Tang Y G, Wu C F, Wang L. Preliminary research of HOM for 100 MHz superconducting cavity in the pre-research project of HALS[J]. Journal of Physics: Conference Series, 2019, 1350: 012017. doi: 10.1088/1742-6596/1350/1/012017
    [2]
    温华明, 严陆光, 林良真. 超导在加速器中的应用概况[J]. 低温与超导, 2005, 33(1):46-49. (Wen Huaming, Yan Liuguang, Lin Liangzhen. Status of Superconductivity in large-scale particle accelerators[J]. Cryogenics And Superconductivity, 2005, 33(1): 46-49 doi: 10.3969/j.issn.1001-7100.2005.01.011
    [3]
    Padamsee H, Knobloch J, Hays T, et al. RF superconductivity for accelerators[J]. Physics Today, 1999, 52(7): 54.
    [4]
    李欣, 陈强, 辛天牧, 等. 射频超导腔加速性能的改进[J]. 强激光与粒子束, 2006, 18(9):1581-1584. (Li Xin, Chen Qiang, Xin Tianmu, et al. Performance improvement of RF superconducting cavity[J]. High Power Laser and Particle Beams, 2006, 18(9): 1581-1584
    [5]
    Valizadeh R, Malyshev O B, Wang S H, et al. Low secondary electron yield engineered surface for electron cloud mitigation[J]. Applied Physics Letters, 2014, 105: 231605. doi: 10.1063/1.4902993
    [6]
    郝建红, 丁武, 董志伟. 磁绝缘传输线振荡器中的次级电子倍增现象[J]. 物理学报, 2006, 55(9):4789-4794. (Hao Jianhong, Ding Wu, Dong Zhiwei. Moltipactor discharge in a magnetically insulated transmission line oscillator[J]. Acta Physica Sinica, 2006, 55(9): 4789-4794 doi: 10.3321/j.issn:1000-3290.2006.09.067
    [7]
    Price D, Benford J N. General scaling of pulse shortening in explosive-emission-driven microwave sources[J]. Plasma Science IEEE Transactions on, 1998, 26(3): 256-262. doi: 10.1109/27.700752
    [8]
    Cimino R, Collins I R, Furman M A, et al. Can low-energy electrons affect high-energy physics accelerators?[J]. Physical Review Letters, 2004, 93(1): 6855-6855.
    [9]
    Ye M, He Y N, Hu S G, et al. Suppression of secondary electron yield by micro-porous array structure[J]. Journal of Applied Physics, 2013, 113: 074904. doi: 10.1063/1.4792514
    [10]
    何鋆, 杨晶, 苗光辉, 等. 高性能多功能介质二次电子发射特性研究平台[J]. 强激光与粒子束, 2020, 32:033003. (He Yun, Yang Jing, Miao Guanghui, et al. High-performance multifunctional apparatus for studying secondary electron emission characteristics of dielectric[J]. High Power Laser and Particle Beams, 2020, 32: 033003
    [11]
    Kijima Y, Saito Y, Furuya T, et al. The secondary electron emission coefficient of the material for the superconducting cavity input coupler[J]. Shinku, 2002, 45(7): 599-603. doi: 10.3131/jvsj.45.599
    [12]
    Noer R, College C, Northfield, et al. Secondary electron yield of NB RF cavity surfaces[C]//The 10th Workshop on RF Superconductivity. 2001: 400-402.
    [13]
    Kuzucan A, Stri H, Taborelli M. Secondary electron yield on cryogenic surfaces as a function of physisorbed gases[J]. Journal of Vacuum Science & Technology A Vacuum Surfaces & Films, 2012, 30: 051401.
    [14]
    Spallino L, Angelucci M, Larciprete R, et al. On the compatibility of porous surfaces with cryogenic vacuum in future high-energy particle accelerators[J]. Applied Physics Letters, 2019, 114: 153103. doi: 10.1063/1.5085754
    [15]
    Spallino L. Material properties compliance with cryogenic vacuum for particle accelerators[J]. Journal of Vacuum Science & Technology B, 2020, 38: 032803.
    [16]
    Calder R, Grobner O, Mathewson A G, et al. Synchrotron radiation induced gas desorption from a Prototype Large Hadron Collider beam screen at cryogenic temperatures[J]. Journal of Vacuum Science & Technology A Vacuum Surfaces & Films, 1996, 14(4): 2618-2623.
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