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WEPGW053 |
Study with Wire Scanner and Beam Loss Monitor at CSNS-LINAC |
2598 |
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- J.L. Sun, R.Y. Qiu, T. Yang
IHEP CSNS, Guangdong Province, People’s Republic of China
- J.M. Tian, T.G. Xu, Zh.H. Xu, L. Zeng
IHEP, Beijing, People’s Republic of China
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China Spallation Neutron Source (CSNS) consists of 80 MeV H− LINAC, 1.6 GeV RCS, RTBT line and one target. Many wire scanners and beam loss monitors (BLM) distributed along the LINAC and the RTBT for the profile and beam loss measurement. For the wire scanner, signal on the wire induced by the secondary electron is used for the profile measurement. Signal lost may happen when the wire or the signal chain shorted, thus a backup readout chain is required for the accident condition. As for the BLM, it is difficult to do the online calibration to see how sensitive the monitor is. Based on the two requests above, a crosscheck study was carried out recently, one wire scanner and the BLM next to it were chose at LINAC and RTBT. Both wire signal and BLM signal were recorded while the wire scanner crossing the beam. We found these two type of signals have the same accuracy for the profile measurement, and ~ 1 μA beam loss induced by the wire disturbance can be detected. Also thermal electron emission suspected happening during the measurement. More detailed experiment will be carried out in December. Secondary electron emission efficiency of the tungsten wire and thermal electron emission rate will be verified then.
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DOI • |
reference for this paper
※ https://doi.org/10.18429/JACoW-IPAC2019-WEPGW053
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About • |
paper received ※ 14 May 2019 paper accepted ※ 21 May 2019 issue date ※ 21 June 2019 |
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THPTS037 |
The Deformation-Stress Simulation and Measurement of Titanium Foil Strip for Hadron Monitor |
4187 |
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- A.X. Wang, J.X. Chen, H.Y. He, L. Liu, X.J. Nie, C.J. Ning, J.L. Sun, G.Y. Wang, J.B. Yu, Y.J. Yu, J.S. Zhang, D.H. Zhu
IHEP CSNS, Guangdong Province, People’s Republic of China
- L. Kang
IHEP, Beijing, People’s Republic of China
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The measurement of beam profile by hadron monitor is in fact the measurement of the positive current after the secondary electrons escaped. According to the situation that the number of beam particles is small and the current signal is weak, the material titanium with high secondary electron generation rate is select by material comparison, and the foil strip type is used to increase the cross section area to obtain lager current level. On account of dead weight itself, as well as thermal expansion and contraction, the foil strip shall be loose. The loosen strip will deviate from its theoretical position, and cause the measuring error. Therefore, the deformation-stress of Ti foil strip (1000*50*0.1) was simulated under the pretension (10~90N) with the finite element software ANSYS. A set of experiment device with pretension adjustment and heating for the foil strip was designed, and then the deformation-stress was tested by a high precision 3-D imaging measurement system. Compared with the simulation results, the pretension would better set at about 50N.
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DOI • |
reference for this paper
※ https://doi.org/10.18429/JACoW-IPAC2019-THPTS037
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|
About • |
paper received ※ 12 May 2019 paper accepted ※ 19 May 2019 issue date ※ 21 June 2019 |
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Export • |
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※ LaTeX,
※ Text/Word,
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