PENG Quan-ling, ZHOU Jian-xin, REN Fang-lin, YIN Bao-gui, DONG Lan, NI Gan-lin, SUN Zhi-rui, LI Li, ZHANG Zhuo, WEN Xue-mei, RUAN Yu-fang, XUE Ji-qin, ZHAI Ji-yuan, Lv Kun, PENG Yue-mei, WANG Dou, SUN Yi-peng, ZHANG Jiu-chang, DENG Chang-dong, YANG Mei, CHEN Fu-san, CHEN Yuan, YU Cheng-hui, WU Ying-zhi. Magnetic Field Measurement of BEPCⅡSuperconducting Magnets by Using Rotating Coil[J]. Atomic Energy Science and Technology, 2010, 44(5): 617-622. DOI: 10.7538/yzk.2010.44.05.0617
Citation: PENG Quan-ling, ZHOU Jian-xin, REN Fang-lin, YIN Bao-gui, DONG Lan, NI Gan-lin, SUN Zhi-rui, LI Li, ZHANG Zhuo, WEN Xue-mei, RUAN Yu-fang, XUE Ji-qin, ZHAI Ji-yuan, Lv Kun, PENG Yue-mei, WANG Dou, SUN Yi-peng, ZHANG Jiu-chang, DENG Chang-dong, YANG Mei, CHEN Fu-san, CHEN Yuan, YU Cheng-hui, WU Ying-zhi. Magnetic Field Measurement of BEPCⅡSuperconducting Magnets by Using Rotating Coil[J]. Atomic Energy Science and Technology, 2010, 44(5): 617-622. DOI: 10.7538/yzk.2010.44.05.0617

Magnetic Field Measurement of BEPCⅡSuperconducting Magnets by Using Rotating Coil

  • Superconducting interaction region (IR) magnets for Beijing Electron Positron Collider Upgrade Project (BEPCⅡ) are used for increasing the BEPCⅡ luminosity, correcting close orbit and coupling. These magnets are placed as close as possible to the interaction point (IP), immersed within the BESⅢ detector solenoid field of 1.0 T. These magnets are designed into two magnet packages at each side of the IP with each contained inside a magnet cryostat. Each superconducting magnet package includes several function magnets of SCQ, SCB/HDC, VDC, SKQ and AS. Some of them, such as SCQ, SCB/HDC, VDC, SKQ were measured by rotating coil, and the integrals field and high order harmonic contents, local field along the beam line are known in details. Comparing these results with that from BNL which were measured inside the vertical Dewar, it’s found that there were only small differences. Comparing with the results from the stretched wire, for SCQ and SCB as examples, it’s found that the differences for the main fields are less than 3×10-3. As a result, the method presented in the paper can be used for absolute magnetic field measurements.
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