wang chao, tian jinshou, zhang meizhi, et al. Design of combined magnetic field system for magnetic-bottle time-of-flight spectrometer[J]. High Power Laser and Particle Beams, 2011, 23.
Citation:
wang chao, tian jinshou, zhang meizhi, et al. Design of combined magnetic field system for magnetic-bottle time-of-flight spectrometer[J]. High Power Laser and Particle Beams, 2011, 23.
wang chao, tian jinshou, zhang meizhi, et al. Design of combined magnetic field system for magnetic-bottle time-of-flight spectrometer[J]. High Power Laser and Particle Beams, 2011, 23.
Citation:
wang chao, tian jinshou, zhang meizhi, et al. Design of combined magnetic field system for magnetic-bottle time-of-flight spectrometer[J]. High Power Laser and Particle Beams, 2011, 23.
State Key Laboratory of Transient Optics and Photonics,Xi’an Institute of Optics and Precision Mechanics,Chinese Academy of Sciences,Xi’an 710119,China;
2.
School of Electronics Engineering,Xi’an University of Post and Telecommunication,Xi’an 710061,China;
3.
School of Science,Air Force Engineering University,Xi’an 710051,China
Based on the primary requirement for the magnetic field system in magnetic-bottle time-of-flight spectrometer, an appropriate combined inhomogeneous magnetic field system is designed. The inhomogeneous higher magnetic field part, with the highest field of 1.2 Ｔ, is produced by the combination of a permanent magnet and a pole piece with optimized shape. The magnet, known as NdFeB magnet, is one of rare earth permanent magnets in N52. The guiding uniform magnetic field of 1.0×10-3 T is provided by solenoid, with length of 3 m and radius of 3 cm. The pitch between the pole piece and the near end of used solenoid is determined to be 5 cm, which can satisfy the actual engineering needs．
DownLoad: