Theorem on Magnet Fringe Field

Technical Report · Sun Dec 31 23:00:00 EST 1995

DOI:https://doi.org/10.2172/1119474· OSTI ID:1119474

Wei, Jie ^[1]; Talman, Richard ^[2]

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1. Brookhaven National Lab. (BNL), Upton, NY (United States). Realativistic Heavy Ion Collider (RHIC)
2. Cornell Univ., Ithaca, NY (United States). Lab. of Nuclear Studies

Transverse particle motion in particle accelerators is governed almost totally by non-solenoidal magnets for which the body magnetic field can be expressed as a series expansion of the normal (b_n) and skew (a_n) multipoles, B_y+iB_x= $$∞\atop{_0^Σ}$$ (b_n + ia_n) (x+iy)ⁿ, where x, y, and z denote horizontal, vertical, and longitudinal (along the magnet) coordinates.

• Research Organization: Brookhaven National Laboratory (BNL), Upton, NY (United States)
• Sponsoring Organization: USDOE Office of Science (SC)
• DOE Contract Number: AC02-98CH10886
• OSTI ID: 1119474
• Report Number(s): BNL--102189-2013-IR
• Country of Publication: United States
• Language: English

Related Subjects

43 PARTICLE ACCELERATORS