DocumentCode :
2414127
Title :
Third-order combined function bending magnets
Author :
Carey, David C.
Author_Institution :
Fermi Nat. Accel. Lab., Batavia, IL, USA
fYear :
1989
fDate :
20-23 Mar 1989
Firstpage :
1289
Abstract :
It is pointed out that a complete third-order description of a charged particle optical system must include a combined function bending magnet. The magnetic field can have dipole, quadrupole, sextupole, and octupole terms. Midplane symmetry is assumed. Each additional order in the optical analysis requires inclusion of an additional multipole in the field expansion. First-, second-, and third-order expansions require quadrupole, sextupole, and octupole terms, respectively. Third-order matrix elements can be derived by an iterative Green´s function solution of the differential equations of motion. Third-order transfer matrix elements arise not only from third-order terms in the equations of motion, but also from the cascading effect of second-order terms. Solutions have been derived and incorporated into the computer program Transport and Turtle
Keywords :
Green´s function methods; beam handling equipment; Green´s function; Transport and Turtle; charged particle optical system; combined function bending magnet; dipole; octupole; quadrupole; sextupole; third order matrix elements; third-order; Accelerator magnets; Differential equations; Green´s function methods; Laboratories; Magnetic analysis; Magnetic fields; Magnetic separation; Particle accelerators; Particle beams; Physics;
fLanguage :
English
Publisher :
ieee
Conference_Titel :
Particle Accelerator Conference, 1989. Accelerator Science and Technology., Proceedings of the 1989 IEEE
Conference_Location :
Chicago, IL
Type :
conf
DOI :
10.1109/PAC.1989.73425
Filename :
73425
Link To Document :
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