• 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