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Lecture 6 - Transverse Optics III

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Courant and Snyder invariant fro one particle anywhere in the ring ... Conditions. Just like: HENCE. bounded. ACINST6 - E. Wilson 3 Oct--04 - Slide 11 ... – PowerPoint PPT presentation

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Title: Lecture 6 - Transverse Optics III


1
Lecture 6 - Transverse Optics III
ACCELERATOR PHYSICS MT 2004 E. J. N.
Wilson
2
Contents of previous lecture - Transverse Optics
II
  • Equation of motion in transverse co-ordinates
  • Check Solution of Hill
  • Twiss Matrix
  • Solving for a ring
  • The lattice
  • Beam sections
  • Physical meaning of Q and beta
  • Smooth approximation

3
Lecture 6 - Transverse Optics III Contents
  • Effect of a drift length and a quadrupole
  • Focusing in a sector magnet
  • The lattice
  • Calculating the Twiss parameters
  • Meaning of Twiss parameters
  • Stability diagram
  • Liouvilles theorem

4
Effect of a drift length and a quadrupole
Drift length
Quadrupole
5
Focusing in a sector magnet
6
The lattice (1 of SPS)

7
Calculating the Twiss parameters
THEORY
COMPUTATION (multiply elements)
Real hard numbers
Solve to get Twiss parameters
8
Meaning of Twiss parameters
  • e is either
  • Emittance of a beam anywhere in the ring
  • Courant and Snyder invariant fro one particle
    anywhere in the ring

9
Example of Beam Size Calculation
  • Emittance at 10 GeV/c

10
Stability diagram for FODO
Conditions
bounded
Just like
If motion is bounded then m must be real
HENCE
11
Liouvilles theorem
  • The area of a contour which encloses all the
    beam in phase space is conserved
  • This area pe is the emittance
  • It is the same all round the ring
  • NOT TRUE
  • during acceleration
  • in an electron machine where synchrotron emission
    damps

12
Summary
  • Effect of a drift length and a quadrupole
  • Focusing in a sector magnet
  • The lattice
  • Calculating the Twiss parameters
  • Meaning of Twiss parameters
  • Stability diagram
  • Liouvilles theorem
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