for beam lines with paraxial beams
Code: COSY Infinity:
(x, a, y, b, l, dK, dm, dz)
Needed for complex ion-optical systems including several
charge states
different masses
velocities (e.g. Wien Filter)
higher order corrections
Not defined in the figure are:
dK = dK/K = rel. energy
dm = dm/m = rel. energy
dz = dq/q = rel. charge change
a = px/p0
b = py/p0
All parameters are relative
to “central ray” properties
Not defined in the figure are:
dp/p = rel. momentum
l = beam pulse length
All parameters are relative
to “central ray”
central ray
Note: Notations in the Literature is not consistent! Sorry, neither will I be.
Slide 11
Ray at initial
Location 1
TRANSPORT Coordinate System
Slide 12
Ray at initial
Location 0
Ray after element at
Location t
6x6 Matrix
representing
optic element
(first order)
Note: We are not building “random” optical elements.
Many matrix elements = 0
because of symmetries, e.g. mid-plane symmetry
(2)
Slide 13
TRANSPORT matrices of a Drift and a Quadrupole
For reference of TRANSPORT code and formalism:
K.L. Brown, F. Rothacker, D.C. Carey, and Ch. Iselin,
TRANSPORT: A computer program for designing
charged particle beam transport systems, SLAC-91,
Rev. 2, UC-28 (I/A), also: CERN 80-04 Super Proton
Synchrotron Division, 18 March 1980, Geneva,
Manual plus Appendices available on Webpage:
ftp://ftp.psi.ch/psi/transport.beam/CERN-80-04/
David. C. Carey, The optics of Charged Particle Beams,
1987, Hardwood Academic Publ. GmbH, Chur Switzerland
Slide 14
Transport of a ray though a system of beam line elements
Ray at initial
Location 0
(e.g. a target)
Ray at final
Location n
6x6 Matrix
representing
first optic element
(usually a Drift)
xn = Rn Rn-1 … R0 x0
Complete system is represented by
one Matrix Rsystem = Rn Rn-1 … R0
(3)
(4)
Slide 15
Geometrical interpretation of some TRANSPORT matrix elements
Wollnik, p. 16
Focusing Function
(x|a) Wollnik
= dx/dQ physical meaning
= (x|Q) RAYTRACE
= R12 TRANSPORT
Achromatic system:
R16 = R26 = 0
Slide 16
Defining a BEAM