Strong focusing
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In accelerator physics strong focusing or alternating-gradient focusing is the principle that the net effect on a particle beam of charged particles passing through alternating field gradients is to make the beam converge. By contrast "Weak focusing" is the principle that nearby circles, described by charged particles moving in a uniform magnetic field, only intersect once per revolution.
Earnshaw's theorem shows that simultaneous focussing in two directions at once is impossible. However, ridged poles of a cyclotron or two or more spaced quadrupole magnets (arranged in quadrature) alternately focus horizontally and vertically.[1]
Strong focusing was first invented at Brookhaven National Laboratory and deployed on the Alternating Gradient Synchrotron there. The theory was developed in 1957 by E. D. Courant and H. S. Snyder.[2] The theory revolutionised cyclotron design, and permitted very high field strengths to be employed, while massively reducing the size of the magnets needed by minimising the size of the beam. All current cyclotrons use strong focusing.
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[edit] Quadrupole magnets
Modern systems often use quadrupole magnets to focus the beam down as magnets give a more powerful deflection effect than earlier electrostatic systems at high beam kinetic energies. The quadrupole magnets refocus the beam after each deflection section.
This can be shown schematically as:
The quadrupoles are often laid out in what are called FODO patterns (where F focusses vertically and defocusses horizontally, and D focusses horizontally and defocusses vertically and O is a space or deflection magnet):
Following the beam particles in their trajectories through the focussing arrangement, the following oscillation patterns would be seen:
(Note: there is a known error in the above diagram- the field lines should alternate direction over time.)
[edit] Mathematical modelling
The effect of a set of focusing magnets can be expressed as a matrix.[3]
[edit] See also
- Electron gun uses cylindrical symmetric fields such as provided by a Wehnelt cylinder to focus an electron beam
