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Beam<br />

Synchronism y condition<br />

The distance between accelerating gaps is proportional to particle velocity<br />

Electric field<br />

(tti (at time tt) 0 )<br />

1<br />

0.5<br />

0<br />

0 2 0 4 0 6 0 8 0 1 0 0 1 2 0 z<br />

-0 .5<br />

-1<br />

l=βλ/2<br />

Example: a linac superconducting 4-cell<br />

accelerating structure<br />

Synchronism condition:<br />

t (travel between centers of cells) = T/2<br />

l 1<br />

=<br />

βc<br />

2 f<br />

l<br />

β c<br />

= =<br />

2 = = f<br />

βλ<br />

2<br />

1. In an ion linac cell length has to increase (up to a factor 200 !) and the linac will<br />

be made of a sequence of different accelerating structures (changing cell<br />

length, frequency, operating <strong>mode</strong>, etc.) matched to the ion velocity.<br />

2. For electron linacs, β =1, l =λ/2 → An electron linac will be made of an injector +<br />

a series i of f id identical ti l accelerating l ti structures, t t with ith cells ll all ll the th same length l th<br />

Note: in the example above, we have synchronism only if we neglect the<br />

increase in beta inside the structure !<br />

4

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