mode - CERN Accelerator School
mode - CERN Accelerator School
mode - CERN Accelerator School
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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