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mode - CERN Accelerator School

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<strong>mode</strong> 0<br />

<strong>mode</strong> π/2<br />

<strong>mode</strong> 2π/3<br />

<strong>mode</strong> π<br />

More on standing wave<br />

structures<br />

E<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

0 50 100150 200 250<br />

1.5<br />

1<br />

0.5<br />

0<br />

-0.5 0<br />

-1<br />

-1.5<br />

50 100150 200 250<br />

1.5<br />

1<br />

0.5<br />

0<br />

-0.5 0 50 100 150 200 250<br />

-1<br />

-1.5<br />

1.5<br />

1<br />

0.5<br />

0<br />

-0.5 0 50 100 150 200 250<br />

Standing wave <strong>mode</strong>s are named from the<br />

phase difference between adjacent cells: in<br />

the example above, <strong>mode</strong> 0, π/2, 2π/3, π.<br />

In standing wave structures, cell length can<br />

be matched to the particle velocity !<br />

-1<br />

-1.5<br />

z<br />

→ These STANDING WAVE MODES<br />

are generated by the sum of 2<br />

traveling waves in opposite<br />

directions, adding always in the same<br />

way in the different cells.<br />

→ For acceleration, the particles must<br />

be in phase with the E-field on axis.<br />

We have already seen the π <strong>mode</strong>:<br />

synchronism condition for cell length<br />

l = βλ/2.<br />

→ Standing wave structures can be<br />

used for any β (→ ions and<br />

electrons) and can follow the<br />

increase in β of the ions.<br />

Synchronism conditions:<br />

0-<strong>mode</strong> : l = βλ<br />

π/2 <strong>mode</strong>: 2 l = βλ/2<br />

π <strong>mode</strong>: l = βλ/2<br />

13

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