mode - CERN Accelerator School
mode - CERN Accelerator School
mode - CERN Accelerator School
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Mechanical errors differences in<br />
frequency q y between cells <br />
to respect the new boundary conditions<br />
the electric field will be a linear<br />
combination of all <strong>mode</strong>s, with weight<br />
1<br />
2 2<br />
f − f<br />
(general case of small perturbation to an<br />
eigen<strong>mode</strong> system, system<br />
the new solution is a linear combination<br />
of all the individual <strong>mode</strong>s)<br />
The nearest <strong>mode</strong>s have the highest<br />
effect, and when there are many <strong>mode</strong>s<br />
on the dispersion curve (number of<br />
<strong>mode</strong>s = number of cells !) the<br />
difference in E-field between cells can<br />
be extremely high.<br />
Stability of long chains of<br />
coupled resonators<br />
0<br />
<strong>mode</strong> 0<br />
<strong>mode</strong> d π/2 /2<br />
<strong>mode</strong> 2π/3<br />
<strong>mode</strong> π<br />
ω<br />
E<br />
0 6.67 13.34 20.01 26.68 33.35<br />
0<br />
π/2<br />
1<br />
0.8<br />
0.6<br />
0.4<br />
0.2<br />
0<br />
0 50 100 150 200 250<br />
1.5<br />
1<br />
0.5<br />
0<br />
-0.5 0<br />
-1<br />
-1.5<br />
50 100 150 200 250<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<br />
-1<br />
-1.5<br />
50 100150 200 250<br />
π<br />
k<br />
z<br />
45