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Theory, Design and Tests on a Prototype Module of a Compact ...

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16 2. LINAC AND SCL ACCELERATORS<br />

f [GHz]<br />

3.08<br />

3.06<br />

3.04<br />

3.02<br />

3<br />

2.98<br />

2.96<br />

2.94<br />

f<br />

ac<br />

f<br />

cc<br />

2.92<br />

0 0.2 0.4 0.6 0.8 1<br />

φ/π<br />

f [GHz]<br />

3.1<br />

3.08<br />

3.06<br />

3.04<br />

3.02<br />

3<br />

2.98<br />

2.96<br />

f<br />

ac<br />

f<br />

cc<br />

2.94<br />

0 0.2 0.4 0.6 0.8 1<br />

φ/π<br />

Figure 2.9. The dispersi<strong>on</strong> diagrams in the case <strong>of</strong> a<br />

biperiodic structure with fa = 3 GHz, fc = 3 GHz,<br />

k = 0.04, k2 = 0.005 <str<strong>on</strong>g>and</str<strong>on</strong>g> k3 = 0 <strong>on</strong> the left <str<strong>on</strong>g>and</str<strong>on</strong>g><br />

fc = fa/ √ 1 − k2 <strong>on</strong> the right.<br />

fa; the total number <strong>of</strong> cavities is therefore 4N + 1. The coupling<br />

between accelerating <str<strong>on</strong>g>and</str<strong>on</strong>g> coupling cavities is k, between n<strong>on</strong>-adjacent<br />

accelerating cells is k2, <str<strong>on</strong>g>and</str<strong>on</strong>g> between coupling cells is k3. With the<br />

hypothesis <strong>of</strong> infinite quality factor, the dispersi<strong>on</strong> formula is [14]<br />

k 2 cos 2 <br />

φ = 1 − f 2 a<br />

f 2 <br />

+ k2 cos 2φ 1 −<br />

q<br />

f 2 c<br />

f 2 <br />

+ k3 cos 2φ , (2.8)<br />

q<br />

where φ is the phase advance. In the previous secti<strong>on</strong> we saw that<br />

for a finite structure the phase advance can assume <strong>on</strong>ly a finite set<br />

<strong>of</strong> value, the number <strong>of</strong> which is equal to the number <strong>of</strong> res<strong>on</strong>ators.<br />

The previous relati<strong>on</strong> (2.8) shows that there are two soluti<strong>on</strong> for the<br />

φ = π/2 frequency:<br />

f ac<br />

π/2 =<br />

fa<br />

√ , f<br />

1 − k2<br />

cc<br />

π/2 =<br />

fc<br />

√ ,<br />

1 − k3<br />

that deals to a forbidden range <strong>of</strong> frequency, which is the stop-b<str<strong>on</strong>g>and</str<strong>on</strong>g>, as<br />

it is shown in figure 2.9 (left). If k2 = 0, then is sufficient to choose<br />

fa = fc, where if k2 = 0 <strong>on</strong>e has to choose fc = fa/ √ 1 − k2, the result<br />

<strong>of</strong> this sec<strong>on</strong>d case is shown in the figure 2.9 (right).<br />

4. LIBO Specificati<strong>on</strong>s<br />

LIBO is a 3 GHz side coupled prot<strong>on</strong> linac. It was c<strong>on</strong>ceived as a<br />

LInac BOoster 5 , intended to be mounted downstream <strong>of</strong> a cyclotr<strong>on</strong><br />

<strong>of</strong> about 60 MeV (<strong>of</strong> which many exist in hospitals <str<strong>on</strong>g>and</str<strong>on</strong>g> physics laboratory),<br />

with the aim to boost the energy <strong>of</strong> the prot<strong>on</strong> beam up to<br />

200 MeV, an energy needed for therapy <strong>of</strong> deep seated tumors. All the<br />

matters c<strong>on</strong>cerning this secti<strong>on</strong> are reported in [22, 23, 24, 25].<br />

The beam intensity needed for prot<strong>on</strong>therapy is relatively small,<br />

about 2 · 10 10 particles per sec<strong>on</strong>d, i.e. a few nanoamperes, while the<br />

5 This is the origin <strong>of</strong> word LIBO.

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