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Superconducting RF cavities for High Current Energy Recovery Linacs

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Cavity Design<br />

1<br />

B<br />

alpha<br />

a<br />

Normalized units<br />

0.8<br />

0.6<br />

E pk /E acc<br />

0.4 H pk /E acc [mT/(MV/m)]<br />

Iris Radius - R iris<br />

R/Q [Ω]<br />

0.2<br />

cell coupling<br />

dF/dR equator [MHz/mm]<br />

0<br />

6 6.5 7 7.5 8 8.5 9 9.5 10<br />

Iris Radius [cm]<br />

1<br />

D<br />

A<br />

b<br />

d<br />

Riris<br />

L<br />

Iris Radius, R iris<br />

8.5 [cm]<br />

Wall Angle, α<br />

25 [deg]<br />

Equatorial Ellipse, R = B 1.0<br />

A<br />

Iris Ellipse, r = b 1.1<br />

a<br />

Cav. wall to iris plane, d 2.5 [cm]<br />

Half Cell Length, L = λβ 10.65 [cm]<br />

4<br />

H = D − (R iris + b + B) 4.195 [cm]<br />

Cavity Beta, β = v 1.0<br />

c<br />

Normalized units<br />

Normalized units<br />

Normalized units<br />

0.9<br />

0.8<br />

E pk /E acc<br />

H pk /E acc [mT/(MV/m)]<br />

0.7<br />

R/Q [Ω]<br />

cell coupling<br />

Wall Angle (α)<br />

dF/dR equator [MHz/mm]<br />

0.6<br />

10 12 14 16 18 20 22 24 26<br />

1<br />

0.95<br />

0.9<br />

0.85<br />

0.8<br />

1<br />

0.95<br />

0.9<br />

0.85<br />

α [deg]<br />

Iris Ellipse Ratio (r=b/a)<br />

1 1.5 2 2.5<br />

Iris ellipse ratio<br />

E pk /E acc<br />

H pk /E acc [mT/(MV/m)]<br />

R/Q [Ω]<br />

cell coupling<br />

dF/dR equator [MHz/mm]<br />

dF/dR equator [MHz/mm]<br />

0.8<br />

0.6 0.8 1 1.2 1.4 1.6 1.8 2<br />

Equator ellipse ratio<br />

Equator Ellipse Ratio (R=B/A)

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