1 ELECTROMAGNETIC DESIGN
The designs for the two types of SNS cavities were dominated by the desire to keep the electric peak surface field at or below 27.5 MV/m and the magnetic peak surface field below 60 mT. At the same time the Lorentz force detuning coefficient should not exceed a value of . By choosing a cell-to-cell coupling of 1.5% for these six-cell cavities a reasonably small ratio of peak surface fields and accelerating fields could be realized [1], if four different half cell shapes were used. The fundamental power coupler (FPC) requirement for a value of about implied larger iris and equator diameters for the end half cells at the FPC side (see figure 1) compared to the center cells. Simulation calculations done with the center cell geometries and the full cavities showed that multipacting was unlikely. The specifications for the Lorentz coefficient require welded stiffening rings between the cell irises at a radius of 80 mm. The SNS cavities have Nb55Ti flanges throughout (DESY-type), sealed with AlMg3 gaskets: one at each tapered beam pipe end, two ports (one for each end) for the HOM couplers, rotated 115 degrees with respect to each other, a port for the field probe and one for the FPC. The coaxial FPC is the KEK design scaled to 805 MHz [2]. SNS cavities' electromagnetic parameters
Cavity | 0.61 | 0.81 |
---|---|---|
Frequency [MHz] | 805.000 | 805.000 |
2.71 | 2.19 | |
[mT/(MV/m)] | 5.72 | 4.72 |
279 | 483 | |
179 | 260 | |
Cell-to-cell [%] | 1.53 | 1.52 |
) | −2.07 | −0.43 |