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LCLS Conceptual Design Report - Stanford Synchrotron Radiation ...

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ε n,rms (µm)<br />

3<br />

2<br />

1<br />

4-2001<br />

8560A1<br />

L C L S C O N C E P T U A L D E S I G N R E P O R T<br />

98 MV/m 123 MV/m 147 MV/m 172 MV/m<br />

E o = 143 MV/m<br />

ε n,rms = 1.06 µm<br />

B z = 3.193 kG<br />

0<br />

2 3 4<br />

B z (kG)<br />

Figure 6.10 Emittance versus cathode field strength and peak solenoidal magnetic field.<br />

Prototype guns have been operated for limited periods with fields up to 140 MV/m. However,<br />

as the field is increased above 100 MV/m, not only does the dark current typically increase rather<br />

dramatically (quickly exceeding the photocurrent), but the frequency and intensity of rf<br />

breakdowns also increases. RF breakdowns tend to leave pits in the cathode surface that lead to<br />

nonuniform emission. At the GTF, using a Cu cathode, 120 MV/m has been the typical operating<br />

field.<br />

PARMELA simulations (See Section 6.6.4, Sensitivity Study) indicate the ratio of the field in<br />

the full cell to half cell should be close to unity. Unbalanced fields can lead to large correlated<br />

energy spreads exiting the gun (as designed into thermionic rf guns) and subsequent emittance<br />

growth. The <strong>LCLS</strong> gun will incorporate calibrated field probes in both cells to set and monitor<br />

the field ratio.<br />

6.3.3 Symmetrization<br />

The emittance growth due to multipole modes of Ez in a gun cavity with a conventional<br />

asymmetric rf coupler (as for the earlier BNL 1.5-cell gun) is estimated to contribute ~1 µm to the<br />

transverse emittance [22]. This growth is dominated by the dipole mode and the contribution<br />

from the higher order modes is less than 0.1 µm. Therefore the higher order modes can be<br />

neglected. Symmetrization in the prototype gun is achieved by including a second identical<br />

“coupling” hole (which is also used for vacuum pumping) directly across from the rf waveguide<br />

coupling hole. This reduces the field amplitude dipole term by an order of magnitude over the<br />

unsymmetrized case. Further symmetrization of the dipole field phase can be achieved by<br />

utilizing a symmetric power feed instead of a single-sided feed. This is done with a magic tee<br />

6-18 ♦ I NJECTOR

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