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LCLS Conceptual Design Report - Stanford Synchrotron Radiation ...

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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 />

scanned during a period when the outside temperature was stable. The pulse-to-pulse amplitude<br />

stability over 2 seconds is 0.06% rms, measured at the PAD, as shown in Figure 7.59.<br />

Phase [ ° S−band]<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

0 5 10<br />

Time [sec]<br />

15 20<br />

200<br />

150<br />

100<br />

50<br />

0.071 ° rms<br />

0<br />

0.2 0.4 0.6 0.8 1<br />

Phase [ ° S−band]<br />

Figure 7.58 Pulse-to-pulse phase variations, and histogram, measured at PAD of a single klystron<br />

shows 0.07-degree S-band rms variation over 17 seconds.<br />

RF Amplitude [arb. units]<br />

sigma = 0.06%<br />

Time [klystron pulses]<br />

Figure 7.59 Pulse-to-pulse relative amplitude variations measured at the PAD of a single klystron<br />

shows 0.06% rms variation over 2 sec (horizontal axis is in 1/30-sec ticks).<br />

Analysis of the performance of the present linac shows that individual SLAC klystrons, when<br />

selected for superior stability, can meet <strong>LCLS</strong> pulse-to-pulse jitter tolerances over a short (~2 sec)<br />

time scale. Some improvements are planned for the rf distribution and control system. These will<br />

facilitate beam-based feedback control to be applied to the <strong>LCLS</strong> linac sections. Phase and<br />

amplitude control of individual klystrons will be implemented for parts of the linac as well as<br />

global sector controls. The phase gymnastics for PEP II injection need to be decoupled from the<br />

7-84 ♦ A C C E L E R A T O R

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