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LCLS Conceptual Design Report - Stanford Synchrotron Radiation ...

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New<br />

Solid-State<br />

Sub-Booster<br />

and Electronic<br />

Phase Shifter<br />

IPA -<br />

Isolator<br />

Phase<br />

Attenuator<br />

Klystron<br />

SLED<br />

Cavity<br />

Output<br />

Coupler<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 />

Sector Drive Line<br />

SSSB<br />

PIOP<br />

driver<br />

CAMAC<br />

Figure 7.60 Control system components at each klystron station.<br />

Sector Phase Reference Line<br />

PAD –<br />

Phase<br />

Amplitude<br />

Detector<br />

The Modulator-Klystron Support Unit (MKSU), which contains the drive hardware for the<br />

IPA, will need to be modified to accommodate the additional drivers for a low-power phase<br />

shifter and high power attenuator.<br />

A new Parallel Input/Output Processor (PIOP) for the CAMAC control of the MKSU will be<br />

designed to accommodate the higher resolution and characteristics of the low-power phase<br />

shifter. The new PIOP will also incorporate software to allow for pulse-to-pulse feedback and<br />

more diagnostics. The existing PIOP is based on obsolete hardware and cannot be upgraded<br />

without extensive redesign work.<br />

7.7.3.3 Master Oscillator<br />

The present Main Drive Line (MDL) transmits 476 MHz along the linac from sector-0 where<br />

it is derived from a master oscillator VCO at 8.5-MHz. The 8.5-MHz coincides with the<br />

revolution frequency of the damping rings. The frequency shifts on the MDL for the purposes of<br />

PEP II injection are not compatible with the fixed frequency, mode-locked laser of the <strong>LCLS</strong><br />

photoinjector.<br />

A second master oscillator will instead be housed at the <strong>LCLS</strong> injector, as shown in Figure<br />

7.61. This new master oscillator will be phase locked to the MDL to allow for straight ahead<br />

beams being run down the <strong>LCLS</strong> portion of the linac for end station experiments. The master<br />

oscillator will be based on a crystal oscillator VCO in a temperature-stabilized oven. The crystal<br />

frequency will be chosen to be compatible with the mode-lock frequency of the laser and be a<br />

sub-harmonic of 2856 MHz.<br />

7-86 ♦ A C C E L E R A T O R

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