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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 />

The attenuator translation stages will provide motion in the X and Y directions with a<br />

precision of < 1 mm.<br />

Diagnostics Tanks<br />

Space is available downstream from the gas and solid attenuators for beam diagnostic<br />

measurements such as pulse intensity and pulse shape. The diagnostics will monitor the operation<br />

of the attenuators. See Section 9.4.2.<br />

Beam Stop with Burn-Through Detector<br />

At the downstream end of the Front End Enclosure there is an insertable beam stop. This<br />

device consists of an upstream beryllium section to reduce the peak power of the FEL beam, and<br />

downstream copper and heavy metal sections to absorb the full spectrum of the <strong>LCLS</strong>. The beam<br />

stop includes an integral burn-through detector, which, in case the beryllium section fails to<br />

insert, will protect the radiation absorbers and shut down the <strong>LCLS</strong>. The radiation absorbers are<br />

duplicated with separate control systems so that the risk of a radiation accident is negligible.<br />

Figure 9.9 Concept of the insertable beam stop with burn-through detector.<br />

9.2.2.2 Hutch A1<br />

The first hutch in Hall A (Figure 9.10) will contain optical elements which condition the x-<br />

ray beam for the Hall A experiments. Only one such element will be included in the initial <strong>LCLS</strong>,<br />

though space is made available for future optics. Hall A is intended primarily for high-intensity<br />

experiments, using the full bandwidth of the coherent FEL beam.<br />

9-14 ♦ — R A Y B E A M T R A N S P O R T A N D D I A G N O S T I C S

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