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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 stages used to position the apertures will have positioning precision < 10 µm and angular<br />

precision of < 1 mrad.<br />

Attenuator<br />

Some experiments require a local attenuator for calibration and to prevent damage to<br />

sensitive components during alignment. The local attenuator will have a design very similar to the<br />

solid attenuator located upstream in the Front End Enclosure (see Section 9.2.2.1).<br />

Beam Intensity Monitors<br />

Beam intensity monitors are required to measure the absolute flux incident on the samples<br />

and the amount of flux transmitted through the samples. These monitors will be of the ion<br />

chamber type described in the facility diagnostics section (Section 9.4.2.3).<br />

Sample Chamber<br />

The sample chamber in Hutch A2 will be instrumented for studies required to characterize the<br />

interaction between the FEL pulse and matter. In addition to sample holders and photon<br />

spectrometers, it will include electron and ion time-of-flight spectrometers.<br />

Beam Stop<br />

At the back end of Hutch A2 is an insertable beam stop with integral burn-through detector.<br />

9.2.2.4 Hutch A4<br />

Hutch A4 will initially be used for commissioning diagnostics, which will be housed in a<br />

diagnostics tank. See Section 9.4.2.<br />

Fixed Mask and Beam Stop<br />

At the back end of Hutch A4 is an insertable beam stop with integral burn-through detector.<br />

Behind the beam stop is a fixed mask with 4.5 mm diameter aperture, identical to the fixed masks<br />

in the Front End Enclosure. As with those masks, its purpose is to cut the divergence of the<br />

spontaneous radiation, so that all transmitted radiation remains within the beam pipe. The<br />

coherent FEL radiation cannot strike this mask, and so peak power is not a concern.<br />

9.2.2.5 Inter-Hall Transport<br />

A beam pipe connects the two main halls through a tunnel. It is about 250 m long. Access<br />

will be available along the length of the tunnel. In the center of the tunnel, a diagnostics tank will<br />

permit beam intensity and position measurements.<br />

9.2.2.6 Hutch B1<br />

The first hutch in Hall B will contain optical elements, which condition the x-ray beam for<br />

the Hall B experiments (see Figure 9.14). Only one such element will be included in the initial<br />

<strong>LCLS</strong>, though space is made available for future optics. Hall B is intended primarily for<br />

experiments, which prefer to be far from the source, in order to reduce the peak intensity or to<br />

allow focusing to a minimum spot size.<br />

9-20 ♦ — 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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