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LCLS Conceptual Design Report - Stanford Synchrotron Radiation ...

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γεx,y (µm) yn<br />

10<br />

0<br />

–10 –10 0 10<br />

0.8<br />

0.4<br />

0<br />

3-2001<br />

8560A88<br />

γεx<br />

γεy<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 />

xn<br />

ζ x,y (mm)<br />

x'n<br />

10<br />

0<br />

–10 –10 0 10<br />

–1 0<br />

1<br />

0<br />

–1 0 1<br />

∆z (mm) ∆z (mm)<br />

Figure 6.24 Normalized transverse phase space at the exit of L0 for 100K particles. (1) Distribution<br />

of particles in the beam (upper plots). The scales are derived from the right-hand figure<br />

in which the rms emittance ellipse in the x-x' plane (only) is normalized to a circle<br />

having a radius of unity. (2) Transverse normalized slice emittances (lower left plot) in<br />

both planes and mismatch parameter, ζ, (lower right plot) in both planes along the<br />

bunch z-axis. In this figure, the bunch head is at the left, as in the convention of<br />

Chapter 7, Accelerator.<br />

The phase space plots for a series of 9 slices identified in the lower right plot of Figure 6.24<br />

are displayed in Figure 6.25. The blue/dark background in each case is the full projection in the<br />

x-x' plane, identical to the upper right plot of Figure 6.24. The red/light area represents the<br />

distribution in the x-x' plane of the particles in the particular slice. Note that the "halo" (particles<br />

outside the main core) occurs primarily in the first (head) and last (tail) slices.<br />

1.0<br />

0.5<br />

xn<br />

ζ x<br />

ζ y<br />

6-53 ♦ I NJECTOR

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