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High Brightness Electron Beam Diagnostics and their ... - CASA

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Horizontal Dispersion (m)<br />

Arc 1 ‘‘back−leg’’<br />

extr. chic.<br />

Arc 2<br />

−1<br />

20<br />

Figure3.2:HorizontalDispersion(topgraph)<strong>and</strong>transversebetatronfunctions(bottomgraph)<br />

βx 15<br />

βy 10<br />

manyfactorsthatcancausetherealmachinetobedierentfromthenumericalmodel.Amongthe forthenominalsettingsofthemagneticoptics.<br />

5<br />

causesofthesediscrepancies,themostusualarealignmenterrors,magnetdisfunctions,etc...Hence itisofprimeimportance,intherstphaseofcommissioningoftheaccelerator,todiagnosethese defects<strong>and</strong>potentiallyxorunderst<strong>and</strong>themtomatchascloseaspossiblethenumericalmodel Thoughthedriver-acceleratordesignisessentiallyspeciedvianumericalsimulations,thereare 3.3MeasurementoftheTransverseResponse<br />

0<br />

0 20 40 60 80 100<br />

tothe\asbuilt"accelerator.Inthissectionwereportonmeasurementofthetransverselattice<br />

Distance From Cryomodule Exit (m)<br />

responseofthedriveracceleratoralongtherecirculator.Inthisreport,wehaveonlyconcentrated ontwotypesofmeasurements:(1)trytoverifythattherstordertransfermatrixusedinthe modelisclosetothemachine,(2)measurepreciselythedispersion(i.e.thetransverseposition dependenceonenergy)functionintheback-legtransferline.<br />

Betatron Functions (m)<br />

2<br />

1<br />

0<br />

Compressor<br />

Undulator<br />

Decompressor<br />

reinj chic.

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