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

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ε x (mm−mrad)<br />

Nominal<br />

6<br />

4<br />

2<br />

cryounitexitversustheemittancesolenoidmagneticeld.<br />

10<br />

Misaligned<br />

9<br />

Phase-PhaseCorrelationMeasurement Figure6.8:Measured(squares)<strong>and</strong>predictedtransverseemittances(solid<strong>and</strong>dashlines)atthe<br />

8<br />

7<br />

6<br />

5<br />

4<br />

Nominal<br />

3<br />

2<br />

RF-inducedsteeringwhich,inturn,dependsontheinjectionofthebuncheswithrespecttothe<br />

3000 3200 3400 3600 3800<br />

RFacceleratingeldinthecryounit.Henceatthepickupcavitylocation,theTOFofthebunch SimilarlytothebunchcompressioneciencydiagnosticsdescribedintheChapter3,theinjectoris instrumentedwithapickupcavitythatcanbeusedtomeasurethetimeofarrivalofabunch<strong>and</strong> consequentlydeterminephase-phasecorrelationbymodulatingtheRF-phaseofthephotocathode drivelaser.UnfortunatelyinthecaseoftheFELinjector,thepickupcavityislocatedinadispersive regionwhichrendersthetime-of-ight(TOF)dependentonotherparameters4,inparticularto<br />

Solenoid Magnetic Field (Gauss cm)<br />

centroidemittedatthephotocathodesurfacewithinitialphaseiwithrespecttothe\zerocrossing"bunch(i.e.thebunchforwhichtheTOFiszerobydenition)is: whereRFistheTOFcontributionduetotheRF-inducedsteering:RF=Rc!f ;c,i,<strong>and</strong>farerespectivelythelocationofthecryounitexit,thephotocathodesurface,<strong>and</strong>the pickupcavity. TheRFsteeringisdueto(1)theRFtransverseequationofmotioninanacceleratingcavity,<strong>and</strong> (2)theforwardpower<strong>and</strong>highordermodecouplerinducedkicks.Toquantifythecontribution oftheRF-steeringinthephase-phasecorrelationmeasurement,wehavecomparedphase-phase f=RF+Ri!f 55i+Ri!f 56i 51xc+Rc!f 52x0c (6.15)<br />

correlationmapsgeneratedvianumericalsimulationusingparmelawithtwodistinctmodelsof 4ThenecessityofstudyingcarefullythispointwasbroughttomyattentionbyD.R.Douglas<br />

ε y (mm−mrad)<br />

12<br />

10<br />

8<br />

Misaligned

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