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

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densityprole,byactingontheotherthreeparametersitispossibletoreducethebeamcurrent withoutaectingonthephasespacedistribution.Naturallythefactwehavetouseareduced beamcurrentduringthemeasurementofthebeamparameterimpactsontheFELoperation<strong>and</strong> subsequentexperiments.Thereforesuchameasurementisinvasive.AswehaveseeninChapter2,<br />

Intensity (a.u)<br />

2<br />

7<br />

6<br />

5<br />

8<br />

109 4<br />

4<br />

3<br />

2<br />

-6 -3 0 3 6<br />

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.<br />

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10<br />

5<br />

2<br />

-6 -3 0 3 6<br />

Distance (mm)<br />

12<br />

10<br />

5<br />

22<br />

10<br />

5<br />

32<br />

10<br />

5<br />

42<br />

Figure4.12:Rawdatabeamprole(topgraph)<strong>and</strong>beamproleafterprocessing(background whichalsosynchronouslygeneratea5Vrectangularpulsewhosewidth<strong>and</strong>repetitionratearethe replicaofthemacropulse.Suchsignalcalledthe\beamsync"isavailablefromthecontrolsystem totriggerdataacquisitionsystems. Inthepresentcase,wetriggertheimageprocessingboardtograbonlythevideoframethatcon- atarepetitionrateupto74:85MHz.Allthebeamstructureisgeneratedbyamasteroscillator subtracted,ghostpulsecontributionremoved,...).<br />

tainsthebeamimage.Forsuchapurposeweusethefollowingsetup:the\beamsync"isdelayed by0:435msbeforebeingsenttothe\externaltrigger"inputoftheimageprocessingboard.The eachmacropulsecontainsbunches(whosechargecanbearbitraryvariedfrom0pCto135pC6)<br />

SomeprimaryoperationsonthisdatastreamcanbedirectlyperformedbytheCPUoftheimage processingboardinrealtime[39].Suchoperationsincludethecalculationof: delayissetsothatthedigitizeristriggeredatthenextincomingpulse. Thedigitizeddatastreamattheimageboardoutputconsistsofa660484arraymatrix,I(x;y). 6Intheresultspresentedinthisreportthemaximumchargeusedisapproximately60pC<br />

Intensity (a.u)

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