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

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transversebeamsizeeectleadstoanunderestimateofthebunchlengthbyaapproximatelya factorof2.However,theeectofthebeamspotsizeisverysmallontheCSR<strong>and</strong>CTRspectrum. Inthecaseofellipsoidalbunch,i.e.theworstcasethatcanhappenintheIRFEL,theerrorisat the10%level. Hence,wewillassumethemeasurementofCTRorCSRintheIRFELisdirectlyrelatedtothe<br />

BFF (no unit)<br />

1.0<br />

0.8<br />

0.6<br />

0.4<br />

10 8<br />

10 9<br />

10 10<br />

10 11<br />

10 12<br />

10 13<br />

10 14<br />

10 15<br />

10 16<br />

0.2<br />

0.0<br />

10 8<br />

10 9<br />

10 10<br />

10 11<br />

10 12<br />

10 13<br />

10 14<br />

10 15<br />

10 16<br />

10<br />

(Hz)<br />

-12<br />

10 -11<br />

10 -10<br />

10 -9<br />

10 -8<br />

10 -7<br />

10 -6<br />

10 -5<br />

10 -4<br />

10 -3<br />

10 -2<br />

10 -1<br />

10 0<br />

10 8<br />

10 9<br />

10 10<br />

10 11<br />

10 12<br />

10 13<br />

10 14<br />

10 15<br />

10 16<br />

10<br />

(Hz)<br />

-12<br />

10 -11<br />

10 -10<br />

10 -9<br />

10 -8<br />

10 -7<br />

10 -6<br />

10 -5<br />

10 -4<br />

10 -3<br />

10 -2<br />

10 -1<br />

10 0<br />

Figure5.5:Eectoftransversebeamsizeonthe3D-BFF.Forthreedierenttypeofbunch(ellipsoidal,pancake<strong>and</strong>linechargebunch),theBFF(A),theCTR(B)<strong>and</strong>CSR(C)powerspectrum (B) (C)<br />

sizeeectorfromtheangularbunchformfactor. 5.3.1TheuseoftheBFFtocompute<strong>and</strong>monitorthebunchlength 0:3rad<strong>and</strong>aregivenfora20%frequencyb<strong>and</strong>width. longitudinalbunchdistribution,withoutany\contamination"comingfromthetransversebeam arenumericallycomputed.Thepowerspectrumarecomputedassuminganangularacceptanceof<br />

Underthe\linecharge"assumptionmentionedearlier,theBFFonlydependsonthebunchlength. Inthissection,wederiveasimplerelation,withoutmakinganyassumptionsonthebunchdensity function,thatallowsonetocomputethermsbunchlengthfromthebunchformfactor.Let'sstart withtheBFFdenition,byintroducingthewavelengthnumber=1=forconvenience,<strong>and</strong>by replacingtheexponentialfunctionintheFouriertransformbyitsTaylorexpansion:<br />

Power W/ A/20%BW<br />

(A)<br />

Power W/ A/20%BW<br />

z=100 m, r=1000 m<br />

(ellipsoidal bunch)<br />

z=0 m, r=1000 m<br />

(pancake bunch)<br />

z=100 m, r=0 m<br />

(line charge bunch)

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