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

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

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σ z (mm)<br />

0.2<br />

0.1<br />

Figure6.15:Variationofthebunchlengthversusthelinacacceleratingphaseperparmelasimu-<br />

0.1<br />

0<br />

−15 −10 −5 0 5 6 7 8 9<br />

lation(A)<strong>and</strong>measured(B)["measured"meansthebunchdistributionwasrecoveredfromthe<br />

∆φ (Deg) (parmela)<br />

∆φ (Deg) (experiment)<br />

CTRautocorrelationusingthetechniquementionedinChapter5].Comparisonbetweentheex-<br />

4<br />

3<br />

(C) Simulation<br />

(D)<br />

3<br />

2<br />

2 Measurement<br />

1<br />

1<br />

extentenergyspread)degradationinthebendingsystemoftheIRFEL.Forsuchapurposeswe perimental<strong>and</strong>simulatedbunchlongitudinaldistribution(C).TotalCTRpowersignalmeasured<br />

0<br />

0<br />

needtoconsiderinthefewfollowingsectionswhatarethemechanismsthatcanleadtoanincrease duringplot(B)experiment(D).<br />

−0.4 −0.2 0 0.2 0.4 5 6 7 8 9<br />

oftheemittance.Itseemswec<strong>and</strong>ividesuchmechanismintotwocategories:therstonearedue Inthislastsectionwewouldliketoreportonanattempttomeasureemittance(<strong>and</strong>toalesser 6.4StudyofPotentialEmittanceGrowth<br />

z (mm)<br />

∆φ (Deg) (experiment)<br />

tothelattice(betatronmismatch,lamentation,chromaticity);thesecondtypeareduetobunch selfinteraction(becauseofCoulombeldorradiationeld). Agrowthofemittancecomesfromanincreaseofoneoftheposition<strong>and</strong>/ordivergence,i.e.xorx0 inthex-x0phasespace.Let'sstartwithaninitialemittanceattheentranceofabeamlinesection Ifweassume,thatduetoperturbationinthebeamlinesection,theposition<strong>and</strong>divergenceofa particlechangeaccordinglyto: ~"0:8<br />

8Wevoluntaryomitthesubscriptxfortheemittance.inthissection<br />

~"0=hx20ihx02ihx0x0i21=2 x0!x0+x (6.17)<br />

Bunch Population (a.u)<br />

0.4<br />

0.3<br />

(A)<br />

σ z (mm)<br />

CTR signal (Volts)<br />

0.4<br />

0.3<br />

0.2<br />

(B)<br />

x0!x0+x0 (6.18)

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