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

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(a)<br />

ceramic radiator<br />

beam<br />

x-wire beam transverse<br />

x+y<br />

section<br />

2<br />

y-wire<br />

wire<br />

(b)<br />

fluorescence emission<br />

vacuum chamber (spherical wave in<br />

optical region)<br />

Figure4.1:Schematicsofprincipleforthedierenttypeofbeamproledensitymeasurement<br />

vacuum window<br />

optical system<br />

direction of motion<br />

+ detector<br />

(c)<br />

(d)<br />

Metallic foil<br />

forward transition radiation<br />

synchrotron radiation<br />

beam<br />

mirror optical system<br />

anypieceofhardware(vacuumpipe,electronics,...)thatislocatedinthetunnelenclosure.Inthe devices.<br />

+ detector<br />

Magnetic Induction<br />

followingweconsiderthebehaviorofthreekindsofTRradiator:aluminum,gold<strong>and</strong>carbonfoil. acertainthresholditcantriggertheMachineProtectionSystem(MPS)whichwillturnothe canbesolargethatsomeoftheelectroncanbelost.Ifthepercentageoflostparticlesexceeds machine,alsoeveniftheMPSisnotarmed,losingalargefractionofthebeamisalwaysaconcern. Theprotectionsystemthresholddependsonthemachine,<strong>and</strong>insuresthatonecannotdamage<br />

backward transition radiation<br />

vacuum chamber<br />

vacuum window<br />

optical system<br />

4.2.2ThermalStudies<br />

+ detector<br />

foil.Theenergydepositionismainlyduetoionizationlossesoftherelativisticelectronsminusthe energycarriedonbysecondaryelectrons;itwascomputedusingtheEGS4(<strong>Electron</strong><strong>and</strong>Gamma Shower4)code4distributedbyStanfordLinearAcceleratorCenter.Iftheonlymechanismofheat heattransferequation: Theprimaryconcern,aswepreviouslyemphasized,isduetotheenergythebeamdepositsinthe transferisconduction,thetemperatureofabodyinwhichpowerisdepositedisdescribedbythe whereTisthetemperature,thedensity,cp,thespecicheat,thethermalconductivity,Vthe bodywithhighemissivity,heatevacuationviaradiationisanimportantmechanismthatshouldbe volumeofthebody,<strong>and</strong>thedepositedpower. Thisequationcanbenumericallyintegratedbyseveralnite-elementprogram.Inthecaseof 4PrivateCommunicationfromP.K.Kloeppel,November1995<br />

cp@T @tkappa52T=@P @V (4.12)

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