High Brightness Electron Beam Diagnostics and their ... - CASA
High Brightness Electron Beam Diagnostics and their ... - CASA High Brightness Electron Beam Diagnostics and their ... - CASA
undulatorvicinity.Wehavenotmanaged,uptothepresentdate,tounambiguouslydemonstrate whetherthiseectwasduetocoherentsynchrotronradiation.Asecondseriesofrunswereper- measurementreportedinthisreport)wouldroughlydoubletheeectprovidedallelsewereequal, formed,whereweconcentratedonthemeasurementofenergyspreadalongthetransportchannel,butthenitstillwouldnotbesignicant.OncethelatticedesignoftheIRFELUpgradehasma- resultinginnoobservation,withintheprecisionofthemeasurement,ofenergyspreadgeneration (alsothisdataweretakenforoneoperatingpointofthelinaconly). Wecanconclude,ataminimum,thatitshouldbepossiblesetupabeamthatwilltransportaround theBatesarcwithoutsignicantgrowthinenergyspread(whichtranslatestonosignicantgrowth inemittance),andthereforefortheFELUpgradeitseemsreasonabletoplanonputtingtheFEL systemsinthebacklegtransferline-abunchchargeof135pC(versusthe60pCusedforthe tured,thenoneshouldbeabletousetheIRDemotosetupabeamattheentrancetotherst ofmeasurements(emittanceandenergyspread)the135pCcase. BatesbendthatmimicstheIRFELUpgradebeamparameters,andtrytoperformthesametype
[2]Y.Shibata,T.Takahashi,T.Kanai,K.Ishi,andM.Ikezawa,\Diagnosticsofanelectronbeam Bibliography [3]C.Hirschmugl,M.Sagurton,andG.Williams,\Multiparticlecoherencecalculationsfor [1]C.L.BohnandS.V.Benson,\RadiofrequencySuperconductivityAppliedtofree-electron ofalinearacceleratorusingcoeherentradiation",Phys.Rev.,E50num.2,pp.1479-1484(1994) lasers",Part.Acc.,69,pp.623-635(1998) [6]L.Wartsky,\EtudeduRayonnementdetransitionoptiqueproduitpardeselectronsd'energie [5]I.M.Frank,\TransitionRadiationandOpticalPropertiesofMatter",Sov.Phys.Uspekhi,8 [4]NodvickandSaxon,\Multiparticlecoherencecalculationsforsynchrotron-radiationemission", num.5,pp.729-742(1966) Phys.Rev.,A44num.2,pp.1316-1320(1991) synchrotron-radiationemission",Phys.Rev.,A44num.2,pp.1316-1320(1991) [9]A.Hofmann,\TheoryofSynchrotronRadiation",reportSSRLACD-NOTE38,StanfordUni- [7]M.L.Ter-Mikaelian,HighEnergyElectromagneticProcessesinCondensedMedia,Wiley- [8]J.D.Jackson,ClassicalElectrodynamics,WileyEdt,NewYork(1975) 30a70MeV.Applicationauxdiagnosticsdefaisceauxdeparticuleschargees",Ph.DThesis, Universited'Orsay,France [10]M.Sands,\ThePhysicsofElectronStorageRings,AnIntroduction",reportSLAC-121,Stanversity,CA(1986)ford(1970)(alsopublishedasreportUS-28,andUniversityofCalifornia,SantaCruz,CA Interscience,NewYork(1972) [13]S.V.BensonandM.D.Shinn,\DriveLaserforaDCphotocathodegun",Proc.Part.Acc. [11]G.Dattoli,andA.Torre,\Free-ElectronLaserTheory",reportCERN89-03,CERN,Geneva, [12]S.V.Benson,\TunableFree-ElectronLasers",inTunableLasersHandbook,AcademicPress Inc.,pp.443-469(1995) (1970)) [14]D.A.Engwall,\HighBrightnessElectronBeamsfromaDC,High-Voltage,GaAsPhotoemis- Conf.'95IEEEcatalog#97CH35843,pp.1052-1054,Dallas(1995) Switzerland(1989)Stanford(1986) sionGun",Ph.DThesis,UniversityofIllinoisatUrbana-Champaign(1998) 167
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- Page 155 and 156: . .. .. . .. . . .. . .. . . .. . .
- Page 157 and 158: σ x (m) x 10−3 5 4 3 2 1 0 0 5 1
- Page 159 and 160: BeamDynamicsStudies Chapter6 undula
- Page 161 and 162: x,y (mm) 6.0 4.8 3.6 2.4 1.2 x y 0.
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- Page 165 and 166: numericalsolution[56].Thisapproxima
- Page 167 and 168: 0.03 . .... . .. ... . .. ..... . .
- Page 169 and 170: ε x (mm−mrad) Nominal 6 4 2 cryo
- Page 171 and 172: 2.2 2 1.8 Figure6.10:Comparisonofth
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- Page 187: Conclusion Chapter7 Therecirculator
- Page 191 and 192: [29]J.-C.Denard,C.Bochetta,G.Traomb
- Page 193 and 194: [65]B.C.Yunn,\ImpedancesintheIRFEL"
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- Page 199 and 200: B.3.3PARMELA FeaturesofJeersonLabVe
- Page 201 and 202: Initialization MAIN Stop INPUT DECK
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[2]Y.Shibata,T.Takahashi,T.Kanai,K.Ishi,<strong>and</strong>M.Ikezawa,\<strong>Diagnostics</strong>ofanelectronbeam Bibliography<br />
[3]C.Hirschmugl,M.Sagurton,<strong>and</strong>G.Williams,\Multiparticlecoherencecalculationsfor [1]C.L.Bohn<strong>and</strong>S.V.Benson,\RadiofrequencySuperconductivityAppliedtofree-electron ofalinearacceleratorusingcoeherentradiation",Phys.Rev.,E50num.2,pp.1479-1484(1994) lasers",Part.Acc.,69,pp.623-635(1998)<br />
[6]L.Wartsky,\EtudeduRayonnementdetransitionoptiqueproduitpardeselectronsd'energie [5]I.M.Frank,\TransitionRadiation<strong>and</strong>OpticalPropertiesofMatter",Sov.Phys.Uspekhi,8 [4]Nodvick<strong>and</strong>Saxon,\Multiparticlecoherencecalculationsforsynchrotron-radiationemission", num.5,pp.729-742(1966) Phys.Rev.,A44num.2,pp.1316-1320(1991) synchrotron-radiationemission",Phys.Rev.,A44num.2,pp.1316-1320(1991)<br />
[9]A.Hofmann,\TheoryofSynchrotronRadiation",reportSSRLACD-NOTE38,StanfordUni- [7]M.L.Ter-Mikaelian,<strong>High</strong>EnergyElectromagneticProcessesinCondensedMedia,Wiley- [8]J.D.Jackson,ClassicalElectrodynamics,WileyEdt,NewYork(1975) 30a70MeV.Applicationauxdiagnosticsdefaisceauxdeparticuleschargees",Ph.DThesis, Universited'Orsay,France<br />
[10]M.S<strong>and</strong>s,\ThePhysicsof<strong>Electron</strong>StorageRings,AnIntroduction",reportSLAC-121,Stanversity,CA(1986)ford(1970)(alsopublishedasreportUS-28,<strong>and</strong>UniversityofCalifornia,SantaCruz,CA Interscience,NewYork(1972)<br />
[13]S.V.Benson<strong>and</strong>M.D.Shinn,\DriveLaserforaDCphotocathodegun",Proc.Part.Acc. [11]G.Dattoli,<strong>and</strong>A.Torre,\Free-<strong>Electron</strong>LaserTheory",reportCERN89-03,CERN,Geneva, [12]S.V.Benson,\TunableFree-<strong>Electron</strong>Lasers",inTunableLasersH<strong>and</strong>book,AcademicPress Inc.,pp.443-469(1995) (1970))<br />
[14]D.A.Engwall,\<strong>High</strong><strong>Brightness</strong><strong>Electron</strong><strong>Beam</strong>sfromaDC,<strong>High</strong>-Voltage,GaAsPhotoemis- Conf.'95IEEEcatalog#97CH35843,pp.1052-1054,Dallas(1995) Switzerl<strong>and</strong>(1989)Stanford(1986)<br />
sionGun",Ph.DThesis,UniversityofIllinoisatUrbana-Champaign(1998) 167
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