Low Emittance RF Gun Developments for PAL-XFEL Jang-Hui Han, Juho Hong, Munsik Chae, Sung-Ju park Pohang Accelerator Laboratory Accelerator Physics Seminar, DESY, 14 November 2012 Contents • PAL-XFEL project overview • Requirements of PAL-XFEL injector • Baseline Injector • Methods to further improve injector performance • Alternative (Low Emittance) Injector • PAL-XFEL injector test facility Jang-Hui HAN Accelerator Physics Seminar, DESY, 14 November 2012 2 PAL-XFEL Project • S-band 10 GeV linac + 1 hard & 1 soft X-ray undulator beamlines (space for two more hard and one more soft lines reserved) • 60 Hz rep. rate with single or two bunches • The project started in 2011 aiming at construction by 2014 • Building construction ongoing • Commissioning to start in 2015 PAL-XFEL Jang-Hui HAN Accelerator Physics Seminar, DESY, 14 November 2012 PLS II 3 Baseline Linac Layout – – – – – – – – Injector to 139 MeV + Laser heater S-Band cavities for beam acceleration X-band cavity for linearization in time-energy phase space BC1 (1st magnetic bunch compressor) at 0.33 GeV BC2 at 2.5 GeV Beam branch to soft X-ray beamlines at 3 GeV BC3 at 3.5 GeV Linac end at 10 GeV L3:S BC3_S De-Chirper Soft X-ray FEL 3.15 GeV RF Gun L1 X Laser Heater BC1 330 MeV L2 BC2 2.52 GeV BC3_H L3 kicker 3.45 GeV L4 10 GeV Linac Undulator Hall BTL 710 m Jang-Hui HAN Hard X-ray FEL 780 m Accelerator Physics Seminar, DESY, 14 November 2012 Beamline 1000 m 1100 m 4 Two Undulator Lines for Phase 1 e- gun e 3 GeV 10 GeV - PU Two bunches at 60 Hz Planar Undulator x 24 λ = 0.6 nm ~ 0.06 nm PU + EPU λ = 4.5 nm ~ 1.0 nm Kicker EPU SX1 SX2 HX1 HX2 HX3 Exp. Hall Soft X - ray Undulator Hall (~110 m including Dump Section) Hard X - ray Undulator Hall (~225 m including Dump Section) Undulator Line HX1 SX1 Wavelength, nm 0.1 3.0 Beam energy, GeV 10 3.15 Undulator period, mm 24.4 34.0 Undulator gap, mm 7.2 8.3 5 5 Undulator module length, m Jang-Hui HAN Exp. Hall Accelerator Physics Seminar, DESY, 14 November 2012 5 How good Injector needed? • Electron beam quality for – 0.1 nm FEL using 10 GeV electron beam – 1012 photons per pulse at 0.1 nm 30 GW with 0.2 nC bunch – Saturation within 120 m (24 x 5 m long undulators) • Thermally stable at 60 Hz + • Robust and reliable for user service Jang-Hui HAN Accelerator Physics Seminar, DESY, 14 November 2012 6 PAL ITF Gun1 e beam • Developed during last few years at PAL • 1.6 cell, 2.856 GHz • 2 RF coupler ports & 2 vacuum ports at the full cell for RF symmetry • Gun solenoid at 205 mm from cathode (no magnetic field compensation solenoid) • Basic test done at GTF in 2011 • Commissioning started at ITF Jang-Hui HAN Accelerator Physics Seminar, DESY, 14 November 2012 7 Baseline Injector Layout • 2 accelerating sections with focusing solenoids • 120 MV/m max field at cathode, 5.7 MeV beam energy at gun exit • 20 MV/m & 25 MV/m gradients at 1st & 2nd accelerating tubes, 139 MeV beam energy at injector end • Drive laser beam size is minimized to reduce thermal emittance (0.12 mm rms for 200 pC beam 0.11 mm mrad thermal emittance) • 1st accelerating section starts at 2.2 m from the cathode (longer e-beam focal length due to the smaller laser beam at cathode) • Two linac solenoids for beta-function control at the entrance of the laser heater system Jang-Hui HAN Accelerator Physics Seminar, DESY, 14 November 2012 8 Beam Dynamics, Flat-top Laser – 1 Cathode laser Longitudinal shape: - 8 short Gaussian pulses stacked - 8 ps fwhm Transversely uniform 200 pC beam simulation at injector end 0.26 mm mrad transverse projected emittance Jang-Hui HAN Accelerator Physics Seminar, DESY, 14 November 2012 9 Beam Dynamics, Flat-top Laser – 2 Emittance at central slices below 0.3 mm mrad 200 pC 0.3 mm mrad Peak current 26 A Mismatch parameter close to 1 Jang-Hui HAN Accelerator Physics Seminar, DESY, 14 November 2012 10 Beam Dynamics, Flat-top Laser 20 pC Emittance at central slices below 0.1 mm mrad 4 ps flat-top laser pulse profile (4 Gaussian pulses stacked) 0.1 mm mrad Peak current 5 A Jang-Hui HAN Accelerator Physics Seminar, DESY, 14 November 2012 11 Beam Dynamics, Gaussian Laser 200 pC 0.3 mm mrad Gaussian laser pulse profile instead of flat-top Peak current 26 A Jang-Hui HAN Accelerator Physics Seminar, DESY, 14 November 2012 12 Can We further improve Injector? • Thermal emittance • Gun cavity geometry • Position of gun solenoid • Position of first accelerating section – already done for the PAL-XFEL baseline injector Jang-Hui HAN Accelerator Physics Seminar, DESY, 14 November 2012 13 Low Thermal Emittance • Small drive-laser beam size – Electron beam dynamics optimization • Small kinetic energy of emitted electrons from the cathode – Longer wavelength of drive-laser – Higher work function (and high quantum efficiency) Need for R&D of drive-laser and photocathode Photocathode plug enables using various photocathode material with different surface treatment Jang-Hui HAN Accelerator Physics Seminar, DESY, 14 November 2012 14 Keeping Beam Quality through Gun • Immediately after the beam emission, the beam is affected by space charge and mirror charge Strong acceleration field required • On the other hand, strong surface field produces Schottky effect. The kinetic energy of emitted electrons increases. • 120 MV/m peak field at the PAL-XFEL S-band gun • Fast acceleration as well as keeping the electron beam size through the gun cavity is crucial to generate a small emittance beam. Jang-Hui HAN Accelerator Physics Seminar, DESY, 14 November 2012 15 Optimization of a New Gun 1st cell 2nd cell LCLS 2.856 GHz gun Scaled DESY 1.3 GHz gun Jang-Hui HAN Accelerator Physics Seminar, DESY, 14 November 2012 16 Low Emittance Gun (Alternative Gun) In parallel with the baseline injector commissioning at ITF, a new injector with an alternative gun is being developed. Alternative gun (2.856 GHz): A scaled down version of DESY L-band guns Coaxial RF coupler perfect RF symmetry Optimum solenoid position minimized transverse emittance Cathode plug exchangeable under UHV more reliable operation possibility using other cathode materials Improved water-cooling more thermal stablility Jang-Hui HAN Accelerator Physics Seminar, DESY, 14 November 2012 17 Gun + Coupler Jang-Hui HAN Accelerator Physics Seminar, DESY, 14 November 2012 18 Gun Development Status • Gun cavity & coupler – First machining ongoing at a local machining company – Vacuum brazing to be done at PAL – Production to be ready January 2013 • Gun solenoids – Production ready at a local company – Magnetic field measured • Gun test beamline – Under design – First operation planned summer 2013 Jang-Hui HAN Accelerator Physics Seminar, DESY, 14 November 2012 19 Low Emittance Injector Alternative gun + three accelerating sections (focusing solenoids at the first two sections) 120 MV/m max field at gun, 14 MV/m gradient at 1st section, 20 MV/m at 2nd & 3rd sections Mild velocity bunching at 1st section (67), energy chirp corrected by 2nd & 3rd sections (16) Jang-Hui HAN Accelerator Physics Seminar, DESY, 14 November 2012 20 Nominal Bunch Charge, 200 pC • 8 ps flat-top: eight Gaussian pulses stacked • 4 ps flat-top: four Gaussian pulses stacked • Short Gaussian (no complicated pulse shaping) Jang-Hui HAN Accelerator Physics Seminar, DESY, 14 November 2012 21 Low Bunch Charge, 20 pC • 4 ps flat-top: four Gaussian pulses stacked • Short Gaussian (no complicated pulse shaping) Jang-Hui HAN Accelerator Physics Seminar, DESY, 14 November 2012 22 PAL Injector Test Facility 19.2 m 19200 LASER CLEAN ROOM 150 CO NTROL ROOM 17770 ) serHeater (tobeinstaledin2013 La e& WG): amli n e( Be sTyp Pump 5" 30l/s- >9EA .7 Pa: 2 P W/ V 7EA >E l/s- 7 150 "0 5 . 15 Pb:: 6 A l /s-> "4 Pc " 80l/s- >2EA Pd: 6 HB-S-DC- HB L OO 1SP r_ to cs_ re rw o Clo E/Be L 1 w ) 4(HE r_s_ to cw e r lo o C/Be 3 w L OO 2 SP M_ BP 1 i d# A/CSoleno Pc Pc Elbow P W/ V Pa Pa VP ISOL P_CPR S W/ V Pa TT PD T- A PS-HB HB-TWI S _5 GV _4 GV ool LHsp SiC Pa HB-S-DC- HB PD TT T- A HB-TWI S Pc Pb S p2 ayCu d ra& Fa mp2 u mD a Be S PS-HB S EB EB VP 60) DC( 1 Pc ) EB(144x144 VP(210) Pc ) EB(144x144 LCW Jang-Hui HAN 3 n_ Scree 4 n_ Scree P W/ V SiC HB-S-DC- HB S 60) DC( 1 VP(210) p1 ayCu d ra& Fa mp1 u mD a Be Pb Pc VP DC P W/ V HB-S-DC- HB S EB Pc er nn WireSca 5 M_ BP TCAV _2 ICT Pa DC Pc VP PcVP Elbow DC SiC Pb W_CPR _3 GV A/C#2 _2 PM _2 GV VP Pb Pb 2 i d# A/CSoleno A/C#1 r ato li m Co Pb TWIST upler center :59.3 et oco athod C 2 .5 Fl cel length: 32 u : 23 ngt lees ceicl k aslf th s :h20 n IriH 3 r_ to cs_ re rw o Clo E/Be L 2 w 2 n_ Scree TWIST id no ole nS Gu 1 M_ nd BP EBe 2L r_ cto r_ E _1 L 1re no e reC r ScL aserMir o _1 ICT GV _1 PM Pb Pa Gun Pa Pa Pa Accelerator Physics Seminar, DESY, 14 November 2012 S. J. Park 23 Purpose of ITF • Commissioning of PAL-XFEL injector (one gun + two accelerating sections) including laser heater and RF deflector • Test of new guns, laser, diagnostics, control, cooling, … • Practice of beam operation, education of new operators Jang-Hui HAN Accelerator Physics Seminar, DESY, 14 November 2012 24 ITF Status I Jang-Hui HAN Accelerator Physics Seminar, DESY, 14 November 2012 25 ITF Status II • RF station installed • GTF gun with solenoid installed • 2 linac tubes with solenoids installed • Laser system installed in the laser room • Laser optics being installed in the tunnel • RF network being installed • RF conditioning being started First beam foreseen in the next weeks Jang-Hui HAN Accelerator Physics Seminar, DESY, 14 November 2012 26 Summary • Baseline injector – PAL ITF gun1 + two accelerating sections – Fully satisfy PAL-XFEL basic requirement – Installed at PAL-XFEL ITF, RF conditioning ongoing, first beam foreseen this month • Alternative injector – Alternative gun + three accelerating sections – Will provide further low emittance – Thermally more stable, photocathode easily exchangeable – Under production, first beam foreseen summer 2013 Jang-Hui HAN Accelerator Physics Seminar, DESY, 14 November 2012 27 Thanks Jang-Hui HAN Accelerator Physics Seminar, DESY, 14 November 2012 28