1. Beam Shaping and Permanent Magnet Quadrupole Focusing with Applications to the Plasma Wakefield Accelerator R. Joel England J. B. Rosenzweig, G. Travish, A. Doyuran, O. Williams, B. O’Shea UCLA Department of Physics and Astronomy Particle Beam Physics Laboratory Los Angeles, CA USA D. Alesini INFN Laboratori Nazionali di Frascati Rome, Italy Workshop on the Physics and Applications of High Brightness Electron Beams Erice, Sicily Oct 9-14, 2005

2. The Plasma Wakefield Accelerator (PWFA) Overdense Plasma n b 1 current neutralized n b < n p ; k p  r << 1 self-focused Underdense Plasma n b /n p >  2 unfocused  2 > n b /n p > 1 ion focused (blowout) Rosenzweig, et al. PRA, 44, R6189 (1991) Wake Fields in Blowout Regime Bingham, R. Nature, 394, 617 (1998). Blowout Regime Mechanism: Plasma electrons disturbed by drive beam. Longitudinal space-charge wave generated. Ion channel created, pulls electrons back. Ion focusing is linear in r. Accelerating electric field, E acc ≈ n 0 1/2 [V/cm]

3. Overview of Drive Beam Issues for Blowout Regime of PWFA Longitudinal bunch shape High beam brightness High charge Strong Focusing Betatron matching Creation of a Witness Bunch Chen, P., Su, J., and Dawson, J. SLAC PUB 3662 (1985). triangle doorstepideal Transformer Ratio: Longitudinal bunch shape High beam brightness High charge Strong Focusing Betatron matching Creation of a Witness Bunch

4. The UCLA Neptune Laboratory Beam Charge:100-300 pC Beam energy:up to 15 MeV Emittance:  N = 6 mm mrad Power Source:18 MW Klystron RF Frequency:2.856 GHz Cathode laser: 60-80 µJ at = 266 nm Laser pulse length:5 ps RMS 7&2/2 Cell PWT Linac 1.6-Cell Photoinjector

5. Neptune Dogleg Compressor S-Bahn Compressor S-Bahn is a “dogleg” or dispersionless translating section. Half-chicane with focusing elements between the bends. Can be operated in a nondispersive mode with symmetric beta function and 2π betatron advance. Like a chicane, may be used as a bunch-length compressor. Nominal first order temporal dispersion (R 56 =-5cm) is suitable for beam-shaping.

6. InitialFinal: Sextupoles Off Final: Sextupoles On Neptune Dogleg Compressor PARMELA Simulation Results: 1000 particles, 300pC  x,N (initial) =4.9 µm 1.6 11.5  x,N =9.9 µm+12.7 µm = 22.6 µm space-charge nonlinear total GUNPWTFinal FocusPre-Focus sextupoles

7. Neptune Dogleg Compressor ELEGANT: Simulated Witness Beam Region of high dispersion in x Strong correlation b/w x and z Insert mask in x to sever beam in z No mask inserted Undercorrected with sextupoles to elongate profile With 1cm mask inserted at above location ramped drive beam witness beam For PWFA application, drive beam needs a witness beam to accelerate.

8. Temporal Bunch Shaping: Diagnostic Deflecting Mode Cavity Courtesy of D. Alesini J.D. Fuerst, et. al., DESY Report CDR98, 1998 Lowest dipole mode is TM 110 Zero electric field on-axis (in pillbox approx.) Deflection is purely magnetic Polarization selection requires asymmetry on axis  r = 0 Pillbox Fields

9. ELEGANT Simulations V 0 = 0 ; P = 0 V 0 = 272 kV ; P = 12 kW V 0 = 545 kV ; P = 48 kW V 0 = 609 kV ; P = 61 kW Initial Current Profile ELEGANT Simulation Results Using RFDF element with 9 cells 10,000 macroparticles Shunt Impedance: R T = 6.12 MΩ Power: P = V 0 2 /R T

10. Deflecting Cavity: HFSS Design HFSS Geometry of 1/2 structure DIMENSION VALUE [mm] a5 b18.800 b118.8125 b2 b3 t3.054 d16.07 b b b1 b2 b3 t d X-Band, 9-cell design. Collaboration with INFL Frascatti. Will be built at UCLA; diffusion bonded at SLAC. Powered by a VA-24G X-Band klystron @ 50 kW. Frequency: 9.59616GHz

11. Deflecting Cavity: HFSS Design Resonance of the π-Mode out of phase by 90˚ E-field H-field

12. Deflecting Cavity: Polarization Separation Undesired Desired +1358 MHz +53 MHz -7 MHz -2 MHz Holes Rods Rods give greater better mode separation but shift the desired mode too much Holes give less mode separation (5 MHz) but only perturb desired mode by 2 MHz (within range of temperature tuning). Holes look like better option: 5 MHz is large compared to the resonance width

13. Prototype Cavity

14. Q=300 pC ; L=2mm;  z = 0.5 mm Constraints on Brightness & Emittance blowout regime transformer ratio betatron matching ~50 µm ~10 mm mrad ~150 mA/µm 2 n 0min ~ 2.8x10 13 cm -3

15. PowerTrace 1.08 Simulation standard iron quads PMQs (110 T/m) Permanent Magnet Quad Focusing ELEGANT Simulation Result  =25.7; E=13.13 MeV; Q = 300 pC  x =42 µm;  x =9.2 mm mrad  y =36 µm;  y =6.79 mm mrad  z =0.46 mm;   =1.77%

16. Scaling to Higher Charge: 4 nC UCLA-Parmela 2.0, 1000 particles Q = 4 nC; pt-to-pt space charge scaling applied to laser at cathode: GUNPWTFinal FocusPre-Focus simulation of gun and linac w/solenoid for emittance compensation sextupoles  N ~ 25 mm mrad

17. Scaling to Higher Charge: 4 nC ELEGANT, 1000 particles dispersion killed to 1st Order scaling applied to laser at cathode: GUNPWTFinal FocusPre-Focus simulation of sbahn and final focus horizontal dispersion killed to first order (R 16,R 26 ) 2nd order longitudinal dispersion T 566 killed sextupoles longitudinal ph. space and profile at end tail is 3rd order (U 5666 ) octupoles needed?

18. Scaling to Higher Charge: 4 nC ELEGANT, 1000 particles dispersion killed to 2nd Order scaling applied to laser at cathode: GUNPWTFinal FocusPre-Focus sextupoles longitudinal ph. space and profile at end simulation of sbahn and final focus horizontal dispersion killed to second order 2nd order longitudinal dispersion not killed tail is 2nd and 3rd order (T 566, U 5666 )

19. Q=4 nC ; L=4mm;  z = 1 mm Scaling to Higher Charge: 4 nC ~250 µm ~100 mm mrad ~7 mA/µm 2 n 0min ~ 0.8x10 13 cm -3

20. Conclusions PWFA drive issues: ramped profile, strong focus, high charge Ramped profile: - improved transformer ratio (R > 2) - feasible using dogleg compression with sextupoles - deflecting cavity diagnostic (50 fs resolution) Strong focus: - traditional EM quads + permanent magnet quadrupoles - adequate emittance and brightness (~ 10 µm, 150 mA/µm 2 @ 300 pC) High Charge: - scaling to high charge (~4 nC) at Neptune has some dilemmas - tradeoff between optimal profile and good emittance - extra sextupoles and octupoles may be required - beam sizes become bigger than the beam pipes - implies complete or partial redesign of the compressor