Few Slides from RF Deflector Developments and Applications

Few Slides from RF Deflector Developments and Applications at SLAC Juwen Wang SLAC Accelerator Seminar April 12 2011

Outline 1. Introduction to RF Deflectors 2. Basic Theory and Design of RF Deflectors 3. Deflector Applications (3 Types and 7 Examples) 4. Manufacture and Characterization 5. Future Work

RF Deflector Applications Three Types and 7 Examples - Time-resolved electron bunch diagnostics for the LCLS Measurement of bunch time jitter at LCLS Bunch longitudinal profile diagnostics at DESY Ultra short e- and x-ray beams temporal diagnostics for LCLS - Drive/witness bunch longitudinal profile diagnostics for PWFA at FACET - Increase slice energy spread σE as well as measure of slice parameters for Upgrade ECHO-7 - Separator for High Energy Physics Experiments

What the RF Deflectors Look Like? Final Assembly of a 1 m X-Band Deflector for LCLS A LOLA-IV Ready for DESY Two Short X -Band Deflectors for ECHO-7 A Short 13 -Cell S-Band LOLA Structure Under Measurement for LCLS Injector

Two transverse RF deflectors at LCLS Paul Emma

Bunch Measurement at LCLS Paul Emma

Upgrade ECHO-7 Experiment at NLCTA Increase Slice Energy Spread and Measurement of Longitudinal Profile TCAV 1 to increase σE TCAV 2 to measure slice parameters Layout and upgrade of the ECHO-7 experiment WHY increasing beam slice energy spread? • Echo-7 experiment demonstrated the ability to control the phase space correlations (D. Xiang, et al, PRL, 105, 114801 (2010)) • The advantage of EEHG over HGHG has not been fully demonstrated because the beam has very small slice energy spread • Scaling to x-ray FEL requires confidence in harmonic generation with the relative beam energy spread on the 10 -4 level but NLCTA has σE /E~10 -5 HOW: Using a rf deflecting cavity to increase beam slice energy spread to ~10 ke. V Dao Xiang

Bunch Time Jitter Measurement at LCLS Paul Emma

Regular X-Band Deflector Cups

Coupler Design Simulation Maximum surface magnetic fields ~400 k. A/m, Pulse heating 22 deg. C for 100 ns pulse. Maximum surface electric fields ~100 MV/m. Fields Normalized 20 MW of transmitted power, or 21. 3 Me. V kick for 89 cm structure V. A. Dolgashev, “Waveguide Coupler for X-band Defectors, ” AAC 2008, SALC-WP-084

Input/Output Coupler Assemblies Mechanical Design Model Completed Coupler Assembly

Assembly of the Deflector

Design Example – III Maximum Kick 6 and 0. 2 MV for ECHO-7 Experiment Name of Structure Type D 27 D 11 2π/3 Backward wave Aperture 2 a 10. 00 mm Cavity Diameter 2 b 29. 77 mm Cell Length d 8. 7475 mm Disk Thickness 2. 0 mm Quality Factor Q 6320 Kick Factor k 2. 849 x 1016 V/C/m/m Transverse Shunt Impedance r┴ 41. 9 MΩ/m Group Velocity Vg/c - 3. 165 % Total Flange-Flange Length L 43. 6 cm 29. 6 cm Filling Time Tf 26. 8 ns 12 ns 0. 147 0. 063 15 MW for 6 MV Kick 77 k. W for 0. 2 MV Kick 84 MV/m 6 MV/m 0. 29 MA/m 0. 02 MA/m Attenuation Factor τ Input Peak RF Power Maximum Electric Field Maximum Magnetic Field

A Typical Microwave Measurement Results for 9 -Period Cell. Stack Working 2 pi/3 Mode Desired Horizontal Kick Dipole Modes Unwanted polarized Mode 80 MHz lower Vertical Kick Dipole Modes

S 11 Resonant Modes and Dispersion Curve for Horizontal Deflecting Modes Backward Wave 2π/3 horizontal deflecting Mode

D 27 Amplitude and Cumulated Phase Shift

Beam at Maximum Kick Phase In Deflecting Plane of a Short TW RF Deflector • Top: distribution of deflection (V/m/4 W) • Bottom: Integrated deflection (V/4 W) There are high electric and magnetic fields in the coupler regions. Due to their standing wave characteristic, the total contribution to the kick is equivalent to 1/2+1/2 cell. Zhenghai Li

Future Application – I Ultra short electron and x-ray beams temporal diagnostics with X-band deflector V (t ) e- sz RF ‘streak’ Dy X-band TCAV D 90° bd ü High resolution, ~ few fs; ü Applicable for all radiation wavelength; ü Wide diagnostic range, few fs to few hundred fs; ü Profiles, single shot; ü No interruption with LCLS operation; ü Both e-beam and x-ray. Dipole energy 2× 1 m tim e bs Yuantao

Future Application – II Plasma Wakefield Acceleration (PWFA) experiments at FACET Measurement of longitudinal profile for both Drive Beam and Witness Beam Plasma Wakefield Acceleration (PWFA) experiments at FACET will use unique two-bunch beam. (not real data) Acceleration of witness bunch depends strongly on longitudinal profile of the two bunches as well as the interbunch spacing. Will also try non-Gaussian “ramped” driver bunch, which could provide especially high transformer ratio. Good single-shot measurement of longitudinal profile is essential for interpreting experimental results. PWFA Ramped Driver Concept witness ramped driver [1] M. J. Hogan, et al. , New J. Phys. 12 055030 (2010) [2] R. J. England, et al. , Phys. Rev. Lett. 100 214802 (2008) Ez Mike Litos