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Overview of the RFCC Module and 201-MHz Cavity Design

Overview of the RFCC Module and 201-MHz Cavity Design. Derun Li Lawrence Berkeley National Laboratory. RFCC Module Preliminary Design Review June 4, 2008. Outline. Introduction of RFCC module of MICE cooling channel and charge of the review Review of the 201-MHz cavity design

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Overview of the RFCC Module and 201-MHz Cavity Design

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  1. Overview of the RFCC Module and 201-MHz Cavity Design Derun Li Lawrence Berkeley National Laboratory RFCC Module Preliminary Design Review June 4, 2008

  2. Outline • Introduction of RFCC module of MICE cooling channel and charge of the review • Review of the 201-MHz cavity design • MuCool 201-MHz prototype cavity: baseline design for MICE • Prototype: collaboration between LBNL, JLab, University of Mississippi and Oxford University • Physics design and cavity fabrications • Cavity body • RF coupler • Be windows • Tuners • Recent progress • Vendor identification • Engineering CAD model • Integration and interface • Summary Derun Li - Lawrence Berkeley National Lab - June 4, 2008

  3. International Muon Ionization Cooling Exp. RFCC RFCC Spectrometer Solenoid 1 AFC AFC Spectrometer Solenoid 2 Absorber and Focusing Coil (AFC) Derun Li - Lawrence Berkeley National Lab - June 4, 2008

  4. Eight 201-MHz Cavities for MICE Eight201-MHz RF cavities MICE Cooling Channel Courtesy of S. Q. Yang, Oxford Univ. RFCC modules Derun Li - Lawrence Berkeley National Lab - June 4, 2008

  5. SC coupling Coil Curved Be window Cavity Couplers Vacuum Pump 201-MHz cavity RFCC Module Derun Li - Lawrence Berkeley National Lab - June 4, 2008

  6. Charge of this Review • Evaluate the preliminary engineering design of RFCC module • Evaluate engineering design of MICE 201-MHz RF cavity • Is LBNL ready to purchase long lead cavity materials and components? • Copper sheets for cavity bodies • Thin, curved beryllium windows • Ceramic RF windows • Evaluate engineering design and fabrication scheme of the 201-MHz cavity to determine readiness to initiate cavity body fabrication • Spinning of cavity shells • e-beam welding • Port extruding • Tuners • Cavity support • Evaluate overall module concept • Interface with other modules • Site interfaces • Integration and shipping • Detailed design of CC is not part of this review Derun Li - Lawrence Berkeley National Lab - June 4, 2008

  7. RFCC Design Review Agenda 14:00 Overview: prototype cavity, physics design and recent progress by Derun Li 14:40 201 MHz Mechanical Design and Analysis by Allan DeMello 15:20 Other Cavity Components by Allan DeMello 15:40 Coffee Break  15:55 Overall RFCC Module Mechanical Design by Allan DeMello 16:25 Shipping, Installation and Interfaces by Steve Virostek 16:45 RFCC Schedule and Manpower by Steve Virostek 17:00 Discussion All 17:15 Committee closed session 17:45 Closeout All Derun Li - Lawrence Berkeley National Lab - June 4, 2008

  8. MuCool 201-MHz RF Prototype Cavity • MICE 201-MHz cavity design is based on MuCool prototype cavity with minor differences • Prototype cavity • Physics Design • Couplers and ceramic RF windows • Engineering • Fabrication: cavity body, ports, tuners, etc. • Large, pre-curved and thin 42-cm diameter Be windows • Commissioning and operation • RF Conditioning and background • High gradients (~ 16 MV/m) • With the thin and curved Be windows • With external magnetic fields Derun Li - Lawrence Berkeley National Lab - June 4, 2008

  9. The Cavity Body Profile Spherical section at the equator to ease addition of ports (±~ 6.5o) Elliptical-like (two circles) nose to reduce peak surface field Stiffener ring 2o tilt angle 42-cm 6-mm Cu sheet allows for uses of spinning technique and mechanical tuners similar to SCRF ones 121.7-cm De-mountable Pre-curved Be windows to terminate RF fields at the iris Low peak surface E-field at iris Derun Li - Lawrence Berkeley National Lab - June 4, 2008

  10. Cavity Design Parameters • The cavity design parameters • Frequency: 201.25 MHz • β = 0.87 • Shunt impedance (VT2/P): ~ 22 MΩ/m • Quality factor (Q0): ~ 53,500 • Be window diameter and thickness: 42-cm and 0.38-mm • Nominal parameters for MICE and cooling channels in a neutrino factory • 8 MV/m (~16 MV/m) peak accelerating field • Peak input RF power: 1 MW (~4.6 MW) per cavity • Average power dissipation per cavity: 1 kW (~8.4 kW) • Average power dissipation per Be window: 12 watts (~100 watts) Derun Li - Lawrence Berkeley National Lab - June 4, 2008

  11. 201 MHz Cavity Concept Spinning of half shells using thin copper sheets and e-beam welding to join the shells; extruding of four ports; each cavity has two pre-curved Beryllium windows, but also accommodates different windows Derun Li - Lawrence Berkeley National Lab - June 4, 2008

  12. Shell Measurement at LBNL Measured frequency of shell-1: 196.97 MHz; Simulated frequency: 197.32 MHz,  f ~ 350 kHz • CMM scans to measure the • spun profiles of shells • Frequency and Q measurements • Copper tapes for better RF • contacts Profile measurements: 3 CMM scans per half shell conducted at 0o, 45o, 90o, respectively Derun Li - Lawrence Berkeley National Lab - June 4, 2008

  13. Fabrication of the MuCool Cavity • Two 6-mm thick copper shells are formed from annealed, flat sheet using a spinning technique • Two half shells are e-beam welded together at equator to form the cavity • Separate copper nose piece rings are e-beam welded to cavity iris (aperture) • RF and vacuum ports are formed by pulling a die through a hole cut across the equator weld (extruding) • Externally brazed tubes provide cooling • Cavity inside surfaces are finished by mechanically buffing and electro-polishing • Two thin, pre-curved beryllium windows are mounted on cavity aperture • Cavity is mounted between two thick aluminum vacuum support plates • See Allan DeMello’s talks for details for fabrication and QC Derun Li - Lawrence Berkeley National Lab - June 4, 2008

  14. Prototype RF Coupler • Two loop couplers each cavity to give critical coupling • Prototype coupling loop design uses standard off-the-shelf copper co-axial components • Parts were joined by torch brazing at LBNL • Coupling loop has integrated water cooling lines • Two SNS style RF windows mfg. by Toshiba • High power tested up to 2.5 MW per coupler, 10 kW (avg.) Ceramic RF window RF Window Conditioning Loop coupler made at LBNL SNS RF window Derun Li - Lawrence Berkeley National Lab - June 4, 2008

  15. Thin and Curved Be Windows • Each cavity has two Be windows • 42-cm diameter and 0.38-mm thick • Window is formed at high temperature and later brazed to copper frames • Thin TiN coatings on both sides of the window • One window curves into the cavity and one curves out • Already high power tested up to 5 MW in 201-MHz cavity at MTA, FNAL 42-cm Derun Li - Lawrence Berkeley National Lab - June 4, 2008

  16. Low Power RF Measurements at MTA • f =199.578 MHz • Q0 =49,000 ~ 51,000(with flat copper windows; better than • 90% of the design value) • Two couplers • Balanced • Coupling adjustments Derun Li - Lawrence Berkeley National Lab - June 4, 2008

  17. Dial indicators Tuner Concept and Measurements • Mechanical tuning plates at four locations • Dial indicators to measure displacement between Al plates • Tuning measurement in air • Equivalent to MICE cavity under vacuum • Adjusted up to 2-mm with 8 steps of 0.25-mm each • Measured tuner sensitivity • 156 kHz/mm per side • Calculated tuner sensitivity • 230 kHz/mm per side • Discrepancy is due to deflection of the Al plates Derun Li - Lawrence Berkeley National Lab - June 4, 2008

  18. RF Test Setup at MTA The 805-MHz and 201-MHz cavities at MTA, FNAL for RF breakdown studies with external magnetic fields. 201 MHz cavity 805 MHz pillbox cavity Derun Li - Lawrence Berkeley National Lab - June 4, 2008

  19. High Power RF Tests with Cu & Be Windows • The cavity was first tested with flat copper windows and reached ~ 16 MV/m quickly and quietly • The cavity then was tested with thin and curved Be windows and again reached to ~19 MV/m quickly • Cavity frequency had to be retuned • Cavity frequency was stable during the operation, however, we did observe frequency shift due to RF heating on the windows • Frequency shift of ~ 125 kHz (from 0 to ~ 19 MV/m, 150-micro-second pulse, 10-Hz repetition rate) in ~ 10 minutes, well within the tuning range (230 kHz/mm per side,  2-mm range) • With a few hundred Gauss stray field from Lab-G magnet, the cavity gradient can be maintained at 19 MV/m • To test with stronger external magnetic fields • Move the cavity closer to Lab-G magnet • SC coupling coil for MuCool Derun Li - Lawrence Berkeley National Lab - June 4, 2008

  20. Lab-G magnet The 201-MHz cavity Tests with Stronger Magnetic Fields • New vacuum pumping system • Separation of the nearest curved Be window from the face of Lab-G magnet is 10-cm (before was 110-cm) • Maximum magnetic field near the Be window 1.5 Tesla (at 5 Tesla in magnet) • Test Results: • Multipactoring was observed over the entire magnetic field range up to 1.1-T at nearest Be window • A strong correlation exists between cavity vacuum and radiation levels • We have achieved ~ 14 MV/m at 0.75-T to the nearest curved thin Be window • The test results are very encouraging, data analysis is being conducted Derun Li - Lawrence Berkeley National Lab - June 4, 2008

  21. Recent Progress • RFCC engineering CAD model • RF and Engineering design of 201-MHz RF cavity • Integration and interface • Vendor identifications Derun Li - Lawrence Berkeley National Lab - June 4, 2008

  22. Recent Progress: RF Cavity Design • See A. DeMello’s talks on details • Vendor Identification • Engineering CAD model • Integration and interface • Improved Be window design • Tuners and support • Cavity post processing • Cavity RF design • 3-D CST MWS RF parameterized model with ports and curved Be windows • Hard to reach the design frequency by spinning • Frequencies between cavities should be able to achieve within  100 kHz • Approaches • Modification the spinning form • Targeting for higher frequency • Fixed tuner to tune cavity close to design frequency (deformation of cavity body) • Tuners are in push-in mode  lower frequency Derun Li - Lawrence Berkeley National Lab - June 4, 2008

  23. Numerical Study with B Field • Preliminary studies, in collaboration with colleagues at SLAC using Omega-3P and Track-3P codes • Cavity with flat windows: 5 MV/m on axis; 2-T uniform external magnetic field; scan of a few points from one cavity side Trajectories with external B = 2-T field Trajectories without external B field E field contour Derun Li - Lawrence Berkeley National Lab - June 4, 2008

  24. Summary • MICE cavity design is heavily based on successful MuCool 201-MHz prototype RF cavity and lessons learned • Fabrication and post processing • Cavity conditioning and operation • Engineering design of the cavity is essentially complete • CAD model of the cavity, tuners, support and vacuum • Fabrication schemes • Significant progress on engineering designs of RFCC module • Possible operation at LN temperature? • Current design accommodates LN operation, but it looks very challenging Derun Li - Lawrence Berkeley National Lab - June 4, 2008

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