1. 201-MHz NCRF Cavity Program Derun Li Center for Beam Physics Lawrence Berkeley National Laboratory MUTAC Review at Fermilab March 16, 2006

2. Collaborators M. Dickson, R. MacGill, J. Staples, S. Virostek, M. Zisman Lawrence Berkeley National Laboratory A. Bross, A. Moretti, B. Norris, Z. Qian Fermi National Accelerator Laboratory J. Norem Argonne National Laboratory R. Rimmer, L. Phillips, G. Wu Jefferson National Laboratory Y. Torun Illinois Institute of Technology D. Summers University of Mississippi W. Lau, S. Yang Oxford University, UK

3. Outline Introduction 201 MHz Cavity Progress –Cavity design and fabrication Cleaning, vacuum and assembly Shipping –Installation at MTA, FNAL Installation: vacuum, RF couplers and probes, power transmission lines, baking system, … Low power microwave measurements –Progress on curved Be windows 21-cm (radius) curved Be windows for 201 MHz cavity Asymmetric heating of the curved windows Transient studies: pulse heating and to steady state –Preliminary tests of the cavity Summary

4. Introduction – High gradient RF cavities to compensate for lost longitudinal energy – Strong magnetic field to confine muon beams – Lose energy in LH absorbers Goal: – Development of NC 201-MHz cavity that can operate at ~ 16 MV/m under a few Tesla solenoidal B fields Ionization Cooling LH Absorbers RF Cavities Designing, engineering, fabricating, conditioning and operating a cavity at 16 MV/m with B is a challenging

5. Introduction (Cont ’ d) NCRF R&D Programs Develop highest possible NCRF accelerating structure to meet the requirements for NF or MC Prototype of 201 MHz cavity –Completed cavity design and fabrication –Cavity installation at MTA in Sept. 2005 Assembly and vacuum RF power plumbing –RF conditioning started in late Feb. 2006 Experimental studies at 805 MHz with and without external magnetic fields up to 5-Tesla (2.5 Tesla for MICE) –Completed 5-cell cavity with open iris test at Lab G –Designed, fabricated and tested pillbox-like cavity with demountable windows at Lab G and moved and resumed recently at MTA, FNAL –Tests with two curved Be windows Reached 32 MV/m easily without external magnetic field More tests are in progress with magnetic fields versus achievable gradient –Button test

6. Cavity Status at Last MUTAC Where we were at last MUTAC in Berkeley (Apr-2005) Welding of cooling tube to cavity Extruding of four ports and vacuum leak tight Placed purchase order of curved Be windows Work needs to be done at the time:  Cavity interior buffing  Chemical cleaning and high pressure water rinse of the cavity interior  Surface cleaning + electro-polishing (EP)  High power RF conditioning of RF couplers with windows  Low power microwave measurements of the cavity with windows: Frequency Quality factor Q Couplings  RF coupler measurement and tuning  Packing and shipping to MTA, FNAL

7. Extruded ports outer and inner surface finish Outside Inside cavity body cooling tube cooling tube ports and ports and flanges flanges leak tight leak tight The Cavity at J-Lab in Apr-2005

8. Best possible surface treatment: like SCRF cavities Final interior buffing of cavity is performed to ensure the surfaces are ready for electropolishing Less buffing needed near equator where fields are lower An automated process of buffing was developed using a rotary buffing wheel and a cavity rotation fixture Some local hand work required to clean up some areas A series of pads with graduated coarseness was used Goal was scratch depth shallow enough for EP removal Cavity Progress: Final Interior Buffing

9. Cavity Progress: EP Setup EP setup and the U-shape electrode for EP at J-Lab

10. After buffing, cavity underwent a chemical cleaning processAfter buffing, cavity underwent a chemical cleaning process Test bars with various degrees of buffing were run through an electropolish processTest bars with various degrees of buffing were run through an electropolish process Cavity was rotated with a U-shaped electrode fixed in placeCavity was rotated with a U-shaped electrode fixed in place Initial polish failed due to depletion of the solution, and rebuffing was requiredInitial polish failed due to depletion of the solution, and rebuffing was required 2nd EP successfully removed scratches in high field regions2nd EP successfully removed scratches in high field regions Final process is a high pressure water rinse of cavity surfaceFinal process is a high pressure water rinse of cavity surface Interior Surface Electropolish

11. Coupling loops were fabricated using standard copper co-axCoupling loops were fabricated using standard copper co-ax Most coupler parts were joined by torch brazing – vacuum leaks were found in two of the outer conductor jointsMost coupler parts were joined by torch brazing – vacuum leaks were found in two of the outer conductor joints Coupling loop contains an integrated cooling tubeCoupling loop contains an integrated cooling tube The coupler was designed to mate with an SNS style RF window manufactured by ToshibaThe coupler was designed to mate with an SNS style RF window manufactured by Toshiba High power conditioning performed at SNS (ORNL)High power conditioning performed at SNS (ORNL) Cavity RF Couplers and Assembly

12. Coupler Conditioning Two loop couplers Conditioning started during PAC-05 week at SNS, ORNL Good vacuum ~ low 10 -8 Torr Achieved 600 kW in TW mode (matched load) Achieved 10 kW average power (~ 9 kW for nominal NF parameters) 2.4 MW peak powerAchieved 2.4 MW peak power in SW mode (at variable short positions) Two ceramic windows work flawlessly within two weeks of RF conditioning 805 MHz RF Power Two couplers RF Load

13. Shipment to the MTA at FNAL System assembly included: tuner plates, port blank-offs, diagnostic spool, window cover plates, gate valve and window pump-out tubes Final leak check conducted prior to shipping Cavity was back-filled with nitrogen in its assembled state and packaged in a custom made crate for shipping to the MTA Coupler shipment

14. Final Assembly & Measurement at MTA Cavity assembly was mounted on the support and couplers were installed in a portable clean room Dummy copper windows (flat) are used initially Couplers were set and frequency was measured Bakeout system hardware was installed System is leak tight View port with RF probes RF loop couplers End plate with diagnostic ports

15. Low Power Measurements at MTA f = 199.578 MHz Q 0 = 49,000 ~ 51,000 (better than 90% of the design value) Two couplers ─ balanced ─ coupling adjustments S 11 Measurement

16. Tuner 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 –~ 78 kHz/mm Calculated tuner sensitivity –115 kHz/mm –Disagreements are due to deflection of the Al plates Dial indicators

17. Curved Be Windows Two windows available now (LBNL) –42-cm in diameter and 0.38-mm in thickness –Good braze (between the two annular copper frames and the thin beryllium foil) –Achieved the designed window profile –Thin Ti-N coatings on both sides Ready for HP tests 42-cm

18. Asymmetric RF Heating ANSYS simulations –A 15 o slice cavity model –Solve for RF fields –8.4 kW average heating power –20 C o water cooling –Heat flux and temperature distribution –Stress and displacement –Frequency shifts Heat flux (w/m 2 ) Temperature (C o )  T ~ 130 C o  T ~ 70 C o Frequency shift of 94 kHz from room temperature to full RF power due to Cavity body expansion (small) Window displacement (major) Tuner Tuning sensitivity 115 kHz/mm  500 kHz range

19. Asymmetric RF Heating (cont’d) Thermal stress Elastic stress limit of beryllium is 310 MPa High!

20. RF Pulse Heating on the Windows ANSYS Transient simulations: –Solve for RF fields 4.5 MW –Scaled (normalized) the fields to 4.5 MW peak power 124.4 us15 Hz –Apply the power distribution within 124.4 us pulse and 15 Hz repetition rate –Temperature rise –Window and cavity deformation using the temperature distribution –Cavity frequency shift Temperature rise by a single pulse ~ 1 C o at r = R = 21-cm ~ 1 C o at r = R = 21-cm Cavity frequency change: ~ 80 Hz ~ 80 Hz center middle edge

21. RF Heat Transient to Steady State 8.4 kW average heating power: same pulse and rep. rate Monitor temperature at three locations on the windows at r = 0; r = R/2; r = R = 21-cm From 20 C o to steady state, it takes ~ 13 mins with frequency shift of 94 kHz. This frequency shift is well within the cavity bandwidth and can be tuned easily by mechanical tuners Cavity frequency stability with the Be windows under RF heating (from transient to steady state) is not a problem

22. Preliminary Test: Setup at MTA Loop power coupler Portable clean room Movable cavity support The cavity 201 MHz coaxial RF power line RF probes Vacuum pump Radiation monitor

23. Cavity Design Parameters The cavity design parameters –Frequency: 201.25 MHz – β = 0.87 –Shunt impedance (VT 2 /P): ~ 22 MΩ/m –Quality factor (Q 0 ): ~ 53,500 –Be window radius and thickness: 21-cm and 0.38-mm Nominal parameters for cooling channels in a muon collider or a neutrino factory –~ 16 MV/m peak accelerating field –Peak input RF power ~ 4.6 MW per cavity (85% of Q 0, 3  filling time) –Average power dissipation per cavity ~ 8.4 kW –Average power dissipation per Be window ~ 100 watts

24. Preliminary Test Conditioning started in late Feb. 2006 with –Flat copper windows (plates) with Ti-N coatings –RF diagnostics: field, power & radiation measurements –Good vacuum ~ high 10 -9 Torr Without external magnetic field, the cavity was conditioned very quietly and quickly to reach ~ 16 MV/m successfully Gradient is limited by RF power of 4.2 MW due to the modulator. 2 [MV/m]/division 0.1 ms/division

25. Summary The cavity reached design gradient of 16 MV/m successfully with almost no hard MPs: –Careful handling of the cavity –Good and clean surface finish EP and high pressure water rinsing –Ti-N coatings of the windows Test plan being actively developed to include test studies with –Thin and curved Be windows –RF heating on the windows: transient and steady state –External magnetic fields and achievable gradients versus the magnetic fields –Numerical and experimental studies of MP for the 201 MHz cavity