1 / 42

R&D status of ILC Positron Source KURIKI Masao (Hiroshima/KEK) ‏ 구리기 마사오 ( 히로시마 대학 )

R&D status of ILC Positron Source KURIKI Masao (Hiroshima/KEK) ‏ 구리기 마사오 ( 히로시마 대학 ). Table of Contents. Introduction RDR baseline configuration and its R&D. Alternative configuration and its R&D. TDP for ILC positron source Summary. ILC and Positron Source.

anise
Download Presentation

R&D status of ILC Positron Source KURIKI Masao (Hiroshima/KEK) ‏ 구리기 마사오 ( 히로시마 대학 )

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. R&D status of ILC Positron Source KURIKIMasao(Hiroshima/KEK) ‏구리기마사오 (히로시마대학)

  2. Table of Contents • Introduction • RDR baseline configuration and its R&D. • Alternative configuration and its R&D. • TDP for ILC positron source • Summary

  3. ILC and Positron Source • Undulator is the baseline design. • Two alternatives: • Conventional (electron driven) is a fall back. • Laser Compton is an advanced alternative. • Any schemes are not fully established. Need a certain amount of R&D for ILC positron source.

  4. Baseline Design • It relies upon gamma rays generated by passing 150 GeV electron through 168m undulator. • Undulator is “inserted” to part way of ML (150GeV). • A positron source driven by 0.5 GeV electron is a back up for high availability and machine commissioning.

  5. Undulator Parameters

  6. R&D efforts for the baseline (1) • This system is a totally new approach; Feasibility of the system should be confirmed in various levels. • Devices • System and sub-system • In addition, the ILC baseline e+ source is not an isolated system from the whole ILC and has inter-system dependencies. • Careful considerations are necessary from the system point of view. • E+ is generated at the same time for the collision. • E+ time structure is identical to that in ML.

  7. R&D efforts for the baseline (2) • The R&D efforts for critical devices are on going. • Super-conducting helical undulator. • Rotating conversion target. • Capture devices (pending due to no budget). • Several considerations from the system engineering point of view have been made. • E+ timing issue : a mathematical puzzle among DR harmonic number, bunch spacing in ML, round trip duration from e- DR to e+ DR, etc. • Keep Alive e+ source : machine commissioning, fast recovery from the system failure,etc.

  8. Undulator Cryo-module Overview 50K Al Alloy Thermal shield. Supported from He bath U beam Support rod Stainless steel vacuum vessel with Central turret Stainless Steel He bath contains100L liq He. Supported by 4 rods attached to the vacuum vessel U Beam used to support/align the magnet. Beam Tube Magnet cooled to 4.2K by liq He in bath. S Carr

  9. Undulator Cryomodule U Beam Heat Shield Helical Undulator He Vessel

  10. Quench Test & Field Measurement • All two magnets finally satisfied the specification. • Field profile is measured by hall probe, showing a good quality.

  11. Conversion Target • Water-cooled electromagnet • Variable pole gap (0mm to 160mm)‏ • Peak field > 1 T at wheel • Ti alloy wheel. Photon beam Ken Davies - Daresbury Laboratory • Torque Sensor • 15 kW drive motor L Jenner

  12. Target Prototype Experiment will start when personnel guards are in place Should be completed by end of 2008

  13. Matching Device • The generated positrons is a point like with a large transverse momentum spread. • That should be converted to a parallel beam for further acceleration; The matching device does it. • Depending on the matching device, it increases capture efficiency from 10% to 40%.

  14. DC Solenoid • High field (6T) and high capture efficiency(30%). • Similar to other DC SC magnets; It is technically matured. • It is not feasible for ILC since 100's of kW of eddy current in a fast rotating metal target.

  15. Shielded Flux Concentrator • Ramping from 0T to 7 T in 2cm (no field on target). • Capture Efficiency ~21% • Difficult technically to sustain 1ms pulse train length. • Further study needed to prove feasibility (prototype).

  16. Quarter Wave Transformer • Ramping from 0T to 1 T in 5cm (no field on target). • Capture efficiency ~ 15%. • Technically matured and realizable (actual baseline).

  17. Summary for baseline • R&D efforts for critical devices are in progress (undulator, target, etc). • Although Matching device is one of the most important, the R&D is stopped. • QWT is the only realistic solution at this moment and it should be actual baseline as long as there is no big progress on R&D for MD.

  18. Alternative Design • e- driven scheme (conventional) and Laser Compton scheme are considered to be alternative schemes. • e- driven scheme is a back-up alternative. • Laser Compton is an advanced alternative. • Because the baseline design is a totally new approach, a conservative alternative is very important as a technical backup. • Laser Compton is attractive, but it is technically immature; It is advanced alternative.

  19. e- driven scheme • e- drive beam impinges on a conversion target. • 6 GeV 2E+10 e- bunch. • Amorphous W (W-Re alloy), crystalline W, diamond, liquid Pb-Sn,etc. • Capture devices. • E+ booster up to 5 GeV: The technology depends on the pulse structure; SC for long pulse case (~1ms) and NC for short pulse case (<50μs). • The most important and difficult issue is conversion target.

  20. CHANNELING FOR ILC & CLIC e+ sourceR. Chehab • A single target works for CLIC, but multi-target is needed for ILC limited by PEDD. • A single target might work for ILC in Low P parameter. “x” meters e+ Only the photons are impinging on the converter: that limits the energy deposition in the amorphous target. γ e- e+, e-,  e- Crystal Amorphous Radiator Converter

  21. Liquid lead target Driving motor • A prototype in BINP has been operated 20000h without any troubles. • Pb 90% Sn 10%, 300˚C, Cog-wheel pump. • Brazing technique for BN window has been established. Cog-wheel pump Vacuum pump Target head Liquid Pb-Sn jet in vacuum transport tubes

  22. Laser Compton Scheme • A few GeV (1.8GeV for example) electron bunch collides with 1μm laser photon stored in optical cavity. • Several 10s MeV gamma impinges in a conversion target. • A dedicated electron driver is reasonable. • Obtaining enough positron, is a technical challenge. • High intensity electron beam: Linac, Storage ring, ERL • High intensity photon beam: High power laser, optical cavity. • Stacking scheme: DR stacking, Pre-DR, etc.

  23. Compton Ring • A storage ring for electron driver:5.3nC, 6.2ns, 1ps, 1.8GeV, 0.6Jx5CP. • Positron bunch(Ne+:2.0E+8) is generated. • 10 bunches are stacked on a same bucket. This process is repeated 10 times with 10ms interval for beam cooling. • Finally, Ne+:2E+10 is obtained.

  24. ERL • ERL(Energy Recovery Linac) is employed as the dedicated electron driver. • 0.48nC, 18.5ns (54MHz) ~ 26mA, E=1.8GeV • Nγ=2.3E+9 by 0.6 Jx5 CP, Ne+=2.0E+7 • By a semi-CW operation (50ms), 1000 times stacking in DR is performed and Ne+=2.0E+10 is obtained.

  25. Pulse Stacking Optical Cavity

  26. Pulsed Laser Injected Cavity R. Chiche

  27. High power ps fiber amplifier E. Cormier

  28. Experiment at KEK-ATF PD 16~28MeV 420mm γray CSI Electron beam Collision angle 12 degree e beam Mode lock laser γ/collison λ:1064nm 10W=28nJ , 2.8ns spacing Pulse length : 7ps Finess = 780 = 30 μm

  29. Stacking Simulation F. Zimmermann • # of positron by a single collision is not sufficient -> need stacking. • Stacking simulation in DR (multi-turn injection) shows 10.6% of injected e+ are lost! stacking efficiency ~90%. • The tolerance of the injection loss would be qualified.

  30. CLIC Compton Scheme • Collaboration on Positron Generationstrongly supported by CLIC and ILC managements (J.P. Delahaye@PosiPol08)

  31. PosiPol-Collaboration • Laser-Compton has a large potential as a future technology. • Many common efforts can be shared in a context of various applications. • X-ray/SR sources for industrial and medical applications, • Beam diagnostics with Laser, • Polarized Positron Generation for ILC, CLIC, SuperB, .. • State-of-the-art technologies are quickly evolved with world-wide synergy. • PosiPol collaboration has been started in 2006. • The last annual meeting was held at Hiroshima in July 08. The next meeting will be held at near CERN in 2009.

  32. WWW of PosiPol R&Ds 4th Generation light source ERL/Ring ILC e+ CLIC e+ e+ source Laser Compton SuperB Material Science Scientific Application LW monitor/ Polarimetry Medical applications X-ray source Optical Cavity Industrial applications e- source ILC, ERL High power laser

  33. Technical Design Phase Minimum machine studies Re-baseline in 2010 (publish in interim report)‏ • TDP is a multi-phase approach towards TDR. • TDP-1 is focused on • Risk mitigation • Cost reduction • TDP-2 is a real technical design phase based on the design established on TDP-1.

  34. ILC Positron Source:MM • Undulator is moved to the end of ML (250GeV). • Energy scan <100GeV is difficult. • Dedicated pulse for e+ generation with ½L. • QWT instead of AMD, which has lower capture efficiency; The undulator length is 350m. • KAS share the common target with gamma1 source; yield is only 1% of the nominal intensity.

  35. Further Considerations on MM • Improved Low P parameter : half # of bunches in a pulse. • It is a big fair wind for the electron driven. • Potential target damage, which is the most serious issue on electron driven scheme, is relaxed. • There are active R&D on noble ideas. • No doubts that Conventional is really “conventional”.

  36. TDP Summary • Basic R&D is very important in TDP1. • Re-baseline at the end of TDP-1 is the mile-stone. • According to the investigation based on the latest technology, the status is: • The conventional method is important as a fall-back. Low P parameter and noble target technologies make it feasible and reliable. • Technical difficulty forces the undulator system bigger and bigger and it does not seem “mimimal machine”. • From the pure technical point of view, the baseline is the electron driven and undulator and laser compton are upgrade alternatives.

  37. Summary • R&D status of ILC positron source is reviewed. • Undulator scheme is the baseline design. • SC helical Undulator, rotating rim target prototype. • Need study for matching device. • e- driven scheme is important as a backup. • There are several active R&Ds based on noble ideas. It is the best scheme for MM. • Laser Compton is an advanced alternative. • Aggressive R&D efforts. • Still need more technical maturity. • ILC-CLIC collaboration.

  38. Thank youfor your attention.귀하의 관심을 주셔서 감사합니다

  39. TDP-2 TDP-2: • Technical requirements documentation • Technical design work  cost update • Value Engineering • Cost & Schedule • 18 month period

  40. Liquid Pb-Sn Target • Liquid Pb target + BN window is very strong against high peak power, but less average power. • Pulsed operation (e.g. 100 bunches with 6.2ns spacing, 0.6μs, 150Hz) moderates thermal effects. • In the pulse operation, capture efficiency is higher and incident electron can be fewer. Average power (kW) Operation point Energy/100ps GeV/mm21012 • P. Logachov et al. in APAC2007

  41. RDR Source Layout Ti-alloy fast rotating target for gamma -> e+ conversion. Capture devices : AMD or QWT + L-band NC accelerator with solenoid focusing. Backup source (500MeV e-, 10% intensity).

  42. Flux Concentrator for KEB upgrade

More Related