Nanometre scale beam handling at the ATF Philip Bambade Laboratoire de l’Accélérateur Linéaire Université Paris 11, Orsay, France Seminar at DESY 7 May.

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Nanometre scale beam handling at the ATF Philip Bambade Laboratoire de l’Accélérateur Linéaire Université Paris 11, Orsay, France Seminar at DESY 7 May 2014

ILC TDR Layout Damping Rings Polarised electron source E+ source Ring to Main Linac (RTML) (including bunch compressors) e- Main Linac e+ Main Linac ParametersValue C.M. Energy GeV Peak luminosity1.8 x10 34 cm -2 s -1 Beam Rep. rate5 Hz Pulse duration0.73 ms Average current 5.8 mA (in pulse) E gradient in SCRF acc. cavity 31.5 MV/m +/-20% Q 0 = 1E10

3 Tunnel implementations (laser straight) Central MDI & Interaction Region CLIC

 

Nanometre scale beam handling R&D at the ATF (KEK, Japan)

ATF に参加している代表的研究機関 - ATF International Collaboration - 先端加速器試験装置( ATF ) 欧州原子核研究機構 (CERN) ドイツ (Germany) 電子シンクロトロン研究所 (DESY) フランス (France) IN2P3; LAL, LAPP イギリス (UK) Univ. of Oxford Royal Holloway Univ. of London STFC, Daresbury Univ. of Manchester Univ. of Liverpool Univ. College London イタリア (Italy) INFN, Frascati スペイン (Spain) IFIC-CSIC/UV ロシア (Russia) Tomsk Polytechnic Univ. 日本 (Japan) 高エネルギー加速器研究機構 (KEK) 東北大学 (Tohoku Univ.) 東京大学 (Univ. of Tokyo) 早稲田大学 (Waseda Univ.) 名古屋大学 (Nagoya Univ.) 京都大学 (Kyoto Univ.) 広島大学 (Hiroshima Univ.) 中国 (China) 中国科学院高能物理研究所 (IHEP) 韓国 (Korea) ポハン加速器研究所 (PAL) キョンプク大学 (KNU) インド (India) Raja Ramanna Centre for Advanced Technology アメリカ (USA) SLAC 国立加速器研究所 ローレンス・バークレー国立研究所 (LBNL) フェルミ国立加速器研究所 (FNAL) ローレンス・リバモア国立研究所 (LLNL) ブルックヘブン国立研究所 (BNL) コーネル大学 (Cornell Univ.) ノートルダム大学 (Notre Dome Univ.) Members of E-JADE WP2

Parameters ATF2 ILCCLIC Beam Energy [GeV] L* [m]  x/y [m.rad] / / / IP  x/y [mm] 4 / / / 0.07 IP  ’ [rad]  E [%] ~ 0.1 ~ 0.3 Chromaticity ~  / L* ~ 10 4 ~ Number of bunches1-3~ Bunch population IP  y [nm] SuperKEKB / ATF2 = scaled ILC FFS start point of CLIC FFS (SuperKEKB + FCC-ee/CEPC) concept of local compact chromaticity correction ~ / ~ β y < σ z

Main LC beam delivery issues addressed by ATF / ATF2 Beam instrumentation Stabilization 4+1 dim. beam tuning & control for small IP spot Halo control - nm-level position - profile (x, y, tilt) - passive / active mechanical stabilization - beam / vibration measurement based feed-back/forward - emittance minimization via radiation damping - mitigation of 1 st, 2 nd and 3 rd order optical aberration  wakefields - convergence time  dynamical errors (sismic & thermal effect) - modeling, generation, propagation, monitoring… - collimation (physical, optics) 

ATF / ATF2 project goals  Very small damping ring vertical emittance - from  10 pm  4 pm (achieved !)  1-2 pm  Small vertical beam size “goal 1” - achieve  y  37 nm (cf. 5 / 1 nm in ILC / CLIC) - validate “compact local chromaticity correction”  Stabilization of beam center “goal 2” - down to  2nm - bunch-to-bunch feedback (  300 ns, for ILC)  R&D on nanometer resolution instrumentation  Train young accelerator scientists on “real system” - maintain and develop expertise by practicing operation  open & unique facility

Experimentation with ATF2 nanometre beams DR extraction setup, stability Match optics into FF buffer section for input errors 2 nd order telescope fine tuning of local errors

Measuring nanometre beam sizes at ATF2 Laser wavelength 532 nm Modulation of Compton scattered photon rate from beam interaction with laser interference fringe pattern

History of measured minimum beam size Still being improved. Bunch charge  electrons  1/5-1/10  nominal Horizontal   40 mm  10  nominal

Beam Size Tuning after 3 weeks shutdown Small beam (~60 nm) observed ~32 hours from operation start ~10 hours of IP beam size tuning  y (nm) Time (hours) from Operation Start after 3 Weeks Shutdown Week 2014 April 7 Beam Size Tuning after 3 days shutdown Small beam (~60 nm) observed ~16 hours from operation start ~8 hours of IP beam size tuning Week 2014 April 14

ATF2 goal 2 : nm-beam position stabilization Triplet of New IPBPM Low-Q short gap cavity light weight BPM Sensitivity tested at ATF LINAC Readout electronics tested at ATF2 New kicker Installed near the ATF2-IP Used since autumn 2012 KEK KNU LAL JAI/Oxford New vacuum chamber Precise positioning of IPBPM triplet IP Beam

In vacuum IP-BPMs and piezo movers BPM A&B BPM C Piezo Movers (PI) Piezo Movers (Cedrat) BPMs –Bolted aluminum plates, no brazing because of In- vacuum. –BPM A&B bolted together. –BPM C is independent. Piezo mover –BPM units are mounted on the base with three piezo movers. –Dynamic range of each mover is +/- 150 um. IP Slide from Terunuma Initial alignment need to be better than this. Installed summer 2013

Methodology for stabilization Goal 1 (beam size  37 nm) beam jitter < 10 nm Goal 2 (nm-scale stability with feedback) beam jitter  2 nm 1.Measure stability at one of IP-BPMs after shifting the beam waists there 2.Infer position from measurements at the two other IP-BPMs 3.Use fast kicker just upstream of IP to correct second bunch within ATF2 train 4.Use fast feedback upstream to check for improved IP stability 5.Use fast kicker upstream for corrections based on IP-BPMs 6.Infer IP beam jitter based on IP-BPM measurement for use in beam size analysis alignment - calibrate scale factors - study system resolution  123 IP beam kicker

18 Best standard jitter measurement 66nm (single)  49nm (avg.)

WP2 : Nanometre scale beam handling at the ATF Objectives 1.Achievement and maintenance of nanometre scale beam size 2.Measurement and feedback to stabilise beam position at nanometre level 3.Development of advanced beam diagnostics instrumentation 4.Control of beam halo and background mitigation 5.Training of junior scientists and students in accelerator science Participant Short Name CERN CNRS CSIC KEK RHUL UOXF UoT Person-months per Participant  Usual ATF beam operation: weeks / year + maintenance (except 2014)

Main focus of work Task 2.1 Beam Size Minimisation (CERN, CNRS, KEK & UoT): Reduce effective β* parameter by improving corrections of optical aberrations. Install, commission and operate two new octupole correction magnets. Study alternative optics. Task 2.2 Wake Field (CERN, CSIC, KEK & RHUL): Calculate and measure wakefields from beam position monitors and collimators. Test novel wake field free steering algorithm. Task 2.3 Ground Motion (CERN, CNRS & KEK): Measure ground motion (GM) using 14 installed GM sensors synchronised with beam position measurements to assess novel GM based feed-forward algorithm. Test newly developed GM sensor. Task 2.4 Halo Collimation and Backgrounds (CNRS, CSIC, KEK & RHUL): Calculate and measure beam halo propagation. Develop and test two new retractable collimators for halo reduction. Simulate beam induced backgrounds with GEANT4. Task 2.5 Beam Instrumentation and control (CNRS, KEK, RHUL, UOXF & UoT): Operate, simulate and optimise performances of existing instrumentation, including laser wire and nanometre resolution beam position and size monitors. Install, commission and operate new radiation hard diamond sensor beam tail monitor. Develop and test new submicron optical transition/diffraction radiation beam emittance diagnostics. Task 2.6 Beam Position Feedback (KEK & UOXF): Install, commission and operate fast digital feedback for nanometre level beam position stabilization at the collision point. Use beam tracking simulation to model and benchmark feedback performance.

Deliverables Month 12 HaloCollBgds-1: Report on halo measurement and control using diamond sensor and collimators. Month 12 Instr-1: Report on performance optimisation of installed high resolution beam position and size instrumentation. Month 24 Instr-2: Design report of optical transition/diffraction radiation combined measurement station including initial beam tests. Month 18 GM-1: Reports on synchronisation of GM and orbit measurements and on new GM sensor performance. Month 24 BeamSize-1: Report on performance of installed octupole magnet pairs in correcting third order optical aberrations. Month 24 Wakefield-1: Report on wakefield simulation and measurements including mitigation plans and implications for the Linear Collider. Month 24 Feedback-1: Report on operation of collision point feedback system. Month 24 HaloCollBgds-2: Report on integrated simulation and evaluation of beam transport including beam instrumentation and charged particle backgrounds. Month 36 Wakefield-2: Report on wakefield free steering performance to mitigate wakefields. Month 36 GM-2: Final report on correlation between GM and orbit measurements and implications for GM based feed-forward. Month 48 Feedback-2: Final report on performance of interaction-point feedback system, and implications for its implementation in the Linear Collider. Month 48 BeamSize-2: Final report on beam size minimisation in horizontal and vertical dimensions using optimised optics, and implications for the Linear Collider.

Stay tuned for very small & very stable beams in ATF2 in ! ATF/ATF2 is a great opportunity for students and staff, in an international environment, especially for beam dynamics and instrumentation  Essential learning experience towards ILC/Japan & CLIC And also useful for other projects… H2020 / RISE / E-JADE will be of great importance to support the significant mobility to KEK needed for ATF2 research Thank you for your attention ! Conclusions and prospects