Greeting for 7th TB and ATF2 joint meeting

Slides:



Advertisements
Similar presentations
~1m undulator IP Pol. e + source based on Compton scattering with FEL & 4 mirror cavity Low energy electron beam Gamma-ray FEL photon beam LCWS2014 in.
Advertisements

Status of g ray generation at KEK-ATF ► Introduction ► Status of the cavity R&D ► Out Look French Labs. : LAL (Orsay) in Collaboration with CELIA (Laser.
Before aperture After aperture Faraday Cup Trigger Photodiode Laser Energy Meter Phosphor Screen Solenoids Successful Initial X-Band Photoinjector Electron.
Beam loading compensation 300Hz positron generation (Hardware Upgrade ??? Due to present Budget problem) LCWS2013 at Tokyo Uni., Nov KEK, Junji.
Demonstration of the Beam loading compensation (Preparation status for ILC beam loading compensation experiments at ATF injector in this September) (PoP.
Conventional Source for ILC (300Hz Linac scheme and the cost) Junji Urakawa, KEK LCWS2012 Contents : 0. Short review of 300Hz conventional positron source.
1 Junji Urakawa (KEK, Japan) at Sapphire day, Under development of Quantum Beam Technology Program(QBTP) supported by MEXT from to
Accelerator R&D on LC - Activities of ATF & STF - 1. Introduction 2. ATF 3. STF 4. Summary Seiya Yamaguchi, KEK The US/Japan Collaboration in High Energy.
1 Plans for KEK/ATF 1. Introduction 2. Related Instrumentations at ATF 3. Experimental Plans for Fast Kicker R&D at ATF Junji Urakawa (KEK) at ILC Damping.
STF Status and Future plan H. Hayano, KEK, LCWS12 Arlington System Test session 1.
Low Emittance RF Gun Developments for PAL-XFEL
Compton Experiment at ATF LCWS10 28-March-2010 T. Takahashi (Hiroshima) / T. Omori (KEK) for collaborators.
Electron Source Configuration Axel Brachmann - SLAC - Jan , KEK GDE meeting International Linear Collider at Stanford Linear Accelerator Center.
1 Proposal for a CESR Damping Ring Test Facility M. Palmer & D.Rubin November 8, 2005.
T.Takahashi Hiroshima Optical Cavity R&D around KEK-ATF T.Takahashi Hiroshima Univ. Nov LCWS08 at Chicago.
Greeting for 10 th ATF2 project and TB/SGC joint meeting 1.
Compton Experiment at ATF Compton Meeting at LAL Orsey 2-Dec-2008 Tsunehiko OMORI (KEK) with many thanks to Compton collaborators.
–10.06 Milan Italy LUCX system and dark current (1) LUCX project (2) Phase Ⅰ and results (3) Phase Ⅱ and dark current Liu shengguang and LUCX.
The SPS as a Damping Ring Test Facility for CLIC March 6 th, 2013 Yannis PAPAPHILIPPOU CERN CLIC Collaboration Working meeting.
LUCX FACILITY INTRODUCTION : PRESENT STATUS AND FUTURE PLANS A. Aryshev On behalf of QB group and THz collaboration Mini-workshop for advanced THz and.
Electron Sources for ERLs – Requirements and First Ideas Andrew Burrill FLS 2012 “The workshop is intended to discuss technologies appropriate for a next.
ILC R&D at KEK Beam Control Technology –ATF –ATF2 Acceleration Technology –High-gradient Cavities L-band R&D Stand –Linac System  STF –Construction of.
ATF status M. Ross October 15, 2004 The ATF is the largest test facility built exclusively for linear collider RD –Utility not reduced by the selection.
Status of the Compton Experiment at the ATF TILC09 18-April-2009 T.Takahashi Hiroshima University for collaborators.
Compton Experiment at ATF DR 2009 Summary and Plan ATF2 Project Meeting 15-Dec-2009 T. Omori (KEK) for collaborators.
T.Takahashi Hiroshima /11/5 Tohru Takahashi Hiroshima University 高橋 徹 広島大学.
Future Circular Collider Study Kickoff Meeting CERN ERL TEST FACILITY STAGES AND OPTICS 12–15 February 2014, University of Geneva Alessandra Valloni.
Laser-Undulator Compact X-ray source (LUCX) POSIPOL2006 Workshop at CERN 1/23 Experimental Plan of X-ray Generation using Optical Resonator using Optical.
Global Design Effort ILC Damping Rings: R&D Plan and Organisation in the Technical Design Phase Andy Wolski University of Liverpool and the Cockcroft Institute,
1 Experiments with pulse supplies and strip-lines at ATF, Plans for fast extraction kicker for ATF2 1. Fast Kicker R&D at ATF 2. Instrumentation at ATF.
1 Junji Urakawa (KEK, Japan) at PosiPol2012, Under development of Quantum Beam Technology Program(QBTP) supported by MEXT from to
1 1 H. Hayano and ATF group ATF Status August/2004 H. Hayano and ATF group Multibunch emittance Instrumentation developments Plans for run Multibunch.
Laser electron beam x 30 Multi-Compton chamber system γ-ray cm Conceptual design in 2005 Snowmass X 5 at present Big progress During R&D.
ISG – Damping Ring Physics and Design Group ATF – 2003// focus on the TRC challenge Marc Ross – 1.Instability about which little is known: Fast ion,
Compton Gamma-ray Generation Experiment by Using an Optical Cavity in ATF POSIPOL 2007 Workshop at LAL Hirotaka Shimizu Hiroshima University.
ILC R&D Activities at KEK Superconducting Linac Development Beam-handling Technology Development.
ESLS Workshop Nov 2015 MAX IV 3 GeV Ring Commissioning Pedro F. Tavares & Åke Andersson, on behalf of the whole MAX IV team.
Operation Status of the RF Systems and Taiwan Photon Source
Laser electron beam x 30 Multi-Compton chamber system γ-ray cm Conceptual design in 2005 Snowmass X 5 at present Good progress During R&D From Conventional.
1 Junji Urakawa, KEK Introduction 1. Photo-cathode RF gun 2. Pulsed laser storage cavity 3. Quantum beam project Quantum beam project( )
Applications by means of the accelerator technologies based on cERL
Degradation and Recovery of Cavity Performance
Sara Thorin, MAX IV Laboratory
Auxiliary Positron Source
Oversea collaborators
BUNCH LENGTH MEASUREMENT SYSTEM FOR 500 KV PHOTOCATHODE DC GUN AT IHEP
WP11: electron and proton beam testing
Paul Scherrer Institut
Compton X-ray generation in a small S-band accelerator
Junji Urakawa (KEK) for ATF International Collaboration
Pol. positron generation scheme for ILC
ATF Intrabeam Scattering Results
The Cornell High Brightness Injector
Compton effect and ThomX What possible future?
Machine Operation and Progresses in SSRF
Performance Degradation cERL Injector Cryomodule
Electron Source Configuration
ERL accelerator review. Parameters for a Compton source
Summary of Gamma-Gamma session
LAL meeting on e+ studies, Oct. 2010
CEPC Injector Damping Ring
The Proposed Conversion of CESR to an ILC Damping Ring Test Facility
2012/10/31 10am version… Abstract #: Conference: NSS (Oral)
Advanced Research Electron Accelerator Laboratory
ATF project meeting, Feb KEK, Junji Urakawa Contents :
Instability measurement plans at ATF
N. Terunuma (KEK) ILC2010, Beijing, March 29th, /2/28.
Linac/BC1 Commissioning P
Proposal for a CESR Damping Ring Test Facility
小型X線源の性能確認実験計画 高輝度・RF電子銃研究会 広島大学 高エネルギー加速器研究機構 浦川順治
Presentation transcript:

Greeting for 7th TB and ATF2 joint meeting

Accelerator Test Facility ATF2 beam line (2008~) Extraction line Damping Ring Photo-cathode RF gun (electron source) S-band Linac f ECS for multi-bunch beam

ATF – beam operation schedule ATF2 ON Commissioning to start in Dec. 2008 We got the temporary permission to operate ATF2 in Dec.. I think we will get the formal permission from MEXT in Jan.. Then, we can carefully operate ATF2 for beam commissioning. Thank you for your understanding in this situation.

Necessary Deliverables from TF for BDS and DR Test Facility Deliverable Date Hardware development, Optics and stabilisation demonstrations: ATF Demo. of reliable operation of fast kickers meeting the specifications for the ILC damping ring. 2010 Generation of 1 pm-rad low emittance beam 2009 ATF2 Demo. of compact Final Focus optics (design demagnification, resulting in a nominal 35 nm beam size at focal point). Demo. of prototype SC and PM final doublet magnets 2012 Stabilisation of 35 nm beam over various time scales. Electron cloud mitigation studies: CESR-TA Re-config. (re-build) of CESR as low-emittance e-cloud test facility. First meas. of e-cloud build-up using instrumented sections in dipoles and drifts sections (large emittance). 2008 Achieve lower emittance beams. Meas. of e-cloud build up in wiggler chambers. Characterisation of e-cloud build-up and instability thresholds as a func. of low vertical emittance (≤20 pm) DAΦNE Fast kicker design and pulser reliability check Characterisation of e-cloud build-up and instability thresholds SLAC/LLNL Fast kicker pulser development

7th ATF2 Project Meeting, 15-18 Dec. 2008 Thanks to many colleagues from the ATF Collaboration, those on these photo. 7th ATF2 Project Meeting, 15-18 Dec. 2008 5 5

High-Intensity Compact X-ray Source Must be demonstrated by JFY2012 Includes 25 MV SC acceleration and deceleration (but perhaps, deceleration can be omitted) Beam current (9mA) and pulse length (1ms) same as ILC, but bunch spacing 6.15nsec

Better to combine with STF2 for saving manpower and money Build QB in STF tunnel Identify 25MV acceleration cavity = STF capture cavity, though QB does not need 2 cavities Can share the RF gun (but not the laser --- different pulse structure) But the price is the schedule delay Interruption for at least half a year, likely ~1 year (installation of QB beam-line and tuning for X-ray) To minimize the delay, plan to finish QB before 2012 summer vacation.

2. Photo-cathode RF gun Cs2Te Photo-cathode, 1.6 Cell S-band RF Gun Multi-bunch beam generation

Fig.5 Momentum distribution of bunch train

100 bunches/pulse energy spread is less than 0.5%. Fig. 7 Upper-left : ICT signal of 100 bunches, upper-right : 100 bunches on the OTR screen, bottom figure : energy of each bunch in the train

Laser Pulse Stacking Chamber, 3m long S-band accelerating tube and S-band accelerating tube (3m) Chicane Bending magnet Q-magnet solenoid RF Gun Cathode: Cs-Te PRM: Beam Profile Monitor OTR target or Al2O3 (Cr3+ doped) Emittance measurement Beam energy and energy spread measurement Collision point BPM: Beam position monitor BPM PRM PRM PRM ICT Faraday Cup ICT & Faraday Cup: Beam current monitor e- beam Side view Top view Laser Pulse Stacking Chamber, 3m long S-band accelerating tube and Photo-cathode RF Gun

Emittance measurement Collision point εx: 3.0 [mm・mrad] QF1 QD1 Beam current : 2.5nC/train, 3bunches Beam profile at Collision point εy: 4.7 [mm・mrad] σx: 86um σy: 36um CP1G (OTR)

Optical Circuit P-LW-CAV installed in APR2007. e- beam e- beam

X-ray Generation 43MeV end station to separate X-ray and e-beam. 33keV X-ray is deflected by Crystals. Pulsed laser stacking chamber

Laser Undulator Compact X-ray (LUCX) Project at KEK-ATF Multi-bunch photo-cathode RF Gun 43MeV Multi-bunch beam+ Super-Cavity = 33keV X-ray. X-ray Detector S-band Acc. Structure Beam size at CP 60mm in s Multi-bunch e- beam 300nC at gun At present, laser waist size is 30mm in s. We should reduce both beam size at CP down to 30mm. 33keV X-ray generation based on inverse Compton scattering was started from May 2007 with Super-Cavity. Storage Laser power 40kW, 7psec(FWHM), next step :1MW

3. Pulsed laser storage cavity From two-mirror cavity to four-mirror cavity under International collaboration with LAL. 50 mJ / pulse, waist = 8 m e- beam laser beam

R/D Status in Japan Moderate Enhancement ~ 1000 Moderate spot size ~ 30 micron Simple cavity stucture with two mirrors Get experinence with 43MeV and 1.3GeV e- beam Laser Undulator Compact X-ray (LUCX) Project at KEK-ATF 43MeV Multi-bunch beam+ Super-Cavity = 33keV X-ray. Expected X-ray is generated.

SCRF acceleration technology 4. Quantum beam project Characteristic of proposed machine Compact (less than 10m) quasi-monochromatic (less than 1%) High Flux ( 100 times than Compact normal Linac X-ray:1011 photons/sec 1% b.w.) High Brightness (1017 photons/sec mrad2 mm2 0.1% b.w.) Ultra-short pulse X-ray (40 fs ~) SCRF acceleration technology Key technology is Structural Nano-material Highly fine genetic analysis, evaluation, X-ray Imaging http://mml.k.u-tokyo.ac.jp/

400 times by CW operation : ERL SCRF Cavity Ultra-low loss(10nΩ) long pulse acceleration high intensity and low emittance Pulsed laser storage Storage energy : 100 times Beam size < 8 m Laser Inverse Compton scattering High intensity, high quality, monochromatic X-ray 400 times by CW operation : ERL Photo-cathode RF gun Low emittance beam 3mmmrad Short pulse, 162.5MHz bunch train 20

Pulsed Laser Storage Beam orbit control Achieved by ATF From 2-mirror cavity to 4-mirror cavity 0.5 mJ / pulse, waist = 30 m 50 mJ / pulse, waist = 8 m Beam orbit control Achieved by ATF Laser wire waist:  ~ 3 m Electron beam size: ~ 2 m

Compact and reliable Multi-beam Klystron R&D Organization & Responsibility Toshiba Compact Klystron Compact and reliable Multi-beam Klystron R&D High power RF Committee for project evaluation Main Institute KEK SC RF Accelerator development System design, Operation, Performance Measurement Education for young sientists ATF, STF High stable HV PS Hitachi DC High Voltage Source Hiroshima U. Laser storage RF Gun Photo-cathode Pulsed Laser Storage High Quality and Intensity e- source JAEA DC High Voltage PS Photo-Cathode ERL Electron Source Device Waseda U. X-ray detector Laser Compton Exp. Compact Accelerator U. of Tokyo Photo-cathode Input coupler 22

Annual Schedule and Budget Item 2008 2009 2010 2011 2012 S. Cavity Development ($1.5M/year), HRF + Cly ($0.8M/year) Upgrade of SC Cavity performance Compact RF power source system Control system for SCRF Construction of Test Accelerator・Confirm the performance Electron Source ($0.5M/year) High Q and long life photo-cathode 500 kV DC High Voltage High Intensity Beam Generation Pulsed Laser Storage System ($0.4M/year) X-ray Detector ($0.1M/year) Design and R&D on laser storage 23

Impact by Compact High Brightness Photon Beam 1) Performance of 2nd Generation PF will be obtained in usual Lab. Space! Analysis of Genome @A University Evaluation of Material @Lab. of B Company Precise X-ray Imaging @C Hospital 2) Sub-psec X-ray is generated→Study fast transient phenomena Chemical reaction in solvent, Activity of protein, Impulse destroy, Photon induced phase transition  3) Precise Nuclear Isotope detection by NRF (Solve energy and environmental problems) 24

Target of component technology Present status Target Key points Electron source 300 nC/pulse 10,000nC/pulse (2008-2009) 48,000 nC/pulse (2010-2012) Pulse laser, new photo-cathode, 1 msec pulse length SC Cavity Pulse: 25 MV/m CW: 12 MV/m Pulse: 30 MV/m CW: 20 MV/m Non-defect and clean surface, Precise electron beam welding, High precision forming, Non-contamination material Pulsed laser storage 0.5 mJ/pulse, Waist: 30 m 50 mJ/pulse, Waist: 8 m 4-mirror optical cavity Colliding control m beam orbit control Sub- m beam orbit control minimizing environmental effect, Fast feedback control

Compact high brightness X-ray source using SC Cavity Quantum beam project(2008-2012) approved by MEXT Compact high brightness X-ray source using SC Cavity Photo-cathode RF Gun Pulsed Laser storage Cavity 30 MeV/m SC. 9 cell Cavity Decelerating Exp. X-ray Detector ERL R&D 25 MeV まで加速 decelerate to 1MeV He refrigerator 26

Join and Enjoy 忘年会(End year Party) in this evening. Thank you for your attention.