BEAM ACCELERATION EXPERIMENT IN X-BAND 11.424 GHZ LINAC FOR COMPTON SCATTERING X-RAY GENERATION Hirotoshi Masuda The University of Tokyo.

Slides:



Advertisements
Similar presentations
12GeV Project CD-4 Leigh Harwood Associate Project Manager Accelerator Systems.
Advertisements

New Radiation Safety Interlock System for the SPring-8 Accelerator Complex C. Saji, M. Toko, T. Matsushita, R. Furuta, H. Hanaki, S. Hashimoto 1), Y. Hashimoto,
Beam Dynamics in MeRHIC Yue Hao On behalf of MeRHIC/eRHIC working group.
RF-Gun cavity for high charge electron generation Takuya Natsui.
Radiation Physics | ELBE | SRF Photo Injector for Electron- Laser Interaction LA 3 NET conference: Laser applications at accelerators, Mallorca,
Tessa Charles Australian Synchrotron / Monash University 1 Bunch Compression Schemes for X-band FELs.
Chris Tennant Jefferson Laboratory March 15, 2013 “Workshop to Explore Physics Opportunities with Intense, Polarized Electron Beams up to 300 MeV”
An Advanced Linear Accelerator Facility for Microelectronic Dose Rate Studies P.E. Sokol and S.Y.Lee Indiana University.
Medical Imaging Mohammad Dawood Department of Computer Science University of Münster Germany.
Thomson Scattering X-ray Source at Tsinghua University
RF Waveguide & Structures Linac Coherent Light Source Stanford Synchrotron Radiation Laboratory Stanford Linear Accelerator Center.
Recirculating pass optics V.Ptitsyn, D.Trbojevic, N.Tsoupas.
MVE MURI 99 Kick-off Meeting R. Barker, Technical Monitor Started 1 May 99 October 1999 An X-Band Photoinjector for Intense MM-Wave and Tunable X-Ray Generation.
Before aperture After aperture Faraday Cup Trigger Photodiode Laser Energy Meter Phosphor Screen Solenoids Successful Initial X-Band Photoinjector Electron.
MuCool RF Status MICE Collaboration Meeting June 7-10, 2006, Fermilab A. Moretti June 9, 2006.
Accelerator Physics  Basic Formalism  Linear Accelerators  Circular Accelerators  Magnets  Beam Optics  Our Accelerator Greg LeBlanc Lead Accelerator.
ALPHA Storage Ring Indiana University Xiaoying Pang.
Beam loading compensation 300Hz positron generation (Hardware Upgrade ??? Due to present Budget problem) LCWS2013 at Tokyo Uni., Nov KEK, Junji.
Conventional Source for ILC (300Hz Linac scheme and the cost) Junji Urakawa, KEK LCWS2012 Contents : 0. Short review of 300Hz conventional positron source.
Design on Target and Moderator of X- band Compact Electron Linac Neutron Source for Short Pulsed Neutrons Kazuhiro Tagi.
Gamma Beam Systems a simple introduction. Purpose of the machine Deliver a high performance photon beam: Variable energy Highly polarized High intensity.
LLRF Phase Reference System The LCLS linac is broken down into 4 separate linac sections. The LCLS injector will reside in an off axis tunnel at the end.
EuroNNAc Workshop, CERN, May 2011 External Injection at INFN-LNF ( integrating RF photo-injectors with LWFA ) Luca Serafini - INFN/Milano High Brightness.
Beam Therapy Equipment
2009/3/3US High Gradient Research Collaboration Workshop 1 Design Studies of an X-band Multi- beam Klystron S. Fukuda KEK Accelerator Laboratory, KEK.
7.8GHz Dielectric Loaded High Power Generation And Extraction F. Gao, M. E. Conde, W. Gai, C. Jing, R. Konecny, W. Liu, J. G. Power, T. Wong and Z. Yusof.
The LHC: an Accelerated Overview Jonathan Walsh May 2, 2006.
1 Junji Urakawa (KEK, Japan) at Sapphire day, Under development of Quantum Beam Technology Program(QBTP) supported by MEXT from to
Thomas Jefferson National Accelerator Facility Page 1 23 rd Annual HUGS Program June 2-20, 2008 CEBAF Overview HUGS08 June 3 CEBAF Overview HUGS08 June.
Possible further extensions in the new LEPS beamline in Spring-8 S. Daté Accelerator Division, SPring-8/JASRI LEPS Collab. Meeting Academia Sinica, Jan.
Summary of issues. RF-Gun cavity – Disk and washer (DAW) : very fast RF ageing, 2 MeV is not enough. – Quasi travelling wave side couple structure : Lower.
Steve LidiaICFA Workshop, Chia LagunaJuly, 2002 Flat Beam Photoinjectors for Ultrafast Synchrotron Radiation Sources Steve Lidia Lawrence Berkeley National.
Compton/Linac based Polarized Positrons Source V. Yakimenko BNL IWLC2010, Geneva, October 18-22, 2010.
FNAL, May 10, Introduction for Beam Diagnostics Laboratory Main Mission: R&D on charged particle beam diagnostics for e + /e - linear colliders.
Compton polarimetry for EIC Jefferson Lab Compton Polarimeters.
Overview of ERL MEIC Cooler Design Studies S.V. Benson, Y. Derbenev, D.R. Douglas, F. Hannon, F. Marhauser, R. A Rimmer, C.D. Tennant, H. Zhang, H. Wang,
Introduction to Synchrotron Radiation
1 BROOKHAVEN SCIENCE ASSOCIATES NSLS II: Accelerator System Overview NSLS II Advisory Committees October 18/19, 2006 Satoshi Ozaki.
ELECTRON MOVING AT CONSTANT VELOCITY
Compact X-ray & Emittance Measurement by Laser Compton Scattering Zhi Zhao Jan. 31, 2014.
–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.
Y. Roblin, D. Douglas, F. Hannon, A. Hofler, G. Krafft, C. Tennant EXPERIMENTAL STUDIES OF OPTICS SCHEMES AT CEBAF FOR SUPPRESSION OF COHERENT SYNCHROTRON.
STF phase 2 plan H. Hayano, STF phase 2 Accelerator Layout cavities: 2 capture cavities with short ILC-cross-section cryomodule + 26 cavities.
Y. R. Roblin Hall A beamline and accelerator status.
LUCX FACILITY INTRODUCTION : PRESENT STATUS AND FUTURE PLANS A. Aryshev On behalf of QB group and THz collaboration Mini-workshop for advanced THz and.
Commissioning and Utilisation of ERLP David Holder ASTeC, Daresbury Laboratory.
MeRHIC Internal Cost Review October, Dmitry Kayran for injector group MeRHIC Internal Cost Review October 7-8, 2009 MeRHIC: Injection System Gun.
1 CTF3 CLEX day July 2006 CLEX day 2006 Introduction G.Geschonke CERN.
Laser-Undulator Compact X-ray source (LUCX) POSIPOL2006 Workshop at CERN 1/23 Experimental Plan of X-ray Generation using Optical Resonator using Optical.
2 February 8th - 10th, 2016 TWIICE 2 Workshop Instability studies in the CLIC Damping Rings including radiation damping A.Passarelli, H.Bartosik, O.Boine-Fankenheim,
Bremsstrahlung Example of conservation of energy Radiative energy loss by fast electron when slowed near nucleus Results in spectrum of energies from many.
1 RTML Emittance Measurement Station Yuri Kubyshin (1), Robert Apsimon (2), Hector García (1,2) (1) Technical University of Catalonia (UPC) (2) CERN CLIC.
Conventional source developments (300Hz Linac scheme and the cost, Part-II) Junji Urakawa, KEK PosiPol-2012 at DESY Zeuthen Contents : 0. Short review.
1 Junji Urakawa (KEK, Japan) at PosiPol2012, Under development of Quantum Beam Technology Program(QBTP) supported by MEXT from to
Sergey Antipov, J. Qiu, C. Jing, A. Kanareykin Euclid Techlabs LLC
THE ANDRZEJ SOŁTAN INSTITUTE FOR NUCLEAR STUDIES INSTYTUT PROBLEMÓW JADROWYCH im. Andrzeja Sołtana
–11.03 Hawaii Multi bunch acceleration on LUCX system Ⅰ. LUCX project Ⅱ. Simulation results for Compton scattering Ⅲ. Calculation on beam loading.
Copyright 2007, Toshiba Corporation. Prospects of X-band Klystron Based on Experience of High Power Klystron Development in TETD 31 st /Jan./2013 Toshiba.
Overview Turkish Projects TAC / TARLA Avni Aksoy Ankara University Institute of Accelerator Technologies.
Development of High Brightness Electron Photoinjectors at ASTeC B.L. Militsyn Accelerator Science and Technology Centre Science & Technology Facility Council,
ESLS Workshop Nov 2015 MAX IV 3 GeV Ring Commissioning Pedro F. Tavares & Åke Andersson, on behalf of the whole MAX IV team.
Sara Thorin, MAX IV Laboratory
Plans of XFELO in Future ERL Facilities
Energy calibration issues for FCC-ee I. Koop, BINP, Novosibirsk
Injector Topics for Discussion
Compact linear accelerator FLUTE: status update
Cooler e-source Magnetized Beam LDRD Progress Report
High Charge Low Emittance RF Gun for SuperKEKB
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
Cooler e-source Magnetized Beam LDRD Progress Report
Presentation transcript:

BEAM ACCELERATION EXPERIMENT IN X-BAND GHZ LINAC FOR COMPTON SCATTERING X-RAY GENERATION Hirotoshi Masuda The University of Tokyo

outline Background X-ray source of X-band Linac at UT Beam line and RF Recently update  RFgun  Alpha magnet Compton scattering Conclusion and next step

background X-rays of keV are great use in medical science, biology, and material science Most synchrotron radiation sources are too large to be widely used for monochromatic X-rays. One solution to realize a remarkable compactness is laser-electron collision 50m

X-ray source of X-band Linac at UT

RF waveguide and beamline

RF system

RFgun update problem

RFgun update Resonant frequency Shunt inpedance 67MΩ/m Q-value 9232

Magnetic field evaluation of alpha-magnet Figure3 magnetic field simulation of alpha magnet

Beam parameter

Compton scattering

installed the slit (2mm,3mm) in the achromatic arc for reducing the background X-ray noise

Beam vibration

Output RF error effects electron beam vibration

conclution and next plan The thermionic cathode RF gun was upgraded and succeeded in stable operation in high power test. we could transport 38.5mA beam to beam dump. We alomost established the whole system of the the compact X-ray source and are woring on collision test between electron beam and laser for X-ray generation. We change alpha-magnet to achromatic arc for compressing electron beam from RFgun.

conclution and next plan The thermionic cathode RF gun was upgraded and succeeded in stable operation in high power test. we could transport 38.5mA beam to beam dump. We alomost established the whole system of the the compact X-ray source and are woring on collision test between electron beam and laser for X-ray generation. We change alpha-magnet to achromatic arc for compressing electron beam from RFgun.

Phase adjustmet of 3 dB hybrid