The HIGS2 Concept A Next Generation Compton Gamma-ray Source
|
|
- Dominic Nelson
- 5 years ago
- Views:
Transcription
1 The HIGS2 Concept A Next Generation Compton Gamma-ray Source Y. K. Wu FEL Laboratory, TUNL and Department of Physics, Duke University June 3, 2013 Acknowledgment: M. Busch, M. Emanian, J. Faircloth, G. Swift, P. Wang, P. Wallace; H. Hao, J. Li, S. Mikhailov, V. Popov, W. Z. Wu (DFELL, TUNL) Ph.D. Students: J. Yan, W. Zhou (Duke) Collaborators: Jun Ye, François Labaye (JILA) Work supported by U.S. Grant and Contract: DOE DE-FG02-01ER41175 and AFOSR MFELFA
2 Outline A Brief Overview of High Intensity Gamma-ray Source (HIGS) Worldwide Effort in Developing Compton Gamma-ray Sources The HIGS2 Concept Challenges and Critical Issues in Developing the HIGS2
3 Overview of High Intensity Gamma-ray Source (HIGS) Facility at TUNL
4 HIGS Accelerators High Intensity Gamma-ray Source (HIGS) Accelerators Accelerator Facility 160 MeV Linac pre-injector 160 MeV 1.15 GeV Booster injector 250 MeV 1.15 GeV Storage ring FELs: OK-4 (linear) and OK-5 (circular) Typical User Operation Modes FEL: single-bunch, up to 95 ma HIGS: two-bunch, ma
5 Operation Principle of HIGS HIGS Research Two electron bunches + two FEL pulses New Target Room? Target rooms 52.8 m Compton Gamma-ray Source A Photon and Electron Collider
6 Compton Scattering Photon Energy Relativistic ecircular Polarization max Head-on Collision: E ℏ 4 ℏ C. Sun and Y. K. Wu, Phys. Rev. ST Accel. Beams 14, (2011)
7 Compton Scattering Photon Energy Relativistic ecircular Linear Polarization Polarization max Head-on Collision: E ℏ 4 ℏ C. Sun and Y. K. Wu, Phys. Rev. ST Accel. Beams 14, (2011)
8 HIGS Capabilities: 3.5 ka OK-5 Gamma Energy Tuning Range with OK-5 FEL (3.5 ka) Gamma-ray energy range MeV (FEL: 1060 to 190 nm)
9 HIGS User Flux Capabilities with OK-5 FEL Highest Total Flux (2011): >2x 1010 γ 9 11 MeV HIGS World's Most Intense Compton γ-ray Source New Mirrors in 2010
10 3e. Gamma-ray Beam Pointing Stability Stability of Electron/Photon Collision Angle Pointing stabiliy: 2.5 µrad (peak-to-peak, 36 hr)
11 3-year HIGS Operation Summary HIGS Operation Summary (Aug Jul. 2011) Accelerator Operation Reliability: ~96% (Aug Jul. 2011)
12 3d. Gamma-ray Beam Imaging Gamma-beam Imager Part of Ph.D. thesis work of Changchun Sun
13 Worldwide Effort In Developing Compton Gamma-ray Sources
14 Compton Gamma-ray Facilities and Projects Around the World Past, Present, and Future Past Facilities: LADON, LEGS, GRAAL Operational Facilities and Development Projects: HIGS, LEPS, @SAGA ELI-NP MAX-IV Lab Canadian LS GRAAL MEGa-ray LEGS HIGS ELI-NP LADON ROKK NewSUBARU SAGA ETL-LCP LEPS UVSOR SLEGS Y. K. Wu, Duke University (2012)
15 New Compton Gamma-ray Sources ELI-NP, Extreme Light Infrastructure, Europe Facility/Project: ELI-NP Institution: Extreme Light Infrastructure (up to 4 facilities) Country: Europe Energy (MeV): 1 13 Accelerator: x-band Linac, 600 MeV, 250 pc, 120 Hz, high reprate: 12,000 (100 micro-bunches) Laser: Ring-down cavity (12 khz) 8 13 Total flux: 8x10 ph/pulse, 10 ph/s (an older design) Total flux: 2 orders of magnitude lower (a newer design) Status: Funded Sources: 1. The White Book of ELI Nuclear Physics Bucharest-Magurele, Romania, the ELI-Nuclear Physics working group, 2.
16 The HIGS2 Concept
17 The HIGS2 Concept Next Generation High Intensity Gamma-ray Source (HIGS2) Version 2012 Research Programs Hadronic Parity Violation Nuclear Astrophysics Dark-matter Search Projected Performance ~2 micron FP cavity: 2 12 MeV Total Flux: few gamma/s Pol: Linear, or Circular (rapid switch) Energy resolution (FWHM): < 0.5% A Prospectus Document for NSAC (Aug. 2012) HIGS2: The Next Generation Compton g-ray Source, M. W. Ahmed, A. E. Champagne, C. R. Howell, W. M. Snow, R. P. Springer, Y. Wu
18 2012/05/23
19 The HIGS2 Concept HIGS2 Layout (Version, 2012) am e b e am e b e Mirrors of FB cavity Lcav = m PFB (avg) > 10 kw, 90 MHz, fiber laser Collaborator: Jun Ye, JILA and U. of Colorado at Boulder
20 The HIGS2 Concept Expected Electron Beam Parameters Expected Electron Beam Parameters Parameter/Item Value Accelerator Duke Storage Ring New Magnetic Optics Interaction Point Design Beam Energy (MeV) Beam Current (ma) In development Bunch Pattern 32 Evenly Spaced Bunch Rep-rate (MHz) Bunch Separation (ns) 11.2 Charge/Bunch (nc) Bunch Duration (ps, FW) Accelerator Development Comments In development Phase I Developing new magnetic optics: design and optimization Realizing high current operation: current limit, stability Developing E-beam diagnostics, and characterizing e-beam Phase II Engineering design, followed by fabricating, testing, and preparing hardware components for the HIGS2 Upgrading injector Upgrading beam feedback and diagnostics Phase III: System integration and commissioning
21 The HIGS2 Concept Projected Laser Beam Parameters Projected Laser Beam Parameters Parameter/Item Value Comments Drive Laser System Fiber Laser What type of fiber laser? Wavelength (nm) TBD Input for HIGS2 Workshop Average Power (W) Pulse Rep-rate (MHz) Pulse Duration (ps, FW) 5 20 Fabry-Perot Cavity 2-mirror resonator Cavity Length (m) In-cavity Power (kw) Goal: λ/λ < 10-3 Laser and FP Cavity Development Phase I Prototype laser Prototype FP cavity Phase II Developing production laser system Developing production FP cavity Developing optical diagnostics for polarization controls and monitoring Phase III: System integration and commissioning
22 The HIGS2 Concept Time Structures of Electron and Laser Beams
23 HIGS2 Projected Performance Summary A Prospectus Document for NSAC (Aug. 2012) HIGS2: The Next Generation Compton g-ray Source, M. W. Ahmed, A. E. Champagne, C. R. Howell, W. M. Snow, R. P. Springer, Y. Wu
24 Challenges and Critical Issues for Developing the HIGS2 Challenges with Developing Electron Source and Accelerators New 32-bunch Operation Mode for Duke Storage Ring (Prelim Results) New, Optimized Magnetic Optics (Prelim Results) Stabilizing Electron Beam Operation Challenges with the Photon Source Drive Laser FP Cavity
25 Development of Electron Source and Accelerators New 32-bunch Operation Mode for Duke Storage Ring: ma (in progress) New, Optimized Magnetic Optics for Storage Ring: Physics Design (in progress) Stability of Electron Beam Operation Orbit stability (fast motion, long-term) Transverse beam size stability Longitudinal beam size stability Beam parameters for various operation parameters Impact of top-off injection
26 HIGS2 Development New Mode of Operation: 32-bunch Beam (Prelim Results) Test Results with 32-Bunch Beam Operation with Longitudinal Feedback ( 2013) E-beam Energy (MeV) Max Curr (ma) Stability Limitation Comments Long. Stable Inj. Rate Slow damping Long. Stable Inj. Rate Slow damping Long. Stable Inj. Rate Issues: Max current limited by injection Low injection rate (4 6 ma/min, initially) Further stability improvement needed (transverse)
27 HIGS2 Development Accelerator Development Projects Accelerator Development Projects High Current 32-bunch operation (continuing) Developing New Storage Ring Magnetic Optics (continuing) Related to Injector and Injection Scheme Increasing charge injection rate (x5) Improving stability and reliability of linac injector (new klystrons/modulators) Reducing negative impact on the stored beam during injection Related Storage Ring Fast orbit feedback system Transverse feedback system to combat coupled bunch instabilities Fast orbit stability during top-off operation Characterizing beam performance for various operation parameters Related Laser System IP optimization Synchronization with the Drive Laser Infrastructure Modification
28 HIGS2 Development Photon Beam System Development of Drive Laser and Fabry-Perot Cavity Drive Laser What wavelength? What type of fiber laser? Narrow spectrum of the laser beam Stability of the laser beam power, fast and slow time scales Polarization controls and fast switches of helicity Fabre-Perot Cavity Design of the FB cavity Matching with the electron beam Related feedback and stabilization systems, and optical diagnostics Mirror lifetime and radiation damage Stability of the photon beam in FP cavity, fast and slow time scales
29 HIGS2 Development Photon Beam System State-of-the-art Fiber Lasers JILA (Joint institute of U. of Colorado and NIST) Erbium fiber laser (1.5 microns) Ytterbium fiber laser (1 micron) High Power FB Cavity with frequency comb technology, 10 kw (stable beam) Spectral width: how to achieve Higher power: stability? 10-3 or What Wavelength? Thulium fiber laser (2 microns) Challenges Freq. Comb? better? Polarization controls and switch Power stability
30 The HIGS2 Project TEAM (Unfunded Effort as of June 2013) DFELL, TUNL, Led by Ying K. Wu Engineers and Technical Staff: Matthew Busch, Mark Emamian, Joe Faircloth, Gary Swift, Pat Wallac; Marty Johnson, Maurice Pentico, Vern Rathbone Scientists: Hao Hao, Jingyi Li, Stepan Mikhailov, Victor Popov, Wenzhong Wu, Ying K. Wu Graduate Students: Jun Yan, Weizheng Zhou New Hires: Additional scientific, engineering and technical staff JILA (U. of Colorado and NIST), Led by Jun Ye Scientists, graduate students, and other staff Focus on the drive laser system and Fabry-Perot cavity system Other Collaborators (TBD) With Nuclear Physicists, Laser Physicists, and Accelerator Physicists
31 HIGS2 Major Areas of Cost for HIGS2 Source Development Main Areas Photon Source Electron Beam Source HIGS2 Flux Performance and Reliability Subsystems IR Laser Prototype and Production Laser System Fabry-Perot Cavity Prototype and Production Systems and Related Optical Systems Collision Beamline and Magnetic/Vacuum System Accelerator Diagnostics and Controls Accelerator Infrastructure Injector Upgrade (Linac, and other subsystems) Beam Feedback and Advanced Manipulation/Controls Comments JILA JILA and DFELL DFELL DFELL DFELL DFELL DFELL with Collaborators TBD
32 HIGS2 Facility and Scientific Program HIGS2 Facility ===> <=== Scientific Program
33 HIGS2 Development Gamma-ray Parameters From Nuclear Physicists For Each Experiment or a Set of Experiments Name of Experiment Gamma-Beam Parameters Gamma-ray Energy Range (MeV) Energy Resolution (FWHM) (%) Gamma-ray Flux on Target (g/s) Degree of Polarization Linear Circular Helicity Switch (Yes/No) Rate (Hz) Stability of Flux Stability of Polarization More... Min. Requirement Preferred Comments
34 Compton Gamma-beam Radiograph 2
35 Thank You!
HIGS - A High-intensity, Mono-energetic, and Tunable Source of Polarized Gamma-rays
HIGS - A High-intensity, Mono-energetic, and Tunable Source of Polarized Gamma-rays Duke FEL Laboratory Triangle Universities Nuclear Laboratory, Duke University May 25, 2010 Acknowledgment: M. Busch,
More informationHigh Energy Photons at HI S
High Energy Photons at HIS Rob Pywell High Intensity Gamma Source Duke University Thanks to Dr. Ying Wu, Duke University, for supplying some of the information in this talk. Precision Photo-Reaction Measurements
More informationStorage Ring Compton Gamma Sources
Storage Ring Compton Gamma Sources DFELL, Triangle Universities Nuclear Laboratory Department of Physics, Duke University August 30, 2010 Acknowledgment: M. Busch, M. Emanian, J. Faircloth, S. Hartman,
More informationStorage Ring Compton Light Sources
Storage Ring Compton Light Sources Acknowledgment: M. Busch, M. Emanian, J. Faircloth, S. Hartman, J. Li, S. Mikhailov, V. Popov, G. Swift, P. Wang, P. Wallace (DFELL) M. Ahmed, T. Clegg, H. Gao, C. Howell,
More informationCharacterizations and Diagnostics of Compton Light Source
Characterizations and Diagnostics of Compton Light Source Advance Light Source (ALS) (LBNL) Ying K. Wu Duke Free Electron Laser Laboratory (DFELL) Acknowledgments: DFELL: B. Jia, G. Swift, H. Hao, J. Li,
More informationERL FACILITY AT CERN FOR APPLICATIONS
ERL FACILITY AT CERN FOR APPLICATIONS Erk Jensen (CERN) Big thanks to contributors: A. Bogacz (JLAB), O. Brüning, R. Calaga, V. Chetvertkova, E. Cormier (CELIA), R. Jones, M. Klein, A. Valloni, D. Pellegrini,
More informationCompton Scattering Effect and Physics of Compton Photon Beams. Compton Photon Sources around the World, Present and Future
!!! #! ! # Compton Scattering Effect and Physics of Compton Photon Beams Compton Photon Sources around the World, Present and Future Compton X-ray Sources: Facilities, Projects and Experiments Compton
More informationFew-Body HIgS
Few-Body Physics @ HIgS Werner Tornow Duke University & Triangle Universities Nuclear Laboratory Outline High-Intensity Gamma-ray Source (HIgS) A=3 g- 3 He three-body breakup with double polarization Outlook
More informationAn Overview of the Activities of ICS Sources in China
An Overview of the Activities of ICS Sources in China Chuanxiang Tang *, Yingchao Du, Wenhui Huang * tang.xuh@tsinghua.edu.cn Department of Engineering physics, Tsinghua University, Beijing 100084, China
More information2. THE HIGS FACILITY 2.1 The Free-Electron Laser Source
2. THE HIGS FACILITY 2.1 The Free-Electron Laser Source In recent years the development of intense, short-wavelength storage ring FELs has created an opportunity for the development of intense high-energy
More informationPaul Huffman! Investigating Hadronic Parity Violation Using the γd np Reaction at the Proposed HIGS2 facility at TUNL
Investigating Hadronic Parity Violation Using the γd np Reaction at the Proposed HIGS2 facility at TUNL Paul Huffman! North Carolina State University Triangle Universities Nuclear Laboratory!!!! M.W. Ahmed!
More informationSLAC Summer School on Electron and Photon Beams. Tor Raubenheimer Lecture #2: Inverse Compton and FEL s
SLAC Summer School on Electron and Photon Beams Tor Raubenheimer Lecture #: Inverse Compton and FEL s Outline Synchrotron radiation Bending magnets Wigglers and undulators Inverse Compton scattering Free
More informationExtreme Light Infrastructure - Nuclear Physics ELI - NP
Extreme Light Infrastructure - Nuclear Physics ELI - NP Nicolae-Victor Zamfir National Institute for Physics and Nuclear Engineering (IFIN-HH) Bucharest-Magurele, Romania www.eli-np.ro Bucharest-Magurele
More informationHow to Prepare an Experiment using the Gamma Beam System at ELI-NP
EUROPEAN UNION GOVERNMENT OF ROMANIA Structural Instruments 2007-2013 Project co-financed by the European Regional Development Fund How to Prepare an Experiment using the Gamma Beam System at ELI-NP Catalin
More informationFrench-Ukrainian workshop Kevin Dupraz 1 ELI-NP-GBS. Extreme Light Infrastructure Nuclear Physics Gamma Beam Source
1 ELI-NP-GBS Extreme Light Infrastructure Nuclear Physics Gamma Beam Source The 3 ELI s pillars 2 ELI-Beamlines In Czech Republic: Ultra-short and intense beams for interdisciplinary applications. ELI-NP
More informationTuning Techniques And Operator Diagnostics for FACET at SLAC National Accelerator Laboratory. Chris Melton SLAC Accelerator Operations
Tuning Techniques And Operator Diagnostics for FACET at SLAC National Accelerator Laboratory Chris Melton SLAC Accelerator Operations FACET Tuning And Diagnostics What is FACET? FACET Performance Challenges
More informationThomX Machine Advisory Committee. (LAL Orsay, March ) Ring Beam Dynamics
ThomX Machine Advisory Committee (LAL Orsay, March 20-21 2017) Ring Beam Dynamics A. Loulergue, M. Biagini, C. Bruni, I. Chaikovska I. Debrot, N. Delerue, A. Gamelin, H. Guler, J. Zang Programme Investissements
More informationFLASH/DESY, Hamburg. Jörg Rossbach University of Hamburg & DESY, Germany - For the FLASH Team -
First Lasing below 7nm Wavelength at FLASH/DESY, Hamburg Jörg Rossbach University of Hamburg & DESY, Germany - For the FLASH Team - email: joerg.rossbach@desy.de FLASH: The first FEL user facility for
More informationWG2 on ERL light sources CHESS & LEPP
Charge: WG2 on ERL light sources Address and try to answer a list of critical questions for ERL light sources. Session leaders can approach each question by means of (a) (Very) short presentations (b)
More informationPhotoneutron reactions studies at ELI-NP using a direct neutron multiplicity sorting method Dan Filipescu
EUROPEAN UNION GOVERNMENT OF ROMANIA Sectoral Operational Programme Increase of Economic Competitiveness Investments for Your Future Structural Instruments 2007-2013 Extreme Light Infrastructure Nuclear
More informationLow Energy RHIC electron Cooling (LEReC)
Low Energy RHIC electron Cooling (LEReC) LEReC overview: project goal and cooling approach Alexei Fedotov MEIC Collaboration Meeting 30 31 LEReC Project Mission/Purpose The purpose of the LEReC is to provide
More informationShort Introduction to CLIC and CTF3, Technologies for Future Linear Colliders
Short Introduction to CLIC and CTF3, Technologies for Future Linear Colliders Explanation of the Basic Principles and Goals Visit to the CTF3 Installation Roger Ruber Collider History p p hadron collider
More informationX-ray Free-electron Lasers
X-ray Free-electron Lasers Ultra-fast Dynamic Imaging of Matter II Ischia, Italy, 4/30-5/3/ 2009 Claudio Pellegrini UCLA Department of Physics and Astronomy Outline 1. Present status of X-ray free-electron
More informationIII. CesrTA Configuration and Optics for Ultra-Low Emittance David Rice Cornell Laboratory for Accelerator-Based Sciences and Education
III. CesrTA Configuration and Optics for Ultra-Low Emittance David Rice Cornell Laboratory for Accelerator-Based Sciences and Education Introduction Outline CESR Overview CESR Layout Injector Wigglers
More informationFuture Light Sources March 5-9, 2012 Low- alpha mode at SOLEIL 1
Introduction: bunch length measurements Reminder of optics Non- linear dynamics Low- alpha operation On the user side: THz and X- ray short bunch science CSR measurement and modeling Future Light Sources
More informationELIC: A High Luminosity And Efficient Spin Manipulation Electron-Light Ion Collider Based At CEBAF
ELIC: A High Luminosity And Efficient Spin Manipulation Electron-Light Ion Collider Based At CEBAF Lia Merminga and Yaroslav Derbenev Center for Advanced Studies of Accelerators, Jefferson Laboratory,
More informationELIC Design. Center for Advanced Studies of Accelerators. Jefferson Lab. Second Electron-Ion Collider Workshop Jefferson Lab March 15-17, 2004
ELIC Design Ya. Derbenev, K. Beard, S. Chattopadhyay, J. Delayen, J. Grames, A. Hutton, G. Krafft, R. Li, L. Merminga, M. Poelker, E. Pozdeyev, B. Yunn, Y. Zhang Center for Advanced Studies of Accelerators
More informationExperimental Optimization of Electron Beams for Generating THz CTR and CDR with PITZ
Experimental Optimization of Electron Beams for Generating THz CTR and CDR with PITZ Introduction Outline Optimization of Electron Beams Calculations of CTR/CDR Pulse Energy Summary & Outlook Prach Boonpornprasert
More informationInstabilities in the Duke Storage Ring
Feedback Systems for Control of Coupled-bunch Instabilities in the Duke Storage Ring by Wenzhong Wu Department of Physics Duke University Date: Approved: Ying K. Wu, Supervisor Stephen Teitsworth Seog
More informationCompact Wideband THz Source
Compact Wideband THz Source G. A. Krafft Center for Advanced Studies of Accelerators Jefferson Lab Newport News, VA 3608 Previously, I have published a paper describing compact THz radiation sources based
More informationThe New Superconducting RF Photoinjector a High-Average Current & High-Brightness Gun
The New Superconducting RF Photoinjector a High-Average Current & High-Brightness Gun Jochen Teichert for the BESSY-DESY-FZD-MBI collaboration and the ELBE crew High-Power Workshop, UCLA, Los Angeles 14
More information4GLS Status. Susan L Smith ASTeC Daresbury Laboratory
4GLS Status Susan L Smith ASTeC Daresbury Laboratory Contents ERLP Introduction Status (Kit on site ) Plan 4GLS (Conceptual Design) Concept Beam transport Injectors SC RF FELs Combining Sources May 2006
More informationWhat is an Energy Recovery Linac and Why is there one in your Future?
What is an Energy Recovery Linac and Why is there one in your Future? Sol M. Gruner CHESS, Physics Dept. Cornell University Ithaca, NY 14853 Outline 1. Who needs another synchrotron source? 2. What is
More informationOverview on Compton Polarimetry
General Issues O spin motion & alignment tolerances O beam-beam effects & upstream vs. Downstream Compton Polarimetry Basics O beam parameters & Compton detection methods O kinematics, cross sections &
More informationHigh Energy Gain Helical Inverse Free Electron Laser Accelerator at Brookhaven National Laboratory
High Energy Gain Helical Inverse Free Electron Laser Accelerator at Brookhaven National Laboratory J. Duris 1, L. Ho 1, R. Li 1, P. Musumeci 1, Y. Sakai 1, E. Threlkeld 1, O. Williams 1, M. Babzien 2,
More informationSimulations of the IR/THz Options at PITZ (High-gain FEL and CTR)
Case Study of IR/THz source for Pump-Probe Experiment at the European XFEL Simulations of the IR/THz Options at PITZ (High-gain FEL and CTR) Introduction Outline Simulations of High-gain FEL (SASE) Simulation
More informationA European Proposal for the Compton Gamma-ray Source of ELI-NP
A European Proposal for the Compton Gamma-ray Source of ELI-NP C. Vaccarezza on behalf of the collaboration 1 Outline The European Collaboration The Source design The electron & laser beam parameters The
More informationVELA/CLARA as Advanced Accelerator Studies Test-bed at Daresbury Lab.
VELA/CLARA as Advanced Accelerator Studies Test-bed at Daresbury Lab. Yuri Saveliev on behalf of VELA and CLARA teams STFC, ASTeC, Cockcroft Institute Daresbury Lab., UK Outline VELA (Versatile Electron
More informationUpdate on and the Issue of Circularly-Polarized On-Axis Harmonics
Update on FERMI@Elettra and the Issue of Circularly-Polarized On-Axis Harmonics W. Fawley for the FERMI Team Slides courtesy of S. Milton & Collaborators The FERMI@Elettra Project FERMI@Elettra is a single-pass
More informationOPTIMIZING RF LINACS AS DRIVERS FOR INVERSE COMPTON SOURCES: THE ELI-NP CASE
OPTIMIZING RF LINACS AS DRIVERS FOR INVERSE COMPTON SOURCES: THE ELI-NP CASE C. Vaccarezza, D. Alesini, M. Bellaveglia, R. Boni, E. Chiadroni, G. Di Pirro, M. Ferrario, A. Gallo, G. Gatti, A. Ghigo, B.
More informationSLS at the Paul Scherrer Institute (PSI), Villigen, Switzerland
SLS at the Paul Scherrer Institute (PSI), Villigen, Switzerland Michael Böge 1 SLS Team at PSI Michael Böge 2 Layout of the SLS Linac, Transferlines Booster Storage Ring (SR) Beamlines and Insertion Devices
More informationPushing the limits of laser synchrotron light sources
Pushing the limits of laser synchrotron light sources Igor Pogorelsky National Synchrotron Light Source 2 Synchrotron light source With λ w ~ several centimeters, attaining XUV region requires electron
More informationUnique features of linac-ring
Unique features of linac-ring erhic Daniel Anderson 1, Ilan Ben-Zvi 1,2,4, Rama Calaga 1,4, Xiangyun Chang 1,4, Manouchehr Farkhondeh 3, Alexei Fedotov 1, Jörg Kewisch 1, Vladimir Litvinenko, 1,4, William
More informationOverview of accelerator science opportunities with FACET ASF
Overview of accelerator science opportunities with FACET ASF Bob Siemann DOE FACET Review, February 19-20, 2008 OUTLINE I. Plasma Wakefield Acceleration II. Plasma Wakefield Based Linear Colliders III.
More information7th IPAC, May 8-13, 2016, Busan, Korea
7th IPAC, May 8-13, 2016, Busan, Korea ER@CEBAF A High-Energy, Multiple-Pass, Energy Recovery Experiment at CEBAF On behalf of the JLab-BNL ER@CEBAF collaboration : I. Ben-Zvi, Y. Hao, P. Korysko, C. Liu,
More informationShort Pulse, Low charge Operation of the LCLS. Josef Frisch for the LCLS Commissioning Team
Short Pulse, Low charge Operation of the LCLS Josef Frisch for the LCLS Commissioning Team 1 Normal LCLS Parameters First Lasing in April 10, 2009 Beam to AMO experiment August 18 2009. Expect first user
More informationWaseda University. Design of High Brightness Laser-Compton Light Source for EUV Lithography Research in Shorter Wavelength Region
Waseda University Research Institute for Science and Engineering Design of High Brightness Laser-Compton Light Source for EUV Lithography Research in Shorter Wavelength Region Research Institute for Science
More informationEmergency information
Emergency information Fire Evacuate. Be aware of building exits. Follow building residents to the assembly area. Do not leave until you are accounted for, and have been instructed to. Earthquake Remain
More informationMaRIE. MaRIE X-Ray Free-Electron Laser Pre-Conceptual Design
Operated by Los Alamos National Security, LLC, for the U.S. Department of Energy MaRIE (Matter-Radiation Interactions in Extremes) MaRIE X-Ray Free-Electron Laser Pre-Conceptual Design B. Carlsten, C.
More informationThe Luminosity Upgrade at RHIC. G. Robert-Demolaize, Brookhaven National Laboratory
The Luminosity Upgrade at RHIC G. Robert-Demolaize, Brookhaven National Laboratory RHIC accelerator complex: IPAC'15 - May 3-8, 2015 - Richmond, VA, USA 2 The Relativistic Heavy Ion Collider (RHIC) aims
More informationDESIGN AND CONSTRUCTION OF LOW ENERGY ELECTRON ACCELERATORS AT SINP MSU
DESIGN AND CONSTRUCTION OF LOW ENERGY ELECTRON ACCELERATORS AT SINP MSU V. Shvedunov Skobeltsyn Institute of Nuclear Physics Lomonosov Moscow State University 26 November 2013 Betatron 1959-1985 Low intensity
More informationOverview of LHC Accelerator
Overview of LHC Accelerator Mike Syphers UT-Austin 1/31/2007 Large Hadron Collider ( LHC ) Outline of Presentation Brief history... Luminosity Magnets Accelerator Layout Major Accelerator Issues U.S. Participation
More informationCEPC Linac Injector. HEP Jan, Cai Meng, Guoxi Pei, Jingru Zhang, Xiaoping Li, Dou Wang, Shilun Pei, Jie Gao, Yunlong Chi
HKUST Jockey Club Institute for Advanced Study CEPC Linac Injector HEP218 22 Jan, 218 Cai Meng, Guoxi Pei, Jingru Zhang, Xiaoping Li, Dou Wang, Shilun Pei, Jie Gao, Yunlong Chi Institute of High Energy
More informationTransverse dynamics Selected topics. Erik Adli, University of Oslo, August 2016, v2.21
Transverse dynamics Selected topics Erik Adli, University of Oslo, August 2016, Erik.Adli@fys.uio.no, v2.21 Dispersion So far, we have studied particles with reference momentum p = p 0. A dipole field
More informationX-band Experience at FEL
X-band Experience at FERMI@Elettra FEL Gerardo D Auria Elettra - Sincrotrone Trieste GdA_TIARA Workshop, Ångström Laboratory, June 17-19, 2013 1 Outline The FERMI@Elettra FEL project Machine layout and
More informationThe Electron-Ion Collider
The Electron-Ion Collider C. Tschalaer 1. Introduction In the past year, the idea of a polarized electron-proton (e-p) or electron-ion (e-a) collider of high luminosity (10 33 cm -2 s -1 or more) and c.m.
More informationOBSERVATION OF TRANSVERSE- LONGITUDINAL COUPLING EFFECT AT UVSOR-II
OBSERVATION OF TRANSVERSE- LONGITUDINAL COUPLING EFFECT AT UVSOR-II The 1st International Particle Accelerator Conference, IPAC 10 Kyoto International Conference Center, May 23-28, 2010 M. Shimada (KEK),
More informationThe Turkish Accelerator Center (TAC) Project. Bora Ketenoğlu. Department of Engineering Physics Ankara University / TURKEY
The Turkish Accelerator Center (TAC) Project Bora Ketenoğlu Department of Engineering Physics Ankara University / TURKEY Contents The emblem & homepage Why do we want to build an accelerator complex? Where
More informationFURTHER UNDERSTANDING THE LCLS INJECTOR EMITTANCE*
Proceedings of FEL014, Basel, Switzerland FURTHER UNDERSTANDING THE LCLS INJECTOR EMITTANCE* F. Zhou, K. Bane, Y. Ding, Z. Huang, and H. Loos, SLAC, Menlo Park, CA 9405, USA Abstract Coherent optical transition
More informationConceptual design of an accumulator ring for the Diamond II upgrade
Journal of Physics: Conference Series PAPER OPEN ACCESS Conceptual design of an accumulator ring for the Diamond II upgrade To cite this article: I P S Martin and R Bartolini 218 J. Phys.: Conf. Ser. 167
More informationLow slice emittance preservation during bunch compression
Low slice emittance preservation during bunch compression S. Bettoni M. Aiba, B. Beutner, M. Pedrozzi, E. Prat, S. Reiche, T. Schietinger Outline. Introduction. Experimental studies a. Measurement procedure
More informationExperimental Path to Echo-75 at NLCTA
Experimental Path to Echo-75 at NLCTA Erik Hemsing on behalf of the ECHO group at SLAC NLCTA ICFA Workshop on Future Light Sources March 5-9, 2012 Thomas Jefferson National Accelerator Facility Motivation
More informationGreenfield FELs. John Galayda, SLAC Kwang-Je Kim, ANL (Presenter) James Murphy, BNL
Greenfield FELs John Galayda, SLAC Kwang-Je Kim, ANL (Presenter) James Murphy, BNL BESAC Subcommittee on BES 20-year Facility Road Map February 22-24, 2003 What is a Greenfield FEL? High-gain FELs are
More informationLinac Driven Free Electron Lasers (III)
Linac Driven Free Electron Lasers (III) Massimo.Ferrario@lnf.infn.it SASE FEL Electron Beam Requirements: High Brightness B n ( ) 1+ K 2 2 " MIN r #$ % &B! B n 2 n K 2 minimum radiation wavelength energy
More informationOverview of Energy Recovery Linacs
Overview of Energy Recovery Linacs Ivan Bazarov Cornell High Energy Synchrotron Source Talk Outline: Historical Perspective Parameter Space Operational ERLs & Funded Projects Challenges ERL Concept: conventional
More informationThe MID instrument.
The MID instrument International Workshop on the Materials Imaging and Dynamics Instrument at the European XFEL Grenoble, Oct 28/29, 2009 Thomas Tschentscher thomas.tschentscher@xfel.eu Outline 2 History
More informationElectron Beam Polarimetry: Status and Prospects. DIS 2005, Madison, April 2005 E. Chudakov (JLab)
Electron Beam Polarimetry: Status and Prospects DIS 2005, Madison, April 2005 E. Chudakov (JLab) Motivation: what accuracy is required for various experiments Methods in use: Optical methods Mott scattering
More informationBeam Diagnostics and Instrumentation JUAS, Archamps Peter Forck Gesellschaft für Schwerionenforschnung (GSI)
Beam Diagnostics and Instrumentation JUAS, Archamps Peter Forck Gesellschaft für Schwerionenforschnung (GSI), 2003, A dedicated proton accelerator for 1p-physics at the future GSI Demands facilities for
More informationVertical Polarization Option for LCLS-II. Abstract
SLAC National Accelerator Lab LCLS-II TN-5-8 March 5 Vertical Polarization Option for LCLS-II G. Marcus, T. Raubenheimer SLAC, Menlo Park, CA 95 G. Penn LBNL, Berkeley, CA 97 Abstract Vertically polarized
More informationLCLS Commissioning Status
LCLS Commissioning Status Paul Emma (for the LCLS Commissioning Team) June 20, 2008 LCLS ANL LLNL UCLA FEL Principles Electrons slip behind EM wave by λ 1 per undulator period ( (λ u ) x K/γ e λ u v x
More informationStatus of Proof-of-Principle Experiment of Coherent Electron Cooling at BNL
Status of Proof-of-Principle Experiment of Coherent Electron Cooling at BNL Outline 2 Why we doing it? What is Coherent electron Cooling System description Subsystem performance Plan for Run 18 e-n Luminosity
More informationElectron acceleration regime envisioned at ELI-Beamlines in the Czech Republic and test experiments.
Electron acceleration regime envisioned at ELI-Beamlines in the Czech Republic and test experiments. Tadzio Levato tadzio.levato@eli-beams.eu SIF 23-09-2014 Content Introduction to the project and the
More informationLepton beam polarisation for the HERA experiments ZEUS and H1
Lepton beam polarisation for the HERA experiments ZEUS and H1 Polarisation at collider machines The HERA storage ring The HERA polarimeters The collider experiments ZEUS and H1 The HERA II upgrade Data
More informationLength of beam system = 910m. S. Reiche X var = ~50m ~ 650m / Y. Kim FEL-KY ~150m. ~60m. LaserHutch2 (access during operation)
Laser Laser HHG Diagnostic ATHOS PORTHOS ARAMIS THz-Pump P A U L S C H E R R E R I N S T I T U T Length of beam system = 910m &'!( Test & Commissioning steps (A,B,C) A11 Conv. Gun & Injector A12 LINAC
More informationDiagnostics Needs for Energy Recovery Linacs
Diagnostics Needs for Energy Recovery Linacs Georg H. Hoffstaetter Cornell Laboratory for Accelerator-based Sciences and Education & Physics Department Cornell University, Ithaca New York 14853-2501 gh77@cornell.edu
More informationDiagnostic Systems for Characterizing Electron Sources at the Photo Injector Test Facility at DESY, Zeuthen site
1 Diagnostic Systems for Characterizing Electron Sources at the Photo Injector Test Facility at DESY, Zeuthen site Sakhorn Rimjaem (on behalf of the PITZ team) Motivation Photo Injector Test Facility at
More informationUndulator radiation from electrons randomly distributed in a bunch
Undulator radiation from electrons randomly distributed in a bunch Normally z el >> N u 1 Chaotic light Spectral property is the same as that of a single electron /=1/N u Temporal phase space area z ~(/
More information4 FEL Physics. Technical Synopsis
4 FEL Physics Technical Synopsis This chapter presents an introduction to the Free Electron Laser (FEL) physics and the general requirements on the electron beam parameters in order to support FEL lasing
More informationDiagnostics at the MAX IV 3 GeV storage ring during commissioning. PPT-mall 2. Åke Andersson On behalf of the MAX IV team
Diagnostics at the MAX IV 3 GeV storage ring during commissioning PPT-mall 2 Åke Andersson On behalf of the MAX IV team IBIC Med 2016, linje Barcelona Outline MAX IV facility overview Linac injector mode
More informationAccelerator R&D Opportunities: Sources and Linac. Developing expertise. D. Rubin, Cornell University
Accelerator R&D Opportunities: Sources and Linac D. Rubin, Cornell University Electron and positron sources Requirements Status of R&D Linac Modeling of beam dynamics Development of diagnostic and tuning
More informationERL upgrade of an existing X-ray facility: CHESS at CESR
ERL-5-8 ERL upgrade of an existing X-ray facility: CHESS at CESR G.H. Hoffstaetter Abstract Cornell University has proposed an Energy-Recovery Linac (ERL) based synchrotron-light facility which uses 5GeV,
More informationNew Electron Source for Energy Recovery Linacs
New Electron Source for Energy Recovery Linacs Ivan Bazarov 20m Cornell s photoinjector: world s brightest electron source 1 Outline Uses of high brightness electron beams Physics of brightness High brightness
More informationPotential use of erhic s ERL for FELs and light sources ERL: Main-stream GeV e - Up-gradable to 20 + GeV e -
Potential use of erhic s ERL for FELs and light sources Place for doubling energy linac ERL: Main-stream - 5-10 GeV e - Up-gradable to 20 + GeV e - RHIC Electron cooling Vladimir N. Litvinenko and Ilan
More informationDevelopment of Soft X-rayX using Laser Compton Scattering
26 th Advanced ICFA Beam Dynamics Workshop on Nanometre-Size Colliding Beams September 2-6, 2002 at Lausanne Development of Soft X-rayX Source using Laser Compton Scattering R. Kuroda*, S. Kashiwagi*,
More informatione + e Factories M. Sullivan Presented at the Particle Accelerator Conference June 25-29, 2007 in Albuquerque, New Mexico e+e- Factories
e + e Factories M. Sullivan Presented at the Particle Accelerator Conference June 25-29, 2007 in Albuquerque, New Mexico 1 Outline Factory Running KEKB PEP-II DAFNE CESR-c BEPCII 2 Summary Factory Running
More informationIon Polarization in RHIC/eRHIC
Ion Polarization in RHIC/eRHIC M. Bai, W. MacKay, V. Ptitsyn, T. Roser, A. Zelenski Polarized Ion Sources (reporting for Anatoly Zelenski) Polarized proton beams in RHIC/eRHIC Polarized He3 for erhic (reporting
More informationRun2 Problem List (Bold-faced items are those the BP Department can work on) October 4, 2002
Run2 Problem List (Bold-faced items are those the BP Department can work on) October 4, 2002 Linac Booster o 4.5-4.8e12 ppp at 0.5 Hz o Space charge (30% loss in the first 5 ms) o Main magnet field quality
More informationOn the future plan of KEK for ILC(International Linear Collider) Junji Urakawa(KEK) Contents
On the future plan of KEK for ILC(International Linear Collider) Junji Urakawa(KEK) 2004.10.24 Contents 0. Outline until now. Review of SC-LC(TESLA) and R&D items. R&D Items at ATF. R&D plans for Superconducting
More informationBIG A Gamma Ray Source at FACET-II
BIG A Gamma Ray Source at FACET-II Laser-Driven Radiation Sources for Nuclear Applications, GWU, December 13-15, 2015 Carsten Hast SLAC Outline FACET-II in a Nutshell BIG: Beams of Intense Gamma-Rays at
More informationEO single-shot temporal measurements of electron bunches
EO single-shot temporal measurements of electron bunches and of terahertz CSR and FEL pulses. Steven Jamison, Giel Berden, Allan MacLeod Allan Gillespie, Dino Jaroszynski, Britta Redlich, Lex van der Meer
More informationFemto second X ray Pulse Generation by Electron Beam Slicing. F. Willeke, L.H. Yu, NSLSII, BNL, Upton, NY 11973, USA
Femto second X ray Pulse Generation by Electron Beam Slicing F. Willeke, L.H. Yu, NSLSII, BNL, Upton, NY 11973, USA r 2 r 1 y d x z v Basic Idea: When short electron bunch from linac (5MeV, 50pC,100fs)
More informationOn-axis injection into small dynamic aperture
On-axis injection into small dynamic aperture L. Emery Accelerator Systems Division Argonne National Laboratory Future Light Source Workshop 2010 Tuesday March 2nd, 2010 On-Axis (Swap-Out) injection for
More informationAccelerator Design and Construction Progress of TPS Project
Accelerator Design and Construction Progress of TPS Project Taiwan Light Source (TLS), a 120-m storage ring originally designed for 1.3 GeV, was commissioned and opened to users in 1993. The energy of
More informationExperimental Measurements of the ORION Photoinjector Drive Laser Oscillator Subsystem
Experimental Measurements of the ORION Photoinjector Drive Laser Oscillator Subsystem D.T Palmer and R. Akre Laser Issues for Electron RF Photoinjectors October 23-25, 2002 Stanford Linear Accelerator
More informationTECHNICAL ADVISORY COMMITTEE (TAC) REPORT 3. May 19-20, 2000
July 17, 2000 TECHNICAL ADVISORY COMMITTEE (TAC) REPORT 3 TAC Committee Members: Bill Colson (Chair, NPS) Dave Attwood (LBL) Jerry Hastings (BNL) Pat O Shea (UMD) Ross Schlueter (LBL) Ron Ruth (SLAC) The
More informationSuper-c-tau factory in Novosibirsk (WP7)
Super-c-tau factory in Novosibirsk (WP7) E. Levichev Budker Institute of Nuclear Physics Novosibirsk, RUSSIA CREMLIN kick-off meeting, 6-7 October 2015 NRC Kurchatov Institute Budker Institute Founded
More informationLayout of the HHG seeding experiment at FLASH
Layout of the HHG seeding experiment at FLASH V. Miltchev on behalf of the sflash team: A. Azima, J. Bödewadt, H. Delsim-Hashemi, M. Drescher, S. Düsterer, J. Feldhaus, R. Ischebeck, S. Khan, T. Laarmann
More informationCONCEPTUAL STUDY OF A SELF-SEEDING SCHEME AT FLASH2
CONCEPTUAL STUDY OF A SELF-SEEDING SCHEME AT FLASH2 T. Plath, L. L. Lazzarino, Universität Hamburg, Hamburg, Germany K. E. Hacker, T.U. Dortmund, Dortmund, Germany Abstract We present a conceptual study
More informationIntroduction to polarimetry at HERA
Introduction to polarimetry at HERA Alex Tapper Electron polarisation at HERA The LPOL The TPOL The LPOL cavity Electron polarisation in storage rings Electron beam deflected around a ring with B field
More informationPULSE-TO-PULSE TRANSVERSE BEAM EMITTANCE CONTROLLING FOR MLF AND MR IN THE 3-GeV RCS OF J-PARC
THO3AB3 Proceedings of HB, East-Lansing, MI, USA PULSE-TO-PULSE TRANSVERSE BEAM EMITTANCE CONTROLLING FOR MLF AND MR IN THE 3-GeV RCS OF J-PARC P.K. Saha, H. Harada, H. Hotchi and T. Takayanagi J-PARC
More information