Compton Scattering Effect and Physics of Compton Photon Beams. Compton Photon Sources around the World, Present and Future
|
|
- Lynne Marshall
- 5 years ago
- Views:
Transcription
1 !!! #!
2 ! #
3 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 Gamma-ray Sources: Facilities and Projects New Technologies Fundamental and Applied Research Using Compton Photon Sources Limitations and Prospects R&D Topics Summary: World Wide Effort on Compton Photon Sources
4 Compton Scattering Effect and Physics of Compton Photon Beams
5 % % & () +,% ) & ),
6 %., /.&/ /!
7 % : ; 3472 < 347= # % & ( ) + ),./,! /!0 1 & %,! / 2
8 & % &, > ) > 5, 2 ) & % , /
9 & % ;., % % 6 : %, % % 6 : % ( &! / 37? :
10 & 5 %,& 5 Α 0 4=Β? ? ;? 700=
11 & ; 40, 3Χ0 6& : 4 1 # % , / :! ;1 )< 4& =
12 & > % > ) >., 65. :? &! / 3? 0 = :
13 & / Ε Φ %,!,?? 2! > 4 1 # % , /
14 & % / / %,,., & 5.,?? Ε ) ), Γ ) Η) 6% 7000 :? %& 67004: %&) %Ε < 5?? /,., %) 5 Ι ) >, 5 Ι > %Ε ) ) Ι ) Ι + >
15 Compton Photon Sources around the World, Present and Future Compton X-ray Sources: Facilities, Projects and Experiments
16 & )%!!?!? ΑΧ0 + ( ϑ!!, 6!! :! % 6 +: 7? 1 640? 310 : )? Χ + )!!? 100! Ε 6Κ200 : 1 Ε Χ ΧΕ30 = ( 6 : Λ ; Ε!?!
17 & )%!? Η ( ϑ 6 Ε, ϑ :! Η % 6 : )? 0 + )! 6100 : Ε ΧΕ30 9 ( 630 5>: 6ΧΕ30 4 (? : Λ ; /,, & (!5 021? #33? <? 7033
18 & )% )? )!? ( ϑ ) )!? % 6 +: = 2Χ & )! Ε (, 6 : 3 7..? & Γ! +2? 3 = 67030: 2 & &? (( ( Μ (7004,03(,
19 & )%!? ( ϑ!! % 6 +: ? Χ0 8 =0 +? ) /, :? Α20?000! Ε ( 6 : 3 + ( Ν!! ϑ?ο ) 7037? Η? 7037??
20 Compton Photon Sources around the World, Present and Future Compton Gamma-ray Sources: Facilities and Projects
21 & % )%?,1? Η ( ϑ )%,1 Η % 6 +: 7? ? )% 7: &? 1. + ) 2Χ3 8 2ΧΧ 62 Χ +:Ι 6)% 7? 7Χ=? 12 +:! Ε 30 9 ( : ( & 3 <? Ν! )%?Ο,? < 7004
22 & % 5.? ;? ( ϑ 5.! <) ; % 6 +: &? ) %)? = 8 9 Χ2 +:! Ε 30 = 8 7Ε30 30 ( 6 Ε Α30 +: ( & <?? < ), ϑ Χ. + / ϑ Χ. + %), 6 :?,Χ 6 : 5.,? :
23 % +. %! &,Χ %) 62 Χ : Χ Χ
24 , %. & 5 & %) 780 nm Mirrors Minimal round-trip loss: ~ 0.107% Finesse ~ 3,000 Effective: R ~ 99.95% =93? ) Α0 0030=
25 % / γ,/ 7 1 7Ε30 1 γ( 5, Ε 93 +? 9 )
26 %. % (
27 High Intensity Gamma-ray Source (HIGS) - World's Most Powerful Compton Gamma-ray Source Max total intensity: > 2x10 10 gamma/second (around 10 MeV) Photon energy range: MeV - HIGS Collaboration 9 International Collaborating Institutions 22 US Collaborating Institutions Industrial Partners , 65. : Ε! Π 7Ε ( : : Α 49Β ?! 30 33, ( :
28 & % )/ Κ, + )? 3 Χ Χ Χ00, ΘΘ? Χ ( ϑ )/ Κ, + ) % 6 +: =0 &? 3 Χ. + ) 774 6Χ 7 :Ι 7 6Χ 10 +:! Ε Ε30 9 ( 630Β : ( ;& & #, 9/ Α... Α? )? ) /
29 & % )%.? &? 1 Ρ /, & / Ρ <, / Ρ,+Β Χ)6.1 Χ)6 / ( ϑ )%. & 6 & : % 6 +: ? ΧΧ0 &? 2 Χ. + ) 7?.! Ε 6Κ200 : 30 Χ 8 30 = ( 6 : ( 6 : ; & & ) 5 ) %Ε & %? &
30 & % %.,? ))<)? 3 Ο! / %) < /,? &?Ο %),<? 7 ( Ν;!? ),?,.,?Ο ) 7037? Η? 7037 ( ϑ %., ))<) % 6 +: 0 Χ Ε, )? 7Χ0 +? 7Χ0? =0 +(? 370 5>? 37? , : ) &, 637 5>:! Ε 1Ε30 = 6 ( :? ( 6 : ;
31 & % %),<? %Ε )? % ( ϑ %),< %Ε ) 6 : % % 6 +: Ε, )? 900 +? 7Χ0? 370 5>? 37? , : ) &, 637 5>:! Ε 1Ε30 1 (? ( 6 : 3 Ο! / %) < /,? &?Ο %),<? 7 Ε,,
32 Highest Average Intensity Compton Sources (2012) X-ray: )? )! ( :., 5.,? ; 6Π7Ε30 30 (? Α30 +: Compton Photon Sources around the World, Present and Future New Technologies
33 & 2 %&) / %? Η 6 : %&) Λ, %&)? 0 0 +? Ε Α30 32,3 (., Χ. + %&)? 1 8 7Χ +? Ε Α30 3= ( 3 & 5 ϑ?!? 3? 300= : 7? Ν, &?Ο &, 7030
34 & 2 ) 5 (? ))<) %&? %&? 6%Ε 7032: Laser: 532 nm, 1W (avg), 10 Hz, 3 cm Rayleigh range E-beam: MeV, 10 Hz, ~100 pc/pulse, eng sprd <5%, norm-emittance, 5pi mm-mrad,., MeV, >30 9 g/pulse? Σ30Β 3? %&? 7 5 (? &!, / 30? =:
35 & 2.,, )) Λ. 6% γ : Φ 3Λδ6% γ :Λ β6% γ : ; 3 ; 5? ), Ε? 7 ; 5? Ν& Ε & %?Ο &)? : 2 ( (7037(0Χ(,,,,,
36 Fundamental and Applied Research Using Compton Photon Sources
37 + 1 &, Research Using Compton X-ray Sources Small-scale synchrotron x-ray sources: all research typically conducted using x-ray beams from storage ring light sources, in particular in imaging, including phase-contrast imaging, micro-tomographic imaging, imaging using a single-pulse Limitations and and Prospects of Compton X-ray Sources Average flux & brightness cannot compete with 3rd-gen storage ring light sources Peak flux & brightness cannot compete with x-ray FEL (also incoherent) Comparable cost to a complex, state-of-the-art undulator beamline at a major light source Increase x-ray accessibility: Making x-ray capabilities available where x-ray science takes place 3 Ν& /% )? Ο > /? /? 7030
38 + 1 / &., Physics Research: Nuclear and HEP Nuclear Structure Few-Nucleon Physics Astrophysics Gerasimov-Drell-Hearn (GDH) Sum Rule Compton Scattering from Nucleons Photon-Pion Physics Hadron structure and quark interactions Hadronic parity violation Physics beyond the Standard Model Complementary Sources CEBAF (Jlab) ELSA Bonn MAMI Mainz ( 5 Ε (;γ. > & Φ & 9? ; 7Χ,!/
39 + 1 / &., Some Areas of Applications of Compton Gamma-ray Beams Accelerator Physics Polarized positron generation E-beam diagnostics (beam size, energy, and polarization) National Security Special nuclear materials detection (non-destructive assay) Energy Industry Nuclear waste management and treatment Medical Applications Isotope production Cancer diagnostics Industrial Applications Industrial product inspection Materials Research Novel scintillators and detectors Applications in fundamental research, space program, industry, and medicine
40 &Γ;! R&D Topics for Compact Light Sources (2010 BES Workshop) Develop IR laser systems: kw avg power, fs pulses, khz reprates Develop laser storage cavities: 10-mJ, ps and fs pulses focused to micron beam sizes Develop high-brightness, high reprate electron sources Develop CW 4K superconducting RF linacs Other R&D Topics Specific to Compton Sources Laser cavities tailored for specific Compton sources in terms of power, reprate, beam size, polarization, and collision geometry (two-mirror resonators, multi-mirror ring resonators, and non-gaussian mode cavities) Storage ring Compton sources: Optimizing final focusing design and mitigate its impact on beam dynamics General impact on beam dynamics at very high intensities Gamma-ray sources: Energy recovery consideration 3 Ν& /% )? Ο > /? /? 7030
41 ,? ϑ? %Ε )!! /<) Η,) ; <! ) ) < < %&!5! <! % 5 5? ;
42 ., ϑ 8?? ) ; <? )%.?.& ) ; ϑ 5.? )%? &? %!),)? Κ + &? Κ / &? Κ. < ϑ )%. Κ &? Κ, +? Κ )? %., Κ))<)? %),< ) %., )%. 5., + ).& ) %),< ) ; < & < / &. %!),) )% + & )%.
43
44 5 & /. 5 & < 97? 7Χ=, : ) 3 Ε 6/ : 349 ) ; < 34= ! Ε Π7Ε30 30 ( Ι Ε Α20 (
Storage 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 informationHIGS - 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 informationEnergy Recovery Linac (ERL) Science Workshop
Energy Recovery Linac (ERL) Science Workshop Sol M. Gruner, CHESS & Physics Dept. Objective: Examine science possible with an ERL x-ray source. Ques.: Ans.: Why do this? Need for more and better SR machines.
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 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 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 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 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 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 informationEnergy Recovery Linac (ERL) Properties. Physics Dept. & Cornell High Energy Synchrotron Source (CHESS) Ithaca, NY Cornell University
Energy Recovery Linac (ERL) Properties Sol M. Gruner Physics Dept. & Cornell High Energy Synchrotron Source (CHESS) Cornell University Ithaca, NY 14853-2501 Acknowledgements T. Allen (Special thanks to
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 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 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 informationThe HIGS2 Concept A Next Generation Compton Gamma-ray Source
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.
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 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 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 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 informationDevelopment status of non-destructive assay of nuclear material by using laser Compton scattered gamma-rays
Development status of non-destructive assay of nuclear material by using laser Compton scattered gamma-rays Ryoichi Hajima Japan Atomic Energy Agency IZEST Tokyo 2013 Nov. 18, 2013 Collaborators Quantum
More informationThe Proposal of Accelerator Based Light Sources for TAC Project
O. Mete Ankara University Physics Engineering Department FEL and Linac Research Group, Ph.D Student 21.11.2006 / Accelerator Physics Seminars The Proposal of Accelerator Based Light Sources for TAC Project
More informationThe UCLA/LLNL Inverse Compton Scattering Experiment: PLEIADES
The UCLA/LLNL Inverse Compton Scattering Experiment: PLEIADES J.B. Rosenzweig UCLA Department of Physics and Astronomy 23 Giugno, 2003 Introduction Inverse Compton scattering provides a path to 4th generation
More informationLinacs. Susan Smith. Daresbury Laboratory Mami and Beyond
Energy Recovery Linacs Susan Smith ASTeC/Cockcroft Daresbury Laboratory Mami and Beyond Introduction to ERLs Contents Operational ERLs Applications Challenges ERL Prototypes and R&D Summary 2 Introduction
More informationResearch with Synchrotron Radiation. Part I
Research with Synchrotron Radiation Part I Ralf Röhlsberger Generation and properties of synchrotron radiation Radiation sources at DESY Synchrotron Radiation Sources at DESY DORIS III 38 beamlines XFEL
More informationInverse Compton Scattering Sources from Soft X-rays to γ-rays
Inverse Compton Scattering Sources from Soft X-rays to γ-rays J.B. Rosenzweig UCLA Department of Physics and Astronomy 21 Ottobre, 2004 Introduction Inverse Compton scattering provides a path to 4th generation
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 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 informationIntroduction to Particle Accelerators & CESR-C
Introduction to Particle Accelerators & CESR-C Michael Billing June 7, 2006 What Are the Uses for Particle Accelerators? Medical Accelerators Create isotopes tracers for Medical Diagnostics & Biological
More informationThe VELA and CLARA Test Facilities at Daresbury Laboratory Peter McIntosh, STFC on behalf of the VELA and CLARA Development Teams
The VELA and CLARA Test Facilities at Daresbury Laboratory Peter McIntosh, STFC on behalf of the VELA and CLARA Development Teams Outline VELA & CLARA Accelerators VELA Commissioning VELA Exploitation
More informationThe Gamma Factory proposal for CERN
The Gamma Factory proposal for CERN Photon-2017 Conference, May 2017 Mieczyslaw Witold Krasny LPNHE, CNRS and University Paris Sorbonne 1 The Gamma Factory in a nutshell Accelerate and store high energy
More informationPol. e + source based on Compton scattering with FEL & 4 mirror cavity 第 8 回全体打合せ, 30 September 2014 KEK, Junji Urakawa
Pol. e + source based on Compton scattering with FEL & 4 mirror cavity 第 8 回全体打合せ, 30 September 2014 KEK, Junji Urakawa Super conducting electron linear accelerator for FEL We assume super radiant mode
More informationElectron Linear Accelerators & Free-Electron Lasers
Electron Linear Accelerators & Free-Electron Lasers Bryant Garcia Wednesday, July 13 2016. SASS Summer Seminar Bryant Garcia Linacs & FELs 1 of 24 Light Sources Why? Synchrotron Radiation discovered in
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 informationOptics considerations for
Optics considerations for ERL x-ray x sources Georg H. Hoffstaetter* Physics Department Cornell University Ithaca / NY Georg.Hoffstaetter@cornell.edu 1. Overview of Parameters 2. Critical Topics 3. Phase
More informationChina high-intensity accelerator technology developments for Neutron Sources & ADS
AT/INT-04 China high-intensity accelerator technology developments for Neutron Sources & ADS J. Wei, Tsinghua University, China S.N. Fu, IHEP, CAS, China International Topical Meeting on Nuclear Research
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 informationFree-electron laser SACLA and its basic. Yuji Otake, on behalf of the members of XFEL R&D division RIKEN SPring-8 Center
Free-electron laser SACLA and its basic Yuji Otake, on behalf of the members of XFEL R&D division RIKEN SPring-8 Center Light and Its Wavelength, Sizes of Material Virus Mosquito Protein Bacteria Atom
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 informationPARTICLE BEAMS, TOOLS FOR MODERN SCIENCE AND MEDICINE Hans-H. Braun, CERN
5 th Particle Physics Workshop National Centre for Physics Quaid-i-Azam University Campus, Islamabad PARTICLE BEAMS, TOOLS FOR MODERN SCIENCE AND MEDICINE Hans-H. Braun, CERN 2 nd Lecture Examples of Modern
More informationIntroduction to Accelerator Physics Part 1
Introduction to Accelerator Physics Part 1 Pedro Castro / Accelerator Physics Group (MPY) Introduction to Accelerator Physics DESY, 28th July 2014 Pedro Castro / MPY Accelerator Physics 28 th July 2014
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 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 informationGeorg Hoffstaetter Cornell Physics Dept. / CLASSE Cornell s ERL team
1 R&D toward an ERL Georg Hoffstaetter Cornell Physics Dept. / Cornell s ERL team DC-gun R&D CW linac R&D SRF injector R&D Undulator R&D 2 Cornell history: The ERL principle Energy recovery needs continuously
More informationPhysics 736. Experimental Methods in Nuclear-, Particle-, and Astrophysics. - Accelerator Techniques: Introduction and History -
Physics 736 Experimental Methods in Nuclear-, Particle-, and Astrophysics - Accelerator Techniques: Introduction and History - Karsten Heeger heeger@wisc.edu Homework #8 Karsten Heeger, Univ. of Wisconsin
More informationIntroduction to Accelerator Physics Part 1
Introduction to Accelerator Physics Part 1 Pedro Castro / Accelerator Physics Group (MPY) Introduction to Accelerator Physics DESY, 27th July 2015 Pedro Castro / MPY Introduction to Accelerator Physics
More informationNew Experiments at the Intensity Frontier
New Experiments at the Intensity Frontier Andreas Ringwald DESY Perspektiven der Teilchenphysik: Strategie-Workshop des KET 25-26 October 2010, Harenberg City-Center, Dortmund, D New Experiments at the
More informationBrightness and Coherence of Synchrotron Radiation and Free Electron Lasers. Zhirong Huang SLAC, Stanford University May 13, 2013
Brightness and Coherence of Synchrotron Radiation and Free Electron Lasers Zhirong Huang SLAC, Stanford University May 13, 2013 Introduction GE synchrotron (1946) opened a new era of accelerator-based
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 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 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 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 informationDouble-Polarization Results with Polarized HD at LEGS
st Pion Photoproduction Double-Polarization Results with Polarized HD at LEGS A. Lehmann (for the LEGS-Spin Collaboration) NStar LEGS Laser Electron Gamma Source Physics Motivation Experiment (SASY detector,
More informationFree-Electron Lasers
Introduction to Free-Electron Lasers Neil Thompson ASTeC Outline Introduction: What is a Free-Electron Laser? How does an FEL work? Choosing the required parameters Laser Resonators for FELs FEL Output
More informationHadron structure with photon and antiproton induced reactions - QCD in the non-perturbative range -
Hadron structure with photon and antiproton induced reactions - QCD in the non-perturbative range - Introduction Present: Photoproduction of Mesons at ELSA and MAMI CB-ELSA/TAPS Experiment Crystal Ball/TAPS
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 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 informationApplications of Accelerators from Basic Science to Industrial Use
Applications of Accelerators from Basic Science to Industrial Use December 13 th, 2016 Kiyokazu Sato TOSHIBA Corporation Keihin Product Operations 2016 Toshiba Corporation 1 /23 Contents 1. Applications
More informationSuperconducting RF Accelerators: Why all the interest?
Superconducting RF Accelerators: Why all the interest? William A. Barletta Director, United States Particle Accelerator School Dept. of Physics, MIT The HEP prespective ILC PROJECT X Why do we need RF
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 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 informationSpin dependent en cross section at small and medium Q2
NuInt04@Gran Sasso, 004/03/18 Session 3, Talk ID 3.5 Spin dependent en cross section at small and medium Q Contents: Introduction Kinematic DIS Regime (Q>1GeV, W>4GeV) Small Q Limit (Q=0 GeV) GDH sum rule
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 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 informationAccelerator Activities at PITZ
Accelerator Activities at PITZ Plasma acceleration etc. Outline > Motivation / Accelerator Research & Development (ARD) > Plasma acceleration Basic Principles Activities SINBAD > ps-fs electron and photon
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 informationFUTURE SPIN EXPERIMENTS AT SLAC
SLAC-PUB-9658 February 2003 FUTURE SPIN EXPERIMENTS AT SLAC Stephen Rock for the Real Photon Collaboration University of Mass, Amherst MA 01003 Abstract. A series of three photo-production experiments
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 informationPhotonuclear Reactions and Nuclear Transmutation. T. Tajima 1 and H. Ejiri 2
Draft Photonuclear Reactions and Nuclear Transmutation T. Tajima 1 and H. Ejiri 2 1) Kansai JAERI 2) JASRI/SPring-8, Mikazuki-cho, Sayou-gun, Hyougo, 679-5198 JAPAN Abstract Photonuclear reactions are
More informationhigh luminosity searches at JLab: mixing, Compton, and beam dump OK Baker (for the LIPSS collaboracon) JLAB Workshop September 20, 2010
high luminosity searches at JLab: mixing, Compton, and beam dump OK Baker (for the LIPSS collaboracon) JLAB Workshop September 20, 2010 overview Recent and near term LIPSS DM searches at FEL hidden sector
More informationUSPAS course on Recirculated and Energy Recovered Linacs Ivan Bazarov, Cornell University Geoff Krafft, JLAB. ERL as a X-ray Light Source
USPAS course on Recirculated and Energy Recovered Linacs Ivan Bazarov, Cornell University Geoff Krafft, JLAB ERL as a X-ray Light Source Contents Introduction Light sources landscape General motivation
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 informationTagged photon facility at Centre for Advanced Technology, Indore: Possible scenarios
PRAMANA c Indian Academy of Sciences Vol. 66, No. 5 journal of May 2006 physics pp. 903 914 Tagged photon facility at Centre for Advanced Technology, Indore: Possible scenarios L M PANT Nuclear Physics
More informationSPARCLAB. Source For Plasma Accelerators and Radiation Compton. On behalf of SPARCLAB collaboration
SPARCLAB Source For Plasma Accelerators and Radiation Compton with Laser And Beam On behalf of SPARCLAB collaboration EMITTANCE X X X X X X X X 2 BRIGHTNESS (electrons) B n 2I nx ny A m 2 rad 2 The current
More informationLinac Based Photon Sources: XFELS. Coherence Properties. J. B. Hastings. Stanford Linear Accelerator Center
Linac Based Photon Sources: XFELS Coherence Properties J. B. Hastings Stanford Linear Accelerator Center Coherent Synchrotron Radiation Coherent Synchrotron Radiation coherent power N 6 10 9 incoherent
More informationLEPS Physics HOTTA, Tomoaki (RCNP, Osaka University) on behalf of the LEPS&LEPS2 collaboration
LCS2014 International Workshop LEPS Physics HOTTA, Tomoaki (RCNP, Osaka University) on behalf of the LEPS&LEPS2 collaboration Outline Overview of the LEPS&LEPS2 beamlines Recent results from LEPS Search
More informationWhy a muon collider?
Why a muon collider? What will we learn? Mary Anne Cummings Northern Illinois Center for Accelerator and Detector Development Northern Illinois University 1 Why consider a Muon Collider? The current story
More informationProgress Report on the A4 Compton Backscattering Polarimeter
A4 Progress Report on the A4 Compton Backscattering Polarimeter Yoshio Imai, Institut für Kernphysik, Universität Mainz 8.6.24 International Workshop on Parity Violation and Hadronic Structure, LPSC Grenoble
More informationPositron program at the Idaho Accelerator Center. Giulio Stancari Idaho State University and Jefferson Lab
Positron program at the Idaho Accelerator Center Giulio Stancari Idaho State University and Jefferson Lab International Workshop on Positrons at Jefferson Lab Newport News, Virginia (USA), 26 March 2009
More informationA Review of ERL Prototype Experience and Light Source Design Challenges. Susan Smith Accelerator Physics ASTeC CCLRC Daresbury Laboratory
A Review of ERL Prototype Experience and Light Source Design Challenges Susan Smith Accelerator Physics ASTeC CCLRC Daresbury Laboratory Content Existing light source ERLs JLAB experience Challenges of
More informationProton LINAC for the Frankfurt Neutron Source FRANZ
Proton LINAC for the Frankfurt Neutron Source FRANZ - IAEA - International Topical Meeting on Nuclear Research Applications and Utilization of Accelerators Oliver Meusel 4-8 May 2009 Vienna, Austria Motivation
More informationLow-Energy Accelerators for High Precision Measurements Sebastian Baunack
Low-Energy Accelerators for High Precision Measurements Sebastian Baunack Johannes Gutenberg-Universität Mainz EINN 2017, Oct. 31 - Nov 4, 2017 Paphos, Cyprus 1 Outline New type of accelerators: ERL High
More informationOpportunities and Challenges for X
Opportunities and Challenges for X -ray Free Electron Lasers for X-ray Ultrafast Science J. Hastings Stanford Linear Accelerator Center June 22, 2004 European XFEL Laboratory How Short is short? defined
More informationThe Large Hadron electron Collider (LHeC) at the LHC
The Large Hadron electron Collider (LHeC) at the LHC F. Zimmermann, F. Bordry, H. H. Braun, O.S. Brüning, H. Burkhardt, A. Eide, A. de Roeck, R. Garoby, B. Holzer, J.M. Jowett, T. Linnecar, K. H. Mess,
More informationA4 Laser Compton polarimetry
A4 Laser Compton polarimetry progress since PAVI06 J. Diefenbach Workshop on Parity Violation 2009, Bar Harbor, Maine - 24.06.2009 Outline Principles of Laser Compton polarimetry Experimental Setup Data
More informationOVERVIEW OF THE LHEC DESIGN STUDY AT CERN
OVERVIEW OF THE LHEC DESIGN STUDY AT CERN 1 CERN CH-1211 Geneve 23, Switzerland E-mail: Oliver.bruning@cern.ch Abstract The Large Hadron electron Collider (LHeC) offers the unique possibility of exploring
More informationMedical Applications of Compact Laser-Compton Light Source
Medical Applications of Compact Laser-Compton Light Source Y. Hwang 1, D. J. Gibson 2, R. A. Marsh 2, G. G. Anderson 2, T. Tajima 1, C. P. J. Barty 2 1 University of California, Irvine 2 Lawrence Livermore
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 informationLaser-Electron Storage Ring Zhirong Huang and Ronald D. Ruth Stanford Linear Accelerator Center, Stanford University, Stanford, CA (October 16,
SLAC{PUB{7556 September 1997 Laser-Electron Storage Ring Zhirong Huang and Ronald D. Ruth Stanford Linear Accelerator Center, Stanford University, Stanford, CA 94309 Abstract A compact laser-electron storage
More informationEingeladene Vorträge auf Konferenzen und Workshops
Eingeladene Vorträge auf Konferenzen und Workshops Polarized Total Photonabsorption Cross Sections Workshop Chiral Dynamics, Bonn, 8.-13.9.2003 Published in Chiral Dynamics 2003 Mesonproduction and Experimental
More informationPhoton Regeneration at Optical Frequencies
Photon Regeneration at Optical Frequencies Andrei Afanasev Hampton University/Jefferson Lab 3 rd rd Joint ILIAS-CERN CERN-WIMPs Training workshop Patras,, Greece, June 22, 2007 Motivation for Axion Search
More informationSynchrotron-Cherenkov radiation observed in laboratory being predicted in astronomy, which will feasible compact X- ray laser
Synchrotron-Cherenkov radiation observed in laboratory being predicted in astronomy, which will feasible compact X- ray laser H. Yamada Ritsumeikan University, Tabletop Synchrotron Laboratory J. Synchrotron
More informationAn ERL-Based High-Power Free- Electron Laser for EUV Lithography
An ERL-Based High-Power Free- Electron Laser for EUV Lithography Norio Nakamura High Energy Accelerator Research Organization(KEK) 2015 EUVL Workshop, Maui, Hawaii, USA, June 15-19, 2015. ERL-EUV Design
More informationLinac Ring Colliders
Linac Ring Colliders L. Merminga and G. Krafft, Jefferson Lab V. Lebedev, FNAL and I. Ben-Zvi, BNL The Future of Particle Physics Snowmass 2001 July 4 2001, Snowmass Village, CO Outline Œ Physics Requirements
More informationSEARCHING FOR DARK PHOTONS WITH POSITRONS AT JEFFERSON LAB
SEARCHING FOR DARK PHOTONS WITH POSITRONS AT JEFFERSON LAB Luca Marsicano INFN Genova,Università Di Genova International Workshop on Physics with Positrons at Jefferson Lab September 12-15, 2017 Thomas
More informationApplications of High Brightness Beams: Energy Recovered Linacs
Applications of High Brightness Beams: Energy Recovered Linacs G. A. Krafft Jefferson Lab Schematic Representation of Accelerator Types RF Installation Beam injector and dump Beamline Ring Linac Recirculating
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 informationFundamental Concepts of Particle Accelerators V : Future of the High Energy Accelerators. Koji TAKATA KEK. Accelerator Course, Sokendai
.... Fundamental Concepts of Particle Accelerators V : Future of the High Energy Accelerators Koji TAKATA KEK koji.takata@kek.jp http://research.kek.jp/people/takata/home.html Accelerator Course, Sokendai
More informationCoherent X-Ray Sources: Synchrotron, ERL, XFEL
Coherent X-Ray Sources: Synchrotron, ERL, XFEL John Arthur SSRL/SLAC Energy Recovery Linac Science Workshop Cornell University 2 December 2000 Supported by the US Dept. of Energy, Office of Basic Energy
More informationPolarimetry in Hall A
Outline E.Chudakov Moller-12 Workshop, Aug 2008 Polarimetry in Hall A 1 Polarimetry in Hall A E.Chudakov 1 1 Hall A, JLab Moller-12 Workshop, Aug 2008 Outline E.Chudakov Moller-12 Workshop, Aug 2008 Polarimetry
More informationBERLinPro. An ERL Demonstration facility at the HELMHOLTZ ZENTRUM BERLIN
BERLinPro An ERL Demonstration facility at the HELMHOLTZ ZENTRUM BERLIN BERLinPro: ERL demonstration facility to prepare the ground for a few GeV ERL @ Berlin-Adlershof Goal: 100MeV, 100mA beam Small emittance,
More information