Synchrotron Radiation in IRAN
|
|
- Mae Henry
- 5 years ago
- Views:
Transcription
1 Synchrotron Radiation in IRAN Helmut Wiedemann, Stanford University Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran 1
2 Synchrotron Radiation is the tool of choice to study atomic and molecular structures Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran 2
3 Synchrotron Radiation is used for Basic and Applied Research in fields like: Material Science Physics Biology Chemistry Medicine Geology Environmental Science Archeology Integrated Circuits Nuclear Physics Forensics Waste Remediation Drug Development wherever atomic and molecular structures are of interest Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran 3
4 how do we generate synchrotron radiation? we build a circular electron accelerator, a storage ring Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran 4
5 main synchrotron/storage ring components photon beam line rf-cavity injection system focusing bending vacuum chamber e - Insertion device beam line Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran 5
6 Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran 6
7 Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran 7
8 why a synchrotron radiation facility in Iran? Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran 8
9 Education University based research (about 50-70%) extension of University research (providing expensive instrumentation) masters and PhD programs : about 100 PhDs/year from NSLS and SSRL Publications (1997): BLs PUBs PRL Science Nature SSRL: NSLS: Nobel Prize to R. Kornberg (Stanford) Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran
10 Technical Development magnet technology (precision machining) ultra high vacuum technology rf-technology optics, spectrometers, imaging precision alignment of large systems control systems computer control/data acquisition electronics measurement techniques operation / maintenance organization/management/administration Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran
11 Industrial/Governmental Involvement drug development future integrated circuits materials like plastic, rubber, fibers, silk corrosion micromachining energy storage (e.g. hydrogen cells for automobiles) governmental application (security) Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran
12 School of Accelerators and Particles at the IPM is studying the design of synchrotron radiation sources has assembled in 2010 an enthusiastic project group of physicist and engineers have compiled a conceptual design report (CDR) identifying critical issues understand functionality of main facility components lattice design and linear/nonlinear beam dynamics ready to build a prototype bending magnet get ready for magnetic measurement prepare to build solid state amplifiers for RF collaborate with foreign laboratories for hands-on training set up a management structure Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran 12
13 ILSF group is forcefully and effectively preparing on broad base these preparations during 2010 set the base to make the next step think about options think about optimization satisfy the particular needs of Iranian users meet particular design goal minimize cost, schedule and effort Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran 13
14 To this effort I would like to add some suggestions: what should be the parameters of the ILSF? when will ISLF be available? ? will the design parameters still be up-to-date then? will technology advance we have to think ahead Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran 14
15 consider design alternatives there are advantages/disadvantages to all designs what are the most important design feature? how can you proceed in existing economic environment? how can technology help us to minimize risk reduce construction and operating costs Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran 15
16 main storage ring parameters? energy current 3 GeV 500 ma photon spectrum source size beam emittance photon beam brightness hard x-rays, > kev as mall as possible, <~ 1 nm undulator radiation source magnet free insertion sections for IDs many 6 12 m long all have impact on construction cost operating cost $$$$$$$ Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran 16
17 electron beam energy and current energy 3 GeV is most common technologies exists to create desired spectrum current as much as possible and affordable technology limit (absorber) at about 500 ma Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran 17
18 Biology most likely will be the most prominent future user community they need photon energies kev, sometimes lower, broad band or variable if monochromatic this also fits most other users Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran 18
19 Bending magnet or wiggler magnet radiation log I log w is broad band up to 3-5 x critical photon energy c 3 2 c 3 c kev 2.22 E 3 GeV m w c E GeV B T Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran 19
20 Beam Emittance source size: as small as possible (diffraction limit) small sample, aberrations energy resolution small beam emittance photon beam brightness B photons 4 x x y y E E ph t photons mm 2 mrad 2 0.1%BW s B 1 2 small beam emittance Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran 20
21 how small an emittance? diffraction limit for ph 4 1Å ph m not possible with present technology E 2 3 many bending magnets larger circumference recent SRs have emittances of ~ 3 5 nm, future rings ~ 1 nm with 10 in Brightness! ILSF 1nm Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran 21
22 Brightness is the photon density in phase space B photons 4 x x y y E E ph t photons mm 2 mrad 2 0.1%BW s need low emittance undulators with many periods N p, because long straight sections for long undulators long straight sections for 2 undulators t E E ph 1 N p bunch length limited to ps for technical reasons Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran 22
23 Undulator Radiation Pattern need long undulators with many periods to get small band width Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran 24
24 Undulator emits quasi-monochromatic radiation l p period length of undulator fundamental wavelength of undulator radiation p K2 p K2 Lorentz Contraction Doppler Effect Undulator strength parameter K 0.934B T p cm where q is the maximum deflection angle from the axis Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran 24
25 l l p K2 2 2 q obs Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran 25
26 Standard Spring-8 in vacuum undulator l p = 32 mm, N p = 140, gap > 8 mm, K max = 2.3, L = 4.5 m Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran 26
27 suggestions for alternative ILSF storage ring option goals while not compromising performance: lower beam emittance (from 3.2 to <=1 nm) more and longer straight sections green machine - minimize power consumption easier design of components lower component costs lower operating costs unwanted impact: increased ring circumference! Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran 27
28 0 2,000 1,000 4,000 3,000 6,000 5,000 8,000 7,000 10,000 9,000 12,000 11,000 14,000 13,000 16,000 15,000-1,400-1,200-1,000 mm x, magnetic midplane field, B_y(x,0.0) use low field bending magnets (0.5T instead 1.4T) produce hard x-ray bending magnet radiation only where needed low field, 0.5 T, 6 0 low field, 0.5 T, T 1 0 low field, 0.5 T, magnetic midplane field, B_y(x,0.0) -1,400-1,200-1, x, mm Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran 28
29 low field bending magnets (0.5T instead 1.4T) benefits: lower beam emittance 1.2 nm (by factor 2.8) higher photon beam brightness (by factor 8) less magnet power (-64%) less radiation from bending magnets use high field inserts for hard x-rays less rf-power (-400 kw) less cooling of vacuum chamber more/longer straight sections (10x10.5m, 10x5.5m) vs (4x7.8m, 16x4m, 12x2.8m) negative circumference increases by 150m Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran 29
30 solid state amplifiers for RF-system: conventional microwave power sources are klystrons expensive and hard to repair solid state amplifiers ~800 to 1000 W combine many to get 100 kw units can be developed locally with local components if one fails, just replace malfunctioning amplifier need 400 kw less in low field magnet option Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran 30
31 before final decision need to consider a variety of lattice options in consultation with users in consultation with technical groups/interests in consultation with management to Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran 31
32 eventually arrive at a truly Iranian design serving Iranian Science Community Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran 32
33 I wish you and the ISLF continuing Good Progress and Good Luck Thank you Synchrotron Radiation in IRAN, Helmut Wiedemann, IPM, May 18, 2011, Tehran 33
Research 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 information3. Synchrotrons. Synchrotron Basics
1 3. Synchrotrons Synchrotron Basics What you will learn about 2 Overview of a Synchrotron Source Losing & Replenishing Electrons Storage Ring and Magnetic Lattice Synchrotron Radiation Flux, Brilliance
More informationInsertion Devices Lecture 2 Wigglers and Undulators. Jim Clarke ASTeC Daresbury Laboratory
Insertion Devices Lecture 2 Wigglers and Undulators Jim Clarke ASTeC Daresbury Laboratory Summary from Lecture #1 Synchrotron Radiation is emitted by accelerated charged particles The combination of Lorentz
More informationIranian Light Source Facility (ILSF) Project
Iranian Light Source Facility (ILSF) Project Hossein Ghasem On behalf of ILSF technical staff School of Particles and Accelerators, IPM 1390 29 28 1 Iranian users requirements Source Energy range Photon
More informationFirst propositions of a lattice for the future upgrade of SOLEIL. A. Nadji On behalf of the Accelerators and Engineering Division
First propositions of a lattice for the future upgrade of SOLEIL A. Nadji On behalf of the Accelerators and Engineering Division 1 SOLEIL : A 3 rd generation synchrotron light source 29 beamlines operational
More informationLight Source I. Takashi TANAKA (RIKEN SPring-8 Center) Cheiron 2012: Light Source I
Light Source I Takashi TANAKA (RIKEN SPring-8 Center) Light Source I Light Source II CONTENTS Introduction Fundamentals of Light and SR Overview of SR Light Source Characteristics of SR (1) Characteristics
More informationPart V Undulators for Free Electron Lasers
Part V Undulators for Free Electron Lasers Pascal ELLEAUME European Synchrotron Radiation Facility, Grenoble V, 1/22, P. Elleaume, CAS, Brunnen July 2-9, 2003. Oscillator-type Free Electron Laser V, 2/22,
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 informationA2. Light Source. ( i ) Units of light intensity
A2. Light Source The important prerequisite for the success of a radiation eperiment is to properly understand the properties of each type of light source. The present document is part of the "SPring-8
More informationJSPS Asien Science Seminar Synchrotron Radiation Science
SESAME Synchrotron Light for Experimental Science and Applications in the Middle East JSPS Asien Science Seminar Synchrotron Radiation Science Dieter Einfeld Amman, October 2002 Introduction Based on the
More informationIntroduction to Accelerator Physics CHESS & LEPP
1 Introduction to Accelerator Physics Content 1. A History of Particle Accelerators 2. E & M in Particle Accelerators 3. Linear Beam Optics in Straight Systems 4. Linear Beam Optics in Circular Systems
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 informationRADIATION SOURCES AT SIBERIA-2 STORAGE RING
RADIATION SOURCES AT SIBERIA-2 STORAGE RING V.N. Korchuganov, N.Yu. Svechnikov, N.V. Smolyakov, S.I. Tomin RRC «Kurchatov Institute», Moscow, Russia Kurchatov Center Synchrotron Radiation undulator undulator
More informationIntroduction to electron and photon beam physics. Zhirong Huang SLAC and Stanford University
Introduction to electron and photon beam physics Zhirong Huang SLAC and Stanford University August 03, 2015 Lecture Plan Electron beams (1.5 hrs) Photon or radiation beams (1 hr) References: 1. J. D. Jackson,
More informationAbstract. 1. Introduction
The New Upgrade of SESAME D.Einfeld1, R.H.Sarraf2, M.Attal3, H.Hashemi4, A.Elsisi5, A.Amro6, H.Hassanzadegan4, K.Tavakoli3, B.Kalantari7, S. Varnasery8, E. Al-Dmour8, D. Foudeh6, H.Tarawneh9, A.Aladwan7
More informationComparison of the brilliance limit between MAX IV 3 GeV ring and NSLS II low beta straights using the same undulator technique
Comparison of the brilliance limit between 3 GeV ring and low beta straights using the same undulator technique Erik Wallén Thu 10 Nov 2011 22:18:57 Contents Contents 1 1 Introduction 2 2 Undulator technique
More informationLattice Design and Performance for PEP-X Light Source
Lattice Design and Performance for PEP-X Light Source Yuri Nosochkov SLAC National Accelerator Laboratory With contributions by M-H. Wang, Y. Cai, X. Huang, K. Bane 48th ICFA Advanced Beam Dynamics Workshop
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 informationTHE SPEAR3 UPGRADE PROJECT AT SLAC *
IWAA2004, CERN, Geneva, 4-7 October 2004 THE SPEAR3 UPGRADE PROJECT AT SLAC * Catherine Le Cocq, Brian Fuss, Michael Gaydosh Stanford Linear Accelerator Center, Stanford, CA, USA 1. INTRODUCTION The Stanford
More informationSummary Report: Working Group 2 Storage Ring Sources Future Light Source Workshop SLAC, March 1-5, S. Krinsky and R. Hettel
Summary Report: Working Group 2 Storage Ring Sources Future Light Source Workshop SLAC, March 1-5, 2010 S. Krinsky and R. Hettel Sessions 1. Low Emittance Ring Design --Y. Cai 2. Novel Concepts --D. Robin
More informationAdvanced Storage Photon Ring Source Upgrade Project:
Advanced Storage Photon Ring Source Upgrade Project: The Shielding World s for Leading the Hard X-ray Light Source Advanced Photon Source - Upgrade Bradley J. Micklich Radiation Physicist Argonne National
More informationThe basics of structural biology. And Why we use synchrotron sources Sean McSweeney ESRF Structural Biology Group
The basics of structural biology And Why we use synchrotron sources Sean McSweeney ESRF Structural Biology Group The rise and rise of structural biology. 2 The aim of the game 3 What information does structure
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 informationEmittance Growth and Tune Spectra at PETRA III
Emittance Growth and Tune Spectra at PETRA III Presentation at the ECLOUD 2010 workshop Rainer Wanzenberg ECLOUD 2010 October 8-12, 2010 Statler Hotel, Cornell University Ithaca, New York USA PETRA III
More informationSCSS Prototype Accelerator -- Its outline and achieved beam performance --
SCSS Prototype Accelerator -- Its outline and achieved beam performance -- Hitoshi TANAKA RIKEN, XFEL Project Office 1 Content 1. Light Quality; SPring-8 v.s. XFEL 2. What are the critical issues? 3. Mission
More informationSynchrotron radiation: A charged particle constrained to move in curved path experiences a centripetal acceleration. Due to it, the particle radiates
Synchrotron radiation: A charged particle constrained to move in curved path experiences a centripetal acceleration. Due to it, the particle radiates energy according to Maxwell equations. A non-relativistic
More informationAccelerator Physics. Accelerator Development
Accelerator Physics The Taiwan Light Source (TLS) is the first large accelerator project in Taiwan. The goal was to build a high performance accelerator which provides a powerful and versatile light source
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 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 informationLinear Collider Collaboration Tech Notes
LCC 0035 07/01/00 Linear Collider Collaboration Tech Notes More Options for the NLC Bunch Compressors January 7, 2000 Paul Emma Stanford Linear Accelerator Center Stanford, CA Abstract: The present bunch
More informationLow Emittance Storage Ring for Light Source. Sukho Kongtawong PHY 554 Fall 2016
Low Emittance Storage Ring for Light Source Sukho Kongtawong PHY 554 Fall 2016 Content Brightness and emittance Radiative effect and emittance Theory Theoretical Minimum Emittance (TME) cell Double-bend
More informationPEP-X Light Source at SLAC
PEP-X Light Source at SLAC Status Report Revision 0 June 10, 2008 PEP-X Study Group: Karl Bane, Lynn Bentson, Kirk Bertsche, Sean Brennan, Yunhai Cai, Alex Chao, Scott DeBarger, Valery Dolgashev, Robert
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 informationName U200 U55 U17 W40 Type Electromagnet Pure Permanent. NdFeB
4 Radiation Sources One of the main motivations to build SLS is to have a very bright source of photons in a wide spectral range. This is achieved on one hand with a very low emittance of the electron
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 informationPreliminary design study of JUICE. Joint Universities International Circular Electronsynchrotron
Preliminary design study of JUICE Joint Universities International Circular Electronsynchrotron Goal Make a 3th generation Synchrotron Radiation Lightsource at 3 GeV Goal Make a 3th generation Synchrotron
More informationand Applications in the Middle East S E S A M E Applications in the Middle East Upgrading of SESAME to 2.5GeV The Yellow Book November 2003
Synchrotron-Light for Synchrotron-Light Experimental Science for Experimental Science and and S E S A M E Upgrading of to 2.5GeV The Yellow Book November 2003 11Dieter th ESLS Einfeld 2 nd ESRF, Council
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 informationMAGNETS AND INSERTION DEVICES FOR THE ESRF II
MAGNETS AND INSERTION DEVICES FOR THE ESRF II OUTLINE Magnetic design R&D and Magnetic measurements IDs & BM sources Summary J. Chavanne G. Lebec C. Benabderrahmane C.Penel On behalf the accelerator upgrade
More informationAccelerator Details: the Antiproton Source
1 di 6 10/05/2006 9.23 Return to Fermilab's Chain of Accelerators (movie clip) Fermilab's Chain of Accelerators Return to Accelerator Details Main Page Why use antiprotons? A collider has an enormous advantage
More informationVacuum System of Synchrotron radiation sources
3 rd ILSF Advanced School on Synchrotron Radiation and Its Applications September 14-16, 2013 Vacuum System of Synchrotron radiation sources Prepared by: Omid Seify, Vacuum group, ILSF project Institute
More informationOVERVIEW OF THE ADVANCED PHOTO&&~E (APS)* Marion M. White, Argonne National Laboratory, Argonne, IL, USA I. INTRODUCTION
OVERVIEW OF THE ADVANCED PHOTO&&~E (APS)* Marion M White, Argonne National Laboratory, Argonne, IL, 60439 USA Abstract The Advanced Photon Source (APS)is a state-of-theart synchrotronlight source facility
More information2. X-ray Sources 2.1 Electron Impact X-ray Sources - Types of X-ray Source - Bremsstrahlung Emission - Characteristic Emission
. X-ray Sources.1 Electron Impact X-ray Sources - Types of X-ray Source - Bremsstrahlung Emission - Characteristic Emission. Synchrotron Radiation Sources - Introduction - Characteristics of Bending Magnet
More informationTrends in X-ray Synchrotron Radiation Research
Trends in X-ray Synchrotron Radiation Research Storage rings Energy Recovery Linacs (ERL) Free Electron Lasers Jochen R. Schneider DESY Development of the brilliance of X-ray sources Since the discovery
More informationSynchrotron radiation: A charged particle constrained to move in curved path experiences a centripetal acceleration. Due to this acceleration, the
Synchrotron radiation: A charged particle constrained to move in curved path experiences a centripetal acceleration. Due to this acceleration, the particle radiates energy according to Maxwell equations.
More informationSPPS: The SLAC Linac Bunch Compressor and Its Relevance to LCLS
LCLS Technical Advisory Committee December 10-11, 2001. SPPS: The SLAC Linac Bunch Compressor and Its Relevance to LCLS Patrick Krejcik LCLS Technical Advisory Committee Report 1: July 14-15, 1999 The
More informationTransverse Field Profile of the NLC Damping Rings Electromagnet Wiggler
LCC 0038 29/04/00 CBP Tech Note - 234 Linear Collider Collaboration Tech Notes Transverse Field Profile of the NLC Damping Rings Electromagnet Wiggler 29 April 2000 17 J. Corlett and S. Marks Lawrence
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 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 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 informationLattice Design for the Taiwan Photon Source (TPS) at NSRRC
Lattice Design for the Taiwan Photon Source (TPS) at NSRRC Chin-Cheng Kuo On behalf of the TPS Lattice Design Team Ambient Ground Motion and Civil Engineering for Low Emittance Electron Storage Ring Workshop
More informationRadiation Protection Considerations for the Cryogenic In-Vacuum Undulator of the EMIL Project at BESSY
Radiation Protection Considerations for the Cryogenic In-Vacuum Undulator of the EMIL Project at BESSY Yvonne Bergmann, Klaus Ott Helmholtz- Zentrum Berlin BESSY II Radiation Protection Department yvonne.bergmann@helmholtz-berlin.de
More informationThe MAX IV Project. Background The Machine(s) The Beamlines. 32nd International Free Electron Laser Conference, Aug 23-27, 2010, Malmö
The MAX IV Project Background The Machine(s) The Beamlines MAX-lab - A laboratory under continuous development MAX II 1500 MeV MAX III 700 MeV MAX I 550 MeV LINAC injektor MAX FEL History: 1985 MAX I 1997
More informationIntroduction to Synchrotron Radiation
Introduction to Synchrotron Radiation Frederico Alves Lima Centro Nacional de Pesquisa em Energia e Materiais - CNPEM Laboratório Nacional de Luz Síncrotron - LNLS International School on Laser-Beam Interactions
More informationPAL LINAC UPGRADE FOR A 1-3 Å XFEL
PAL LINAC UPGRADE FOR A 1-3 Å XFEL J. S. Oh, W. Namkung, Pohang Accelerator Laboratory, POSTECH, Pohang 790-784, Korea Y. Kim, Deutsches Elektronen-Synchrotron DESY, D-603 Hamburg, Germany Abstract With
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 informationHow Does It All Work? A Summary of the IDEAS Beamline at the Canadian Light Source
How Does It All Work? A Summary of the IDEAS Beamline at the Canadian Light Source What Makes Up The Canadian Light Source? 4. Storage Ring 5. Synchrotron Light 6. Beamline 1. Electron Gun 2. Linear Accelerator
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 informationNSRRC Current Status and the TPS Project
NSRRC Current Status and the TPS Project Chien-Te Chen July 21, 2005 1-1 Milestones 1981 Dec. Feasibility study began 1983 Jul. SRRC Project approved by the government 1986 Mar. Preparatory Office of SRRC
More informationWhy do we accelerate particles?
Why do we accelerate particles? (1) To take existing objects apart 1803 J. Dalton s indivisible atom atoms of one element can combine with atoms of other element to make compounds, e.g. water is made of
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 informationReview of Future European Synchrotron Radiation Projects
Review of Future European Synchrotron Radiation Projects Lenny Rivkin Paul Scherrer Institute, Villigen, Switzerland Abstract The future European synchrotron radiation projects offer a wide and bright
More informationLHC Status and CERN s future plans. Lyn Evans
LHC Status and CERN s future plans Lyn Evans Machine layout L. Evans EDMS document no. 859415 2 Cryodipole overview 1250 1000 Equivalent dipoles 750 500 250 0 01-Jan-01 01-Jan-02 01-Jan-03 01-Jan-04 01-Jan-05
More informationCanadian Light Source: Overview
Canadian Light Source: Overview 2010 April Outline CLS project history Accelerator design Accelerator performance and development Beamlines accelerator-related activity Future plans The Case for CLS 10000
More informationFeasibility Study of Short-Wavelength and High-Gain FELs in an Ultimate Storage Ring. Introduction Ultimate Storage Ring Analysis Simulation Summary
Feasibility Study of Short-Wavelength and High-Gain FELs in an Ultimate Storage Ring Koji Tsumaki (JASRI/SPring-8) Introduction Ultimate Storage Ring Analysis Simulation Summary 1 Average Brightness Introdution
More informationTools of Particle Physics I Accelerators
Tools of Particle Physics I Accelerators W.S. Graves July, 2011 MIT W.S. Graves July, 2011 1.Introduction to Accelerator Physics 2.Three Big Machines Large Hadron Collider (LHC) International Linear Collider
More informationFrom Storage Rings to Free Electron Lasers for Hard X-Rays
SLAC-PUB-10300 December 2003 From Storage Rings to Free Electron Lasers for Hard X-Rays Heinz-Dieter Nuhn* *Stanford Linear Accelerator Center, 2575 Sand Hill Rd, Menlo Park, CA 94025 E-mail: nuhn@slac.stanford.edu
More informationThe TESLA Dogbone Damping Ring
The TESLA Dogbone Damping Ring Winfried Decking for the TESLA Collaboration April 6 th 2004 Outline The Dogbone Issues: Kicker Design Dynamic Aperture Emittance Dilution due to Stray-Fields Collective
More informationParticle Accelerators Projects in Iran (Focused on the IPM recent and future projects)
Particle Accelerators Projects in Iran (Focused on the IPM recent and future projects) Hamed Shaker School of Particles and Accelerators, Institute for Research in Fundamental Sciences (IPM) History During
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 informationPhysics 610. Adv Particle Physics. April 7, 2014
Physics 610 Adv Particle Physics April 7, 2014 Accelerators History Two Principles Electrostatic Cockcroft-Walton Van de Graaff and tandem Van de Graaff Transformers Cyclotron Betatron Linear Induction
More informationLASER-COMPTON SCATTERING AS A POTENTIAL BRIGHT X-RAY SOURCE
Copyright(C)JCPDS-International Centre for Diffraction Data 2003, Advances in X-ray Analysis, Vol.46 74 ISSN 1097-0002 LASER-COMPTON SCATTERING AS A POTENTIAL BRIGHT X-RAY SOURCE K. Chouffani 1, D. Wells
More informationRadiation Protection At Synchrotron Radiation Facilities
3 rd ILSF Advanced School on Synchrotron Radiation and Its Applications September 14-16, 2013 Radiation Protection At Synchrotron Radiation Facilities Ehsan Salimi Shielding and Radiation Safety Group
More informationMAX IV, NSLS II, PLS II, LCLS, SACLA, European XFEL,
3 rd rd and 4 th Generation Light Sources Prapong Klysubun March 4, 2014 2014 Accelerator Seminar no. 1 Khao Yai Paradise on Earth, Khao Yai, Nakhon Ratchasima, Thailand P. Klysubun 2014 1 Outline 1. History
More informationComparison of the APS Upgrade to
Comparison of the APS Upgrade to ERL@APS Michael Borland Argonne National Laboratory March 2010 The submitted manuscript has been created by UChicago Argonne, LLC, Operator of Argonne National Laboratory
More informationExploration of a Tevatron-Sized Ultimate Light Source
Exploration of a Tevatron-Sized Ultimate Light Source Michael Borland Argonne National Laboratory March 2012 The submitted manuscript has been created by UChicago Argonne, LLC, Operator of Argonne National
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 informationBeamlines on Indian synchrotron radiation source Indus-1
Beamlines on Indian synchrotron radiation source Indus-1 R. V. Nandedkar Centre for Advanced Technology, Indore 452 013, India In India, at the Center for Advanced Technology (CAT), Indore a 450 MeV electron
More informationLawrence Berkeley National Laboratory Lawrence Berkeley National Laboratory
Lawrence Berkeley National Laboratory Lawrence Berkeley National Laboratory Title: Femto-Second Pulses of Synchrotron Radiation Author: Zholents, A.A. Publication Date: 01-13-2011 Publication Info: Lawrence
More information1 BROOKHAVEN SCIENCE ASSOCIATES
The Storage Ring Control Network of NSLS-II C. Yu, F. Karl, M. Ilardo, M. Ke, C. Spataro, S. Sharma 1 BROOKHAVEN SCIENCE ASSOCIATES Outline Project Overview Survey Networks Overview Error Estimate Measurement
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 informationLC Commissioning, Operations and Availability
International Technology Recommendation Panel X-Band Linear Collider Path to the Future LC Commissioning, Operations and Availability Tom Himel Stanford Linear Accelerator Center April 26-27, 2004 Integrating
More informationParticles and Universe: Particle accelerators
Particles and Universe: Particle accelerators Maria Krawczyk, Aleksander Filip Żarnecki March 24, 2015 M.Krawczyk, A.F.Żarnecki Particles and Universe 4 March 24, 2015 1 / 37 Lecture 4 1 Introduction 2
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 informationDavid Martin High Precision Beamline Alignment at the ESRF IWAA, Grenoble 3-7 October 2016
David Martin High Precision Beamline Alignment at the ESRF IWAA, Grenoble 3-7 October 2016 OVERVIEW The ESRF has just completed the Phase I Upgrade programme. The Phase I Upgrade programme was centered
More informationLord of the Rings. The story of baby MAX how he learned to walk and grew up to be big and strong.
375 Lord of the Rings The story of baby MAX how he learned to walk and grew up to be big and strong. A small ring Sweden s first electron accelerator was built in Stockholm at the Royal Institute of Technology,
More informationSteady State Analysis of Short-wavelength, High-gain FELs in a Large Storage Ring. Abstract
SLAC PUB 12858 October 2007 Steady State Analysis of Short-wavelength, High-gain FELs in a Large Storage Ring Z. Huang, K. Bane, Y. Cai, A. Chao, R. Hettel Stanford Linear Accelerator Center, Menlo Park,
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 informationELECTRON DYNAMICS WITH SYNCHROTRON RADIATION
ELECTRON DYNAMICS WITH SYNCHROTRON RADIATION Lenny Rivkin Ecole Polythechnique Federale de Lausanne (EPFL) and Paul Scherrer Institute (PSI), Switzerland CERN Accelerator School: Introduction to Accelerator
More informationImaging & Microscopy
Coherent X-ray X Imaging & Microscopy => Opportunities Using a Diffraction-Limited Energy Recovery Linac (ERL) Synchrotron Source Q. Shen D. Bilderback, K.D. Finkelstein, E. Fontes, & S. Gruner Cornell
More informationAccelerator Physics, BAU, First Semester, (Saed Dababneh).
Accelerator Physics 501503746 Course web http://nuclear.bau.edu.jo/accelerators/ edu or http://nuclear.dababneh.com/accelerators/ com/accelerators/ 1 Grading Mid-term Exam 25% Projects 25% Final Exam 50%
More informationEffect of Insertion Devices. Effect of IDs on beam dynamics
Effect of Insertion Devices The IDs are normally made of dipole magnets ith alternating dipole fields so that the orbit outside the device is un-altered. A simple planer undulator ith vertical sinusoidal
More informationSLAC-TN-93-2 SLAC/SSRL-0002 January 1993 (SSRL/ACD) COMPARISON OF PLANAR HELICAL UNDULATOR DESIGNS FOR SPEAR BEAMLINE FIVE*
SLAC-TN-93-2 SLAC/SSRL-0002 January 1993 (SSRL/ACD) COMPARISON OF PLANAR HELICAL UNDULATOR DESIGNS FOR SPEAR BEAMLINE FIVE* Roger Car-r Stanford Linear Accelerator Center Stanford Synchrotron Radiation
More informationSynchrotron Radiation. How is synchrotron light made? by accelerating electrons
Synchrotron Radiation How is synchrotron light made? by accelerating electrons Electromagnetic Radiation Electrons accelerating by running up and down in a radio antenna emit radio waves Radio waves are
More informationOptimization of the SIS100 Lattice and a Dedicated Collimation System for Ionisation Losses
Optimization of the SIS100 Lattice and a Dedicated Collimation System for Ionisation Losses P. Spiller, K. Blasche, B. Franczak, J. Stadlmann, and C. Omet GSI Darmstadt, D-64291 Darmstadt, Germany Abstract:
More informationPHYSICAL METHODS, INSTRUMENTS AND MEASUREMENTS Vol. II - Synchrotron Radiation - Malcolm J. Cooper
SYNCHROTRON RADIATION Malcolm J. Cooper University of Warwick, Coventry, UK Keywords: Accelerator, storage ring, X-rays, insertion devices, X-ray optics, diffraction, crystallography, X-ray spectroscopy,
More informationRF systems for the MAX IV rings
RF systems for the MAX IV rings On behalf of the MAX-lab RF team Outline MAX IV overview Ring RF overview Main cavity design Higher harmonic cavity design MAX IV overview; site Start 3.5 GeV Linac Short
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 informationTOWARDS DIFFRACTION LIMITED STORAGE RING BASED LIGHT SOURCES
Proceedings of IPAC2017, Copenhagen, Denmark TOWARDS DIFFRACTION LIMITED STORAGE RING BASED LIGHT SOURCES L. Liu and H. Westfahl Jr. Brazilian Synchrotron Light Laboratory, LNLS, Campinas, Brazil Abstract
More informationCommissioning of PETRA III. Klaus Balewski on behalf of the PETRA III Team IPAC 2010, 25 May, 2010
Commissioning of PETRA III Klaus Balewski on behalf of the PETRA III Team IPAC 2010, 25 May, 2010 PETRA III Parameters Circumference (m) Energy (GeV) ε x (nm rad) ε y (pm rad) Current (ma) # bunches Straight
More information