Canadian Light Source: Overview
|
|
- Ralf Allen
- 5 years ago
- Views:
Transcription
1 Canadian Light Source: Overview 2010 April
2 Outline CLS project history Accelerator design Accelerator performance and development Beamlines accelerator-related activity Future plans
3 The Case for CLS # CA Users Canadian Users # Int'l Users International Users Fr UK Ge US Swed CA ?
4 CLS History Canadian Synchrotron Radiation Facility Operated up to 3 beamlines at SRC in Madison since 1980 s 1991 Canadian Institute for Synchrotron Radiation Proposal 1.5 GeV for soft x-rays Racetrack design with few Insertion Devices Superconducting wiggle bends 1994 Design workshop at University of Saskatchewan (U. of S.) 1.5 GeV, 8-cell Triple-Bend Achromatic (TBA) lattice 104 m circumference Too few straights!
5 CLS History 1995 Revised proposal from U. of S. 2.5 GeV, 12-cell Double-Bend Achromatic (DBA) lattice 127 m circumference Budget estimate almost frozen More ID s, and 20 kev x-rays requested 1999 March 31 - CLS Project approved with Canada Foundation for Innovation (CFI) award to U. of S. 2.9 GeV, 12-sector DBA 171 m circumference, with longer straights Incorporate existing 300 MeV linac into injector
6 CLS Project CLS Project approved on 1999 March M $C to construct: 2.9 GeV booster and third-generation storage ring at least six beamlines Only 22 staff at the start of the project, including: 2 accelerator physicists 1 mechanical engineer 1 electrical engineer 4-person group for IT, controls, diagnostics 2 scientists Challenge: Complete facility in approximately five years Increase technical staff to more than 130 Build organization for operations and future R & D
7 Initial Capital Funding $140.9M Sask 18% Ontario 7% Alberta 7% UofS 4% City of Saskatoon, Sask Power, Boehringer Ingelheim, UofA, UWO 4% NRC/NRCan 6% Canada CFI 40% Western Diversification 16%
8 Initial Facility Layout
9 Synchrotron Light Source Facilities Facility Year Commissioned Energy Circumference Emttance Current ESRF (EU) / 300 APS (US) PLS (KO) SPRING-8 (JP) BESSY-II (DE) SLS (CH) CLS (CA) / 500 SPEAR-3 (US) SOLEIL (FR) ASP (AU) DIAMOND (UK) / 500 SSRF (CN) / 300 PETRA III (DE) / 200 ALBA (ES) TPS (TW) MAX-IV (SE) 2013? 3 ~500 <1.0 ~500 NSLS II (US) ~ ~780 <
10 CLS Linac 220 kv Pulsed electron gun Bunch train length selector ~ 0.1 nc / linac bunch 2856 MHz pre-buncher / buncher Six 2856 MHz, 50 MeV linac sections 250 MeV output energy Asynchronous to 500 MHz in booster ns long pulse train to booster 1 s -1 pulse repetition rate
11 CLS Booster 250 MeV to 2.9 GeV Synchrotron Up to 10 ma circulating current 1 s -1 repetition rate m circumference Compact FODO lattice 8 straight sections available for injection, extraction and RF 1.7 MV RF at 500 MHz, h=171 (3 x 3 x 19) B dipole = 1.33 T at 2.9 GeV ε x (damped) = 550 nm rad at 2.9 GeV
12 CLS Storage Ring 2.9 GeV DBA lattice with 12-fold period m circumference 2.4 MV rf at 500 MHz, h=285 (3 x 5 x 19) E loss per turn: > MeV Bend magnet radiation: λ c = 1.6 Å E c = 7.6 kev ε x = 18.1 nm rad Damping times: τ x = 2.4 ms, τ y = 3.8 ms, τ E = 2.7 ms ~10 mm bunch length
13 Sector details SYNCHROTRON LIGHT TO EXPERIMENTAL STATIONS PLAN VIEW (1 of 12 CELLS) meter SCALE QF QF B SA QF SB QF SA B QF QF
14 Storage Ring Operating Parameters Tunes ν x ν y Emittance nm 14.1 Straights β x β y η x m m 0.15 (0.25) 0.15 m Mom. Comp RF freq MHz voltage 2.4 MV δ acceptance 2.0 %
15 Storage Ring Magnets Dipoles: 2 per cell 1.87 m long T B = 3.87 T/m Quadrupoles: 3 families, 6 total per cell m, m and m magnetic length B < 21.3 T/m Sextupoles: 2 families, 3 total per cell 0.21 m magnetic length B = 245 T/m 2 One family also has dipole corrector coils and skew quadrupole coils
16 500 MHz RF System First light source to operate using only super-conducting rf Adopted a two-stage approach to the RF system Stage 1: Initial installation for 250 ma operation Stage 2: Future RF upgrade to 500 ma operation Initially use one SC cavity, based on Cornell CESR-B design, installed Second cavity is available on site, initially used as a spare, to be installed in Stage kw installed RF power for >250 ma operation. Liquid Helium Refrigeration (Linde TCF-50) was sized for operation of one cavity, with flexibility to expand to service an additional cavity.
17 Superconducting RF Cavity
18 First Light 2003 December 10
19 Machine Function Measurements
20 Orbit Control Based on Bergoz BPM electronics RMS orbit (at BPMs) ~ 1 micron Local bumps with global correction scheme RMS long-term stability ~ 2 microns Current dependency in beam position (needs work) Suspect BPM and vacuum chamber thermal shifts Fast orbit correction to 60 Hz recently tested May not be necessary for vibration control Used to correct perturbations from changing ID gaps Possible use with ramping BMIT wiggler
21 Single Bunch Mode 35 ma per bunch has been achieved Reduced to 15 ma with narrow vacuum chamber > 99.99% bunch purity has been achieved with bunch cleaning using I-Tech transverse feedback system Encountering problems with heating of injection kicker vacuum ceramics
22 Coupling Correction Normal operations is with natural coupling ( ~ 0.5 %) Coupling <0.1% has been achieved
23 Storage Ring Performance Achieved Design Goals ( ) Start First 2 years Long-term (2003) ( ) (> 2008) Horizontal Emittance (nm rad) * Energy (GeV) 1.5, X-Y Coupling <0.1% to 0.3% <10% <1% < 0.2% Tunes ( x / y ) (10.22 / 3.26) (10.22 / 3.26) (10.22 / 3.26) (10.22 / 3.26) Alternate operating points: (10.22 / 4.26) (10.22 / 4.26 ) (10.22 / 4.26 ) (11.22 / 3.26) * RMS orbit stability ( x / y ) (μm) 1.0 / / / 3 30 / 1* RMS orbit position ( x / y ) (μm) 2 / 1 40 / / / 40 Maximum current (ma) (?) 100 ma (hours) 29 > 4 > 6 > 10 / Top-up* Time Structure Multi-bunch Multi-bunch Multi-bunch or single bunch*
24 Facility Performance
25 Facility Performance
26 Current and Planned Beamlines
27 CLS Beamlines PHASE I (Operational) 1. Far Infrared Spectroscopy (Far-IR) - Characterization of IR absorption of simple molecules 2. Mid Infrared Spectromicroscopy (Mid- IR) - Microscopy of biological samples 3. Variable Line Spacing Plane Grating Monochromator (VLS PGM) and 4. High Resolution Spherical Grating Monochromator (SGM) - Understanding chemistry of lighter elements leading to better catalysts, construction materials, fertilizers, etc. 5. Soft X-ray Spectromicroscopy (SM) - Discovering the chemical basis of the structure of materials such as polymers, cells, plants, soil, minerals, and wood 6. Canadian Macromolecular Crystallography Facility (CMCF#1) - Analyzing the structure of proteins and other large biological molecules 7. Hard X-ray MicroAnalysis (HXMA) - X-ray absorption spectroscopy, powder diffraction, micro-probe - Solve issues of toxic elements in enviromental samples
28 Insertion Devices (Phase I) Undulators designed and assembled at CLS VLS-PGM planar undulator: ev SGM planar undulator: ev CMCF SGU: 6 18 kev SM EPU (Apple-II): Planar ev Circular ev HXMA SC 1.94 T Wiggler: 5-40 kev purchased from Budker Institute
29 Brilliance at the CLS
30 Insertion Devices: Chicaned Undulators
31 Double EPU 5-magnet chicane scheme
32 Phase II ( ) 5 CFI approved projects (7 more beamlines) $49 million Includes partial building expansion
33 CLS Beamlines PHASE II (Commissioning) 1. REIX Resonant Elastic and Inelastic X-ray scattering (Second EPU) - Materials science studies with soft x-rays 2. CMCF-2 Protein Crystallography - Bending magnet beamline automated for high-throughput 3. VESPERS - Environmental analysis beamline using x-ray flourescence and diffraction 4. SXRMB - Spectroscopy and x-ray absorption at intermediate energies (2 to 10 kev) 5. SYLMAND - x-ray lithography and LIGA processing 6. and 7. BMIT (ID line has 4.4 Tesla SC wiggler) - Two biomedical beamlines for imaging and therapy studies - Also required building expansion
34 Current Facility Layout
35 Phase III ( ) 3 CFI approved projects (7 more beamlines) $65 million Building expansion Additional $40 million
36 CLS Beamlines PHASE III (Design) 1. BIOXAS (Chicaned PPM wiggler, IVU) - Three beamlines optimized for biological applications of x-ray absorption spectroscopy, especially low-concentration elements 2. QMSC (Double EPU) - Beamline optimized for studying quantum effects in solid state physics - Uses two EPUs to cover a wide energy range (10 ev to ~1.2 kev) 3. BXDS (Chicaned SC wiggler, IVU) - Three beamlines optimized for hard x-ray diffraction and scattering - Primarily solid-state physics and materials studies
37 CLS Future work Phase III beamlines design and construction Includes 4 m long double EPU Building expansion (again!) Near term: CSR for users Single-bunch modes for experiments Fast global orbit feedback, bunch-by-bunch transverse feedback Longer term: Top Up Operation Preliminary radiation measurements have been made and levels are OK Licensing documentation needed however Emphasis on injection with shutters open 500 ma operations Second cavity to be installed New klystron and HV supply
38 The CLS Team
SLS 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 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 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 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 informationEngineering - CLS Day. Thomas Ellis Director of Research Canadian Light Source
Engineering - CLS Day Thomas Ellis Director of Research Canadian Light Source E-gun & Linear Accelerator 250 MeV Canadian Light Source Transfer Line & Booster Ring Commissioned Storage Ring 2.9 GeV 200
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 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 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 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 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 informationLOW EMITTANCE MODEL FOR THE ANKA SYNCHROTRON RADIATION SOURCE
Karlsruhe Institute of Technology (KIT, Karlsruhe, Germany) Budker Institute of Nuclear Physics (BINP, Novosibirsk, Russia) LOW EMITTANCE MODEL FOR THE ANKA SYNCHROTRON RADIATION SOURCE (A.Papash - on
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 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 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 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 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 informationTurn-by-Turn Beam Position Measurements at ANKA with LIBERA ELECTRON
Turn-by-Turn Beam Position Measurements at ANKA with LIBERA ELECTRON E.Huttel, I.Birkel, A.S.Müller, P.Wesolowski About ANKA Test by Frequency Generator Experiences in the Booster Experiences in the Storage
More informationFIRST OPERATION OF THE SWISS LIGHT SOURCE
FIRST OPERATION OF THE SWISS LIGHT SOURCE M. Böge, PSI, Villigen, Switzerland Abstract The Swiss Light Source (SLS) at the Paul Scherrer Institute (PSI) is the most recent 3rd generation light source to
More informationSTATUS REPORT ON STORAGE RING REALIGNMENT AT SLRI
STATUS REPORT ON STORAGE RING REALIGNMENT AT SLRI S. Srichan #, A. Kwankasem, S. Boonsuya, B. Boonwanna, V. Sooksrimuang, P. Klysubun Synchrotron Light Research Institute, 111 University Ave, Muang District,
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 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 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 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 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 informationCOMMISSIONING OF NSLS-II*
COMMISSIONING OF NSLS-II* F. Willeke, BNL, Upton, NY 11973, USA Figure 1: Aerial view of NSLS-II. Abstract NSLS-II, the new 3rd generation light source at BNL was designed for a brightness of 10 22 photons
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 informationLongitudinal Top-up Injection for Small Aperture Storage Rings
Longitudinal Top-up Injection for Small Aperture Storage Rings M. Aiba, M. Böge, Á. Saá Hernández, F. Marcellini and A. Streun Paul Scherrer Institut Introduction Lower and lower horizontal emittances
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 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 informationFirst Collective Effects Measurements in NSLS-II A. Blednykh Accelerator Physicist, BNL/NSLS-II Sep , 2014
First Collective Effects Measurements in NSLS-II A. Blednykh Accelerator Physicist, BNL/NSLS-II Sep. 17-19, 2014 (LOWεRING 2014) 1 BROOKHAVEN SCIENCE ASSOCIATES Outline Phase 1 (25mA / PETRA-III) and Phase
More informationA Project to convert TLS Booster to hadron accelerator 1. Basic design. 2. The injection systems:
A Project to convert TLS Booster to hadron accelerator 1. Basic design TLS is made of a 50 MeV electron linac, a booster from 50 MeV to 1.5 GeV, and a storage ring. The TLS storage ring is currently operating
More informationBoster Synchrotron COMMISSIONING RESULTS LINAC. Storage Ring. Proceedings of IPAC2011, San Sebastián, Spain
Proceedings of IPAC211, San Sebastián, Spain MOXAA1 ALBA SYNCHROTRON LIGHT SOURCE COMMISSIONING D. Einfeld, on behalf of the CELLS - Commissioning Team; CELLS-ALBA, E-829 Cerdanyola del Vallés, Spain,
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 informationSTATUS OF BEPC AND PLAN OF BEPCII
STATUS OF BEPC AND PLAN OF BEPCII C. Zhang for BEPCII Team Institute of High Energy Physics, P.O.Box 918, Beijing 139, China Abstract The status of the Beijing Electron-Positron Collider (BEPC) and plans
More informationFACET-II Design Update
FACET-II Design Update October 17-19, 2016, SLAC National Accelerator Laboratory Glen White FACET-II CD-2/3A Director s Review, August 9, 2016 Planning for FACET-II as a Community Resource FACET-II Photo
More informationMAX-lab. MAX IV Lattice Design: Multibend Achromats for Ultralow Emittance. Simon C. Leemann
Workshop on Low Emittance Rings 2010 CERN Jan 12 15, 2010 MAX-lab MAX IV Lattice Design: Multibend Achromats for Ultralow Emittance Simon C. Leemann simon.leemann@maxlab.lu.se Brief Overview of the MAX
More information1.5-GeV FFAG Accelerator as Injector to the BNL-AGS
1.5-GeV FFAG Accelerator as Injector to the BNL-AGS Alessandro G. Ruggiero M. Blaskiewicz,, T. Roser, D. Trbojevic,, N. Tsoupas,, W. Zhang Oral Contribution to EPAC 04. July 5-9, 5 2004 Present BNL - AGS
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 informationCOMBINER RING LATTICE
CTFF3 TECHNICAL NOTE INFN - LNF, Accelerator Division Frascati, April 4, 21 Note: CTFF3-2 COMBINER RING LATTICE C. Biscari 1. Introduction The 3 rd CLIC test facility, CTF3, is foreseen to check the feasibility
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 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 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 informationSTATUS BESSY II. P. Kuske
STATUS BESSY II P. Kuske Content Introduction: Some Facts about BESSY II On-going Projects: new 50 MeV LINAC Fast Orbit Feedback Top-Up Operation EMIL Modernization Future Projects: BESSY_VSR Other Projects
More informationPlans for CESR (or Life Without CLEO)
CESR-c Plans for CESR (or Life Without CLEO) Mark A. Palmer David L. Rubin Second ILC Accelerator Workshop August 18, 2005 2 Outline CESR-c/CLEO-c Schedule Preliminary Concept Possibilities for CESR as
More informationProposal to convert TLS Booster for hadron accelerator
Proposal to convert TLS Booster for hadron accelerator S.Y. Lee -- Department of Physics IU, Bloomington, IN -- NSRRC Basic design TLS is made of a 50 MeV electron linac, a booster from 50 MeV to 1.5 GeV,
More informationFirst commissioning of the HLS-II storage ring*
Submitted to Chinese Physics C First commissioning of the HLS-II storage ring* LIU Gang-Wen( 刘刚文 ) XUAN Ke( 宣科 ) 1) XU Wei( 徐卫 ) WANG Lin( 王琳 ) LI Wei-Min( 李为民 ) LI Jing-yi( 李京祎 ) National Synchrotron
More information2.6 Electron transport lines
2.6 Electron transport lines 2.6 Electron transport lines Overview The electron transport lines consist of all of the electron beamline segments that are neither part of the Linacs nor part of the injector.
More informationALBA Synchrotron Light Source Commissioning
IPAC-2011: ALBA Commissioning ALBA Synchrotron Light Source Commissioning D. Einfeld, CELLS-ALBA on behalf of the Commissioning Team IPAC-2011: ALBA Commissioning Contents 1.) The project ALBA 2.) Commissioning
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 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 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 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 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 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 informationCOMMISSIONING OF THE MAX IV LIGHT SOURCE
COMMISSIONING OF THE MAX IV LIGHT SOURCE M. Eriksson, E. Al-Dmour, Å. Andersson, M. Johansson, S.C. Leemann, L. Malmgren, P. F. Tavares, S. Thorin, MAX IV Laboratory, Lund University, Lund, Sweden Abstract
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 informationS2E (Start-to-End) Simulations for PAL-FEL. Eun-San Kim
S2E (Start-to-End) Simulations for PAL-FEL Aug. 25 2008 Kyungpook Nat l Univ. Eun-San Kim 1 Contents I Lattice and layout for a 10 GeV linac II Beam parameters and distributions III Pulse-to-pulse stability
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 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 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 informationBESSY Status. Peter Kuske, Helmholtz-Zentrum Berlin, Germany
BESSY Status Peter Kuske, Helmholtz-Zentrum Berlin, Germany XXII European Synchrotron Light Source Workshop, 24 th -25 th November 2014, ESRF, Grenoble, France Content of the Talk I. Statistics II. Challenges
More informationLIS section meeting. PS2 design status. Y. Papaphilippou. April 30 th, 2007
LIS section meeting PS2 design status Y. Papaphilippou April 30 th, 2007 Upgrade of the injector chain (R. Garoby, PAF) Proton flux / Beam power 50 MeV 160 MeV Linac2 Linac4 1.4 GeV ~ 5 GeV PSB SPL RCPSB
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 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 informationX-ray Optics needs for 3 rd and 4 th generation Light Source. Mourad Idir BNL/NSLS II 1 BROOKHAVEN SCIENCE ASSOCIATES
X-ray Optics needs for 3 rd and 4 th generation Light Source Mourad Idir midir@bnl.gov BNL/NSLS II 1 BROOKHAVEN SCIENCE ASSOCIATES OUTLINE 3 rd and 4 th generation Light source Optics needs NSLS II Example
More informationLCLS Accelerator Parameters and Tolerances for Low Charge Operations
LCLS-TN-99-3 May 3, 1999 LCLS Accelerator Parameters and Tolerances for Low Charge Operations P. Emma SLAC 1 Introduction An option to control the X-ray FEL output power of the LCLS [1] by reducing the
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 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 informationILC Damping Ring Alternative Lattice Design (Modified FODO)
ILC Damping Ring Alternative Lattice Design (Modified FODO) Yi-Peng Sun 1,2, Jie Gao 1, Zhi-Yu Guo 2 Wei-Shi Wan 3 1 Institute of High Energy Physics, CAS, China 2 State Key Laboratory of Nuclear Physics
More information6 Bunch Compressor and Transfer to Main Linac
II-159 6 Bunch Compressor and Transfer to Main Linac 6.1 Introduction The equilibrium bunch length in the damping ring (DR) is 6 mm, too long by an order of magnitude for optimum collider performance (σ
More informationHIRFL STATUS AND HIRFL-CSR PROJECT IN LANZHOU
HIRFL STATUS AND HIRFL-CSR PROJECT IN LANZHOU J. W. Xia, Y. F. Wang, Y. N. Rao, Y. J. Yuan, M. T. Song, W. Z. Zhang, P. Yuan, W. Gu, X. T. Yang, X. D. Yang, S. L. Liu, H.W.Zhao, J.Y.Tang, W. L. Zhan, B.
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 informationLattices for Light Sources
Andreas Streun Swiss Light Source SLS, Paul Scherrer Institute, Villigen, Switzerland Contents: Global requirements: size, brightness, stability Lattice building blocks: magnets and other devices Emittance:
More informationLow energy electron storage ring with tunable compaction factor
REVIEW OF SCIENTIFIC INSTRUMENTS 78, 075107 2007 Low energy electron storage ring with tunable compaction factor S. Y. Lee, J. Kolski, Z. Liu, X. Pang, C. Park, W. Tam, and F. Wang Department of Physics,
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 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 informationExperience on Coupling Correction in the ESRF electron storage ring
Experience on Coupling Correction in the ESRF electron storage ring Laurent Farvacque & Andrea Franchi, on behalf of the Accelerator and Source Division Future Light Source workshop 2012 Jefferson Lab,
More informationThe MAX IV Thermionic preinjector
The MAX IV Thermionic preinjector David Olsson ESLS RF, Lund, 2015-09-30 Injection Requirements I Full-energy injection from the LINAC 1.5 GeV and 3 GeV extraction points. Both storage rings will be operated
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 informationOperational Experience with HERA
PAC 07, Albuquerque, NM, June 27, 2007 Operational Experience with HERA Joachim Keil / DESY On behalf of the HERA team Contents Introduction HERA II Luminosity Production Experiences with HERA Persistent
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 informationSimulations and design for soft X-ray beamlines at MAX IV. Rami Sankari
Simulations and design for soft X-ray beamlines at MAX IV Rami Sankari Software for Optical Simulations, Workshop Trieste, 3-7 October 2016 Outline MAX IV Laboratory Description of the beamlines Needs
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 informationOverview of Acceleration
Overview of Acceleration R B Palmer, Scott Berg, Steve Kahn (presented by Steve Kahn) Nufact-04 RF Frequency Acc types and System Studies Linacs RLA s FFAG s Injection/Extraction US Study 2a acceleration
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 informationFACET-II Design, Parameters and Capabilities
FACET-II Design, Parameters and Capabilities 217 FACET-II Science Workshop, October 17-2, 217 Glen White Overview Machine design overview Electron systems Injector, Linac & Bunch compressors, Sector 2
More informationCOMMISSIONING AND STATUS OF THE DIAMOND STORAGE RING
COMMISSIONING AND STATUS OF THE DIAMOND STORAGE RING R.P. Walker, Diamond Light Source (DLS), Oxfordshire, U.K., on behalf of the Diamond Machine Commissioning Team Abstract The commissioning of the Diamond
More informationDesign Status of the PEFP RCS
Design Status of the PEFP RCS HB2010, Morschach, Switzerland J.H. Jang 1) Y.S. Cho 1), H.S. Kim 1), H.J. Kwon 1), Y.Y. Lee 2) 1) PEFP/KAERI, 2) BNL (www.komac.re.kr) Contents PEFP (proton engineering frontier
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 informationLow alpha mode for SPEAR3 and a potential THz beamline
Low alpha mode for SPEAR3 and a potential THz beamline X. Huang For the SSRL Accelerator Team 3/4/00 Future Light Source Workshop 00 --- X. Huang Outline The low-alpha mode for SPEAR3 Potential for a THz
More informationSynchrotron Methods in Nanomaterials Research
Synchrotron Methods in Nanomaterials Research Marcel MiGLiERiNi Slovak University of Technology in Bratislava and Centre for Nanomaterials Research, Olomouc marcel.miglierini@stuba.sk www.nuc.elf.stuba.sk/bruno
More informationCoherent Synchrotron Radiation and Short Bunches in Electron Storage Rings. G. Wüstefeld, BESSY, Berlin (Germany)
Coherent Synchrotron Radiation and Short Bunches in Electron Storage Rings G. Wüstefeld, BESSY, Berlin (Germany) Content content 1. Introduction 2. Low alpha optics for short bunches 3. Coherent radiation
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 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 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 informationCritical R&D Issues for ILC Damping Rings and New Test Facilities
Critical R&D Issues for ILC Damping Rings and New Test Facilities Andy Wolski Cockcroft Institute/University of Liverpool PAC 2007, Albuquerque, New Mexico. 1 ILC Key Parameters Given the main linac parameters:
More informationIntroduction to Accelerators Part 1
Introduction to Accelerators Part 1 Director, ASTeC Daresbury Campus Cockcroft Institute Basic Acceleration Principle A voltage drop accelerates charged particles Electrostatic acceleration in cathode
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 informationILC Damping Ring Alternative Lattice Design **
ILC Damping Ring Alternative Lattice Design ** Yi-Peng Sun *,1,2, Jie Gao 1, Zhi-Yu Guo 2 1 Institute of High Energy Physics, CAS, Beijing 2 Key Laboratory of Heavy Ion Physics, Peking University, Beijing
More information3.2 The MAX IV 3 GeV Storage Ring
25 38. S. Liuzzo et al. Test of Low emittance tuning at Diamond, Proceedings of the IPAC11, 2031, (2011). 39. L. Nadolski, Methods and tools to simulate and analyse nonlinear beam dynamics in electron
More information