Maurizio Vretenar Linac4 Project Leader EuCARD-2 Coordinator
|
|
- Arline Evans
- 5 years ago
- Views:
Transcription
1 Maurizio Vretenar Linac4 Project Leader EuCARD-2 Coordinator
2 Every accelerator needs a linac as injector to pass the region where the velocity of the particles increases with energy. At high energies (relativity) the velocity saturates at the speed of light and it is less expensive to use circular accelerators. In addition, linear accelerators for electrons are used up to very high energy because in a linear path particles do not lose energy for synchrotron radiation. linacs Linac2 (50 MeV) PS Booster (1.4 GeV) PS (25 GeV) SPS (450 GeV) LHC Stand-alone linacs are low-energy accelerators with many applications in medecine and industry (more than linacs in the world mainly for X-ray therapy) The LHC Injection chain 2
3 A linear accelerator is required as injector to any accelerator chain to cover the range where particle velocity increases with energy. At high energy where b ~ const. a synchrotron is economically more convenient. accelerating gaps d d=bl/2=variable d d bc 2 f bl 2 accelerating gap d=2pr=constant Linear accelerator: Circular accelerator: Particles accelerated by a sequence of gaps (all at the same RF phase). Distance between gaps increases proportionally to the particle velocity, to keep synchronicity. Used in the range where b increases. Newton machine Particles accelerated by one (or more) gaps at given positions in the ring. Distance between gaps is fixed. Synchronicity only for b~const, or varying (in a limited range!) the RF frequency. Used in the range where b is nearly constant. Einstein machine
4 100m One of the options for the future of CERN after the LHC: Compact LInear Collider Study supported by a large international collaboration for a 3 TeV electron collider of 48 km length Advanced R&D phase: 12 GHz, 100 MV/m Normal-conducting e+ INJECTION DESCENT TUNNEL e- INJECTION DESCENT TUNNEL COMBINER RINGS DRIVE BEAM INJECTOR BYPASS TUNNEL DRIVE BEAM LOOPS DAMPING RINGS INTERACTION REGION MAIN BEAM INJECTOR 1km DRIVE BEAM DUMPS TURN AROUND Limestones Moraines Molasse Sands and gravels INJECTION TUNNEL CLIC SCHEMATIC (not to scale) e- SIDE LHC e+ SIDE 4 FRANCE SWITZERLAND
5 In final construction phase 160 MeV proton (H-) linac, 100 m Will contribute to increasing the number of protons in the LHC Visit this afternoon at 16:00 No superconductivity (not economically justified in this range of b and duty cycles); Single RF frequency 352 MHz PIMS CCDTL Energy [MeV] DTL Length [m] RFQ DTL CCDTL PIMS chopper line RF Power [MW] RFQ 160 MeV 104 MeV 50 MeV 3 MeV 86 m 5
6 Main oscillator RF feedback system HV AC/DC power converter High power RF amplifier (tube or klystron) AC to DC conversion efficiency ~90% DC to RF conversion efficiency ~50% RF to beam voltage conversion efficiency particle beam, energy W particle beam, energy W+DW magnet powering system vacuum system water cooling system LINAC STRUCTURE accelerating gaps + focusing magnets designed for a given ion, energy range, energy gain Goal: high accelerating gradients (e-field), high frequency Technological challenges: 1. High precision machining and joining of copper parts 2. High-efficiency generation of high Radio-Frequency power
7 Mechanics (Copper!) 1. High RF frequencies small structures, more compact and with higher power efficiency tighter tolerances to achieve the required precision in the electric field (field error ~ tolerances / wavelength) few microns 2. Joining the parts: excellent RF conductance, good vacuum, keep tolerances. Radio-Frequency: 1. Generation of peak power of >100 kw (but for low duty cycle, usually <5%) at frequencies in the range 350 MHz (Linac4) 12 GHz (CLIC). 2. Achieve DC to RF conversion efficiency > 60%. 7
8 TD26 CC SiC Assembly - Diffusion bonding of high precision disk at about 1035 C - Vacuum brazing of bonded disk stack, assembled cooling blocks, couplers, beam pipes and tuning studs at about 1020 C - TIG welding of vacuum flanges
9
10 PIMS (PI-Mode Structure) 12 RF cavities of length 1.5m Tolerances ~ 10 mm Built in collaboration with Poland RFQ (Radio-Frequency Quadrupole) 3 meter length, Tolerances ~ 5 mm Built at CERN
11 Tolerances: ±10 µm for the cavity and ±5 µm for the electrodes
12 - High powers (>100 kw) are produced with klystrons, only 3 companies on the market worldwide. Space for companies producing lower power (<100 kw) solidstate units and associated components (couplers, loads, specialised connectors, etc.). New high-power transistors can open new perspectives bringing the cost/w down
13 Under developement within the new CERN program for medical applications Mini-RFQ at 750 MHz 4 Solid-state RF amplifiers, 100 kw each Compact light-weight system for production of radioisotopes in hospitals: single doses of 18F for PET tomography, short-living isotopes for new imaging techniques. Made of 2 RFQs in cascade reaching 8 MeV energy in a length of 3.2 m. Peak current 1 ma, duty cycle 5%, average current 50 ma. Small size, minimum weight, minimum shielding, high reliability, low electricity consumption in operation and in stand-by.
200 MHz 350 MHz 750 MHz Linac2 RFQ2 202 MHz 0.5 MeV /m Weight : 1000 kg/m Ext. diameter : 45 cm
M. Vretenar, CERN for the HF-RFQ Working Group (V.A. Dimov, M. Garlasché, A. Grudiev, B. Koubek, A.M. Lombardi, S. Mathot, D. Mazur, E. Montesinos, M. Timmins, M. Vretenar) 1 1988-92 Linac2 RFQ2 202 MHz
More informationThe European Spallation Source. Dave McGinnis Chief Engineer ESS\Accelerator Division IVEC 2013
The European Spallation Source Dave McGinnis Chief Engineer ESS\Accelerator Division IVEC 2013 Overview The European Spallation Source (ESS) will house the most powerful proton linac ever built. The average
More informationJUAS 2018 LINACS. Jean-Baptiste Lallement, Veliko Dimov BE/ABP CERN.
LINACS Jean-Baptiste Lallement, Veliko Dimov BE/ABP CERN jean-baptiste.lallement@cern.ch http://jlalleme.web.cern.ch/jlalleme/juas2018/ Credits Much material is taken from: Thomas Wangler, RF linear accelerators
More informationTHE CRYOGENIC SYSTEM OF TESLA
THE CRYOGENIC SYSTEM OF TESLA S. Wolff, DESY, Notkestr. 85, 22607 Hamburg, Germany for the TESLA collaboration Abstract TESLA, a 33 km long 500 GeV centre-of-mass energy superconducting linear collider
More informationHerwig Schopper CERN 1211 Geneva 23, Switzerland. Introduction
THE LEP PROJECT - STATUS REPORT Herwig Schopper CERN 1211 Geneva 23, Switzerland Introduction LEP is an e + e - collider ring designed and optimized for 2 100 GeV. In an initial phase an energy of 2 55
More informationLow-beta Structures. Maurizio Vretenar CERN BE/RF CAS RF Ebeltoft 2010
Low-beta Structures Maurizio Vretenar CERN BE/RF CAS RF Ebeltoft. Low-beta: problems and solutions. Coupled-cell accelerating structures 3. Overview and comparison of low-beta structures 4. The Radio Frequency
More informationDEVELOPMENT OF CAPACITIVE LINEAR-CUT BEAM POSITION MONITOR FOR HEAVY-ION SYNCHROTRON OF KHIMA PROJECT
DEVELOPMENT OF CAPACITIVE LINEAR-CUT BEAM POSITION MONITOR FOR HEAVY-ION SYNCHROTRON OF KHIMA PROJECT Ji-Gwang Hwang, Tae-Keun Yang, Seon Yeong Noh Korea Institute of Radiological and Medical Sciences,
More informationPresent and future beams for SHE research at GSI W. Barth, GSI - Darmstadt
Present and future beams for SHE research at GSI W. Barth, GSI - Darmstadt 1. Heavy Ion Linear Accelerator UNILAC 2. GSI Accelerator Facility Injector for FAIR 3. Status Quo of the UNILAC-performance 4.
More informationRe-commissioning the Recycler Storage Ring at Fermilab
Re-commissioning the Recycler Storage Ring at Fermilab Martin Murphy, Fermilab Presented August 10, 2012 at SLAC National Laboratory for the Workshop on Accelerator Operations The Fermi National Accelerator
More informationDESIGN AND BEAM DYNAMICS STUDIES OF A MULTI-ION LINAC INJECTOR FOR THE JLEIC ION COMPLEX
DESIGN AND BEAM DYNAMICS STUDIES OF A MULTI-ION LINAC INJECTOR FOR THE JLEIC ION COMPLEX Speaker: P.N. Ostroumov Contributors: A. Plastun, B. Mustapha and Z. Conway HB2016, July 7, 2016, Malmö, Sweden
More informationThe Superconducting Radio Frequency Quadrupole Structures Review
The Superconducting Radio Frequency Quadrupole Structures Review Augusto Lombardi INFN- Laboratori Nazionali di Legnaro, via Romea 4 I-35020 Legnaro (PD) Abstract Since 1985 the idea of using the fast
More informationThe ILC Accelerator Complex
The ILC Accelerator Complex Nick Walker DESY/GDE UK LC meeting 3 rd September 2013 Oxford University, UK. 1 ILC in a Nutshell 200-500 GeV E cm e + e - collider L ~2 10 34 cm -2 s -1 upgrade: ~1 TeV central
More information3 General layout of the XFEL Facility
3 General layout of the XFEL Facility 3.1 Introduction The present chapter provides an overview of the whole European X-Ray Free-Electron Laser (XFEL) Facility layout, enumerating its main components and
More informationPhilippe Lebrun & Laurent Tavian, CERN
7-11 July 2014 ICEC25 /ICMC 2014 Conference University of Twente, The Netherlands Philippe Lebrun & Laurent Tavian, CERN Ph. Lebrun & L. Tavian, ICEC25 Page 1 Contents Introduction: the European Strategy
More informationInternational Technology Recommendation Panel. X-Band Linear Collider Path to the Future. RF System Overview. Chris Adolphsen
International Technology Recommendation Panel X-Band Linear Collider Path to the Future RF System Overview Chris Adolphsen Stanford Linear Accelerator Center April 26-27, 2004 Delivering the Beam Energy
More informationNormal-conducting high-gradient rf systems
Normal-conducting high-gradient rf systems Introduction Motivation for high gradient Order of 100 GeV/km Operational and state-of-the-art SwissFEL C-band linac: Just under 30 MV/m CLIC prototypes: Over
More informationDemonstration of exponential growth and saturation at VUV wavelengths at the TESLA Test Facility Free-Electron Laser. P. Castro for the TTF-FEL team
Demonstration of exponential growth and saturation at VUV wavelengths at the TESLA Test Facility Free-Electron Laser P. Castro for the TTF-FEL team 100 nm 1 Å FEL radiation TESLA Test Facility at DESY
More informationX-Band Linear Collider Report*
SLAC DOE Program Review X-Band Linear Collider Path to the Future X-Band Linear Collider Report* D. L. Burke NLC Program Director * Abstracted from recent presentations to the International Technical Recommendation
More informationPhysics Requirements Document Document Title: SCRF 1.3 GHz Cryomodule Document Number: LCLSII-4.1-PR-0146-R0 Page 1 of 7
Document Number: LCLSII-4.1-PR-0146-R0 Page 1 of 7 Document Approval: Originator: Tor Raubenheimer, Physics Support Lead Date Approved Approver: Marc Ross, Cryogenic System Manager Approver: Jose Chan,
More informationACCELERATOR PHYSICS OF HIGH INTENSITY PROTON LINACS
ACCELERATOR PHYSICS OF HIGH INTENSITY PROTON LINACS K. Bongardt and M. Pabst, Forschungszentrum Jülich GmbH, 52425 Jülich, Germany Abstract The accelerator physics of high intensity linacs, either pulsed
More informationFabrication Techniques for the X-band Accelerator Structures. Juwen Wang WORKSHOP ON X-BAND RF TECHNOLOGY FOR FELs March 5, 2010
Fabrication Techniques for the X-band Accelerator Structures Juwen Wang WORKSHOP ON X-BAND RF TECHNOLOGY FOR FELs March 5, 2010 Outline 1. Introduction Brief history Achievements 2. Basics of X-Band Accelerator
More informationProposal of test setup
Proposal of test setup Status of the study The Compact Linear collider (CLIC) study is a site independent feasibility study aiming at the development of a realistic technology at an affordable cost for
More informationNiowave s Growth and the Role of STTR in its Development
Niowave s Growth and the Role of STTR in its Development Terry L. Grimm Niowave, Inc. Lansing MI Presented at National Academies STTR Workshop, Wash DC, May 2015 Outline Superconducting electron linacs
More informationLinear Particle Accelerator Control Performance
Linear Particle Accelerator Control Performance 2007 ExpertTune-TiPS Conference April 17-19, 2007 Austin, TX Johnny Tang Overview of the Spallation Neutron Source Accelerator J. Tang 2 Overview of the
More informationRF Cavity Design. Erk Jensen CERN BE/RF. CERN Accelerator School Accelerator Physics (Intermediate level) Darmstadt 2009
RF Cavity Design Erk Jensen CERN BE/RF CERN Accelerator School Accelerator Physics (Intermediate level) Darmstadt 009 CAS Darmstadt '09 RF Cavity Design 1 Overview DC versus RF Basic equations: Lorentz
More informationStrategy for the engineering integration of the ESS accelerator
Applications of Nuclear Techniques (CRETE15) International Journal of Modern Physics: Conference Series Vol. 44 (2016) 1660208 (7 pages) The Author(s) DOI: 10.1142/S2010194516602088 Nikolaos Gazis nick.gazis@esss.se
More informationPackaging of Cryogenic Components
Packaging of Cryogenic Components William J. Schneider Senior Mechanical Engineer Emeritus November 19-23 2007 1 Packaging of Cryogenic Components Day one Introduction and Overview 2 What is important?
More informationUsing Higher Order Modes in the Superconducting TESLA Cavities for Diagnostics at DESY
Using Higher Order Modes in the Superconducting TESLA Cavities for Diagnostics at FLASH @ DESY N. Baboi, DESY, Hamburg for the HOM team : S. Molloy 1, N. Baboi 2, N. Eddy 3, J. Frisch 1, L. Hendrickson
More informationREVIEW OF FAST BEAM CHOPPING F. Caspers CERN AB-RF-FB
F. Caspers CERN AB-RF-FB Introduction Review of several fast chopping systems ESS-RAL LANL-SNS JAERI CERN-SPL Discussion Conclusion 1 Introduction Beam choppers are typically used for β = v/c values between
More informationSRF Advances for ATLAS and Other β<1 Applications
SRF Advances for ATLAS and Other β
More informationXFEL Cryo System. Project X Collaboration Meeting, FNAL September 8-9, 2010 Bernd Petersen DESY MKS (XFEL WP10 & WP13) 1 st stage. Possible extension
XFEL Cryo System Possible extension 1 st stage Project X Collaboration Meeting, FNAL September 8-9, 2010 (XFEL WP10 & WP13) Outline 2 XFEL accelerator structure TESLA technology Basic cryogenic parameters
More informationDevelopment of a 20-MeV Dielectric-Loaded Accelerator Test Facility
SLAC-PUB-11299 Development of a 20-MeV Dielectric-Loaded Accelerator Test Facility S.H. Gold, et al. Contributed to 11th Advanced Accelerator Concepts Workshop (AAC 2004), 06/21/2004--6/26/2004, Stony
More informationREVIEW ON SUPERCONDUCTING RF GUNS
REVIEW ON SUPERCONDUCTING RF GUNS D. Janssen #, A. Arnold, H. Büttig, U. Lehnert, P. Michel, P. Murcek, C. Schneider, R. Schurig, F. Staufenbiel, J. Teichert, R. Xiang, Forschungszentrum Rossendorf, Germany.
More informationGrounding for EMC at the European XFEL
Grounding for EMC at the European XFEL Herbert Kapitza, Hans-Jörg Eckoldt, Markus Faesing Deutsches Elektronensynchrotron (DESY) D-22603 Hamburg, Germany Email: herbert.kapitza@desy.de Abstract The European
More informationThe impedance budget of the CERN Proton Synchrotron (PS)
The impedance budget of the CERN Proton Synchrotron (PS) Serena Persichelli CERN Hadron Synchrotron Collective effects University of Rome La Sapienza serena.persichelli@cern.ch Why do we study the beam
More information2008 JINST 3 S The RF systems and beam feedback. Chapter Introduction
Chapter 4 The RF systems and beam feedback 4.1 Introduction The injected beam will be captured, accelerated and stored using a 400 MHz superconducting cavity system, and the longitudinal injection errors
More information1997 Particle Accelerator Conference, Vancouver, B.C., Canada, May 12-16, 1997 BNL
t J 1997 Particle Accelerator Conference, Vancouver, B.C., Canada, May 12-16, 1997 BNL-6 4 3 5 5 Modifying CERN SPS Cavities and Amplifiers for Use in RHIC R. Connolly, J. Aspenleiter, S. Kwiatkowski Brookhaven
More informationAdvance on High Power Couplers for SC Accelerators
Advance on High Power Couplers for SC Accelerators Eiji Kako (KEK, Japan) IAS conference at Hong Kong for High Energy Physics, 2017, January 23th Eiji KAKO (KEK, Japan) IAS at Hong Kong, 2017 Jan. 23 1
More informationAccelerator Complex U70 of IHEP-Protvino: Status and Upgrade Plans
INSTITUTE FOR HIGH ENERGY PHYSICS () Protvino, Moscow Region, 142281, Russia Accelerator Complex U70 of -Protvino: Status and Upgrade Plans (report 4.1-1) Sergey Ivanov, on behalf of the U70 staff September
More informationCrab Cavities for FCC
Crab Cavities for FCC R. Calaga, A. Grudiev, CERN FCC Week 2017, May 30, 2017 Acknowledgements: O. Bruning, E. Cruz-Alaniz, K. Ohmi, R. Martin, R. Tomas, F. Zimmermann Livingston Plot 100 TeV FCC-hh: 0.5-3x1035
More informationEngineering Challenges and Solutions for MeRHIC. Andrew Burrill for the MeRHIC Team
Engineering Challenges and Solutions for MeRHIC Andrew Burrill for the MeRHIC Team Key Components Photoinjector Design Photocathodes & Drive Laser Linac Cavities 703.75 MHz 5 cell cavities 3 rd Harmonic
More informationBeam Loss Monitoring (BLM) System for ESS
Beam Loss Monitoring (BLM) System for ESS Lali Tchelidze European Spallation Source ESS AB lali.tchelidze@esss.se March 2, 2011 Outline 1. BLM Types; 2. BLM Positioning and Calibration; 3. BLMs as part
More informationA few results [2,3] obtained with the individual cavities inside their horizontal cryostats are summarized in Table I and a typical Q o
Particle Accelerators, 1990, Vol. 29, pp. 47-52 Reprints available directly from the publisher Photocopying permitted by license only 1990 Gordon and Breach, Science Publishers, Inc. Printed in the United
More informationCalibrating the Cavity Voltage. Presentation of an idea
Calibrating the Cavity Voltage. Presentation of an idea Stefan Wilke, DESY MHF-e 21st ESLS rf meeting Kraków, 15th/16th nov 2017 Accelerators at DESY. linear and circular Page 2 Accelerators at DESY. linear
More informationAttosecond Diagnostics of Muti GeV Electron Beams Using W Band Deflectors
Attosecond Diagnostics of Muti GeV Electron Beams Using W Band Deflectors V.A. Dolgashev, P. Emma, M. Dal Forno, A. Novokhatski, S. Weathersby SLAC National Accelerator Laboratory FEIS 2: Femtosecond Electron
More informationFLASH at DESY. FLASH. Free-Electron Laser in Hamburg. The first soft X-ray FEL operating two undulator beamlines simultaneously
FLASH at DESY The first soft X-ray FEL operating two undulator beamlines simultaneously Katja Honkavaara, DESY for the FLASH team FEL Conference 2014, Basel 25-29 August, 2014 First Lasing FLASH2 > First
More informationThird Harmonic Superconducting passive cavities in ELETTRA and SLS
RF superconductivity application to synchrotron radiation light sources Third Harmonic Superconducting passive cavities in ELETTRA and SLS 2 cryomodules (one per machine) with 2 Nb/Cu cavities at 1.5 GHz
More informationDEVELOPMENT OF QUARTER-WAVE CAVITIES AND FUTURE PROSPECTS FOR SUPERCONDUCTING CAVITIES
EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH ORGANISATION EUROPÉENNE POUR LA RECHERCHE NUCLÉAIRE CERN - TS Department EDMS Nr: 936524 TS-Note-2008-008 Group reference: TS-MME 27 May 2008 DEVELOPMENT OF QUARTER-WAVE
More informationCEBAF Overview June 4, 2010
CEBAF Overview June 4, 2010 Yan Wang Deputy Group Leader of the Operations Group Outline CEBAF Timeline Machine Overview Injector Linear Accelerators Recirculation Arcs Extraction Systems Beam Specifications
More information(CPHS monthly) HATC UCANS KEK UCANS 8
(CPHS monthly) HATC 2010 3 (,,) 1.1 Monthly highlights 1. The June 2009 International Mini-Workshop at Tsinghua not only kicked off the CPHS Project but also fermented the notion of cooperation among compact-neutron-source
More informationTutorial on Design of RF system for Indus Accelerator. Maherdra Lad Head, Radio Frequency Systems Division RRCAT, Indore
Tutorial on Design of RF system for Indus Accelerator Maherdra Lad Head, Radio Frequency Systems Division RRCAT, Indore Basic principle of RF Acceleration RF Power Amplifier The RF source supplies power
More informationRF STATUS OF SUPERCONDUCTING MODULE DEVELOPMENT SUITABLE FOR CW OPERATION: ELBE CRYOSTATS
RF STATUS OF SUPERCONDUCTING MODULE DEVELOPMENT SUITABLE FOR CW OPERATION: ELBE CRYOSTATS J. Teichert, A. Büchner, H. Büttig, F. Gabriel, P. Michel, K. Möller, U. Lehnert, Ch. Schneider, J. Stephan, A.
More informationCrab Cavity Systems for Future Colliders. Silvia Verdú-Andrés, Ilan Ben-Zvi, Qiong Wu (Brookhaven National Lab), Rama Calaga (CERN)
International Particle Accelerator Conference Copenhagen (Denmark) 14-19 May, 2017 Crab Cavity Systems for Future Colliders Silvia Verdú-Andrés, Ilan Ben-Zvi, Qiong Wu (Brookhaven National Lab), Rama Calaga
More informationDevelopment of Superconducting CH-Cavities for the EUROTRANS and IFMIF Project 1
1 AT/P5-01-POSTER Development of Superconducting CH-Cavities for the EUROTRANS and IFMIF Project 1 F. Dziuba 2, H. Podlech 2, M. Buh 2, U. Ratzinger 2, A. Bechtold 3, H. Klein 2 2 Institute for Applied
More informationFAST RF KICKER DESIGN
FAST RF KICKER DESIGN David Alesini LNF-INFN, Frascati, Rome, Italy ICFA Mini-Workshop on Deflecting/Crabbing Cavity Applications in Accelerators, Shanghai, April 23-25, 2008 FAST STRIPLINE INJECTION KICKERS
More informationAPAC 2007, Raja Ramanna Centre for Advanced Technology(RRCAT), Indore, India LHC STATUS. Lyndon Evans, CERN, Geneva, Switzerland
LHC STATUS Lyndon Evans, CERN, Geneva, Switzerland Abstract The installation of the Large Hadron Collider at CERN is now approaching completion. Almost 1100 of the 1232 main bending magnets are installed
More informationTechnology Transfer at CERN
Technology Transfer at CERN Enrico Chesta Head of CERN Technology Transfer and Intellectual Property Management Section Knowledge Transfer Group, FP Department How can CERN have an impact beyond fundamental
More informationCLIC Compact Linear Collider
f1 CLIC Compact LInear Collider Frank Zimmermann for the CLIC Study Team many CLIC contributors! special thanks to Hans Braun, Jean-Pierre Delahaye, & Frank Tecker! Frank Zimmermann UPHUK3 2007, Bodrumr,
More information1.5 GHz Cavity design for the Clic Damping Ring and as Active Third Harmonic cavity for ALBA.
1 1.5 GHz Cavity design for the Clic Damping Ring and as Active Third Harmonic cavity for ALBA. Beatriz Bravo Overview 2 1.Introduction 2.Active operation 3.Electromagnetic design 4.Mechanical design Introduction
More informationHIGH POWER INPUT COUPLERS FOR THE STF BASELINE CAVITY SYSTEM AT KEK
HIGH POWER INPUT COUPLERS FOR THE STF BASELINE CAVITY SYSTEM AT KEK E. Kako #, H. Hayano, S. Noguchi, T. Shishido, K. Watanabe and Y. Yamamoto KEK, Tsukuba, Ibaraki, 305-0801, Japan Abstract An input coupler,
More informationDEVELOPMENT OF A BETA 0.12, 88 MHZ, QUARTER WAVE RESONATOR AND ITS CRYOMODULE FOR THE SPIRAL2 PROJECT
DEVELOPMENT OF A BETA 0.12, 88 MHZ, QUARTER WAVE RESONATOR AND ITS CRYOMODULE FOR THE SPIRAL2 PROJECT G. Olry, J-L. Biarrotte, S. Blivet, S. Bousson, C. Commeaux, C. Joly, T. Junquera, J. Lesrel, E. Roy,
More informationMEASUREMENT OF BEAM LOSSES USING OPTICAL FIBRES AT THE AUSTRALIAN SYNCHROTRON
MEASUREMENT OF BEAM LOSSES USING OPTICAL FIBRES AT THE AUSTRALIAN SYNCHROTRON E. Nebot del Busto (1,2), M. J. Boland (3,4), E. B. Holzer (1), P. D. Jackson (5), M. Kastriotou (1,2), R. P. Rasool (4), J.
More informationSRF FOR FUTURE CIRCULAR COLLIDERS
FRBA4 Proceedings of SRF215, Whistler, BC, Canada SRF FOR FUTURE CIRCULAR COLLIDERS A. Butterworth, O. Brunner, R. Calaga,E.Jensen CERN, Geneva, Switzerland Copyright 215 CC-BY-3. and by the respective
More informationCompact Radio Frequency Technology for Applications in Cargo and Global
Compact Radio Frequency Technology for Applications in Cargo and Global Security Peter McIntosh STFC Daresbury Laboratory CLASP Security Event Tuesday 5 th July 2011, London Compact RF Technologies S-band
More informationThe Current Cyclotron Development Activities at CIAE. Current acyclotron
Current Cyclotron Development Activities Shizhong An, Tianjue Zhang China Institute of Atomic Energy (CIAE) Beijing 2010-11.22 Greatful acknowledged is very fruitful and long lasting collaboration with
More informationLC Technology Hans Weise / DESY
LC Technology Hans Weise / DESY All you need is... Luminosity! L σ 2 N e x σ y σ y σ x L n b f rep Re-writing reflects the LC choices... L P E b c. m. N e σ σ x y... beam power... bunch population... Ac-to-beam
More informationBehavior of the TTF2 RF Gun with long pulses and high repetition rates
Behavior of the TTF2 RF Gun with long pulses and high repetition rates J. Baehr 1, I. Bohnet 1, J.-P. Carneiro 2, K. Floettmann 2, J. H. Han 1, M. v. Hartrott 3, M. Krasilnikov 1, O. Krebs 2, D. Lipka
More informationProgress in High Gradient Accelerator Research at MIT
Progress in High Gradient Accelerator Research at MIT Presented by Richard Temkin MIT Physics and Plasma Science and Fusion Center May 23, 2007 MIT Accelerator Research Collaborators MIT Plasma Science
More informationH. Weise, Deutsches Elektronen-Synchrotron, Hamburg, Germany for the XFEL Group
7+(7(6/$;)(/352-(&7 H. Weise, Deutsches Elektronen-Synchrotron, Hamburg, Germany for the XFEL Group $EVWUDFW The overall layout of the X-Ray FEL to be built in international collaboration at DESY will
More informationDQW HOM Coupler for LHC
DQW HOM Coupler for LHC J. A. Mitchell 1, 2 1 Engineering Department Lancaster University 2 BE-RF-BR Section CERN 03/07/2017 J. A. Mitchell (PhD Student) HL LHC UK Jul 17 03/07/2017 1 / 27 Outline 1 LHC
More informationSuperstructures; First Cold Test and Future Applications
Superstructures; First Cold Test and Future Applications DESY: C. Albrecht, V. Ayvazyan, R. Bandelmann, T. Büttner, P. Castro, S. Choroba, J. Eschke, B. Faatz, A. Gössel, K. Honkavaara, B. Horst, J. Iversen,
More informationNew Tracking Gantry-Synchrotron Idea. G H Rees, ASTeC, RAL, U.K,
New Tracking Gantry-Synchrotron Idea G H Rees, ASTeC, RAL, U.K, Scheme makes use of the following: simple synchrotron and gantry magnet lattices series connection of magnets for 5 Hz tracking one main
More informationSwissFEL Design and Status
SwissFEL Design and Status Hans H. Braun Mini Workshop on Compact X ray Free electron Lasers Eastern Forum of Science and Technology Shanghai July 19, 2010 SwissFEL, the next large facility at PSI SwissFEL
More informationALICE SRF SYSTEM COMMISSIONING EXPERIENCE A. Wheelhouse ASTeC, STFC Daresbury Laboratory
ALICE SRF SYSTEM COMMISSIONING EXPERIENCE A. Wheelhouse ASTeC, STFC Daresbury Laboratory ERL 09 8 th 12 th June 2009 ALICE Accelerators and Lasers In Combined Experiments Brief Description ALICE Superconducting
More informationCEBAF waveguide absorbers. R. Rimmer for JLab SRF Institute
CEBAF waveguide absorbers R. Rimmer for JLab SRF Institute Outline Original CEBAF HOM absorbers Modified CEBAF loads for FEL New materials for replacement loads High power loads for next generation FELs
More informationEmilia Cruz. September 21, 2015
Designing the interaction regions of the upgrades of the LHC Emilia Cruz September 21, 2015 7/7/2016 1 About me Guadalajara, Mexico 7/7/2016 2 About me Bachelors degree: National Autonomous University
More informationOverview of ERL Projects: SRF Issues and Challenges. Matthias Liepe Cornell University
Overview of ERL Projects: SRF Issues and Challenges Matthias Liepe Cornell University Overview of ERL projects: SRF issues and challenges Slide 1 Outline Introduction: SRF for ERLs What makes it special
More informationLHC TRANSVERSE FEEDBACK SYSTEM: FIRST RESULTS OF COMMISSIONING. V.M. Zhabitsky XXI Russian Particle Accelerator Conference
LHC TRANSVERSE FEEDBACK SYSTEM: FIRST RESULTS OF COMMISSIONING V.M. Zhabitsky XXI Russian Particle Accelerator Conference 28.09-03.10.2008, Zvenigorod LHC Transverse Feedback System: First Results of Commissioning
More informationINTRODUCTION TO RADIOFREQUENCY SYSTEMS FOR PARTICLE ACCELERATORS
INTRODUCTION TO RADIOFREQUENCY SYSTEMS FOR PARTICLE ACCELERATORS Elettra-Sincrotrone Trieste S.C.p.A, Italy 39 th International Nathiagali Summer College 4 th 9 th August 2014 2 OVERVIEW Introduction Building
More information5.2.3 DecayChannelSolenoids BeamDynamics Induction Linac Approach
Chapter 5 MUON PHASE ROTATION CHANNEL Contents 5.1 Introduction... 207 5.2 rfapproach... 208 5.2.1 Introduction... 208 5.2.2 rfcavities... 209 5.2.3 DecayChannelSolenoids... 212 5.2.4 BeamDynamics... 218
More informationDrive Beam Photo-injector Option for the CTF3 Nominal Phase
CTF3 Review Drive Beam Photo-injector Option for the CTF3 Nominal Phase Motivation CTF3 Drive Beam Requirements CTF3 RF gun design The Laser (I. Ross / RAL) The Photocathode Cost estimate Possible schedule
More informationC100 Cryomodule. Seven cell Cavity, 0.7 m long (high Q L ) 8 Cavities per Cryomodule Fits the existing Cryomodule footprint
1 new module C100 Cryomodule Seven cell Cavity, 0.7 m long (high Q L ) 8 Cavities per Cryomodule Fits the existing Cryomodule footprint Fundamental frequency f 0 Accelerating gradient E acc 1497 MHz >
More informationDesign of ESS-Bilbao RFQ Linear Accelerator
Design of ESS-Bilbao RFQ Linear Accelerator J.L. Muñoz 1*, D. de Cos 1, I. Madariaga 1 and I. Bustinduy 1 1 ESS-Bilbao *Corresponding author: Ugaldeguren III, Polígono A - 7 B, 48170 Zamudio SPAIN, jlmunoz@essbilbao.org
More informationPower Converters for Accelerators. CERN Course on Power Converters, Baden (CH)
Power Converters for Accelerators 2 WWW (i.e. Where Were We)? Focused on magnet power converters Good overview with many examples 3 Where do we go now? Eckoldt s contribution: Detailed compendium of Topologies
More informationBEPCII-THE SECOND PHASE CONSTRUCTION OF BEIJING ELECTRON POSITRON COLLIDER
BEPCII-THE SECOND PHASE CONSTRUCTION OF BEIJING ELECTRON POSITRON COLLIDER C. Zhang, G.X. Pei for BEPCII Team IHEP, CAS, P.O. Box 918, Beijing 100039, P.R. China Abstract BEPCII, the second phase construction
More informationPROJECT X: A MULTI-MW PROTON SOURCE AT FERMILAB *
PROJECT X: A MULTI-MW PROTON SOURCE AT FERMILAB * Stephen D. Holmes, Fermilab, Batavia, IL, 60510, U.S.A. Abstract As the Fermilab Tevatron Collider program draws to a close a strategy has emerged of an
More informationMarket Survey. Technical Description. Supply of Medium Voltage Pulse Forming System for Klystron Modulators
EDMS No. 1972158 CLIC Drive Beam Klystron Modulator Group Code: TE-EPC Medium Voltage Pulse Forming System for CLIC R&D Market Survey Technical Description Supply of Medium Voltage Pulse Forming System
More informationCERN 64 years of fundamental science, technology, innovation and global collaborations
CERN 64 years of fundamental science, technology, innovation and global collaborations Frédérick Bordry CERN Director for Accelerators and Technology Accelerating Science and Innovation The Mission of
More informationCERN (The European Laboratory for Particle Physics)
462 IEEE TRANSACTIONS ON INSTRUMENTATION AND MEASUREMENT, VOL. 48, NO. 2, APRIL 1999 The Measurement Challenge of the LHC Project Gunnar Fernqvist Abstract In 2005, CERN is planning to commission its next
More informationCircumference 187 m (bending radius = 8.66 m)
4. Specifications of the Accelerators Table 1. General parameters of the PF storage ring. Energy 2.5 GeV (max 3.0 GeV) Initial stored current multi-bunch 450 ma (max 500 ma at 2.5GeV) single bunch 70 ma
More informationBeam Infrared Detection with Resolution in Time
Excellence in Detectors and Instrumentation Technologies Beam Infrared Detection with Resolution in Time Alessandro Drago INFN - Laboratori Nazionali di Frascati, Italy October 20-29, 2015 Introduction
More informationHITACHI Proton Therapy System with Spot Scanning
Workshop on Hadron Therapy of Cancer 27 th April, Erice, Sicily, Italy HITACHI Proton Therapy System with Spot Scanning Kazuo Hiramoto Energy & Environmental Systems Laboratory, Hitachi, Ltd. Contents
More informationCERN - ST Division THE NEW 150 MVAR, 18 KV STATIC VAR COMPENSATOR FOR SPS: BACKGROUND, DESIGN AND COMMISSIONING
EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH ORGANISATION EUROPÉENNE POUR LA RECHERCHE NUCLÉAIRE CERN - ST Division ST-Note-2003-023 4 April 2003 THE NEW 150 MVAR, 18 KV STATIC VAR COMPENSATOR FOR SPS: BACKGROUND,
More informationQUARTER WAVE COAXIAL LINE CAVITY FOR NEW DELHI LINAC BOOSTER*
QUARTER WAVE COAXIAL LINE CAVITY FOR NEW DELHI LINAC BOOSTER* P.N. Prakash and A.Roy Nuclear Science Centre, P.O.Box 10502, New Delhi 110 067, INDIA and K.W.Shepard Physics Division, Argonne National Laboratory,
More informationAcceleration of High-Intensity Protons in the J-PARC Synchrotrons. KEK/J-PARC M. Yoshii
Acceleration of High-Intensity Protons in the J-PARC Synchrotrons KEK/J-PARC M. Yoshii Introduction 1. J-PARC consists of 400 MeV Linac, 3 GeV Rapid Cycling Synchrotron (RCS) and 50 GeV Main synchrotron
More informationAlban Mosnier. CEA-Saclay, DSM/IRFU. Alban Mosnier Sept 29 - Oct 3, 2008 LINAC'08 Victoria British Columbia Canada page 1
THE IFMIF 5 MW LINACS Alban Mosnier CEA-Saclay, DSM/IRFU Alban Mosnier Sept 29 - Oct 3, 2008 LINAC'08 Victoria British Columbia Canada page 1 ITER International Road Map Advanced Materials are at a critical
More informationFLASH Operation at DESY From a Test Accelerator to a User Facility
FLASH Operation at DESY From a Test Accelerator to a User Facility Michael Bieler FLASH Operation at DESY WAO2012, SLAC, Aug. 8, 2012 Vocabulary DESY: Deutsches Elektronen-Synchrotron, Hamburg, Germany
More informationDEVELOPMENT OF ROOM TEMPERATURE AND SUPERCONDUCTING CH-STRUCTURES H. Podlech IAP, Universität Frankfurt/Main, Germany. Abstract
EU contract number RII3-CT-2003-506395 CARE Conf-04-011-HIPPI DEVELOPMENT OF ROOM TEMPERATURE AND SUPERCONDUCTING CH-STRUCTURES H. Podlech IAP, Universität Frankfurt/Main, Germany Abstract Abstract In
More informationLIFE SCIENCES High Energy Physics. High Energy Physics. Providing high power, high voltage and ultimate reliability to the global scientific market
Providing high power, high voltage and ultimate reliability to the global scientific market Introduction Image: CERN Large Hadron Collider About us We have supplied high power, often bespoke, products
More informationADVANCES IN CW ION LINACS*
Abstract Substantial research and development related to continuous wave (CW) proton and ion accelerators is being performed at ANL. A 4-meter long 60.625-MHz normal conducting (NC) CW radio frequency
More information