Tutorial on Design of RF system for Indus Accelerator. Maherdra Lad Head, Radio Frequency Systems Division RRCAT, Indore
|
|
- Francis Nichols
- 5 years ago
- Views:
Transcription
1 Tutorial on Design of RF system for Indus Accelerator Maherdra Lad Head, Radio Frequency Systems Division RRCAT, Indore
2 Basic principle of RF Acceleration RF Power Amplifier The RF source supplies power to setup oscillating electrical field in the cavity. It supplies energy to the beam Compensates for the synchrotron radiation losses. 1.5 Charged Particle Orbit / Path RF Cavity Bunch Electrical Field setup in the cavity
3 Need of RF Systems 1. To Provide Sufficient Gap Voltage for Acceleration /SR Loss 2. Power to the beam for Current build up (synchrotron Radiation loss * I beam) In the Synchrotron & Storage Ring (Electron Cyclic Accelerators) circulating electrons loose energy in the form of electromagnetic radiation. To keep them in equilibrium orbits this loss has to be compensated.the RF system provides energy for acceleration as well as compensates for this radiation loss.
4 Role of RF structure
5
6 INDUS COMPLEX LAYOUT Indus Accelerator complex at RRCAT consists of two Synchrotron Radiation Sources (SRS); 450 MeV Indus-1 and 2.5 GeV Indus-2. The 550 MeV Booster Synchrotron serves as common injector for these storage rings. Three major RF Systems, Booster RF system & Indus-1 Storage ring RF System at MHz and Indus-2 RF system at MHz have been developed, commissioned and deployed successfully. workshop on RF Systmes For Acclereators, IUAC New Delhi
7 Selection of RF frequency
8 Selection of RF frequency : Indus-2 a case study # Properties of required SR : like emittance, bunch length, brightness # Circumference of the ring # Frequency of the RF system of Injector # Availability of the high power RF source for required power level Circumference of Indus-2 ring = m Revolution Frequency (f r ) = 3*10^8 /172.6 = MHz RF Frequency Should be Integer harmonic of the Injector ( Booster synchrotron) RF frequency = MHz and also multiple of Revolution Frequency (f r ) RF Frequency = N* f r = MHz 16 th harmonic = *16 = MHz No. of Bunches (N) = 291
9 Accelerating voltage for Indus-2 Indus-2 Particle Energy Bending Radius = 2.5 GeV = 5.5 m Synchrotron Loss per turn = 628 kev per turn Hence to compensate for energy loss due to SR minimum 628 kv accelerating voltage is required However for sufficient beam life time over voltage factor (more than 2) is required. We provide 1500kV in Indus-2 through four RF cavities
10 RF Power Requirement To Generate Accelerating Voltage 1500 kv is generated through four RF Cavities Each operating at V = 1500/4 = 375 kv RF Cavity power P = V 2 / R sh ( R sh = 6.6 MΩ) = 21.3 kw ( each cavity) Why? To Compensate for Synchrotron Loss Synchrotron Loss Power = Stored Current x SR Loss per turn = 200 ma x 622 kev = 124 kw for 200 ma at 2.5 GeV Total power required for 200mA, 2.5 GeV operation P Total = 21.3* = kw RF
11 Indus-2 RF System Taking into account design margin, four RF stations with 60kW RF power each were installed initially. These have been upgraded to 80kW.
12 Resonant Frequency Shunt Impedance Quality Factor RF Cavities used in Indus
13 T h a n k s
14 RF (LLRF) Instrumentation The RF instrumentation includes RF instruments : Spectrum analyzer, VNA RF Parameter monitoring (power, phase ) a)directional couplers b)rf-dc detectors c)phase detectors d)rf splitters/dividers e)protection workshop equipments on RF :isolators,
15 Optimization of Indus-2 RF System For Higher energy and Current RF Cavity Coupling Coefficient (β) Adjustment For 250mA, 2.5Gev β is adjusted to 2.8 (Over Coupled ) Baking and RF conditioning of Indus-2 RF cavity. B 30 Rflected Power (in %) In put Impedance at coupler side Phase Synchronization of Indus-2 RF Cavities Four RF Cavity signals are synchronized For proper Injection For ramping to High energy Loaded quality factor characterization using VNA Beam Energy (in MeV) With increase in Beam power decrease in reflected power is an indication over coupled β 18 Stn 1 Stn 2 Stn 3 Stn 4 Net Power(kW) Beam Current (ma) proper synchronization phase of four RF cavity Tuner Movement showing the same beam loading in two RF stations Graph showing equal power sharing from each station With optimized RF System parameters, Indus-2 is utilised by users regularly at 150mA, 2.5GeV Recently successful operation for 181mA stored current at full deigned energy of 2.5GeV has also been achieved.
16
17 6 1/8 Coaxial Directional Coupler Coupling Factor: db Directivity : 30 db workshop on RF
18 RF-DC detectors & Phase detectors workshop on RF
19
20
21
22
23 workshop on RF
24 workshop on RF
25 workshop on RF
26 workshop on RF
27 workshop on RF
28 workshop on RF
29 workshop on RF
30 Synchrotron Radiation Spectrum workshop on RF
Project of RF System for 2.2 GeV Electron Storage Ring Zelenograd SR Source.
Project of RF System for 2.2 GeV Electron Storage Ring Zelenograd SR Source. I.K. Sedlyarov V.S. Arbuzov, E.I Gorniker, A.A. Kondakov, S.A. Krutikhin, G.Ya. Kurkin, I.V.Kuptsov, V.N. Osipov, V.M. Petrov,
More informationMAX II RF system 100 MHz technology Lars Malmgren 10th ESLS RF Meeting Dortmund September 27-28, 2006
MAX II RF system 1 MHz technology Lars Malmgren 1th ESLS RF Meeting Dortmund September 27-28, 26 Facts and figures MAX-II Frequency [MHz] Harmonic number No of cavity cells No of transmitters Cell radius
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 informationA Synchrotron Phase Detector for the Fermilab Booster
FERMILAB-TM-2234 A Synchrotron Phase Detector for the Fermilab Booster Xi Yang and Rene Padilla Fermi National Accelerator Laboratory Box 5, Batavia IL 651 Abstract A synchrotron phase detector is diagnostic
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 informationJørgen S. Nielsen Institute for Storage Ring Facilities, Aarhus, University of Aarhus Denmark
Jørgen S. Nielsen Institute for Storage Ring Facilities, Aarhus, University of Aarhus Denmark What is ISA? ISA operates and develops the storage ring ASTRID and related facilities ISA staff assist internal
More informationBooster High-level RF Frequency Tracking Improvement Via the Bias-Curve Optimization
FERMILAB-TM-227-AD Booster High-level RF Frequency Tracking Improvement Via the Bias-Curve Optimization Xi Yang Fermi National Accelerator Laboratory Box 5, Batavia IL 651 Abstract It is important to improve
More informationConverters for Cycling Machines
Converters for Cycling Machines Neil Marks, DLS/CCLRC, Daresbury Laboratory, Warrington WA4 4AD, U.K. DC and AC accelerators; Contents suitable waveforms in cycling machines; the magnet load; reactive
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 informationSuperconducting RF System. Heung-Sik Kang
Design of PLS-II Superconducting RF System Heung-Sik Kang On behalf of PLS-II RF group Pohang Accelerator Laboratory Content 1. Introduction 2. Physics design 3. Cryomodules 4. Cryogenic system 5. High
More informationRF Upgrade at DELTA. P. Hartmann DELTA, TU Dortmund
RF Upgrade at DELTA P. Hartmann DELTA, TU Dortmund DELTA parameters: Personnel: Beam energy: 550 MeV 1.5 GeV Beam current: 130mA @ 1.5GeV Beam lifetime: 12h @ 130 ma Availability: 95 % Operational: 3000
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 informationThe HPRF system for a new 6 GeV synchrotron light source in Beijing
中国科学院高能物理研究所 INSTITUTE OF HIGH ENERGY PHYSICS CHINESE ACADEMY OF SCIENCES The HPRF system for a new 6 GeV synchrotron light source in Beijing (RF group, IHEP) The HEPS HPRF team Power coupler & power source
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 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 informationDetailed Design Report
Detailed Design Report Chapter 2 MAX IV 3 GeV Storage Ring 2.6. The Radio Frequency System MAX IV Facility CHAPTER 2.6. THE RADIO FREQUENCY SYSTEM 1(15) 2.6. The Radio Frequency System 2.6. The Radio Frequency
More informationMain Injector Cavity Simulation and Optimization for Project X
Main Injector Cavity Simulation and Optimization for Project X Liling Xiao Advanced Computations Group Beam Physics Department Accelerator Research Division Status Meeting, April 7, 2011 Outline Background
More informationDark current Monitor for the European XFEL D. Lipka, W. Kleen, J. Lund-Nielsen, D. Nölle, S. Vilcins, V. Vogel; DESY Hamburg
Dark current Monitor for the European XFEL D. Lipka, W. Kleen, J. Lund-Nielsen, D. Nölle, S. Vilcins, V. Vogel; DESY Hamburg Content 2 Dark current Principle of detecting weakly charged bunches with resonator
More informationResonator System for the BEST 70MeV Cyclotron
Resonator System for the BEST 70MeV Cyclotron 20 nd International Conference on Cyclotrons and their Applications Vancouver, Canada, September 16-20, 2013 Vasile Sabaiduc, Dipl. Eng. Accelerator Technology
More informationJørgen S. Nielsen Center for Storage Ring Facilities (ISA) Aarhus University Denmark. ESLS-RF 22 (8/ ), ASTRID2 RF system 1
Jørgen S. Nielsen Center for Storage Ring Facilities (ISA) Aarhus University Denmark ESLS-RF 22 (8/11 2018), ASTRID2 RF system 1 ASTRID2 is the new synchrotron light source in Aarhus, Denmark, since 2013
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 informationBeam Instability Investigations at DELTA
10 th ESLS-RF Meeting, September 27-28, Dortmund Beam Instability Investigations at Thomas Weis for the group Dortmund University Synchrotron Radiation Center Content: Status of the Facility Instability
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 informationDesign and performance of LLRF system for CSNS/RCS *
Design and performance of LLRF system for CSNS/RCS * LI Xiao 1) SUN Hong LONG Wei ZHAO Fa-Cheng ZHANG Chun-Lin Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, China Abstract:
More informationMaurizio Vretenar Linac4 Project Leader EuCARD-2 Coordinator
Maurizio Vretenar Linac4 Project Leader EuCARD-2 Coordinator Every accelerator needs a linac as injector to pass the region where the velocity of the particles increases with energy. At high energies (relativity)
More informationProject X Cavity RF and mechanical design. T. Khabiboulline, FNAL/TD/SRF
Project X Cavity RF and mechanical design T. Khabiboulline, FNAL/TD/SRF TTC meeting on CW-SRF, 2013 Project X Cavity RF and mechanical design T 1 High ß Low ß 0.5 HWR SSR1 SSR2 0 1 10 100 1 10 3 1 10 4
More informationA 3 GHz SRF reduced-β Cavity for the S-DALINAC
A 3 GHz SRF reduced-β Cavity for the S-DALINAC D. Bazyl*, W.F.O. Müller, H. De Gersem Gefördert durch die DFG im Rahmen des GRK 2128 20.11.2018 M.Sc. Dmitry Bazyl TU Darmstadt TEMF Upgrade of the Capture
More informationBetatron tune Measurement
Betatron tune Measurement Tom UESUGI, Y. Kuriyama, Y. Ishi FFA school, Sep. 8-9, Osaka, 218 CONTENTS Betatron oscillation and tune How to measure tunes KURNS FFAG, Diagnostics BETATRON OSCILLATION AND
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 information10th ESLS RF Meeting September ALBA RF System. F. Perez. on behalf of the ALBA RF Group. ALBA RF System 1/21
ALBA RF System F. Perez on behalf of the ALBA RF Group ALBA RF System 1/21 Synchrotron Light Source in Cerdanyola (Barcelona, Spain) 3 GeV accelerator 30 beamlines (7 on day one) 50-50 Spanish Government
More informationLawrence Berkeley Laboratory UNIVERSITY OF CALIFORNIA
d e Lawrence Berkeley Laboratory UNIVERSITY OF CALIFORNIA Accelerator & Fusion Research Division I # RECEIVED Presented at the International Workshop on Collective Effects and Impedance for B-Factories,
More information200 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 BESSY Higher Order Mode Damped Cavity - Further Improvements -
The BESSY Higher Order Mode Damped Cavity - Further Improvements - Ernst Weihreter Reminder of Technical Problems Solutions Conclusions BESSY HOM Damped Cavity Project collaboration: (EC funded) - BESSY
More informationShort-Pulse X-ray at the Advanced Photon Source Overview
Short-Pulse X-ray at the Advanced Photon Source Overview Vadim Sajaev and Louis Emery Accelerator Operations and Physics Group Accelerator Systems Division Mini-workshop on Methods of Data Analysis in
More informationNew apparatus for precise synchronous phase shift measurements in storage rings 1
New apparatus for precise synchronous phase shift measurements in storage rings 1 Boris Podobedov and Robert Siemann Stanford Linear Accelerator Center, Stanford University, Stanford, CA 94309 Measuring
More informationSlide Title. Bulleted Text
Slide Title 1 Slide Outline Title Brief view of the C-AD Complex Review of the RHIC LLRF Upgrade Platform Generic Implementation of a Feedback Loop RHIC Bunch by Bunch Longitudinal Damper Cavity Controller
More informationEE 3324 Electromagnetics Laboratory
EE 3324 Electromagnetics Laboratory Experiment #10 Microstrip Circuits and Measurements 1. Objective The objective of Experiment #8 is to investigate the application of microstrip technology. A precision
More information1.8 MW Upgrade of the PSI Proton Accelerator Facility
1.8 MW Upgrade of the PSI Proton Accelerator Facility Pierre A. Schmelzbach for the PSI Accelerator Divisions This talk: analyzes the potential for improvements from the ion source to the spallation target
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 informationIntroduction to Synchrotron Radio Frequency System
3 rd ILSF Advanced School on Synchrotron Radiation and Its Applications September 14-16, 2013 Introduction to Synchrotron Radio Frequency System Khorshid Sarhadi Head of ILSF RF Group 15 Sep. 2013 1 Outline
More informationEMMA the World's First Non-Scaling FFAG Accelerator
EMMA the World's First Non-Scaling FFAG Accelerator Susan Smith STFC Daresbury Laboratory CONTENTS Introduction Contents What are ns-ffags? and Why EMMA? The international collaboration EMMA goals and
More informationANALYSIS OF 3RD OCTAVE BAND GROUND MOTIONS TRANSMISSION IN SYNCHROTRON RADIATION FACILITY SOLARIS Daniel Ziemianski, Marek Kozien
ANALYSIS OF 3RD OCTAVE BAND GROUND MOTIONS TRANSMISSION IN SYNCHROTRON RADIATION FACILITY SOLARIS Daniel Ziemianski, Marek Kozien Cracow University of Technology, Institute of Applied Mechanics, al. Jana
More informationBaseband simulation model of the vector rf voltage control system for the J-PARC RCS
Journal of Physics: Conference Series PAPER OPEN ACCESS Baseband simulation model of the vector rf voltage control system for the J-PARC RCS To cite this article: Fumihiko Tamura et al 2018 J. Phys.: Conf.
More informationJ. Jacob: Status of the ESRF RF upgrade
17th ESLS RF Meeting 2013 HZB BESSY 18th 19th September Status of the ESRF RF upgrade J. Jacob J.-M. Mercier V. Serrière M. Langlois G. Gautier [CINEL] 1 RF upgrade phase 1 until 2015 - reminder Replacement
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 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 informationStatus of the 1.5 GeV Synchrotron Light Source DELTA and Related Accelerator Physics Activities
Status of the 1.5 GeV Synchrotron Light Source and Related Accelerator Physics Activities 2006 RuPAC, September 10-14, Novosibirsk Thomas Weis for the machine and accelerator physics group Dortmund University
More informationSystem Integration of the TPS. J.R. Chen NSRRC, Hsinchu
System Integration of the TPS J.R. Chen NSRRC, Hsinchu OUTLINE I. Main features of the TPS II. Major concerns and intersystem effects of an advanced synchrotron light source III. Subsystems and intersystem
More informationThe VARIAN 250 MeV Superconducting Compact Proton Cyclotron
The VARIAN 250 MeV Superconducting Compact Proton Cyclotron VARIAN Medical Systems Particle Therapy GmbH Friedrich-Ebert-Str. 1 D-51429 BERGISCH GLADBACH GERMANY OUTLINE 1. Why having a Superconducting
More informationX-Ray Detection Using SOI Monolithic Sensors at a Compact High-Brightness X-Ray Source Based on Inverse Compton Scattering
Abstract #: 1054 Conference: NSS (Oral) Accelerator Technologies and Beam Line Instrumentation X-Ray Detection Using SOI Monolithic Sensors at a Compact High-Brightness X-Ray Source Based on Inverse Compton
More informationAutomatic phase calibration for RF cavities using beam-loading signals. Jonathan Edelen LLRF 2017 Workshop (Barcelona) 18 Oct 2017
Automatic phase calibration for RF cavities using beam-loading signals Jonathan Edelen LLRF 2017 Workshop (Barcelona) 18 Oct 2017 Introduction How do we meet 10-4 energy stability for PIP-II? 2 11/9/2017
More informationLow Level RF. Part 2: Cavity Controller, Problems and Cures CAS RF. P. Baudrenghien CERN-BE-RF. 3. What will go wrong? 4. Power amplifier limits
Low Level RF Part 2: Cavity Controller, Problems and Cures 3. What will go wrong? 4. Power amplifier limits 5. Beam Loading 6. Longitudinal instabilities in Synchrotrons 7. LLRF Cures CAS RF P. Baudrenghien
More informationSingle Bunch Impurity Measurement at SPring-8 8 Storage Ring
Single Bunch Impurity Measurement at SPring-8 8 Storage Ring Kazuhiro TAMURA (JASRI/SPring-8) 1 Outlilne Overview of SPring-8 accelerator complex operation modes Bunch Purity Monitor light shutter system
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 informationTURN-BY-TURN BPM SYSTEM USING COAXIAL SWITCHES AND ARM MICROCONTROLLER AT UVSOR
TURN-BY-TURN BPM SYSTEM USING COAXIAL SWITCHES AND ARM MICROCONTROLLER AT UVSOR Tomonori Toyoda, Kenji Hayashi, and Masahiro Katoh, IMS, Okazaki, Japan Abstract A major upgrade of the electron storage
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 informationCoherent Synchrotron Radiation in the ANKA Storage Ring
Coherent Synchrotron Radiation in the ANKA Storage Ring Marcel Schuh On behalf of the ANKA THz-Group Laboratory for Applications of Synchrotron Radiation (LAS) / Institute of Synchrotron Radiation (ISS)
More informationRF System Models and Longitudinal Beam Dynamics
RF System Models and Longitudinal Beam Dynamics T. Mastoridis 1, P. Baudrenghien 1, J. Molendijk 1, C. Rivetta 2, J.D. Fox 2 1 BE-RF Group, CERN 2 AARD-Feedback and Dynamics Group, SLAC T. Mastoridis LLRF
More informationStatus of the MAX IV RF systems. PPT-mall 2
Status of the MAX IV RF systems PPT-mall 2 Lars Malmgren Med linje On Behalf of the MAX IV RF Group Åke Andersson, Joel Andersson, Richard Grandford, Sven-Olof Heed, Per Lilja, Dionis Kumbaro, Lars Malmgren,
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 informationNormal-Conducting Photoinjector for High Power CW FEL
LA-UR-04-5617,-5808 www.arxiv.org: physics/0404109 Normal-Conducting Photoinjector for High Power CW FEL Sergey Kurennoy, LANL, Los Alamos, NM, USA An RF photoinjector capable of producing high continuous
More informationMEASURES TO REDUCE THE IMPEDANCE OF PARASITIC RESONANT MODES IN THE DAΦNE VACUUM CHAMBER
Frascati Physics Series Vol. X (1998), pp. 371-378 14 th Advanced ICFA Beam Dynamics Workshop, Frascati, Oct. 20-25, 1997 MEASURES TO REDUCE THE IMPEDANCE OF PARASITIC RESONANT MODES IN THE DAΦNE VACUUM
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 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 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 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 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 informationCHAPTER 6 BOOSTER RF SYSTEMS
CHAPTER 6 BOOSTER RF SYSTEMS 6.1 NEW PSB RF CAVITIES H = 1 (0.6 1.8 MHz) The addition of cavities accelerating on RF harmonic h = 1 and supplemented with a h = 2 system, contributed to the reduction of
More informationDoes the short pulse mode need energy recovery?
Does the short pulse mode need energy recovery? Rep. rate Beam power @ 5GeV 1nC @ 100MHz 500MW Absolutely 1nC @ 10MHz 1nC @ 1MHz 50MW 5MW Maybe 1nC @ 100kHz 0.5MW No Most applications we have heard about
More informationExperiment-4 Study of the characteristics of the Klystron tube
Experiment-4 Study of the characteristics of the Klystron tube OBJECTIVE To study the characteristics of the reflex Klystron tube and to determine the its electronic tuning range EQUIPMENTS Klystron power
More informationExperiences of the QSBPM System on MAX II
Experiences of the QSBPM System on MAX II Peter Röjsel MAX-lab, Lund University, Lund, Sweden Abstract. The MAX II is a third-generation synchrotron radiation source. The first beamline is in operation
More informationDesign of S-band re-entrant cavity BPM
Nuclear Science and Techniques 20 (2009) 133 139 Design of S-band re-entrant cavity BPM LUO Qing SUN Baogen * HE Duohui National Synchrotron Radiation Laboratory, School of Nuclear Science and Technology,
More informationCommissioning of the ALICE SRF Systems at Daresbury Laboratory Alan Wheelhouse, ASTeC, STFC Daresbury Laboratory ESLS RF 1 st 2 nd October 2008
Commissioning of the ALICE SRF Systems at Daresbury Laboratory Alan Wheelhouse, ASTeC, STFC Daresbury Laboratory ESLS RF 1 st 2 nd October 2008 Overview ALICE (Accelerators and Lasers In Combined Experiments)
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 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 informationBioimaging of cells and tissues using accelerator-based sources
Analytical and Bioanalytical Chemistry Electronic Supplementary Material Bioimaging of cells and tissues using accelerator-based sources Cyril Petibois, Mariangela Cestelli Guidi Main features of Free
More informationPredictions of LER-HER limits
Predictions of LER-HER limits PEP-II High Current Performance T. Mastorides, C. Rivetta, J.D. Fox, D. Van Winkle Accelerator Technology Research Div., SLAC 2e 34 Meeting, May 2, 27 Contents In this presentation
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 informationBeam Diagnostics, Low Level RF and Feedback for Room Temperature FELs. Josef Frisch Pohang, March 14, 2011
Beam Diagnostics, Low Level RF and Feedback for Room Temperature FELs Josef Frisch Pohang, March 14, 2011 Room Temperature / Superconducting Very different pulse structures RT: single bunch or short bursts
More informationReducing space charge tune shift with a barrier cavity
8th ICFA ;dvanced i3ean Dynamic Workshop on Space Charge Dominated Beams and X - y l i c a t i o n s of Hi$i Brightness B e a m s, Bloominston, 10/11-13/95. ' I BNL-62493 y, Reducing space charge tune
More informationELECTRON LINACS. Alessandro Fabris. Elettra-Sincrotrone Trieste S.C.p.A, Italy. 39 th International Nathiagali Summer College 4 th 9 th August 2014
ELECTRON LINACS Elettra-Sincrotrone Trieste S.C.p.A, Italy 39 th International Nathiagali Summer College 4 th 9 th August 2014 2 OVERVIEW Introduction Travelling wave structures Standing wave structures
More informationPhysics Design and Technology. Development of CSNS Accelerator
Physics Design and Technology Development of CSNS Accelerator Second CSNS International Accelerator Technology Advisory Committee Review Meeting Institute of High Energy Physics, CAS January, 2010, Beijing,
More informationThermionic Bunched Electron Sources for High-Energy Electron Cooling
Thermionic Bunched Electron Sources for High-Energy Electron Cooling Vadim Jabotinski 1, Yaroslav Derbenev 2, and Philippe Piot 3 1 Institute for Physics and Technology (Alexandria, VA) 2 Thomas Jefferson
More informationERLP Status. Mike Dykes
ERLP Status Mike Dykes Content ASTeC RF & Diagnostics Group Work of the Group 4GLS ERLP Photo-injector Accelerating Modules Summary High Power RF Engineering Andy Moss SRS Support; DIAMOND; ERLP; MICE;
More informationAnalogue electronics for BPMs at GSI - Performance and limitations
Joint ARIES Workshop on Electron and Hadron Synchrotrons Barcelona, 12-14 th November 2018 Analogue electronics for BPMs at GSI - Performance and limitations W. Krämer & W. Kaufmann (GSI) Dept. of Beam
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 informationCOMMISSIONING OF A COMPACT SYNCHROTRON RADIATION SOURCE AT HIROSHIMA UNIVERSITY
COMMISSIONING OF A COMPACT SYNCHROTRON RADIATION SOURCE AT HIROSHIMA UNIVERSITY K. Yoshida, M. Andreyashkin, K. Goto, E. Hashimoto, G. Kutluk, K. Matsui, K. Mimura,H. Namatame, N. Ojima, K. Shimada, M.
More informationEC 1402 Microwave Engineering
SHRI ANGALAMMAN COLLEGE OF ENGINEERING & TECHNOLOGY (An ISO 9001:2008 Certified Institution) SIRUGANOOR,TRICHY-621105. DEPARTMENT OF ELECTRONICS AND COMMUNICATION ENGINEERING EC 1402 Microwave Engineering
More informationDesign considerations for the RF phase reference distribution system for X-ray FEL and TESLA
Design considerations for the RF phase reference distribution system for X-ray FEL and TESLA Krzysztof Czuba *a, Henning C. Weddig #b a Institute of Electronic Systems, Warsaw University of Technology,
More informationPerformance of the Reference and Timing Systems at SPring-8
Performance of the Reference and Timing Systems at SPring-8 Outline Yuji Ohashi SPring-8 1. Introduction 2. Tools 3. Performances 4. New synchronization scheme between 508 and 2856 MHz 5. Summary Y.Kawashima
More informationREVIEW OF HIGH POWER CW COUPLERS FOR SC CAVITIES. S. Belomestnykh
REVIEW OF HIGH POWER CW COUPLERS FOR SC CAVITIES S. Belomestnykh HPC workshop JLAB, 30 October 2002 Introduction Many aspects of the high-power coupler design, fabrication, preparation, conditioning, integration
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 informationLow-Level RF. S. Simrock, DESY. MAC mtg, May 05 Stefan Simrock DESY
Low-Level RF S. Simrock, DESY Outline Scope of LLRF System Work Breakdown for XFEL LLRF Design for the VUV-FEL Cost, Personpower and Schedule RF Systems for XFEL RF Gun Injector 3rd harmonic cavity Main
More informationNational Accelerator Laboratory
Fermi National Accelerator Laboratory FERMILAB-Conf-96/103 Trigger Delay Compensation for Beam Synchronous Sampling James Steimel Fermi National Accelerator Laboratory P.O. Box 500, Batavia, Illinois 60510
More informationUppsala, June 17 th - 19 th, 2013
TIARA Workshop on RF Power Generation for Accelerators Uppsala, June 17 th - 19 th, 2013 Massamba DIOP, R. LOPES, P. MARCHAND, F. RIBEIRO SSA operation at SOLEIL BOOSTER 35 kw STORAGE RING 180 kw SOLEIL
More informationFLASH 2. FEL seminar. Charge: 0.5 nc. Juliane Rönsch-Schulenburg Overview of FLASH 2 Hamburg,
FLASH 2 FEL seminar Juliane Rönsch-Schulenburg Overview of FLASH 2 Hamburg, 2016-03-22 Charge: 0.5 nc Overview 1. FLASH 2 Overview 1.Layout parameters 2. Operation FLASH2. 1.Lasing at wavelengths between
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 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 informationR.Bachimanchi, IPAC, May 2015, Richmond, VA
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 informationStatus of the HOM Damped Cavity Project
Status of the HOM Damped Cavity Project E. Weihreter / BESSY for the HOM Damped Cavity Collaboration BESSY, Daresbury Lab, DELTA, MaxLab, NTHU Project funded by the EC under contract HPRI-CT-1999-50011
More information