Experimental results and recent developments on the EU 2 MW 170 GHz coaxial cavity gyrotron for ITER
|
|
- Rolf Cain
- 5 years ago
- Views:
Transcription
1 Experimental results and recent developments on the EU 2 MW 170 GHz coaxial cavity gyrotron for ITER S. Kern 1, J.-P. Hogge 2, S. Alberti 2, K. Avramides 3, G. Gantenbein 1, S. Illy 1, J. Jelonnek 1, J. Jin 1, F. Li 2, I. Gr. Pagonakis 1, B. Piosczyk 1, T. Rzesnicki 1, M. K. Thumm 1, I. Tigelis 4, M. Q. Tran 2 and the whole EU home team at EGYC KARLSRUHE INSTITUTE OF TECHNOLOGY, (IHM) 1 Karlsruhe Institute of Technology (KIT), (IHM), Association EURATOM-KIT, D Karlsruhe, Germany 2 Centre de Recherche en Physique des Plasmas (CRPP), Association Euratom-Confédération Suisse,EPFL, CH-1015 Lausanne, Switzerland 3 National Technical University of Athens (part of HELLAS), School of Electrical and Computer Engineering, 9 Iroon Polytechniou st., GR15773 Athens, Greece 4 National and Kapodistrian University of Athens (part of HELLAS), Faculty of Physics, Athens, Greece. European GYrotron Consortium (EGYC) KIT University of the State of Baden-Wuerttemberg and National Research Center of the Helmholtz Association
2 Overview Introduction Summary and consequences of former experiments Design modifications to the industrial CW prototype Tests of the refurbished CW prototype SAT and RF test Post-test evaluations Experiments with the short pulse pre-prototype Future plans S. Kern et al., Experimental results and recent developments on the EU 2 MW 170 GHz coaxial
3 Introduction The EGYC consortium develops under F4E contract 170 GHz gyrotrons in support of EU s contribution to ITER s ECRH system. - EGYC is currently CRPP, KIT, HELLAS, IFP-CNR. The industrial partner is Thales Electron Devices (TED). Until now, the goal was a 2 MW coaxial cavity gyrotron. Three CW prototypes at increasing pulse length goals (1s/60s/3600s) foreseen, only one build so far. A 1 MW conventional tube development as fallback was started Due to essential delays, switch to the fallback solution is probable. This presentation reports on latest results and future plans for the coaxial cavity project S. Kern et al., Experimental results and recent developments on the EU 2 MW 170 GHz coaxial
4 Summary of former experiments In 2008 first experiments with CW prototype at CRPP: Serious problems with the electron gun: low frequency oscillations (~100 MHz region) low voltage standoff with magnetic field applied -> Analysis shows the existence of potential traps in the gun RF output beam pattern insufficient (77% Gaussian content) -> Application of new launcher design methods RF power limited to 1.4 MW in short pulse due to mentioned problems Power capability of the collector successfully tested (2.2 MW/10s) Pre-prototype short pulse tests at KIT until end 2008: Power limitation by limited magnetic field (6.7 T instead of 6.87 T) -> Application of additional normal conducting (NC) coil Indications of beam-tunnel oscillations (159 GHz) -> Application of corrugated beam tunnel Same RF beam as in prototype S. Kern et al., Experimental results and recent developments on the EU 2 MW 170 GHz coaxial
5 Resulting modifications to the CW prototype The CW prototype was refurbished with design improvements: New gun design following improved design rules New launcher design Corrugated beam tunnel Additional modifications in mechanical construction: Ion getter pumps moved to lower magnetic field Large ceramic isolator mounting revised for lower force during bakeout Validation tests with the short pulse pre-prototype at KIT in 2009: Corrugated beam tunnel applied -> No parasitic oscillations New launcher design as above -> 96 % Gaussian content Achieving 6.87 T with NC coil -> operation at nominal parameters -> nominal operation: % efficiency (w/o depr. collector)! S. Kern et al., Experimental results and recent developments on the EU 2 MW 170 GHz coaxial
6 Mechanical issues with refurbished CW prototype Refurbishment and modification started in 2009 Manufacturing problems caused massive delays - some clearly attributed to the attempt to refurbish a large device. The refurbishment of the mirror box was considered critical by the manufacturer, after brazings became untight at bakeout. In particular, one RF absorber had to be removed. Delivery date moved from summer 2010 to finally end September The tube was untight on delivery. It could be sealed and still showed good vacuum properties after pumping. Achievable pulse length was unclear then. After four days of successful RF operation, another RF absorber broke and flooded the tube with water, terminating any further experiment. Reasons still have to be investigated in detail, ultimate cause is accidental operation in wrong mode rotation. After experiment, additional problems of alignment were found S. Kern et al., Experimental results and recent developments on the EU 2 MW 170 GHz coaxial
7 SAT test of the prototype gyrotron Site acceptance test (SAT) was successful: Excellent HV stand-off without and with magnetic field Cooling tests OK Beam extraction tests OK (58 kv / 75 A after 2 days of conditioning) Coaxial insert.vs. electron beam alignment OK Body current higher than expected, but acceptable Body.vs. electron beam alignment ~OK (coarse measurement, made in x direction only) -> The tube was formally accepted. Green light to proceed with RF tests was given by TED on December 2 nd S. Kern et al., Experimental results and recent developments on the EU 2 MW 170 GHz coaxial
8 RF tests of the prototype gyrotron (Dec ) After 4-5 days of RF conditioning, the tube delivered 2 MW / 170 GHz (short pulse ~1ms) with an efficiency of 45 % at 75 A (nominal value) and 90.5 kv (60 kv kv), (nominal: 90kV, 55kV + 35kV) No particular optimization, no evident sign of saturation, not finally conditioned S. Kern et al., Experimental results and recent developments on the EU 2 MW 170 GHz coaxial
9 RF beam pattern of the prototype Mode TE 34,19 Mode TE 35,19? Logbook shot #10410, S. Kern et al., Experimental results and recent developments on the EU 2 MW 170 GHz coaxial
10 RF beam pattern of the prototype Mode TE 34,19 Comparison Simulation pre-prototype 96 % GC refurbished prototype S. Kern et al., Experimental results and recent developments on the EU 2 MW 170 GHz coaxial
11 RF tests of the prototype gyrotron: Summary Positive results Negative results 2 MW / 170GHz short pulse efficiency of 45 % (using depressed collector), non-optimized, at nominal beam parameters 75 A, 90.5 kv, depression voltage 30.5 kv (nominal: 35 kv) Very good RF beam pattern -> second validation of launcher redesign Unexpected, but acceptable body current Unclear alignment situation Absorber broken, total loss of tube No long pulses were possible! Unclear observations No low frequency oscillations Excellent voltage standoff -> validation of gun redesign / design principles No evidence for parasitical RF (160GHz range) -> n th validation of corrugated beam tunnel All design modifications were verified to a high degree!! Unexpectedly high starting currents (~60 A!) Tube prone to operation in wrong mode rotation -> results in high stray radiation -> ultimate cause for broken internal absorber! Body current -> compare to pre-prototype tests These effects could be related to misalignment! Nevertheless, the risk of total loss of a tube due to a breaking absorber is inacceptable -> redesign of internal absorber scheme S. Kern et al., Experimental results and recent developments on the EU 2 MW 170 GHz coaxial
12 Post-test evaluations: Alignment The magnet alignment (ASG magnet at CRPP) could only be checked after the experiment. Results of subsequent check: Magnetic axis is shifted by 0.7 mm in y-direction (check with tube indicating good alignment done in x-direction only!). Additional result: Due to some loose stabilisation rods, the tube can be easily bend by millimeters, resulting in basically undefined alignment! -> The relative body-beam alignment along y could have been anything between good and bad! -> Investigations on the influence of tube alignment are needed for evaluation of the observations! S. Kern et al., Experimental results and recent developments on the EU 2 MW 170 GHz coaxial cavity gyrotron for ITER, EC17 Workshop, May 2012, Deurne, The Netherlands
13 Experimental setup of the pre-prototype Experiments with the KIT pre-prototype are currently running in short pulse in the following configuration: Further improved launcher design: smoothed launcher surface Electron gun refurbished by TED: New emitter ring New cathode and anode shape, identical to CW prototype -> this includes a small halo shield with ~2mm electron beam clearance Ready for depressed collector operation Gyrotron housing reworked to fit into 220 mm bore hole -> KIT OI magnet was equipped with cooled CW NC coil S. Kern et al., Experimental results and recent developments on the EU 2 MW 170 GHz coaxial
14 I Xdipol / A before the alignment Alignment procedure and measurements Shift of the electron beam position using dipole coils Emission uniformity test and alignment of coaxial insert measurement 10 5 dr/idipol=0.1mm/a Verification of the gyrotron position Start / End of the probe Iy I Ydipol / A Concentricity of the coaxial insert with respect to the electron beam: δr ~ 0.04mm Concentricity of the electron beam with respect to cavity wall: δr 0.1 mm -> excellent alignment conditions S. Kern et al., Experimental results and recent developments on the EU 2 MW 170 GHz coaxial
15 P RF / MW efficiency / % Latest experimental results of the pre-prototype Current results of the ongoing short-pulse tests are: RF power:1.9 28% efficiency (w/o depr. collector), not optimized Reduced stray radiation: 4% instead of 7% Good beam pattern 50 2,0 45 1,8 40 1,6 35 1,4 30 1,2 1,0 0,8 0, U C / kv S. Kern et al., Experimental results and recent developments on the EU 2 MW 170 GHz coaxial
16 Latest experimental results of the pre-prototype Comparison to CW prototype tests: Low starting currents (10A) No unusual danger of operating in wrong rotation Good voltage standoff But: strong LF oscillations during startup due to gun rear part or small remaining potential traps? Body current at design parameters -> can be avoided by parameter settings -> but calls for investigations: reasons are unclear, halo shield design? - electron beam radius appears 1.8 mm larger than expected! S. Kern et al., Experimental results and recent developments on the EU 2 MW 170 GHz coaxial
17 Latest experimental results of the pre-prototype Next steps: Further conditioning Preparation for depressed collector test Tests of the influence of mislalignment S. Kern et al., Experimental results and recent developments on the EU 2 MW 170 GHz coaxial
18 New Launcher / q.o. system measurements The smoothed launcher shows an equally good RF beam pattern as its predecessor. Measured stray radiation is essentially reduced to 4 % of the RF output power Former results: 7 % original KIT design 5.5 % IAP design burned paper spot window thermal image 85 mm from window thermal image 1000 mm from window S. Kern et al., Experimental results and recent developments on the EU 2 MW 170 GHz coaxial
19 Future plans 2nd Industrial CW prototype: formal decision pending, 1MW decision probable Agreement on necessary modifications on scientific side achieved In view of their future relevance, KIT will continue experiments with coaxial cavity gyrotrons if necessary on stretched time scales. The KIT short-pulse pre-prototype gyrotron will be sequentially extended for longer pulse lengths. This is made possible through a modular approach which enables an easy exchange of components. Next experimental steps with this Modular Gyrotron Concept : (1) Test other components in short pulse: different launchers, modified electron guns, different beam tunnels (2) Add CW collector and CVD window -> ~100 ms pulse length (3) Replace remaining short pulse components (cavity,q.o. system, beam tunnel, gyrotron housing) by cooled CW parts -> 10 s pulse length In parallel: broad band operation tests (around 140 GHz /1.8MW already done) S. Kern et al., Experimental results and recent developments on the EU 2 MW 170 GHz coaxial
20 Modular gyrotron setup steps Current step: First depressed collector tests Launcher test CW gun with prototype shape - cathode nose easily exchangeable 2 nd : short pulse component tests Beam tunnel, launcher, anode shape 3 rd : CW collector and window Increase of pulse length to ~ 100 ms 4th: fully CW compatible CW cooling added, new RF absorber scheme New redesigned electron gun Increase of pulse length up to 10s (KIT power supply limit) S. Kern et al., Experimental results and recent developments on the EU 2 MW 170 GHz coaxial
21 Plans for a hypothetical 2 nd CW prototype Component, topic, observation Internal absorbers, mirror box Launcher, Q.o. system Halo shield Collector Beam tunnel, parasitic modes Tube alignment Modes with wrong rotation High starting currents High body current Better cooling of shaft Any other tube component Summary Changes Remove and discuss replacement: Preferably two relief windows with or without stainless steel pipes Replace the launcher by the new version, presently under test (lower stray radiation already proven) Increase halo shield radius by 0.5-2mm To be short term optimized No change No change Revised by TED; possibility for controlled alignment tests added No change No change No change No change No change Next step activities cooled stainless steel pipes coated/uncoate d/inside carbon tubes - relief windows - mirror vessel partly or totally coated (CrO, CR 2 O 3 ) with external cooling Consider tube inspection S. Kern et al., Experimental results and recent developments on the EU 2 MW 170 GHz coaxial
22 Summary The latest test results with EU 2 MW 170 GHz coaxial cavity tubes were reported. CW prototype results: 2 MW / 170 GHz / 45 % non-optimized in very short time All design modifications validated No long pulse validation of RF performance or cooling (except collector) Tube damaged, internal RF absorber scheme needs redesign Short pulse pre-prototype results: 1.9 MW 28 % (without depressed collector, not finally conditioned) Smoothed launcher validated: stray radiation reduced to 4 % Depressed collector operation under preparation Future plans: 2 MW or 1 MW ITER development: F4E decision pending Coaxial experiments towards long pulse continue at KIT S. Kern et al., Experimental results and recent developments on the EU 2 MW 170 GHz coaxial
23 Acknowledgement The authors acknowledge gratefully the continuing support of TED and F4E staff in these projects, in particular F. Albajar, F. Cismondi and T. Bonicelli at F4E as well as R. Marchesin, C. Lievin, F. Legrande and P. Benin at TED. This work was supported by Fusion for Energy under Grant F4E-2009-GRT-049 (PMS-H.CD)-01 and within the European Gyrotron Consortium (EGYC). The views and opinions expressed herein do not necessarily reflect those of the European Commission. EGYC is a collaboration among CRPP, Switzerland; KIT, Germany; HELLAS, Greece; IFP-CNR, Italy. Thank you for your attention! S. Kern et al., Experimental results and recent developments on the EU 2 MW 170 GHz coaxial
Recent ITER-Relevant Gyrotron Tests
Journal of Physics: Conference Series Recent ITER-Relevant Gyrotron Tests To cite this article: K Felch et al 2005 J. Phys.: Conf. Ser. 25 13 View the article online for updates and enhancements. Related
More informationTEST RESULTS OF THE 84 GHZ / 200 KW / CW GYROTRON
TEST RESULTS OF THE 84 GHZ / 200 KW / CW GYROTRON V.I. Belousov, A.A.Bogdashov, G.G.Denisov, V.I.Kurbatov, V.I.Malygin, S.A.Malygin, V.B.Orlov, L.G.Popov, E.A.Solujanova, E.M.Tai, S.V.Usachov Gycom Ltd,
More informationCPI Gyrotrons For Fusion EC Heating
CPI Gyrotrons For Fusion EC Heating H. Jory, M. Blank, P. Borchard, P. Cahalan, S. Cauffman, T. S. Chu, and K. Felch CPI, Microwave Power Products Division 811 Hansen Way, Palo Alto, CA 94303, USA e-mail:
More informationDevelopment of high power gyrotron and EC technologies for ITER
1 Development of high power gyrotron and EC technologies for ITER K. Sakamoto 1), K.Kajiwara 1), K. Takahashi 1), Y.Oda 1), A. Kasugai 1), N. Kobayashi 1), M.Henderson 2), C.Darbos 2) 1) Japan Atomic Energy
More informationDEVELOPMENT OF A 10 MW SHEET BEAM KLYSTRON FOR THE ILC*
DEVELOPMENT OF A 10 MW SHEET BEAM KLYSTRON FOR THE ILC* D. Sprehn, E. Jongewaard, A. Haase, A. Jensen, D. Martin, SLAC National Accelerator Laboratory, Menlo Park, CA 94020, U.S.A. A. Burke, SAIC, San
More informationDesign, Fabrication and Testing of Gun-Collector Test Module for 6 MW Peak, 24 kw Average Power, S-Band Klystron
Available online www.ejaet.com European Journal of Advances in Engineering and Technology, 2014, 1(1): 11-15 Research Article ISSN: 2394-658X Design, Fabrication and Testing of Gun-Collector Test Module
More informationRF Power Generation II
RF Power Generation II Klystrons, Magnetrons and Gyrotrons Professor R.G. Carter Engineering Department, Lancaster University, U.K. and The Cockcroft Institute of Accelerator Science and Technology Scope
More informationDevelopment of Multiple Beam Guns for High Power RF Sources for Accelerators and Colliders
SLAC-PUB-10704 Development of Multiple Beam Guns for High Power RF Sources for Accelerators and Colliders R. Lawrence Ives*, George Miram*, Anatoly Krasnykh @, Valentin Ivanov @, David Marsden*, Max Mizuhara*,
More informationCEPC Klystron Development
CEPC Klystron Development Zusheng Zhou On behalf of High Efficiency RF Source R&D Collaboration Institute of High Energy Physics Sep. 26, 2018, HKUST, Hong Kong 1 Outline Strategy and plan 650MHz/800kW
More informationA New 4MW LHCD System for EAST
1 EXW/P7-29 A New 4MW LHCD System for EAST Jiafang SHAN 1), Yong YANG 1), Fukun LIU 1), Lianmin ZHAO 1) and LHCD Team 1) 1) Institute of Plasma Physics, Chinese Academy of Sciences, Hefei, China E-mail
More informationA HIGH POWER LONG PULSE HIGH EFFICIENCY MULTI BEAM KLYSTRON
A HIGH POWER LONG PULSE HIGH EFFICIENCY MULTI BEAM KLYSTRON A.Beunas and G. Faillon Thales Electron Devices, Vélizy, France S. Choroba DESY, Hamburg, Germany Abstract THALES ELECTRON DEVICES has developed
More informationOperating Experience and Reliability Improvements on the 5 kw CW Klystron at Jefferson Lab
Operating Experience and Reliability Improvements on the 5 kw CW Klystron at Jefferson Lab Richard Walker & Richard Nelson Jefferson Lab, Newport News VA Jefferson Lab is a $600M Department of Energy facility
More informationDevelopment of klystrons with ultimately high - 90% RF power production efficiency
Development of klystrons with ultimately high - 90% RF power production efficiency A. Baikov (MUFA), I. Syratchev (CERN), C. Lingwood, D. Constable (Lancaster University) Introduction FCC has high power
More informationLow Frequency Gyrotrons for Fusion
13th Joint Workshop on Electron Cyclotron Emission and Electron Cyclotron Resonance Heating Nizhny Novgorod, Russia May 17-20, 2004 РАН Low Frequency Gyrotrons for Fusion НПП ГИКОМ V.E. Zapevalov, Yu.K.
More informationDepartment of Electronics and Communication Engineering Shrinathji Institute of Technology & Engineering, Nathdwara (Raj.)
Sensitivity and Misalignment Analysis of MIG for 120 GHz, 3MW Gyrotron Manoj Kumar Sharma 1, Mahesh Kumar Porwal 2 1 M Tech-IV Semester, 2 Associate Professor Department of Electronics and Communication
More informationStatus of BESSY II and berlinpro. Wolfgang Anders. Helmholtz-Zentrum Berlin for Materials and Energy (HZB) 20th ESLS-RF Meeting
Status of BESSY II and berlinpro Wolfgang Anders Helmholtz-Zentrum Berlin for Materials and Energy (HZB) 20th ESLS-RF Meeting 16.-17.11.2016 at PSI Outline BESSY II Problems with circulators Landau cavity
More informationExperience with the Cornell ERL Injector SRF Cryomodule during High Beam Current Operation
Experience with the Cornell ERL Injector SRF Cryomodule during High Beam Current Operation Matthias Liepe Assistant Professor of Physics Cornell University Experience with the Cornell ERL Injector SRF
More information2 Work Package and Work Unit descriptions. 2.8 WP8: RF Systems (R. Ruber, Uppsala)
2 Work Package and Work Unit descriptions 2.8 WP8: RF Systems (R. Ruber, Uppsala) The RF systems work package (WP) addresses the design and development of the RF power generation, control and distribution
More informationKLYSTRON GUN ARCING AND MODULATOR PROTECTION
SLAC-PUB-10435 KLYSTRON GUN ARCING AND MODULATOR PROTECTION S.L. Gold Stanford Linear Accelerator Center (SLAC), Menlo Park, CA USA Abstract The demand for 500 kv and 265 amperes peak to power an X-Band
More informationIOT RF Power Sources for Pulsed and CW Linacs
LINAC 2004 Lübeck, August 16 20, 2004 IOT RF Power Sources H. Bohlen, Y. Li, Bob Tornoe Communications & Power Industries Eimac Division, San Carlos, CA, USA Linac RF source property requirements (not
More information3 cerl. 3-1 cerl Overview. 3-2 High-brightness DC Photocathode Gun and Gun Test Beamline
3 cerl 3-1 cerl Overview As described before, the aim of the cerl in the R&D program includes the development of critical components for the ERL, as well as the construction of a test accelerator. The
More information45 MW, 22.8 GHz Second-Harmonic Multiplier for High-Gradient Tests*
US High Gradient Research Collaboration Workshop. SLAC, May 23-25, 2007 45 MW, 22.8 GHz Second-Harmonic Multiplier for High-Gradient Tests* V.P. Yakovlev 1, S.Yu. Kazakov 1,2, and J.L. Hirshfield 1,3 1
More information650MHz/800kW Klystron Development at IHEP
650MHz/800kW Klystron Development at IHEP Shilun Pei, IHEP On behalf of HERSC (High Efficiency RF Source R&D Collaboration) in China Presentation at the IAS Program on High Energy Physics January 22, 2018,
More informationPulsed Klystrons for Next Generation Neutron Sources Edward L. Eisen - CPI, Inc. Palo Alto, CA, USA
Pulsed Klystrons for Next Generation Neutron Sources Edward L. Eisen - CPI, Inc. Palo Alto, CA, USA Abstract The U.S. Department of Energy (DOE) Office of Science has funded the construction of a new accelerator-based
More informationDetailed Design Report
Detailed Design Report Chapter 4 MAX IV Injector 4.6. Acceleration MAX IV Facility CHAPTER 4.6. ACCELERATION 1(10) 4.6. Acceleration 4.6. Acceleration...2 4.6.1. RF Units... 2 4.6.2. Accelerator Units...
More informationHigh-power klystrons. The benchmark in scientific research. State-of-the-art RF sources for your accelerator
> High- klystrons The benchmark in scientific research State-of-the-art RF sources for your accelerator Thales has been one of the leading manufacturers of RF and microwave sources for decades, and is
More informationESA STUDY CONTRACT REPORT SUBJECT : CONTRACTOR ESA CONTRACT N
ESA STUDY CONTRACT REPORT ESA CONTRACT N 4000101265 SUBJECT : 100W Q/V-BAND TRAVELLING WAVE TUBE ESA CR ( ) No * STAR CODE No of volumes : 1 This is volume No 1 CONTRACTOR Thales Electronic Systems GmbH
More informationRF Solutions for Science.
RF Solutions for Science www.thalesgroup.com State-of-the-art RF sources for your scientific needs High-power klystrons HIGH KLYSTRONS WITH RF LONG PULSE above 50 μs Thales has been one of the leading
More informationRF plans for ESS. Morten Jensen. ESLS-RF 2013 Berlin
RF plans for ESS Morten Jensen ESLS-RF 2013 Berlin Overview The European Spallation Source (ESS) will house the most powerful proton linac ever built. The average beam power will be 5 MW which is five
More informationSRS and ERLP developments. Andrew moss
SRS and ERLP developments Andrew moss Contents SRS Status Latest news Major faults Status Energy Recovery Linac Prototype Latest news Status of the RF system Status of the cryogenic system SRS Status Machine
More informationEPJ Web of Conferences 95,
EPJ Web of Conferences 95, 04012 (2015) DOI: 10.1051/ epjconf/ 20159504012 C Owned by the authors, published by EDP Sciences, 2015 The ELENA (Extra Low Energy Antiproton) project is a small size (30.4
More informationINFN School on Electron Accelerators. RF Power Sources and Distribution
INFN School on Electron Accelerators 12-14 September 2007, INFN Sezione di Pisa Lecture 7b RF Power Sources and Distribution Carlo Pagani University of Milano INFN Milano-LASA & GDE The ILC Double Tunnel
More informationNext Linear Collider. The 8-Pack Project. 8-Pack Project. Four 50 MW XL4 X-band klystrons installed on the 8-Pack
The Four 50 MW XL4 X-band klystrons installed on the 8-Pack The Demonstrate an NLC power source Two Phases: 8-Pack Phase-1 (current): Multi-moded SLED II power compression Produce NLC baseline power: 475
More informationX-Band Klystron Development at
X-Band Klystron Development at SLAC Slide 1 The Beginning X-band klystron work began at SLAC in the mid to late 80 s to develop high frequency (4x SLAC s-band), high power RF sources for the linear collider
More informationThis work was supported by FINEP (Research and Projects Financing) under contract
MODELING OF A GRIDDED ELECTRON GUN FOR TRAVELING WAVE TUBES C. C. Xavier and C. C. Motta Nuclear & Energetic Research Institute, São Paulo, SP, Brazil University of São Paulo, São Paulo, SP, Brazil Abstract
More informationAREAL- Phase 1. B. Grigoryan on behalf of AREAL team
AREAL- Phase 1 Progress & Status B. Grigoryan on behalf of AREAL team Contents Machine Layout Building & Infrastructure Laser System RF System Vacuum System Cooling System Control System Beam Diagnostics
More informationSummary of the 1 st Beam Line Review Meeting Injector ( )
Summary of the 1 st Beam Line Review Meeting Injector (23.10.2006) 15.11.2006 Review the status of: beam dynamics understanding and simulations completeness of beam line description conceptual design of
More informationDEVELOPMENT OF X-BAND KLYSTRON TECHNOLOGY AT SLAC
DEVELOPMENT OF X-BAND KLYSTRON TECHNOLOGY AT SLAC George Caryotakis, Stanford Linear Accelerator Center P.O. Box 4349 Stanford, CA 94309 Abstract * The SLAC design for a 1-TeV collider (NLC) requires klystrons
More informationRF Upgrades & Experience At JLab. Rick Nelson
RF Upgrades & Experience At JLab Rick Nelson Outline Background: CEBAF / Jefferson Lab History, upgrade requirements & decisions Progress & problems along the way Present status Future directions & concerns
More informationCNT FIELD EMISSION CATHODE CATALOG. XinRay Systems Inc. April 2014
CNT FIELD EMISSION CATHODE CATALOG April 2014 Version 1 1 TABLE OF CONTENTS: 1. ABBREVIATIONS... 2 2. INTRODUCTION... 3 3. PRODUCT AT A GLANCE... 6 4. CARBON NANOTUBE (CNT) CATHODE INFORMATION CHART*...
More informationPseudospark-sourced Micro-sized Electron Beams for High Frequency klystron Applications
Pseudospark-sourced Micro-sized Electron Beams for High Frequency klystron Applications H. Yin 1*, D. Bowes 1, A.W. Cross 1, W. He 1, K. Ronald 1, A. D. R. Phelps 1, D. Li 2 and X. Chen 2 1 SUPA, Department
More informationScreen investigations for low energetic electron beams at PITZ
1 Screen investigations for low energetic electron beams at PITZ S. Rimjaem, J. Bähr, H.J. Grabosch, M. Groß Contents Review of PITZ setup Screens and beam profile monitors at PITZ Test results Summary
More informationPerformance of a DC GaAs photocathode gun for the Jefferson lab FEL
Nuclear Instruments and Methods in Physics Research A 475 (2001) 549 553 Performance of a DC GaAs photocathode gun for the Jefferson lab FEL T. Siggins a, *, C. Sinclair a, C. Bohn b, D. Bullard a, D.
More informationStatus of CTF3. G.Geschonke CERN, AB
Status of CTF3 G.Geschonke CERN, AB CTF3 layout CTF3 - Test of Drive Beam Generation, Acceleration & RF Multiplication by a factor 10 Drive Beam Injector ~ 50 m 3.5 A - 2100 b of 2.33 nc 150 MeV - 1.4
More informationCommissioning the TAMUTRAP RFQ cooler/buncher. E. Bennett, R. Burch, B. Fenker, M. Mehlman, D. Melconian, and P.D. Shidling
Commissioning the TAMUTRAP RFQ cooler/buncher E. Bennett, R. Burch, B. Fenker, M. Mehlman, D. Melconian, and P.D. Shidling In order to efficiently load ions into a Penning trap, the ion beam should be
More informationHigh QE Photocathodes lifetime and dark current investigation
High QE Photocathodes lifetime and dark current investigation Paolo Michelato INFN Milano - LASA Main Topics High QE photocathode lifetime QE vs. time (measurements on several cathodes, FLASH data) QE
More informationChris Gilmour Studies into the Design of a Higher Efficiency Ku Band ring-loop Travelling Wave Tube SWS using the CST PIC Software.
Chris Gilmour Studies into the Design of a Higher Efficiency Ku Band ring-loop Travelling Wave Tube SWS using the CST PIC Software.... the power in microwaves! History TMD have been making ring-loop TWTs
More informationSLS RF operation report 2003
SLS RF operation report 2003 M. Pedrozzi, Jean-Yves Raguin Paul Scherrer Institute, 5232 Villigen PSI, Switzerland SUMMARY LINAC report SR Superconducting Third Harmonic system report SR 500 MHz system
More informationK800 RF AMPLIFIER TUBE UPGRADE
R. F. Note 107 John Vincent August 5, 1988 K800 RF AMPLIFIER TUBE UPGRADE Contents: 1. Introduction 2. RCA 4648 Operating Experience and Evaluation. 3. Tube Selection Criteria 4. Cost and Availability
More informationOptimization of a triode-type cusp electron gun for a W-band gyro-twa
Optimization of a triode-type cusp electron gun for a W-band gyro-twa Liang Zhang, 1, a) Craig R. Donaldson, 1 and Wenlong He 1 Department of Physics, SUPA, University of Strathclyde, Glasgow, G4 0NG,
More informationUpgrading LHC Luminosity
1 Upgrading LHC Luminosity 2 Luminosity (cm -2 s -1 ) Present (2011) ~2 x10 33 Beam intensity @ injection (*) Nominal (2015?) 1 x 10 34 1.1 x10 11 Upgraded (2021?) ~5 x10 34 ~2.4 x10 11 (*) protons per
More informationThe Construction Status of CSNS Linac
The Construction Status of CSNS Linac Sheng Wang Dongguan branch, Institute of High Energy Physics, CAS Sep.2, 2014, Geneva Outline The introduction to CSNS accelerators The commissoning of ion source
More informationIOT OPERATIONAL EXPERIENCE ON ALICE AND EMMA AT DARESBURY LABORATORY
IOT OPERATIONAL EXPERIENCE ON ALICE AND EMMA AT DARESBURY LABORATORY A. Wheelhouse ASTeC, STFC Daresbury Laboratory ESLS XVIII Workshop, ELLETRA 25 th 26 th November 2010 Contents Brief Description ALICE
More informationFinal Report. U.S. Department of Energy Grant Number DE-FG02-04ER83916
Development of a 200 MHz Multiple Beam Klystron Final Report U.S. Department of Energy Grant Number DE-FG02-04ER83916 July 2004 - March 2005 Calabazas Creek Research, Inc. 20937 Comer Drive Saratoga, CA
More informationCEBAF 8 kw CW KLYSTRON SPECIFICATION EE0043, Rev. H January 15, 1998
Thomas Jefferson National Laboratory Specification CEBAF 8 kw CW KLYSTRON SPECIFICATION EE0043, Rev. H January 15, 1998 Approved by: Richard Nelson Date William Merz Date Claus Rode Date EE0044, Rev. H
More informationTECHNICAL SPECIFICATION Multi-beam S-band Klystron type BT267
TECHNICAL SPECIFICATION Multi-beam S-band Klystron type BT267 The company was created for the development and manufacture of precision microwave vacuum-electron-tube devices (VETD). The main product areas
More informationHigh Brightness Injector Development and ERL Planning at Cornell. Charlie Sinclair Cornell University Laboratory for Elementary-Particle Physics
High Brightness Injector Development and ERL Planning at Cornell Charlie Sinclair Cornell University Laboratory for Elementary-Particle Physics June 22, 2006 JLab CASA Seminar 2 Background During 2000-2001,
More informationDESIGN AND PERFORMANCE OF L-BAND AND S-BAND MULTI BEAM KLYSTRONS
DESIGN AND PERFORMANCE OF L-BAND AND S-BAND MULTI BEAM KLYSTRONS Y. H. Chin, KEK, Tsukuba, Japan. Abstract Recently, there has been a rising international interest in multi-beam klystrons (MBK) in the
More informationThe field cage for a large TPC prototype
EUDET The field cage for a large TPC prototype T.Behnke, L. Hallermann, P. Schade, R. Diener December 7, 2006 Abstract Within the EUDET Programme, the FLC TPC Group at DESY in collaboration with the Department
More informationPulses inside the pulse mode of operation at RF Gun
Pulses inside the pulse mode of operation at RF Gun V. Vogel, V. Ayvazyan, K. Floettmann, D. Lipka, P. Morozov, H. Schlarb, S. Schreiber FLASH Seminar, DESY March 29, 2011 Contents Why we need a PiPmode
More informationPhotoinjector Laser Operation and Cathode Performance
Photoinjector Laser Operation and Cathode Performance Daniele Sertore, INFN Milano LASA Siegfried Schreiber, DESY Laser operational experience Laser beam properties Cathode performances Outlook TTF and
More informationPUBLICATION. Measurement setup at light source operational: Milestone M4.3
CERN-ACC-2016-0110 Future Circular Collider PUBLICATION Measurement setup at light source operational: Milestone M4.3 Perez, Francis (ALBA) et al. 24 August 2016 The European Circular Energy-Frontier Collider
More information!"!3
Abstract A single-mode 500 MHz superconducting cavity cryomodule has been developed at Cornell for the electronpositron collider/synchrotron light source CESR. The Cornell B-cell cavity belongs to the
More informationStatus of the FAIR Project. Jürgen Henschel FAIR Project Leader / Technical Director GSI & FAIR
Status of the FAIR Project Jürgen Henschel FAIR Project Leader / Technical Director GSI & FAIR Finland France Germany India Poland Romania Russia Slovenia Sweden UK FAIR Strategic objectives FAIR phase
More informationDesign Studies For The LCLS 120 Hz RF Gun Injector
BNL-67922 Informal Report LCLS-TN-01-3 Design Studies For The LCLS 120 Hz RF Gun Injector X.J. Wang, M. Babzien, I. Ben-Zvi, X.Y. Chang, S. Pjerov, and M. Woodle National Synchrotron Light Source Brookhaven
More informationTeltron Delection Tube D
Teltron Delection Tube D 1011119 Overview The electron-beam deflection tube is intended for investigating the deflection of electron beams in electrical and magnetic fields. It can be used to estimate
More informationEUROFEL-Report-2007-DS EUROPEAN FEL Design Study
EUROFEL-Report-2007-DS4-095 EUROPEAN FEL Design Study Deliverable N : D 4.3 Deliverable Title: Task: Authors: Generation of 3rd harmonic photons at 90 nm DS-4 see next page Contract N : 011935 Project
More informationPresent Status and Future Upgrade of KEKB Injector Linac
Present Status and Future Upgrade of KEKB Injector Linac Kazuro Furukawa, for e /e + Linac Group Present Status Upgrade in the Near Future R&D towards SuperKEKB 1 Machine Features Present Status and Future
More informationOperation of CEBAF photoguns at average beam current > 1 ma
Operation of CEBAF photoguns at average beam current > 1 ma M. Poelker, J. Grames, P. Adderley, J. Brittian, J. Clark, J. Hansknecht, M. Stutzman Can we improve charge lifetime by merely increasing the
More informationFirst Simultaneous Top-up Operation of Three Different Rings in KEK Injector Linac
First Simultaneous Top-up Operation of Three Different Rings in KEK Injector Linac Masanori Satoh (Acc. Lab., KEK) for the injector upgrade group 2010/9/16 1 Overview of Linac Beam Operation 2010/9/16
More informationANKA RF System - Upgrade Strategies
ANKA RF System - Upgrade Strategies Vitali Judin ANKA Synchrotron Radiation Facility 2014-09 - 17 KIT University of the State Baden-Wuerttemberg and National Laboratory of the Helmholtz Association www.kit.edu
More informationIOT Charakterization at BESSY ( HZB)
IOT Charakterization at BESSY ( HZB) Agenda: Wolfgang Anders, Hans Georg Hoberg, Andreas Heugel BESSY, Berlin ESLS-RF Workshop 1.-2.10.2008 Diamond BESSY + HMI HZB MLS in Operation Bessy Transmitter IOT
More informationTOSHIBA Industrial Magnetron E3328
TOSHIBA E3328 is a fixed frequency continuous wave magnetron intended for use in the industrial microwave heating applications. The average output power is 3kW in the frequency range from 2450 to 2470
More information3B SCIENTIFIC PHYSICS
B SCIENTIFIC PHYSICS Triode S 11 Instruction sheet 1/15 ALF 1 5 7 1 Guide pin Connection pins Cathode plate Heater filament 5 Grid Anode 7 -mm plug for connecting anode 1. Safety instructions Hot cathode
More informationCLIC Feasibility Demonstration at CTF3
CLIC Feasibility Demonstration at CTF3 Roger Ruber Uppsala University, Sweden, for the CLIC/CTF3 Collaboration http://cern.ch/clic-study LINAC 10 MO303 13 Sep 2010 The Key to CLIC Efficiency NC Linac for
More informationADVANCED HIGH-POWER MICROWAVE VACUUM ELECTRON DEVICE DEVELOPMENT
ADVANCED HIGH-POWER MICROWAVE VACUUM ELECTRON DEVICE DEVELOPMENT H. P. Bohlen, Inc., Palo Alto, CA Abstract The microwave 1 power requirements of particle accelerators have been growing almost exponentially
More informationTowards an X-Band Power Source at CERN and a European Structure Test Facility
Towards an X-Band Power Source at CERN and a European Structure Test Facility Erk Jensen and Gerry McMomagle CERN The X-Band Accelerating Structure Design and Test-Program Workshop Day 2: Structure Testing
More informationLinac 4 Instrumentation K.Hanke CERN
Linac 4 Instrumentation K.Hanke CERN CERN Linac 4 PS2 (2016?) SPL (2015?) Linac4 (2012) Linac4 will first inject into the PSB and then can be the first element of a new LHC injector chain. It will increase
More informationHall-B Beamline Commissioning Plan for CLAS12
Hall-B Beamline Commissioning Plan for CLAS12 Version 1.5 S. Stepanyan December 19, 2017 1 Introduction The beamline for CLAS12 utilizes the existing Hall-B beamline setup with a few modifications and
More informationGENCOA Key Company Facts. GENCOA is a private limited company (Ltd) Founded 1995 by Dr Dermot Monaghan. Located in Liverpool, UK
GENCOA Key Company Facts GENCOA is a private limited company (Ltd) Founded 1995 by Dr Dermot Monaghan Located in Liverpool, UK Employs 34 people 6 design (Pro E 3D CAD) 4 process development & simulation
More informationSRF-gun Development Overview. J. Sekutowicz 17 th September, 2015 SRF15, Whistler, Canada
SRF-gun Development Overview J. Sekutowicz 17 th September, 2015 SRF15, Whistler, Canada Acknowledgment Many thanks to: A. Arnold, J. Hao, E. Kako, T. Konomi, D. Kostin, J. Lorkiewicz, A. Neumann, J. Teichert
More informationRF Power Klystrons & 20 Year Look. R. Nelson 7/15/15
RF Power Klystrons & 20 Year Look R. Nelson 7/15/15 RF Power klystrons 8 x 13 kw klystrons Page 2 Why A klystron? Best (only) choice at the time - 1988 Easy to use: Input (drive), output (to CM), power
More informationCyclotron Institute upgrade project. H. L. Clark, F. Abegglen, G. Chubarian, G. Derrig, G. Kim, D. May, and G. Tabacaru
Cyclotron Institute upgrade project H. L. Clark, F. Abegglen, G. Chubarian, G. Derrig, G. Kim, D. May, and G. Tabacaru On January 3, 2005 the Cyclotron Institute Upgrade Project (CIUP) began with the approval
More informationPEP II Design Outline
PEP II Design Outline Balša Terzić Jefferson Lab Collider Review Retreat, February 24, 2010 Outline General Information Parameter list (and evolution), initial design, upgrades Collider Ring Layout, insertions,
More informationCathode Studies at FLASH: CW and Pulsed QE measurements
Cathode Studies at FLASH: CW and Pulsed QE measurements L. Monaco, D. Sertore, P. Michelato S. Lederer, S. Schreiber Work supported by the European Community (contract number RII3-CT-2004-506008) 1/27
More informationRUNNING EXPERIENCE OF FZD SRF PHOTOINJECTOR
RUNNING EXPERIENCE OF FZD SRF PHOTOINJECTOR Rong Xiang On behalf of the BESSY-DESY-FZD-MBI collaboration and the ELBE team FEL 2009, Liverpool, United Kingdom, August 23 ~ 28, 2009 Outline Introduction
More informationDELIVERY RECORD. Location: Ibaraki, Japan
DELIVERY RECORD Client: Japan Atomic Energy Agency (JAEA) High Energy Accelerator Research Organization (KEK) Facility: J-PARC (Japan Proton Accelerator Research Complex) Location: Ibaraki, Japan 1 October
More informationOak Ridge Spallation Neutron Source Proton Power Upgrade Project and Second Target Station Project
Oak Ridge Spallation Neutron Source Proton Power Upgrade Project and Second Target Station Project Workshop on the future and next generation capabilities of accelerator driven neutron and muon sources
More informationTechnical Procedure for Scanning Electron Microscope/ Energy Dispersive X-Ray System (SEM/EDX) for non-gsr Casework
Technical Procedure for Scanning Electron Microscope/ Energy Dispersive X-Ray System (SEM/EDX) for non-gsr Casework 1.0 Purpose This technical procedure shall be followed for the operation of the Scanning
More informationDesign and Simulation of High Power RF Modulated Triode Electron Gun. A. Poursaleh
Design and Simulation of High Power RF Modulated Triode Electron Gun A. Poursaleh National Academy of Sciences of Armenia, Institute of Radio Physics & Electronics, Yerevan, Armenia poursaleh83@yahoo.com
More informationThe SLAC Polarized Electron Source *
SLAC-PUB-9509 October 2002 The SLAC Polarized Electron Source * J. E. Clendenin, A. Brachmann, T. Galetto, D.-A. Luh, T. Maruyama, J. Sodja, and J. L. Turner Stanford Linear Accelerator Center, 2575 Sand
More informationLASER REGISTRATION FORM (LS-1)
Appendix 1 LASER REGISTRATION FORM (LS-1) LASER REGISTRATION FORM (LS-1) Laser Ref. No: Supervisor Training Example Policy Note: This form is to be completed and a copy sent to the Departmental Laser Supervisor,
More informationStatus of RF Power and Acceleration of the MAX IV - LINAC
Status of RF Power and Acceleration of the MAX IV - LINAC Dionis Kumbaro ESLS RF Workshop 2015 MAX IV Laboratory A National Laboratory for synchrotron radiation at Lunds University 1981 MAX-lab is formed
More informationKarin Rathsman, Håkan Danared and Rihua Zeng. Report from RF Power Source Workshop
Accelerator Division ESS AD Technical Note ESS/AD/0020 Karin Rathsman, Håkan Danared and Rihua Zeng Report from RF Power Source Workshop 10 July 2011 Report on the RF Power Source Workshop K. Rathsman,
More informationJefferson Lab Experience with Beam Halo, Beam Loss, etc.
Jefferson Lab Experience with Beam Halo, Beam Loss, etc. Pavel Evtushenko with a lot of input from many experienced colleagues Steve Benson, Dave Douglas, Kevin Jordan, Carlos Hernandez-Garcia, Dan Sexton,
More informationDevelopment of High Power Vacuum Tubes for Accelerators and Plasma Heating
Development of High Power Vacuum Tubes for Accelerators and Plasma Heating Vishnu Srivastava Microwave Tubes Division, CSIR-Central Electronics Engineering Research Institute, Pilani-333031, Rajasthan,
More informationStatus of SOLARIS. Paweł Borowiec On behalf of Solaris Team
Status of SOLARIS Paweł Borowiec On behalf of Solaris Team e-mail: pawel.borowiec@uj.edu.pl XX ESLS-RF Meeting, Villingen 16-17.11.2016 Outline 1. Timeline 2. Injector 3. Storage ring 16-17.11.2016 XX
More informationA PASSION FOR PERFECTION. OktaLine. The Power Pump Portfolio. Roots Pumps for Every Low and Medium Vacuum Application.
A PASSION FOR PERFECTION OktaLine The Power Pump Portfolio. Roots Pumps for Every Low and Medium Vacuum Application. OktaLine The Power Pump Portfolio. Roots Pumps for Every Low and Medium Vacuum Application.
More informationPEP II STATUS AND PLANS *
PEP II STATUS AND PLANS * John T. Seeman + Stanford Linear Accelerator Center, Stanford University, Stanford, CA 94309 USA The PEP II B-Factory 1 project is an e + e - colliding beam storage ring complex
More informationReview of Diamond SR RF Operation and Upgrades
Review of Diamond SR RF Operation and Upgrades Morten Jensen on behalf of Diamond Storage Ring RF Group Agenda Stats X-ray and LN2 pressure results Cavity Failure Conditioning in the RFTF Cavity Simulations
More information