The VARIAN 250 MeV Superconducting Compact Proton Cyclotron

Size: px
Start display at page:

Download "The VARIAN 250 MeV Superconducting Compact Proton Cyclotron"

Transcription

1

2 The VARIAN 250 MeV Superconducting Compact Proton Cyclotron VARIAN Medical Systems Particle Therapy GmbH Friedrich-Ebert-Str. 1 D BERGISCH GLADBACH GERMANY

3 OUTLINE 1. Why having a Superconducting Cyclotron? 2. Machine Key Data 3. Operating VARIAN Machines Uptime Statistics Automated Operation (Startup + Optimization) 4. Production of Next Machines Production Site Factory Assembly Test Cells and Beam Testing 5. Recent Developments Solid State Amplifier Digital Low Level RF RF Commissioning Results 6. Conclusion 3

4 Why having a Superconducting Cyclotron? Why having a superconducting cyclotron? It s fascinating technology! A cyclotron is an elegant solution for efficiently generating high energy beams with a compact, reliable and cost-effective machine. There are high magnetic fields! There s superconductivity! (It s cool ) There is non-trivial RF technology! There are plasmas! It s applied relativity! Let s see if we find some quantum mechanics involved 4

5 Why having a Superconducting Cyclotron? This is what I tell my team on one hand 5

6 Why having a Superconducting Cyclotron? This is what I tell my team on one hand but on the other hand it is clear for everybody that these are unfortunately not the points that drive a business. VARIAN s commitment to this technology derives from a different approach. Timothy E. Guertin VARIAN s President and Chief Executive Officer: Varian Medical Systems mission is to explore and develop radiation technology that protects and saves lives. Our goal is to help save 100,000 more lives each year. That s enough to fill a large stadium. To meet this challenge, we equip the world with new tools for fighting cancer [ ]. The people of Varian Medical Systems share this mission and goal. Together, we are a partner for life. 6

7 Why having a Superconducting Cyclotron? We want to achieve this mission goal by providing the best tumor treatment delivery available, which currently is pencil beam scanning of energetic particles. (You will hear evidence for this in other talks during this workshop.) Technical boundary: Beam scanning requires a stable, intense cw beam, everything else makes the whole thing much more complicated. Commercial boundary: Particle therapy requires a large invest of the customer for building, technical equipment, and other infrastructure. To keep this limited to a reasonable amount we restrict ourselves to protons and small building footprints. This marks the boundary conditions for the accelerator: The machine of choice here is a compact isochronous AVF cyclotron. 7

8 Why having a Superconducting Cyclotron? Looking a bit deeper, it turns out that a superconducting cyclotron brings along even more advantages: Superconducting coil, low power consumption High magnetic field possible Small machine, high beam energy Saturated iron Larger pole gap over full radius High extraction efficiency, high beam currents Reproducible field and beam operation 8 Practically operator-free operation Low activation Fast access, easy maintenance, high uptime

9 VARIAN PT SC Cyclotron Key Data (Engineering Goals) Beam - Energy 250 MeV - Extracted current (max) 800 na - Emittance of extracted beam < 3 / 5 π mm mrad (2σ) - Momentum spread p/p ±0.04% (i.e. 250MeV) - Number of turns Extraction efficiency (multi-turn extraction mode) ~80% - Dynamic range for intensity modulation 1:800 - Fast intensity modulation via electrostatic deflector, >10% in 100 µs Iron Yoke - Outer diameter 3.1 m - Height 1.6 m - Weight <90 t SC Magnet - Stored energy 2.5 MJ - Central field 2.4 T - Max. field at the coil <4 T - Operating current 160 A - Rated power of cryocoolers 40 kw RF System - Frequency 72.8 MHz (2 nd harmonic) - Voltage source to puller extraction radius 80 kv / 130 kv - RF power 115 kw 9

10 VARIAN SC Proton Cyclotron Facility Integration 10

11 3. Operating Machines Uptime Statistics Automated Operation Morning Startup Optimization Procedures 11

12 Operating VARIAN PT SC Cyclotrons 1. Paul Scherrer Institut PSI (CH), treating patients since beginning of Rinecker Proton Therapy Center RPTC (D), treating patients since beginning of The RPTC facility is widely equipped with VARIAN technology, like superconducting compact 250 MeV proton cyclotron degrader for energy adjustment energy selection system for energy filtering beam lines for beam transportation 4 rotational isocentric gantries for 360 irradiation + 1 fixed beam for head / neck treatments delivery nozzles providing pencil beam spot scanning safety systems treatment control software 12

13 Uptime during Patient Treatment Ramp-Up RPTC presentation on PTCOG 48 conference 6 months after start of operation: Poster presented by RPTC at PTCOG 48 13

14 RPTC Operating Time / Facility Uptime User at RPTC treats patients up to 6 days/week, 8-10 hrs/day All 4 scanning gantries are clinical Upgrade of gantry / scanning nozzle functionality is still continued during nights and weekends Treatment facility including cyclotron is operated 24hrs on 6-7 days/week Service is performed every Sunday The RPTC uptime of 97% for the complete treatment facility since startup was determined by the user for daily patient treatment The Superconducting Cyclotron has of course a higher uptime (PSI > 99%) How is this achieved? Reliable Machine Reproducible Conditions Fully Automated Control System 14

15 Automated Morning Startup Procedure Cyclotron is in overnight state (sc magnet on, RF reduced or off) What happens after pressing and? Devices change their state (e.g. ramp-up of power supplies)... controlled by transition functions. Cyclotron reaches fully automatic the state 15

16 Automated Cyclotron Startup: 10min to Beam Devices Ramp-Up Automatic Phase Calibration Automatic Phase Regulation Beam Operation I magnet = I 0 I magnet = I (iron temp) I magnet = I (beam phase) P RF = P full P RF = P reduced U extr.defl = std U defl = U beam off I IS = std I beam within specification H 2 flow = std t / min 16

17 Automated Optimization Procedures Example: Beam Centering Parameters, e.g. start values, step widths, limits, Actual values of field bump before / after automatic optimization 17

18 Automated Optimization Procedures Badly centered beam orbit precession detected on moving head of a straight probe: Field Bump Starting Point Beam Centering: Graphics Output Optimization of Phase and Amplitude for Centering Field Bump Optimized Field Bump 18

19 Automated Optimization Procedures Slit Opening Offsets Slit Positioning Beam Current Transmission Check Beam Suppression Measurement RF Power Scan Beam Centering Extraction Field Bump Optimization Extraction Deflector Optimization 19

20 4. Production of Next Machines Production Site Factory Assembly Test Cells and Beam Testing 20

21 VARIAN PT Production Site Overview Production site near Cologne / Germany Allows assembly of up to 6 cyclotrons in parallel 21

22 VARIAN PT Production Site Overview Production site near Cologne / Germany Allows assembly of up to 6 cyclotrons in parallel and the corresponding beamline modules. 22

23 Production of Next Machines Fine machined iron and all major components for the next cyclotrons are ready; next coil windings are finished and assembly of pole caps is underway. Long lead items (especially iron yokes) for the following machines are ordered. Build sequence is ramped up from ~2 cyclotrons per year at the moment magnetic testing coil winding machine assembly cryostat welding incoming pole caps and yoke rings 23

24 VARIAN PT SC Cyclotrons Factory Commissioning Cyclotron #3 is completely pre-assembled at Varian s PT manufacturing premises. It has passed the testing and shimming of the superconducting magnet and is currently tested (with beam!) in the factory. It will be shipped in summer to its destination in 2 large lots (upper / lower part). 24

25 Cyclotron and Scanning Nozzle Test Cells 25

26 Cyclotron and Scanning Nozzle Test Cells Adjacent to the manufacturing hall VARIAN has built concrete bunkers for cyclotron and scanning nozzle tests. This enables the delivery of fully factory beam tested systems. Cyclotron #3 is currently operated in one of these Test Cells. 26

27 Cyclotron and Scanning Nozzle Test Cells 27

28 Cyclotron and Scanning Nozzle Test Cells All RF components Ion source Slit systems Extractors Diagnostics etc. are currently undergoing a system integration and beam FAT. 28

29 5. Recent Developments Solid State Amplifier Digital Low Level RF RF Commissioning Results 29

30 Recent Developments: Solid State RF Amplifier RF power amplifier used at PSI and RPTC: 3-stage tetrode tube based several electrical cabinets for power transformers, high voltage supplies, and the tubes New design in use transistor based 120 parallel working RF power modules in 6 cabinets Supplied by Cryoelectra GmbH 30

31 Recent Developments: Solid State RF Amplifier Test setup completed a >1000h test Allowed reflected power limit >15% Via its redundancy, the design features a higher - availability, - serviceability, - cost reduction,... The digitally controlled modularized system provides extended diagnostics capabilities. 31

32 Recent Developments: Digital LLRF VARIAN will use a digital LLRF with its future systems. The dllrf is already integrated into the cyclotron system that is currently under test. Like the SSAmp, the dllrf is designed for high redundancy. This yields a high fault tolerance and increases system uptime. The dllrf is faster than the previously used system and provides much more diagnostic signals and functionality. 32

33 Recent Developments: RF Commissioning Results Solid State Amplifier & Digital LLRF Very Fast RF Conditioning in Pulsed Mode (5% - 20% duty cycle) Work on Cyclotron Hardware, in parallel: dllrf Calibrations Cavity Check 33

34 Developments: Digital LLRF Control System 34

35 RF Ramp-Up to 120kW ~1 minute 35

36 Conclusion The VARIAN Superconducting Compact Proton Cyclotrons feature superior properties that make them turn-key operational machines and predestine them for use in pencil beam scanning therapy. cw beam high energy 2 of such cyclotrons are already in clinical use. high current stable beam position Several more machines are in production. small footprint high extraction All machines will be factory tested with beam. efficiency low activation VARIAN is continuously developing its technology fast and easy access further and introducing new features. for maintenance Recent breakthrough developments include high uptime Transistor RF Power Amplifiers and operator-free operation Digital Low Level RF electronics. low power consumption 36

37 THANK YOU! Students, talk to us! Our team is continuously growing 37

38 The VARIAN 250MeV Superconducting Compact Proton Cyclotron 38

COMMISSIONING OF THE ACCEL 250 MEV PROTON CYCLOTRON

COMMISSIONING OF THE ACCEL 250 MEV PROTON CYCLOTRON COMMISSIONING OF THE ACCEL 250 MEV PROTON CYCLOTRON A.E. Geisler, J. Hottenbacher, H.-U. Klein, D. Krischel, H. Röcken, M. Schillo, T. Stephani, J.H. Timmer, Accel Instruments GmbH, Bergisch Gladbach,

More information

Superconducting Medical Accelerators at IBA

Superconducting Medical Accelerators at IBA Superconducting Medical Accelerators at IBA Wiel Kleeven and Eric Forton on behalf of IBA 1), AIMA 2) JINR 3) ASG 4) Sigmaphi 5) 1) Ion Beam Applications, Louvain-la-Neuve, Belgium 2) AIMA, Developpement,

More information

OPTIMIZED MAGNET FOR A 250 MEV PROTON RADIOTHERAPY CYCLOTRON

OPTIMIZED MAGNET FOR A 250 MEV PROTON RADIOTHERAPY CYCLOTRON OPTIMIZED MAGNET FOR A 250 MEV PROTON RADIOTHERAPY CYCLOTRON J. Kim and H. Blosser 1. Introduction The design of a K250 superconducting cyclotron has been recently improved from the original design of

More information

HITACHI Proton Therapy System with Spot Scanning

HITACHI 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 information

200 MHz 350 MHz 750 MHz Linac2 RFQ2 202 MHz 0.5 MeV /m Weight : 1000 kg/m Ext. diameter : 45 cm

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 information

The Current Cyclotron Development Activities at CIAE. Current acyclotron

The 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 information

1.8 MW Upgrade of the PSI Proton Accelerator Facility

1.8 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 information

RF Upgrade at DELTA. P. Hartmann DELTA, TU Dortmund

RF 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 information

Evaluation of STPA in the Safety Analysis of the Gantry 2 Proton Radiation Therapy System Martin Rejzek, Paul Scherrer Institute, Switzerland

Evaluation of STPA in the Safety Analysis of the Gantry 2 Proton Radiation Therapy System Martin Rejzek, Paul Scherrer Institute, Switzerland Evaluation of STPA in the Safety Analysis of the Gantry 2 Proton Radiation Therapy System Martin Rejzek, Paul Scherrer Institute, Switzerland 11.04.2012 STAMP/STPA Workshop - Massachusetts Institute of

More information

Mapping of the New IBA Superconducting Synchrocyclotron (S2C2) for Proton Therapy

Mapping of the New IBA Superconducting Synchrocyclotron (S2C2) for Proton Therapy Mapping of the New IBA Superconducting Synchrocyclotron (S2C2) for Proton Therapy J. Van de Walle, W. Kleeven, C. L'Abbate, Y. Paradis, V. Nuttens - IBA M. Conjat, J. Mandrillon, P. Mandrillon - AIMA Developpement

More information

New Tracking Gantry-Synchrotron Idea. G H Rees, ASTeC, RAL, U.K,

New 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 information

LINAC EXPERIENCE IN THE FIRST TWO YEARS OF CNAO (CENTRO NAZIONALE ADROTERAPIA ONCOLOGICA)

LINAC EXPERIENCE IN THE FIRST TWO YEARS OF CNAO (CENTRO NAZIONALE ADROTERAPIA ONCOLOGICA) LINAC EXPERIENCE IN THE FIRST TWO YEARS OF OPERATION @ CNAO (CENTRO NAZIONALE ADROTERAPIA ONCOLOGICA) S. Vitulli, E. Vacchieri, CNAO Foundation, Pavia, Italy A. Reiter, B. Schlitt, GSI, Darmstadt, Germany

More information

Pedroni Eros Paul Scherrer Institute - Villigen PSI, Switzerland

Pedroni Eros Paul Scherrer Institute - Villigen PSI, Switzerland Pedroni Eros Paul Scherrer Institute - Villigen PSI, Switzerland Center for proton therapy - PSI Gantry 2, the next generation gantry of PSI: a new system for promoting pencil beam scanning as a universal

More information

SUPERCONDUCTING GANTRY AND OTHER DEVELOPMENTS AT HIMAC

SUPERCONDUCTING GANTRY AND OTHER DEVELOPMENTS AT HIMAC SUPERCONDUCTING GANTRY AND OTHER DEVELOPMENTS AT HIMAC Y. Iwata *, K. Noda, T. Shirai, T. Murakami, T. Fujita, T. Furukawa, K. Mizushima, Y. Hara, S. Suzuki, S. Sato, and K. Shouda, NIRS, 4-9-1 Anagawa,

More information

Present 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 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 information

Pedroni Eros Paul Scherrer Institute - Villigen PSI, Switzerland

Pedroni Eros Paul Scherrer Institute - Villigen PSI, Switzerland Pedroni Eros Paul Scherrer Institute - Villigen PSI, Switzerland Center for proton therapy - PSI GANTRY DESIGN AND RECENT EXPERIENCE AT PSI 2nd Workshop on Hadron Beam Therapy of Cancer ERICE May 23 th,

More information

Tutorial 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 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 information

HIGH MAGNETIC FIELD SUPERCONDUCTING MAGNETS FABRICATED IN BUDKER INP FOR SR GENERATION

HIGH MAGNETIC FIELD SUPERCONDUCTING MAGNETS FABRICATED IN BUDKER INP FOR SR GENERATION HIGH MAGNETIC FIELD SUPERCONDUCTING MAGNETS FABRICATED IN BUDKER INP FOR SR GENERATION K.V. Zolotarev *, A.M. Batrakov, S.V. Khruschev, G.N. Kulipanov, V.H. Lev, N.A. Mezentsev, E.G. Miginsky, V.A. Shkaruba,

More information

DESIGN AND CONSTRUCTION PROGRESS OF CYCIAE-100, A 100 MEV H- CYCLOTRON AT CIAE *

DESIGN AND CONSTRUCTION PROGRESS OF CYCIAE-100, A 100 MEV H- CYCLOTRON AT CIAE * DESIGN AND CONSTRUCTION PROGRESS OF CYCIAE-100, A 100 MEV H- CYCLOTRON AT CIAE * CYCIAE-100 Project Team, Written by Tianjue Zhang #, Zhenguo Li and Chengjie Chu China Institute of Atomic Energy, P.O.Box

More information

Gantry design and experience at PSI

Gantry design and experience at PSI Gantry design and experience at PSI Eros Pedroni for the R&D Technology Team Center for Proton Therapy Paul Scherrer Institute Villigen-PSI SWITZERLAND Workshop on Hadron Beam Therapy of Cancer Erice April

More information

CEBAF Overview June 4, 2010

CEBAF 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

3 General layout of the XFEL Facility

3 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 information

History and Products

History and Products History and Products 1963-1992 - 2009 Cryoelectra GmbH ELBE Workshop in Dresden-Rossendorf 14. März 2013 Early University Work 1966 (Bonn University) Work in digital controlled electronics for particle

More information

Status of Proton Beam Commissioning at MedAustron Ion Beam Therapy Center

Status of Proton Beam Commissioning at MedAustron Ion Beam Therapy Center Status of Proton Beam Commissioning at MedAustron Ion Beam Therapy Center A. Garonna, A. Wastl, C. Kurfuerst, T. Kulenkampff, C. Schmitzer, L. Penescu, M. Pivi, M. Kronberger, F. Osmic, P. Urschuetz On

More information

STATUS OF THE KOLKATA K500 SUPERCONDUCTING CYCLOTRON

STATUS OF THE KOLKATA K500 SUPERCONDUCTING CYCLOTRON STATUS OF THE KOLKATA K500 SUPERCONDUCTING CYCLOTRON Rakesh K. Bhandari (for VECC Staff) Variable Energy Cyclotron Centre, Department of Atomic Energy, Kolkata 700 064, India Abstract A superconducting

More information

FLASH at DESY. FLASH. Free-Electron Laser in Hamburg. The first soft X-ray FEL operating two undulator beamlines simultaneously

FLASH 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 information

Acceleration 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 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 information

COCIR SELF-REGULATORY INITIATIVE FOR MEDICAL IMAGING EQUIPMENT COMPUTED TOMOGRAPHY MEASUREMENT OF ENERGY CONSUMPTION

COCIR SELF-REGULATORY INITIATIVE FOR MEDICAL IMAGING EQUIPMENT COMPUTED TOMOGRAPHY MEASUREMENT OF ENERGY CONSUMPTION COCIR SELF-REGULATORY INITIATIVE FOR MEDICAL IMAGING EQUIPMENT COMPUTED TOMOGRAPHY MEASUREMENT OF ENERGY CONSUMPTION Revision: 1 Date: June 2015 Approved: June 2015 TABLE OF CONTENT 1. INTRODUCTION...

More information

STATUS OF THE SUPERCONDUCTING CYCLOTRON PROJECT AT VECC

STATUS OF THE SUPERCONDUCTING CYCLOTRON PROJECT AT VECC STATUS OF THE SUPERCONDUCTING CYCLOTRON PROJECT AT VECC Bikash Sinha and R. K. Bhandari Variable Energy Cyclotron Centre, Department of Atomic Energy, Kolkata 700 064, India Abstract A superconducting

More information

Re-commissioning the Recycler Storage Ring at Fermilab

Re-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 information

Maurizio Vretenar Linac4 Project Leader EuCARD-2 Coordinator

Maurizio 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 information

Current Industrial SRF Capabilities and Future Plans

Current Industrial SRF Capabilities and Future Plans and Future Plans Capabilities in view of Design Engineering Manufacturing Preparation Testing Assembly Taking into operation Future Plans Participate in and contribute to development issues, provide prototypes

More information

Bunch-Shape Measurements at PSI s High Power Cyclotrons and Proton Beam Lines

Bunch-Shape Measurements at PSI s High Power Cyclotrons and Proton Beam Lines Bunch-Shape Measurements at PSI s High Power Cyclotrons and Proton Beam Lines Rudolf Dölling, Paul Scherrer Institut, CH-5232 Villigen-PSI technique - measurement locations, measurement principle - setup

More information

Demonstration 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 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 information

High acceleration gradient. Critical applications: Linear colliders e.g. ILC X-ray FELs e.g. DESY XFEL

High acceleration gradient. Critical applications: Linear colliders e.g. ILC X-ray FELs e.g. DESY XFEL High acceleration gradient Critical applications: Linear colliders e.g. ILC X-ray FELs e.g. DESY XFEL Critical points The physical limitation of a SC resonator is given by the requirement that the RF magnetic

More information

Compact Radio Frequency Technology for Applications in Cargo and Global

Compact 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 information

Workshop,, Nov , Hirschberg. DITANET-Workshop

Workshop,, Nov , Hirschberg. DITANET-Workshop DITANET-Workshop Workshop,, Nov. 24-25 25 2009, Hirschberg A Cryogenic Current Comparator for FAIR M. Schwickert, H. Reeg, GSI Beam Diagnostics Department W. Vodel, R. Geithner, Friedrich-Schiller-Universität

More information

RF CAVITY SIMULATIONS FOR SUPERCONDUCTING CYCLOTRON C400 Y. Jongen, M. Abs, W. Kleeven, S. Zaremba IBA, Louvain-la-Neuve, Belgium

RF CAVITY SIMULATIONS FOR SUPERCONDUCTING CYCLOTRON C400 Y. Jongen, M. Abs, W. Kleeven, S. Zaremba IBA, Louvain-la-Neuve, Belgium Ó³ Ÿ. 2011.. 8, º 4(167).. 647Ä654 ˆ ˆŠ ˆ ˆŠ Š ˆ RF CAVITY SIMULATIONS FOR SUPERCONDUCTING CYCLOTRON C400 Y. Jongen, M. Abs, W. Kleeven, S. Zaremba IBA, Louvain-la-Neuve, Belgium A. A. Glazov, S. V. Gurskiy,

More information

Initial Results from a Cryogenic Proton Irradiation of a p-channel CCD

Initial Results from a Cryogenic Proton Irradiation of a p-channel CCD Centre for Electronic Imaging Initial Results from a Cryogenic Proton Irradiation of a p-channel CCD Jason Gow Daniel Wood, David Hall, Ben Dryer, Simeon Barber, Andrew Holland and Neil Murray Jason P.

More information

Herwig Schopper CERN 1211 Geneva 23, Switzerland. Introduction

Herwig 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 information

Beam Control: Timing, Protection, Database and Application Software

Beam Control: Timing, Protection, Database and Application Software Beam Control: Timing, Protection, Database and Application Software C.M. Chu, J. Tang 储中明 / 唐渊卿 Spallation Neutron Source Oak Ridge National Laboratory Outline Control software overview Timing system Protection

More information

FAST RF KICKER DESIGN

FAST 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 information

Low-Level RF. S. Simrock, DESY. MAC mtg, May 05 Stefan Simrock DESY

Low-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 information

Mul$- bunch accelera$on in FFAG. Takeichiro Yokoi(JAI)

Mul$- bunch accelera$on in FFAG. Takeichiro Yokoi(JAI) Mul$- bunch accelera$on in FFAG Takeichiro Yokoi(JAI) Introduc$on For high intensity applica9on such as ADSR, high repe99on opera9on is a requirement to diminish the influence of space charge force For

More information

Design of ESS-Bilbao RFQ Linear Accelerator

Design 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 information

REVIEW OF HIGH POWER CW COUPLERS FOR SC CAVITIES. S. Belomestnykh

REVIEW 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 information

Circumference 187 m (bending radius = 8.66 m)

Circumference 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 information

Jørgen 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/ ), 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 information

Does the short pulse mode need energy recovery?

Does 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 information

SARAF commissioning & safety issues. L. Weissman on behalf of the SARAF team SPIRAL week 2010

SARAF commissioning & safety issues. L. Weissman on behalf of the SARAF team SPIRAL week 2010 SARAF commissioning & safety issues L. Weissman on behalf of the SARAF team SPIRAL week 2010 1 Outline commissioning of SARAF project : RFQ status Cryomodule status Accumulated beam operation experience

More information

Resonator System for the BEST 70MeV Cyclotron

Resonator 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 information

Normal-conducting high-gradient rf systems

Normal-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 information

cyclotron RF systems sb/cas10061/1

cyclotron RF systems sb/cas10061/1 cyclotron RF systems sb/cas10061/1 outline cyclotron basics resonator design techniques transmission line 3D finite element tuning power coupling RF control flat topping some specific examples sb/cas100562

More information

RF STATUS OF SUPERCONDUCTING MODULE DEVELOPMENT SUITABLE FOR CW OPERATION: ELBE CRYOSTATS

RF 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 information

HFCC 2018 Bratislava Product Launch: Low Power Solid-State Shortwave

HFCC 2018 Bratislava Product Launch: Low Power Solid-State Shortwave HFCC 2018 Bratislava Product Launch: Low Power Solid-State Shortwave 27.08.2018 1 Our Mission Science MedTech Ampegon designs and delivers high power systems for world-class research facilities. «We offer

More information

Progress in High Gradient Accelerator Research at MIT

Progress 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 information

Experiences of the QSBPM System on MAX II

Experiences 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 information

Status of berlinpro and BESSY II Installation of SSA. Helmholtz-Zentrum Berlin for materials and energy (HZB)

Status of berlinpro and BESSY II Installation of SSA. Helmholtz-Zentrum Berlin for materials and energy (HZB) Status of berlinpro and BESSY II Installation of SSA Wolfgang Anders, Helmholtz-Zentrum Berlin for materials and energy (HZB) 19th ESLS-RF Meeting 30.9.-1.10.2015 MaxLab outline BERLinPro Status building

More information

IQM Detector Characteristics: Signal reproducibility

IQM Detector Characteristics: Signal reproducibility The Integral Quality Monitor (IQM) System is a real-time beam verification system that monitors the accuracy of radiation delivery throughout each patient treatment without any user interaction. IQM continuously

More information

Bioimaging of cells and tissues using accelerator-based sources

Bioimaging 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 information

Lattice Design for PRISM-FFAG. A. Sato Osaka University for the PRISM working group

Lattice Design for PRISM-FFAG. A. Sato Osaka University for the PRISM working group Lattice Design for PRISM-FFAG A. Sato Osaka University for the PRISM working group contents PRISM overview PRISM-FFAG dynamics study & its method PRISM Phase Rotated Intense Slow Muon source Anticipated

More information

Status and Upgrade. P. Elleaume. XVIII ESLS Workshop, November P. Elleaume, ESRF. Slide: 1

Status and Upgrade. P. Elleaume. XVIII ESLS Workshop, November P. Elleaume, ESRF. Slide: 1 ESRF Status and Upgrade P. Elleaume Slide: 1 Statistics 2008-2010 Availability (%) Mean time between failures (hrs) Mean duration of a failure (hrs) 2008 2009 2010* 98.30 99.04 98.83 64.50 75.80 70.80

More information

Status of the European XFEL Accelerator Construction Project. Reinhard Brinkmann, DESY

Status of the European XFEL Accelerator Construction Project. Reinhard Brinkmann, DESY Status of the European XFEL Accelerator Construction Project Reinhard Brinkmann, DESY European XFEL Introduction Some specifications Photon energy 0.3-24 kev Pulse duration ~ 10-100 fs Pulse energy few

More information

LCLS-II SXR Undulator Line Photon Energy Scanning

LCLS-II SXR Undulator Line Photon Energy Scanning LCLS-TN-18-4 LCLS-II SXR Undulator Line Photon Energy Scanning Heinz-Dieter Nuhn a a SLAC National Accelerator Laboratory, Stanford University, CA 94309-0210, USA ABSTRACT Operation of the LCLS-II undulator

More information

Beam Delivery Techniques: Passive Scattering Proton Beams. Zuofeng Li and Roelf Slopsema University of Florida Proton Therapy Institute

Beam Delivery Techniques: Passive Scattering Proton Beams. Zuofeng Li and Roelf Slopsema University of Florida Proton Therapy Institute Beam Delivery Techniques: Passive Scattering Proton Beams Zuofeng Li and Roelf Slopsema University of Florida Proton Therapy Institute 1 Disclaimer UFPTI uses IBA Proton Therapy System Proton Beam: production,

More information

Company Profile Ampegon Group

Company Profile Ampegon Group Company Profile Ampegon Group Contents 1 Introduction 3 1.1 About us 3 1.2 Quality Statement 3 1.3 Customer Services 3 1.4 Activities Ampegon AG 3 1.5 Activities Ampegon Antenna Systems GmbH 4 1.6 Activities

More information

Inductive adder prototype pulse generator for FCC-hh kickers

Inductive adder prototype pulse generator for FCC-hh kickers Inductive adder prototype pulse generator for FCC-hh kickers D. Woog Acknowledgements: M.J. Barnes, J. Holma, T. Kramer 14/04/2018 David Woog FCC WEEK 2018 1 Content Inductive adder introduction Requirements

More information

Superconducting RF System. Heung-Sik Kang

Superconducting 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 information

Commissioning 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 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 information

HETERONUCLEAR IMAGING. Topics to be Discussed:

HETERONUCLEAR IMAGING. Topics to be Discussed: HETERONUCLEAR IMAGING BioE-594 Advanced MRI By:- Rajitha Mullapudi 04/06/2006 Topics to be Discussed: What is heteronuclear imaging. Comparing the hardware of MRI and heteronuclear imaging. Clinical applications

More information

ALICE SRF SYSTEM COMMISSIONING EXPERIENCE A. Wheelhouse ASTeC, STFC Daresbury Laboratory

ALICE 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 information

Schematic diagram of the DAP

Schematic diagram of the DAP Outline Introduction Transmission mode measurement results Previous emission measurement Trapping mechanics Emission measurement with new circuits Emission images Future plan and conclusion Schematic diagram

More information

ESS RF Development at Uppsala University. Roger Ruber for the FREIA team Uppsala University

ESS RF Development at Uppsala University. Roger Ruber for the FREIA team Uppsala University ESS RF Development at Uppsala University Roger Ruber for the FREIA team Uppsala University ESS-UU Collaboration 2009 ESS and UU start discussion on 704 MHz RF development proposal for ESS dedicated test

More information

MuCool Test Area Experimental Program Summary

MuCool Test Area Experimental Program Summary MuCool Test Area Experimental Program Summary Alexey Kochemirovskiy The University of Chicago/Fermilab Alexey Kochemirovskiy NuFact'16 (Quy Nhon, August 21-27, 2016) Outline Introduction Motivation MTA

More information

Rotating Coil Measurement Errors*

Rotating Coil Measurement Errors* Rotating Coil Measurement Errors* Animesh Jain Superconducting Magnet Division Brookhaven National Laboratory, Upton, NY 11973, USA 2 nd Workshop on Beam Dynamics Meets Magnets (BeMa2014) December 1-4,

More information

5.2.3 DecayChannelSolenoids BeamDynamics Induction Linac Approach

5.2.3 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 information

Radiation Test Report Paul Scherer Institute Proton Irradiation Facility

Radiation Test Report Paul Scherer Institute Proton Irradiation Facility the Large Hadron Collider project CERN CH-2 Geneva 23 Switzerland CERN Div./Group RadWG EDMS Document No. xxxxx Radiation Test Report Paul Scherer Institute Proton Irradiation Facility Responsibility Tested

More information

Impact of the high magnetic field and RF power in a superconducting cyclotron on the operation of a nearby MRI facility

Impact of the high magnetic field and RF power in a superconducting cyclotron on the operation of a nearby MRI facility ISSN 2469-5491 Impact of the high magnetic field and RF power in a superconducting cyclotron on the operation of a nearby MRI facility Chee-Wai Cheng1, Steven G Ferguson2, David Jordan3, Frederick Jesseph1,

More information

EPCA Germany. Cutting Edge Technology. experience matters

EPCA Germany. Cutting Edge Technology. experience matters Cutting Machines EPCA Germany Cutting Edge Technology EPCA Germany stands for long year expertise, in-depth knowledge, excellent service quality and understanding of automation processes. With EPCA Germany

More information

RF Design of Normal Conducting Deflecting Cavity

RF Design of Normal Conducting Deflecting Cavity RF Design of Normal Conducting Deflecting Cavity Valery Dolgashev (SLAC), Geoff Waldschmidt, Ali Nassiri (Argonne National Laboratory, Advanced Photon Source) 48th ICFA Advanced Beam Dynamics Workshop

More information

S-band Magnetron. Tuner revolutions to cover frequency range 4.75 (note 3) Mounting position (note 4) Any Cooling (note 5) Water

S-band Magnetron. Tuner revolutions to cover frequency range 4.75 (note 3) Mounting position (note 4) Any Cooling (note 5) Water S-band Magnetron GENERAL DESCRIPTION is a mechanical tuned pulsed type S-band magnetron intended primarily for linear accelerator. It is water cooled and has circle waveguide output type. It is designed

More information

3.9 GHz Deflecting Mode Cavity

3.9 GHz Deflecting Mode Cavity 3.9 GHz Deflecting Mode Cavity Timothy W. Koeth July 12, 2005 History of 3.9 GHz DMC Cavity Simulations The Other Modes concern and modeling R/Q Wake Field Simulations Design: OM couplers Testing: Vertical

More information

Product Range Electronic Units

Product Range Electronic Units Pyramid Technical Consultants, Inc. 1050 Waltham Street Suite 200 Lexington, MA 02421 TEL: +1 781 402-1700 TEL (UK): +44 1273 492001 FAX: (781) 402-1750 EMAIL: SUPPORT@PTCUSA.COM Product Range Electronic

More information

REVIEW ON SUPERCONDUCTING RF GUNS

REVIEW 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 information

Spaceborne Electron Accelerators

Spaceborne Electron Accelerators Spaceborne Electron Accelerators J.W. Lewellen, C. Buechler, G. Dale, N.A. Moody, D.C. Nguyen LINAC 2016 26 September 2016 Acknowledgements LANL Program Development and Pathfinder funding LANL team members

More information

REVIEW OF FAST BEAM CHOPPING F. Caspers CERN AB-RF-FB

REVIEW 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 information

Jørgen 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 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 information

Beam Transfer to Targets

Beam Transfer to Targets Volume III Update Report Chapter 3 Beam Transfer to Targets 3-1 Authors and Contributors Beam Transfer to Targets The executive summary was prepared by: R Maier 1 and KN Clausen 3 on behalf of the Beam

More information

Project X Cavity RF and mechanical design. T. Khabiboulline, FNAL/TD/SRF

Project 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 information

Design of the magnets for the MAX IV project. Martin Johansson, Beam Dynamics meets Magnets-II workshop, Bad Zurzach, Dec.

Design of the magnets for the MAX IV project. Martin Johansson, Beam Dynamics meets Magnets-II workshop, Bad Zurzach, Dec. Design of the magnets for the MAX IV project Martin Johansson, Beam Dynamics meets Magnets-II workshop, Bad Zurzach, 01-04 Dec. 2014 MAX IV 3 GeV ring magnets key aspects: Relatively small magnet aperture

More information

Distributed source x-ray tube technology for tomosynthesis imaging

Distributed source x-ray tube technology for tomosynthesis imaging Distributed source x-ray tube technology for tomosynthesis imaging Authors: F. Sprenger a*, X. Calderon-Colon b, Y. Cheng a, K. Englestad a, J. Lu b, J. Maltz c, A. Paidi c, X. Qian b, D. Spronk a, S.

More information

EMMA the World's First Non-Scaling FFAG Accelerator

EMMA 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 information

10th ESLS RF Meeting September ALBA RF System. F. Perez. on behalf of the ALBA RF Group. ALBA RF System 1/21

10th 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 information

ELECTRON BEAM DIAGNOSTICS AND FEEDBACK FOR THE LCLS-II*

ELECTRON BEAM DIAGNOSTICS AND FEEDBACK FOR THE LCLS-II* THB04 Proceedings of FEL2014, Basel, Switzerland ELECTRON BEAM DIAGNOSTICS AND FEEDBACK FOR THE LCLS-II* Josef Frisch, Paul Emma, Alan Fisher, Patrick Krejcik, Henrik Loos, Timothy Maxwell, Tor Raubenheimer,

More information

Chapter 9. Magnet System. 9.1 Magnets in the Arc and Straight Sections

Chapter 9. Magnet System. 9.1 Magnets in the Arc and Straight Sections Chapter 9 Magnet System This chapter discusses the parameters and the design of the magnets to use at KEKB. Plans on the magnet power supply systems, magnet installation procedure and alignment strategies

More information

DEVELOPMENT 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 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 information

Beam Commissioning and Operation of New Linac Injector for RIKEN RI Beam Factory

Beam Commissioning and Operation of New Linac Injector for RIKEN RI Beam Factory Beam Commissioning and Operation of New Linac Injector for RIKEN RI Beam Factory RIKEN Nishina Center Kazunari Yamada, K. Suda, S. Arai, M. Fujimaki, T. Fujinawa, H. Fujisawa, N. Fukunishi, Y. Higurashi,

More information

TURN-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 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 information

Progresses on China ADS Superconducting Cavities

Progresses on China ADS Superconducting Cavities Progresses on China ADS Superconducting Cavities Peng Sha IHEP, CAS 2013/06/12 1 Outline 1. Introduction 2. Spoke012 cavity 3. Spoke021 cavity 4. Spoke040 cavity 5. 650MHz β=0.82 5-cell cavity 6. High

More information