SPARC Review Committee Meeting - 16.11.05 M.Mauri - CORA: Design and Construction of a RF compressor for High Brightness Electron Beams CORA: Design and.

Slides:



Advertisements
Similar presentations
Tom Powers Practical Aspects of SRF Cavity Testing and Operations SRF Workshop 2011 Tutorial Session.
Advertisements

WP-M3 Superconducting Materials PArametric COnverter Detector INFN_Genoa Renzo Parodi.
Lorentz force detuning measurements on the CEA cavity
Henrik Loos LCLS FAC Meeting 27 October RF Gun Status LCLS Facility Advisory Committee Meeting October 26, 2005 Mechanical.
30 th September 2004 High Power RF Couplers James Rogers High Power RF Couplers ELSRF Daresbury Laboratory.
Progress of the sub-harmonic bunching system (i.e. upgrading progress of BEPCII present bunching system) Pei Shilun for the SHBS team Accelerator center,
Normal-Conducting Photoinjector for High Power CW FEL Sergey Kurennoy, LANL, Los Alamos, NM, USA An RF photoinjector capable of producing high continuous.
MICE RF Cavity Measurements Derun Li Center for Beam Physics Lawrence Berkeley National Laboratory March 26, 2010 University of California, Riverside,
Injector RF Design Review November 3, 2004 John Schmerge, SLAC LCLS RF Gun Thermal Analysis John Schmerge, SLAC November 3,
Design of Standing-Wave Accelerator Structure
RF Systems and Stability Linac Coherent Light Source Stanford Synchrotron Radiation Laboratory Stanford Linear Accelerator Center.
Cell-Coupled Drift Tube Linac M. Pasini, CERN AB-RF LINAC4 Machine Advisory Committee 1 st meeting CERN January 29-30, 2008.
H. Haseroth Thursday, February 5-8, 2002 MUCOOL / MICE 1 RF & RF power H. Haseroth CERN  Situation of 88 MHz test cavity  Availability of amplifiers.
DESIGN OF A 7-CELLS, HOM DAMPED, SUPERCONDUCTING CAVITY FOR THE STRONG RF FOCUSING EXPERIMENT AT DANE David Alesini, Caterina Biscari, Roberto Boni, Alessandro.
SLHC-PP – WP7 Critical Components for Injector Upgrade Plasma Generator – CERN, DESY, STFC-RAL Linac4 2MHz RF source Thermal Modeling Gas Measurement and.
CLIC Drive Beam Linac Rolf Wegner. Outline Introduction: CLIC Drive Beam Concept Drive Beam Modules (modulator, klystron, accelerating structure) Optimisation.
201 MHz and 805 MHz Cavity Developments in MUCOOL Derun Li Center for Beam Physics Lawrence Berkeley National Laboratory Nufact 2002 Workshop, London,
7.8GHz Dielectric Loaded High Power Generation And Extraction F. Gao, M. E. Conde, W. Gai, C. Jing, R. Konecny, W. Liu, J. G. Power, T. Wong and Z. Yusof.
SRF Results and Requirements Internal MLC Review Matthias Liepe1.
201 MHz NC RF Cavity R&D for Muon Cooling Channels
THE TOP LINAC PROJECT ISS-ENEA Project to demonstrate operability of a compact proton linac in a medium size hospital HIGH POWER RF TESTS OF THE FIRST.
1 C-Band Linac Development Satoshi Ohsawa 2004.Feb.19LCPAC.
Damped C-Band structures for ELI_NP proposal D. Alesini (LNF-INFN, Frascati, Italy) CERN, 18 July 2012.
Preliminary design of SPPC RF system Jianping DAI 2015/09/11 The CEPC-SppC Study Group Meeting, Sept. 11~12, IHEP.
LLRF Cavity Simulation for SPL
06-November-2013 Thermo-Mechanical Tests BE-RF-PM Review of the CLIC Two-Beam Module Program Thermo-Mechanical Tests L. Kortelainen, I. Kossyvakis, R.
RF structure design KT high-gradient medical project kick-off Alberto Degiovanni TERA Foundation - EPFL.
RF system issues due to pulsed beam in ILC DR October 20, Belomestnykh, RF for pulsed beam ILC DR, IWLC2010 S. Belomestnykh Cornell University.
PROPOSAL G.I.A.F. (HYBRID GUN AT HIGH FREQUENCY) INFN-LNF – UNIVERSITY OF ROME “LA SAPIENZA”- UCLA D. Alesini (T), M. Ferrario (R), A. Gallo (T),
L-band (1.3 GHz) 5-Cell SW Cavity High Power Test Results Faya Wang, Chris Adolphsen SLAC National Accelerator Laboratory
Development of the Room Temperature CH-DTL in the frame of the HIPPI-CARE Project Gianluigi Clemente,
1.3GHz Input Coupler for ILC
CLARA Gun Cavity Optimisation NVEC 05/06/2014 P. Goudket G. Burt, L. Cowie, J. McKenzie, B. Militsyn.
Ding Sun and David Wildman Fermilab Accelerator Advisory Committee
RF scheme of electron linear accelerator with energy MeV Levichev A.E. Budker Institute of Nuclear Physics SB RAS.
MICE RF Cavity Measurements Derun Li Center for Beam Physics Lawrence Berkeley National Laboratory July 8, 2010 Rutherford Appleton Laboratory, UK.
Bunch Separation with RF Deflectors D. Rubin,R.Helms Cornell University.
TESLA DAMPING RING RF DEFLECTORS DESIGN F.Marcellini & D. Alesini.
WP8-HGA High Gradient Acceleration M. Biagini (INFN-LNF) WP8 coordinator Tiara Kickoff Meeting, CERN, Feb , 2011.
S. Bettoni, R. Corsini, A. Vivoli (CERN) CLIC drive beam injector design.
ELI and other things A. D’Elia 1. C-BAND STRUCTURES FOR MULTI-BUNCH RF LINACS: ELI_NP PROPOSAL Bunch charge 250 pC Number of bunches 40 Bunch distance.
650 MHz Solid State RF Power development at RRCAT
Operated by the Southeastern Universities Research Association for the U. S. Department of Energy Thomas Jefferson National Accelerator Facility 6 March.
STATUS OF THE NC BUNCHING RFQ (Sub-task: SC-RFQ) Antonio Palmieri INFN-LNL.
1 st TIARA Steering Committee A. Gallo – INFN Frascati deputy of TIARA WP8 leader STATUS OF TIARA WP8.
ELI PHOTOINJECTOR PARAMETERS: PRELIMINARY ANALYSIS AND SIMULATIONS C. RONSIVALLE.
Advancements on RF systems D. Alesini (LNF-INFN) Quinto Meeting Generale Collaborazione LI2FE, Frascati 15-16/03/2011.
Status of the sub-harmonic bunching system for the CLIC DB injector front end Hamed Shaker School of Particles and Accelerators, Institute for Research.
DESIGN STUDY November 28 th - 30 th 2005First EURISOL Design Study TOWN MEETING High Power RF Amplifiers Development at LNL Fabio Scarpa - INFN LNL.
S.M. Polozov & Ko., NRNU MEPhI
Linac beam dynamics Linac dynamics : C. Bruni, S. Chancé, L. Garolfi,
Abstract EuSPARC and EuPRAXIA projects
TTC Topical Workshop - CW SRF, Cornell 12th – 14th June 2013
An X-band system for phase space linearisation on CLARA
M. Migliorati, C. Vaccarezza INFN - LNF
by P. Musumeci and F.Tazzioli
NC Accelerator Structures
Preliminary injector linac design
Physics design on Injector-1 RFQ
Application of the moderate peak power (6 MW) X-band klystron’s cluster for the CLIC accelerating structures testing program. I. Syratchev.
SPARC RF gun status by P. Musumeci Review committee
Developments on Proposed
(INFN – Laboratori Nazionali di Frascati)
CEPC injector high field S-band accelerating structure design and R&D
High Efficiency X-band Klystron Design Study
Update of CLIC accelerating structure design
C. Ronsivalle, L. Picardi, C. Cianfarani, G. Messina, G. L
Status of the CLIC Injector studies
Accelerator Physics Particle Acceleration
USPAS Course on Recirculated and Energy Recovered Linear Accelerators
Presentation transcript:

SPARC Review Committee Meeting M.Mauri - CORA: Design and Construction of a RF compressor for High Brightness Electron Beams CORA: Design and Construction of a RF Compressor for High Brightness Electron Beams Franco Alessandria, Alberto Bacci, Carlo De Martinis, Dario Giove, Marco Mauri, Luca Serafini (INFN - sezione di Milano e Università di Milano) David Alesini, Massimo Ferrario, Alessandro Gallo, Fabio Marcellini (INFN – Laboratori Nazionali di Frascati)

SPARC Review Committee Meeting M.Mauri - CORA: Design and Construction of a RF compressor for High Brightness Electron Beams CORA has been an R&D activity related to the design and the construction of a prototype RF structure able to test the slow-wave velocity bunching theory (1). The parameter which controls the compression process is the phase velocity (vf) of the structure. As it is shown in the formula below the phase velocity can be changed properly detuning the structure. In the CORA scheme the required detuning is obtained controlling the cavity temperature. This makes possible to modify “on-line” the bunch compression factor and find the optimum working point. (1) L. Serafini et al. “Ultra-short Bunch Generation with a Rectlinear Compressor”, PAC2001, Chicago, June 2001, p Introduction The project A compression factor of the order of 10 has been taken as a reasonable goal. This reflects in a change of the vf of the order of 0.1%. The above formula shows that increasing the group velocity of the structure, the phase velocity becomes less sensitive to detuning and, as a consequence, to temperature fluctuations.

SPARC Review Committee Meeting M.Mauri - CORA: Design and Construction of a RF compressor for High Brightness Electron Beams RF compressor main parameters Frequency of the TW structure2856 MHz Accelerating gradient20 MV/m Electrons injection energy6 MeV Electrons extraction energy16 Mev Bunch length at injection10 ps Compression factor7 RF power66 MW MarkIV (SLAC) Alma5 Cavity radius [cm] Iris radius [cm] Septum thickness [cm] Cell length [cm]3.5 Mode 2  /3 Frequency [MHz]2856 Q Shunt imp. [MOhm/m]5341 V g /c  T [°C] Comparison between a constant-impedance SLAC cavity and the proposed RF compressor cavity Temperature variation needed to change the phase velocity of 0.1% Introduction Main parameters

SPARC Review Committee Meeting M.Mauri - CORA: Design and Construction of a RF compressor for High Brightness Electron Beams Topics covered in the following slides: 1.Improvements on the thermal control system 2.Preliminary tests on the 10-cell model structure (Vg=0.034c) 3.Power couplers design and construction Cora started in 2003 with the EM and mechanic design of the structure (using the codes SUPERFISH and ANSYS). After a few months we received from UCLA a 3m-long SLAC structure that was used to carry out RF measurements, to test temperature control schemes and to acquire lab experience. Using this structure we developed all the tools that will be used for the RF compressor. On November and December 2004 in cooperation with the “Soltan Institute for Nuclear Studies” of Warsaw the complete (EM and mechanical) design of the power couplers has been performed. During 2004, a prototype of the RF compressor (made of 8 cells plus 2 end half- cells) was machined in Italy by CINEL. The structure has been measured in our lab and then delivered to CERN for brazing. The brazed 10-cell structure was sent back to Milan (LASA) on October Introduction

SPARC Review Committee Meeting M.Mauri - CORA: Design and Construction of a RF compressor for High Brightness Electron Beams 1.Improvements on the thermal control system System set up PC

SPARC Review Committee Meeting M.Mauri - CORA: Design and Construction of a RF compressor for High Brightness Electron Beams RF Cavity The temperature of the cavity has been mapped using thermocouples and platinum resistance thermometers, A Network Analyzer has been used to monitor the resonance frequency of the cavity Temperatures and frequency were remotely read and stored using LabView. 1.Improvements on the thermal control system System set up

SPARC Review Committee Meeting M.Mauri - CORA: Design and Construction of a RF compressor for High Brightness Electron Beams Chiller A commercial available chiller by Thermo Neslab has been chosen after a deep analysis of the performances with respect to the experimental requirements. The 2 internal PID loops had to be tuned in order to obtain the required thermal stability (fluctuations below 0.1°) and to reduce the response time of the system. 1.Improvements on the thermal control system System set up Model: Neslab HX-150 Cooling capacity  4 kW

SPARC Review Committee Meeting M.Mauri - CORA: Design and Construction of a RF compressor for High Brightness Electron Beams Heater We introduced a heater in the system in order to simulate the thermal load due to RF. With a repetition rate of 10 Hz and pulse length of 5  s we expect to have a dissipation in the cavity of about 1.1kW. The heater can deliver up to 1.5 kW and is remotely controlled. 1.Improvements on the thermal control system System set up

SPARC Review Committee Meeting M.Mauri - CORA: Design and Construction of a RF compressor for High Brightness Electron Beams

The chiller temperature set point has been fixed first at 40.0 °C then moved to 39.7 °C and at the end back to 40.0 °C. During these steps the cavity temperature and cavity RF frequency resonance have been measured as probes of the behaviour of the whole setup. Main experimental results: thermal stability under 1.5 kW load: better than 0.1 °C (confirmed both from RTD temperature probe and RF measure (0.1 °C  5 kHz) time required to reach a new stability condition: for small change ( less than 3.0 °C) in temperature set point : less than 500 sec. for large change ( more than 25.0 °C) in temperature set point : nearly 1200 sec. 1.Improvements on the thermal control system Results Frequency Temperature  T ~ -0.3 °C  f ~ +15 kHz

SPARC Review Committee Meeting M.Mauri - CORA: Design and Construction of a RF compressor for High Brightness Electron Beams 1.Improvements on the thermal control system Results The 3 meter long SLAC cavity (thermally insulated) was in series with the chiller (using a 10 meters long pipeline) and the 1.5 kW thermal load. A stability better than ±0.1° has been achieved with a fixed temperature set point (40°C). The plot shows the temperature fluctuations during measurement of about 4 hours. Reaching the steady state condition from a temperature of 26°C took about half an hour.

SPARC Review Committee Meeting M.Mauri - CORA: Design and Construction of a RF compressor for High Brightness Electron Beams 1.Thermal control system test results Results Few tests have been carried out using a CW 100 W RF generator

SPARC Review Committee Meeting M.Mauri - CORA: Design and Construction of a RF compressor for High Brightness Electron Beams 2.Preliminary tests on 10-cell model structure (Vg=0.034c) Introduction A 10 cells prototype has been designed and built in order to test: -the EM design of the cells (made with SUPERFISH and tested with Microwave Studio) -the mechanical design (in particular with respect to the brazing process) -the control of the phase velocity (using the temperature based mechanism) Disk RF probe hole Cooling channels Dinging hole Cell

SPARC Review Committee Meeting M.Mauri - CORA: Design and Construction of a RF compressor for High Brightness Electron Beams 2.Preliminary tests on 10-cell model structure (Vg=0.034c) Measurements on single cells Measuring the single cells it has been possible to verify that all the cells were machined with a very good repeatability (~ 150 kHz) and in good agreement with the EM simulations (~ 350kHz)

SPARC Review Committee Meeting M.Mauri - CORA: Design and Construction of a RF compressor for High Brightness Electron Beams 2.Preliminary tests on 10-cell model structure (Vg=0.034c) Measurements on the brazed structure

SPARC Review Committee Meeting M.Mauri - CORA: Design and Construction of a RF compressor for High Brightness Electron Beams 2.Preliminary tests on 10-cell model structure (Vg=0.034c) Measurements on the brazed structure Measured Frequency Mode[MHz] (1) About +1.1 MHz, evaluated with FSCALE from LLNL The resonance frequencies of the brazed structure had been measured in air (structure temperature: 40°C). Considering the 2/3  mode (working mode of the RF compressor) and the air-to-vacuum correction (1) the structure is out of tune of about 1 MHz. By means of the tuning system (dinging) the frequency will be corrected to nominal value (2856 MHz)

SPARC Review Committee Meeting M.Mauri - CORA: Design and Construction of a RF compressor for High Brightness Electron Beams 2.Preliminary tests on 10-cell model structure (Vg=0.034c) Measurements on the brazed structure Transient:  t = +0.2 °C in 7 min Overshoot due to the PID

SPARC Review Committee Meeting M.Mauri - CORA: Design and Construction of a RF compressor for High Brightness Electron Beams 2.Preliminary tests on 10-cell model structure (Vg=0.034c) Measurements on the brazed structure

SPARC Review Committee Meeting M.Mauri - CORA: Design and Construction of a RF compressor for High Brightness Electron Beams Phase velocity measurements A preliminary set of measurements have been carried out on the brazed structure thermally conditioned. The first results show that the target value of 0.1% change in phase velocity may be obtained changing the cavity temperature by 2.1 °C (the design value was 1.9 °C). Further measurements will be carried out to deeper investigate the behavior. 2.Preliminary tests on 10-cell model structure (Vg=0.034c) Measurements on the brazed structure

SPARC Review Committee Meeting M.Mauri - CORA: Design and Construction of a RF compressor for High Brightness Electron Beams The input and output couplers of the RF compressor have been designed in order to ensure a good impedance match in the bandwidth of interest minimizing the detuning effects on the structure. The geometry of a 10-cells structure with couplers has been modeled using a three dimensional computer code to optimize the length of the tapered waveguide (from the WR284 to the cavity), the dimensions of the coupling slot, and the coupling cell diameter Criteria of quality : S11 minimization, proper phase advance per cell at working mode, proper E-field pattern on n cells structure. 3. Power couplers design and construction

SPARC Review Committee Meeting M.Mauri - CORA: Design and Construction of a RF compressor for High Brightness Electron Beams Optimal case: S11 = -50 dB (VSWR < 2856MHz Phase advance per cell: 120°±2° 3. Power couplers design and construction

SPARC Review Committee Meeting M.Mauri - CORA: Design and Construction of a RF compressor for High Brightness Electron Beams 3. Power couplers design and construction

SPARC Review Committee Meeting M.Mauri - CORA: Design and Construction of a RF compressor for High Brightness Electron Beams Conclusions By the end of the year: Full EM characterization and tuning of the 10-cells cavity 4-cell model with couplers will be finished and measured (tests with a 100W CW RF amplifier)