FERMI LINAC O VERVIEW The 1.5 GeV 50 Hz Upgrade July 2013 C. Serpico.

Slides:



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

Areal RF Station A. Vardanyan RF System The AREAL RF system will consist of 3 RF stations: Each RF station has a 1 klystron, and HV modulator,
Areal RF Station A. Vardanyan RF System The AREAL RF system will consist of 3 RF stations: Each RF station has a 1 klystron, and HV modulator,
ESS End-to-End Optics and Layout Integration Håkan Danared European Spallation Source Catania, 6 July 2011.
Normal-Conducting Photoinjector for High Power CW FEL Sergey Kurennoy, LANL, Los Alamos, NM, USA An RF photoinjector capable of producing high continuous.
1 X-band Single Cell and T18_SLAC_2 Test Results at NLCTA Faya Wang Chris Adolphsen Jul
Design of Standing-Wave Accelerator Structure
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.
R&D For Accelerating Structures H. Padamsee. TESLA Niobium, one meter length, rf = 1.3 GHz Copper, 53 cm, rf = 11.4 GHz.
MuCool RF Status MICE Collaboration Meeting June 7-10, 2006, Fermilab A. Moretti June 9, 2006.
Beam loading compensation 300Hz positron generation (Hardware Upgrade ??? Due to present Budget problem) LCWS2013 at Tokyo Uni., Nov KEK, Junji.
Demonstration of the Beam loading compensation (Preparation status for ILC beam loading compensation experiments at ATF injector in this September) (PoP.
Alessandro Cappelletti for CTF3 collaboration 5 th May 2010 RESULTS OF BEAM BASED RF POWER PRODUCTION IN CTF3.
HIGH RF POWER TESTING FOR THE CLIC PETS International Workshop on Linear Colliders 20 th October 2010 Alessandro Cappelletti for the CLIC team with.
201 MHz and 805 MHz Cavity Developments in MUCOOL Derun Li Center for Beam Physics Lawrence Berkeley National Laboratory Nufact 2002 Workshop, London,
J. Haimson and B. Mecklenburg Haimson Research Corporation FG02-05ER84362 Work performed under the auspices of the U.S. Department of Energy SBIR Grant.
1 C-Band Linac Development Satoshi Ohsawa 2004.Feb.19LCPAC.
Low Emittance RF Gun Developments for PAL-XFEL
Christopher Nantista ARD R&D Status Meeting SLAC February 3, …… …… …… … ….
XFEL SRF Accelerating Module Prototypes Tests at DESY Fermilab Seminar, July 21st Denis Kostin, MHF-SL, DESY.
Clustered Surface RF Production Scheme Chris Adolphsen Chris Nantista SLAC.
RF structure design KT high-gradient medical project kick-off Alberto Degiovanni TERA Foundation - EPFL.
John Carwardine 5 th June 2012 Developing a program for 9mA studies shifts in Sept 2012.
Andrew Moss ASTeC CM32 9t h February 2012 RAL MICE RF System.
Anders Sunesson RF Group ESS Accelerator Division
L-band (1.3 GHz) 5-Cell SW Cavity High Power Test Results Faya Wang, Chris Adolphsen SLAC National Accelerator Laboratory
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
2.1 GHz Warm RF Cavity for LEReC Binping Xiao Collider-Accelerator Department, BNL June 15, 2015 LEReC Warm Cavity Review Meeting  June 15, 2015.
RF scheme of electron linear accelerator with energy MeV Levichev A.E. Budker Institute of Nuclear Physics SB RAS.
Renovation of the 200 MHz RF system LLRF issues. Cavities redistribution 26 October th LIU-SPS Coordination Meeting 2  2011 : 4 cavities 2 x 4.
Beam Loading experiment at KEK ATF ( Multi-train acceleration at KEK-ATF Injector ) KEK Masafumi Fukuda and Junji Urakawa LCWS /10/052 train acceleration.
0 Plenty Energy Clean Environment Healthy Life Commissioning and Initial Operation of the KOMAC 100-MeV Proton Linac KOMAC / KAERI Kyung-Tae Seol
14th ESLS RF Workshop ELETTRA / Trieste, Italy / 2010 September The Elettra Storage Ring and Top-Up Operation Emanuel Karantzoulis.
1 Al Moretti, APC, Fermilab MAP- Winter Meeting February 28 - March 4, 2011 TJNAF Newport News, VA.
MP - HIPPI General meeting, Abingdon October 28-30, Side Coupled Linac Design at CERN Side Coupled Linac Design at CERN M. Pasini, Abingdon September.
KCS and RDR 10 Hz Operation Chris Adolphsen BAW2, SLAC 1/20/2011.
LINAC4 and the Upgrade of the LHC Injector Complex R. Garoby 26 February, 2013.
Jan Low Energy 10 Hz Operation in DRFS (Fukuda) (Fukuda) 1 Low Energy 10Hz Operation in DRFS S. Fukuda KEK.
Accelerating structure prototypes for 2011 (proposal) A.Grudiev 6/07/11.
C/S band RF deflector for post interaction longitudinal phase space optimization (D. Alesini)
ALBA RF Systems Francis Perez.
Main Technical Issues of theSuper B Injector Main Technical Issues of the Super B Injector SuperB Meeting, Isola d’Elba, May 31st – June 3rd, 2008 D. Alesini,
HISTORY OF SNS DESIGN AND TECHNOLOGY CHOICES PROJECT X WORKSHOP NOVEMBER 12-13, 2007 R. KUSTOM.
Aaron Farricker 107/07/2014Aaron Farricker Beam Dynamics in the ESS Linac Under the Influence of Monopole and Dipole HOMs.
Heung-Sik Kang Pohang Accelerator Laboratory
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.
Areal RF Station A. Vardanyan
Present and possible future schemes for hadron therapy linacs Alberto Degiovanni for the ADAM team HG2017 Workshop , Valencia.
Multi-bunch Operation for LCLS, LCLS_II, LCLS_2025
A 6 GeV Compact X-ray FEL (CXFEL) Driven by an X-Band Linac
Abstract EuSPARC and EuPRAXIA projects
An X-band system for phase space linearisation on CLARA
by P. Musumeci and F.Tazzioli
Optimisation of single bunch linac for FERMI upgrade
NC Accelerator Structures
Application of the moderate peak power (6 MW) X-band klystron’s cluster for the CLIC accelerating structures testing program. I. Syratchev.
TIARA WP8 Status M. Biagini, INFN-LNF, for WP8 TIARA Mid-Term Meeting
CEPC injector high field S-band accelerating structure design and R&D
Recent high-gradient testing results from the CLIC XBoxes
CEPC RF Power Sources System
Status of the CLIC Injector studies
Advanced Research Electron Accelerator Laboratory
ATF project meeting, Feb KEK, Junji Urakawa Contents :
CLIC Feasibility Demonstration at CTF3
Operational Experience with LCLS RF systems
ERL Director’s Review Main Linac
J. Seeman Perugia Super-B Meeting June 2009
Presentation transcript:

FERMI LINAC O VERVIEW The 1.5 GeV 50 Hz Upgrade July 2013 C. Serpico

O UTLINE  FERMI Linac Layout  Operating Paramenters until RUN15  Energy and Rep. Rate Upgrade BTW Accelerating Structures Phase modulation technique  May 2013: the RF conditioning Vacuum bi-directional couplers faults  Hz  Linac Operating Condition  Conclusions Some comments… Summary What is the next? C. Serpico 2/27

L INAC L AYOUT 1/4 Linac Section # of Str. TypeInjector2S0A-S0B Linac14CERN Linac23CERN Linac32BTW Linac45BTW C. Serpico 3/27

L INAC L AYOUT 2/4 S0A – S0B accelerating structures Geometric Parameters ValueUnits Number of Cells 93 Cells' Length 33.33mm Total Length mm Min. Iris Radius 8.02mm Mean Iris Radius 9.73mm Acc. Str. RF Parameters ValueUnitsTypeMixed Operating Mode 2/3 pi Operating Frequency MHz Q factor R067.10Mohm/m Tau0.60Neper Filling Time 0.898µs C. Serpico 4/27

L INAC L AYOUT 3/4 CERN accelerating structure Geometric Parameters ValueUnits Number of Cells 134 Cells' Length 33.33mm Total Length mm Min. Iris Radius 8.02mm Mean Iris Radius 9.73mm Acc. Str. RF Parameters ValueUnits TypeConst. Grad. Operating Mode2/3 pi Operating Frequency MHz Q factor R065.00Mohm/m Tau0.84Neper Filling Time 1.255µs C. Serpico 5/27

L INAC L AYOUT 4/4 BTW accelerating structures Geometric Parameters ValueUnits Number of Cells 162 Cells' Length 37.50mm Total Length mm Iris Radius 5.00mm Acc. Str. RF Parameters ValueUnitsType Const. Imp. Operating Mode 3/4 pi Operating Frequency MHz Q factor R070.00Mohm/m Tau0.61Neper Filling Time 0.753µs SLED RF Parameters ValueUnits Operating Frequency MHz Q factor Beta10 Filling Time C. Serpico 6/27

K1GUN4.8 K2L0_147.0 K2L0_247.0 K3L1_155.2 K3L1_255.2 K4L1_X-20 K5L1_355.2 K5L1_455.2 K6L2_157.5 K6L2_257.5 K7L2_352.0 K8L3_ K9L3_ K10L4_ K11L4_ K12L4_ K13L4_ K14L4_ O PERATING P ARAMENTERS UNTIL RUN15 The Linac has been operated at 10 Hz with an overall energy gain of about 1270 MeV. C – Sections: ~ 55 MeV/section S – Sections: ~ 120 MeV/section Energy Budget on 06/2012 RF PlantKlystron Output Power [MW]Pulse Width [µs] K2  K7 ~322.0 K8  K14 ~223.0 C. Serpico 7/27

In May 4 weeks were foreseen for testing the power plants operation at 50 Hz repetition rate and the RF conditioning up to a power level corresponding to 1.5 GeV beam energy. E NERGY AND R EP. R ATE U PGRADE C. Serpico 8/27

E NERGY AND R EP. R ATE U PGRADE To get 1.5 GeV beam energy at the end of the Linac the 7 BTW S-type accelerating structures have to be pushed up to an energy gain of about 155 MeV/section (corresponding to a gradient of 26 MV/m).  Linac3: two sections  Linac4: presently five sections  From old Elettra injector.  Both Linac 3 and Linac 4 RF power distribution systems are equipped with SLED systems. C. Serpico 9/27

BTW A CCELERATING S TRUCTURES S-type structures are Backward Traveling Wave (BTW) structures comprised of 162 nose cone cavities coupled magnetically. Type Const. gradient, mag. coupled Mode 3 π /4 Frequency MHz Length6.15m Q11000 R sh 71-73MOhm/m Filling time 0.747µs  Past operation of the BTW accelerating structures showed that such structures suffered heavy breakdown phenomena when pushed to high gradient (no phase modulation implemented).  Single cell simulation shows that surface electric field on the magnetic coupling slot becomes of the same magnitude and even higher than the surface electric peak field on the nose. C. Serpico 10/27

T HE P HASE M ODULATION T ECHNIQUE SLED operation with Phase Modulation:  Amplitude of klystron output is kept constant during the RF Pulse  95º Phase Shift 0.77 µs before the end of the pulse  Phase changed gradually (slope = 149º/µs)  Phase kept constant during the last 200 ns of the RF pulse Note: Phase offset and Phase Slope Parameters adjustable by LLRF Sled Phase Modulation - 3 us t (us) Amp (a.u.) Measured Cavity Input Field 3µs pulse E pk-cav /E pk-kly = 1.83 (field ratio) P pk-cav /P pk-kly = 3.34 (power ratio) C. Serpico 11/27

Even if the RF pulse shape is not flat, for a 3 µs overall pulse width the energy gain loss with respect to the normal operation is just 3.3 % T HE P HASE M ODULATION T ECHNIQUE RF width [µs] E pk-cav /E pk-kly [field ratio] Gain Factor Normal Operation Phase Modulation Normal Operation Phase Modulation C. Serpico 12/27

M AY 2013: T HE RF C ONDITIONING From K2 to K7: (S0A-S0B & CERN sections)  Same Klystron Output Power as before (~32 MW)  Same Pulse Length as before  Repetition rate from 10 Hz to 50 Hz From K8 to K14: (equipped with SLED systems)  Klystron Output Power increased up to 32 MW (from the past 22 MW operation)  Pulse Length up to 3.0 µs  Input power to the structure increased from 62 MW up to 91 MW peak.  Repetition rate from 10 Hz to 50 Hz RF conditioning started on 6 th of May and it took about 4 full days to get to the target operating parameters. RF conditioning started on 9 th of May. Kly Output Power [MW] Pulse Width [µs] Rep Rate [Hz] Strucutre Input Power [MW] Up to RUN 15~ RUN 16~ C. Serpico 13/27

 All 3 directional couplers were installed between the output of the SLED system and the input coupler of the accelerating structures.  Vacuum leaks were detected only on the 50dB pick-up ceramic windows.  Cracks on ceramic windows were experienced on directional couplers produced by 2 different firms. During RF conditioning we experienced 3 major faults (on two different plants) on bidirectional couplers as a consequence of breakdown events in accelerating structures. M AY 2013: T HE RF C ONDITIONING Vacuum Bi-directional Couplers Faults C. Serpico 14/27

Bethe hole coupler type:  ~60 dB coupling on Forward Port  ~50 dB coupling on Backward Port  ~23 dB directivity M AY 2013: T HE RF C ONDITIONING Vacuum Bi-directional Couplers Changing the RF design of the coupler is needed! Bethe hole coupler with lower coupling on the Reflected Port (~60 dB) (the available length is 159 mm, mandatory!) C. Serpico 15/27

1.5 G E 50 H Z On 31 st of May an energy of GeV (on crest) at 50 Hz repetition rate was reached. C. Serpico 16/27

L INAC O PERATING C ONDITION  According to the FERMI Commissioning Plan, the commissioning of FEL2 line with a 1.5 GeV beam energy was foreseen starting from 10 th of June.  On 31 st of May, 1.5 GeV beam energy (on crest) was reached with the Linac operating at 50 Hz. While operating Linac with the above parameters, the breakdown rate was high to guarantee the desired uptime for the FEL2 line commissioning. To guarantee a reliable operation of the FERMI Linac during FEL2 commissioning in June, on 3 rd of June it was agreed to bring the Linac back to 10 Hz repetition rate while still pushing the energy gain at 1.46 GeV. Commissioning of FEL2 during June C. Serpico 17/27

L INAC O PERATING C ONDITION A comparison between the 50 Hz and the 10 Hz operation Faults rate and faults rate distribution before and just after switching back to 10 Hz on a 24 hours basis. Faults rate and faults 50Hz, ~1.5 GeV Faults rate and faults 10Hz, ~ 1.5 GeV C. Serpico 18/27

L INAC O PERATING C ONDITION A comparison between the 50 Hz and the 10 Hz operation Vacuum trends before and just after switching back to 10 HzK14 50 Hz Operation 10 Hz Operation 3.0e -9 mbar 1e -9 1e -8 1e -7 1e Hz Operation 10 Hz Operation K8 1.5e -9 mbar 1e -9 1e -8 1e -7 Most of the vacuum spikes have been detected by ion pumps closer to the structures input: breakdown events take place in structures input couplers and structures cells. C. Serpico 19/27

C ONCLUSIONS

S OME COMMENTS …  BTW accelerating structures were rated for working up to 35 MV/m accelerating gradient at 10 Hz repetition rate.  While operating as Elettra injector, such structures suffered heavy breakdown phenomena if pushed to gradient of MV/m. At that time no Phase Modulation technique was implemented.  In September 2011 Phase Modulation techinque was implemented. Some tests were done at 10 Hz on one plant: an overall energy gain of 165 MeV (~27.5 MV/m) was reached without any major issue. BTW accelerating structures …making a long story short … C. Serpico 21/27

S OME COMMENTS …  In May 2013, four weeks of RF conditioning were foreseen to reach a gradient of MV/m on each BTW structure while operating for the first time at 50 Hz repetition rate.  In May 2013 Just after reaching 1.5 GeV (with a gradient of 25 MV/m on each BTW structure) at 50 Hz repetition rate we had the third directional coupler fault.  We decided to reduce the gradient to about 23 MV/m on BTW structures and switch back to 10 Hz repetition rate. BTW accelerating structures …making a long story short … Is Hz a real limit for our BTW structures? C. Serpico 22/27

S OME COMMENTS … Breakdown diagnostic On all the plants Bethe hole bi-directional couplers are installed.  At the output of the klystrons On all the plants the backward power signal is used to shut- off the RF in case of breakdown events to protect the klystron itself.  At the input of the accelerating structures On RF plants equipped with SLED system, the forward power signal is just used for tuning the SLED cavity.  On RF plants equipped with SLED system, bi-directional couplers installed at the output of the klystron are not able to detect any breakdown event originated from the RF structure.  RF breakdown are detected using signals coming from ion pumps installed in the system. C. Serpico 23/27

S UMMARY Increase of operational margin at 1.5 GeV possible with the installation of the 2 accelerating structures already foreseen in the machine layout  1.5 GeV Linac energy (on crest) has been reached at 50 Hz repetition rate.  Stable operation of the Linac with about 1.46 GeV (on crest) beam energy at 10 Hz repetition rate. 1.Phase Modulation Improve pulse shape flatness 2.New Bi-directional Couplers Bethe hole couplers? Mechanical length of 159 mm is mandatory 3.Improve breakdown diagnostic Upgrades Achievements C. Serpico 24/27

W HAT IS THE NEXT … The Machine Advisory Committee (MAC meeting, June 2013) strongly suggested to consider the possibility of installing a SLED system on CERN-type structures. SLED on CERN-type accelerating structures? Acc. Str. RF Parameters ValueUnits Total Length~4.5m Q factor R065.00Mohm/m Tau0.84Neper Filling Time 1.255µs SLED RF Parameters ValueUnits Q factor ~ Beta6 Filling Time 1.5µs P kly RF Pulse Energy Gain Gradient [MW][µs][MeV][MV/m] NO SLED operation ~13 SLED operation ~17 C. Serpico 25/27  About 120 MeV more with a SLED system installed on 7 CERN type accelerating structures.  About 700 k€ SLED operation ~17

W HAT IS THE NEXT … All 6 meter long, BTW accelerating sections are 20 years old structures. A reliable solution to replace them is under investigation.  Each structure could be replaced by one accelerating module endowed with three 2-meter long accelerating structures.  Keeping the same power plant, new accelerating modules could guarantee a slightly higher energy gain.  With a 80 MW peak power klystron (commercially available) a 40 MV/m accelerating gradient could be achieved. A preliminary idea …high gradient 2-m long structures… C. Serpico 26/27

T HANK YOU