Improved on line performance of the installed ALPI Nb sputtered QWRs A.M. Porcellato, S. Stark, F. Stivanello, L. Boscagli F. Chiurlotto, D. Giora, M.

Slides:



Advertisements
Similar presentations
S.M. Deambrosis*^, G. Keppel*, N. Pretto^, V. Rampazzo*, R.G. Sharma°*, F. Stivanello* and V. Palmieri*^ Padova University, Material Science Dept * INFN.
Advertisements

Report from: the High Intensity Stable Beam Working Group HISB-WG Marie-Helene Moscatello (GANIL) Annamaria Porcellato (Legnaro) Uli Ratzinger (GSI) Faical.
RF Specification discussion MICE RF workshop 16 th April 2012.
MICE RF Cavities and RFCC Module Update Derun Li Lawrence Berkeley National Laboratory MICE RF Workshop Daresbury Laboratory, UK April 17, 2012 April 17,
Muon g-2 Muon g-2 Experiment Quarterly Report Aria Soha All Experimenter’s Meeting March 2, 2015.
MICE RF Cavity Design and Fabrication Update Steve Virostek Lawrence Berkeley National Laboratory MICE Collaboration Meeting October 27, 2004.
Plans for 201-MHz Cavities Derun Li Center for Beam Physics Lawrence Berkeley National Laboratory November 18, 2010.
RF Measurement Plan Derun Li Center for Beam Physics Lawrence Berkeley National Laboratory January 20, 2011 MICE Video Conference Meeting.
Integration of Cavities and Coupling Coil Modules Steve Virostek Lawrence Berkeley National Laboratory MICE Collaboration Meeting March 28 – April 1, 2004.
MICE RF Cavity Measurements Derun Li Center for Beam Physics Lawrence Berkeley National Laboratory March 26, 2010 University of California, Riverside,
Status of the 201 MHz Cavity and Coupling Coil Module Steve Virostek Lawrence Berkeley National Laboratory MICE Video Conference March 10, 2004.
D. Li and R. Rimmer, RF Workshop, Fermilab, MHz Cavity Refurbishment and suggestions on future tests Derun Li and Robert Rimmer* Lawrence.
ANL HWR Cryomodule Status Update 27 January 2015 Zachary Conway On behalf of the ANL Linac Development Group Argonne National Laboratory Physics Division.
G. Olry, H-M Gassot, S. Rousselot (IPN Orsay) EuCARD-SRF annual review 2011, 4-5 May, IPN, Orsay Unité mixte de recherche CNRS-IN2P3 Université Paris-Sud.
RF Cavity of CIS Xiaoying Pang Mar. 12 th, 2007 IUCF.
SPL cryo-module conceptual design review Cavity, helium vessel and tuner assembly N. Valverde, G. Arnau, S. Atieh, I. Aviles, O. Capatina, M. Esposito,
201 MHz and 805 MHz Cavity Developments in MUCOOL Derun Li Center for Beam Physics Lawrence Berkeley National Laboratory Nufact 2002 Workshop, London,
201 MHz NC RF Cavity R&D for Muon Cooling Channels
Athmospheric Surface Treatments of Niobium A. Camacho*^, A.A. Rossi* and V. Palmieri*^, * INFN – Legnaro National Laboratories ^ University of Padua.
ESS cavities interfaces
Page 1 Jean Delayen HyeKyoung Park Center for Accelerator Science Department of Physics, Old Dominion University and Thomas Jefferson National Accelerator.
RF power & FPC status Eric Montesinos, CERN BE-RF on behalf of all people involved, great thanks to all of them !
Cavity degradation after vert. test on the way or in the module, James Kerby ~10% agreement in results across laboratories typical ~20% degradation VT.
1 Nb Sputtered Cu QWR: a 20 years experience from an idea to the routine beam acceleration A.M. Porcellato S. Stark V. Palmieri F. Stivanello.
Technical aspects of the ATLAS efficiency & intensity upgrade Peter N. Ostroumov ATLAS Users Workshop, August 8-9, 2009.
Summary of WG 2 - cavities W. Weingarten 15th SPL Collaboration Meeting CERN - 25/26 Nov Cavity WG.
201 MHz Cavity Status and Test Plans at MTA MICE Collaboration Meeting at RAL, UK October 22 ~ 24, 2005 Derun Li Center for Beam Physics Lawrence Berkeley.
F.E.T.S. RFQ Mechanical Design by Peter Savage 7 th January 2010.
STF EP, VT commissioning by FNAL AES001 H. Hayano, KEK
RF Sources and Combiners Emma Wooldridge. 28th-29th April 2004Joint Accelerator Workshop Outline Very quick RF power overview RF power sources –Triodes.
Operations Tandem ALPI PIAVE of LNL accelerators D. Carlucci 2012 August 6th Workshop on Accelerator Operations 1 WAO 2012 August 6, 2012 Davide Carlucci.
ISTC Project #3888 Development, manufacture and experimental investigation of a unique pilot CCDTL accelerating section in the energy range of MeV.
Mid Term Review Meeting, 26 September 2012N. SURNAME1 * The research project has been supported by a Marie Curie Early Initial Training Network Fellowship.
Experience with LEP (and LHC) cryo-modules Workshop on cryogenic and vacuum sectorisations of the SPL O.Brunner – November ’09.
MICE RF Cavities and RFCC Module Update Allan DeMello and Derun Li Lawrence Berkeley National Laboratory MICE CM32 at RAL, UK February 9, 2012 February.
MICE RF Cavity Measurements Derun Li Center for Beam Physics Lawrence Berkeley National Laboratory July 8, 2010 Rutherford Appleton Laboratory, UK.
 =1 cavity: parameters Dimensions for cavity fabrication before any chemical polishing and at room Temp. outer ½ cell pick-up side inner ½ cells outer.
Performance analysis of cryogenic system and cryomodules for the complete superconducting linear accelerator at IUAC, New Delhi. T S Datta ( On behalf.
Cryostat & LHC Tunnel Slava Yakovlev on behalf of the FNAL team: Nikolay Solyak, Tom Peterson, Ivan Gonin, and Timergali Khabibouline The 6 th LHC-CC webex.
7-Sep-2011 CLIC RF Structure Development Meeting «BE/RF» TD26 WITH COMPACT COUPLER FOR CLEX (TD26 CC SiC) ENGINEERING DESIGN this structure will be used.
TAC2 Alpi consolidation in Cryogenics and Cryomodules.
ESS AD RETREAT 5 th December 2011, Lund “A walk down the Linac” SPOKES Sébastien Bousson IPN Orsay.
Slide 1 of 10Matthew Fraser – CI MEW Meeting, 25 th October 2010.
HIE-ISOLDE state of the art and future plans & CLIC Plans A. D’Elia 1.
Preparation procedure and RF processining of cERL-ML power coupler at KEK Hiroshi Sakai, Takaaki Furuya, Masato Sato, Kenji Shinoe, Kensei Umemori, Kazuhiro.
Athmospheric Surface Treatments for improving 6Ghz Niobium cavities V. Palmieri, A. Rossi, K. Atroshchenko, D. Rizetto, A. Camacho, S.Yu. Stark * INFN.
201 MHz Cavity Plans Derun Li Center for Beam Physics Lawrence Berkeley National Laboratory February 11, 2011 MAP Friday Video Conference Meeting.
RF Modeling of the LHC Crab Cavity Zenghai Li SLAC Zenghai Li LARP CM20 April 8-10, 2013.
PXIE RFQ Engineering Design Steve Virostek Engineering Division Lawrence Berkeley National Laboratory April 10, 2012 Project X Collaboration
RFCC Engineering Status and Plans Allan DeMello Lawrence Berkeley National Laboratory MAP Winter Meeting March 6, 2012 March 6, 2012.
RFQ coupler S. Kazakov 07/28/2015. Requirements: Coupler requirements Expected problems: Heating (loop, ceramic window, etc.) Multipactor Solutions: Appropriate.
Engineering of the power prototype of the ESRF HOM damped cavity* V. Serrière, J. Jacob, A. Triantafyllou, A.K. Bandyopadhyay, L. Goirand, B. Ogier * This.
Developments of new treatment techniques for SRF cavities at KEK HORIZONTAL HPR FOR PERFORMANCE RECOVERY Yoshiyuki MORITA Motivation of developing HHPR.
EURISOL CB MEETING – PSI – 15 JUNE 2006 Sébastien Bousson IPN Orsay – Accelerator Division TASK 8 STATUS REPORT INFN – Legnaro IPN Orsay.
WP1: Superconducting Cavity Developments and Tests Walter Venturini Delsolaro Mid Term Review Meeting, 26 September 2012 CATHI Marie Curie Initial Training.
LCWS11 WG4 Fully featured accelerating structure engineering design
Resource Loaded Schedule and Budget Profile
RF Dipole HOM Electromagnetic Design
Bunching system for SPES project
RF Sources and Combiners
T5.2: Harmonization - Material and Component Reference
Technical Issues Facing in the FRIB Cryomodule
Odu/slac rf-dipole prototype
Complementary ISTC Projects #3888, 3889p
by P. Musumeci and F.Tazzioli
THE HIE-ISOLDE SUPERCONDUCTING CAVITIES:
Operation experience of cryogenic system and cryomodules for the superconducting linear accelerator at IUAC, New Delhi. T S Datta ( On behalf of Cryogenics.
HIE-LINAC status report
Pulsed Ion Linac for EIC
SNS PPU CRYOMODULE PDR Cleanroom Assembly Katherine Wilson
Presentation transcript:

Improved on line performance of the installed ALPI Nb sputtered QWRs A.M. Porcellato, S. Stark, F. Stivanello, L. Boscagli F. Chiurlotto, D. Giora, M. De Lazzari Laboratori Nazionali di Legnaro HIAT 09, Venice, 12 June 2009

A.M.Porcellato, Lea Workshop, Padua April 7 th ALPI TANDEM PIAVE ECR

ALPI resonators , 80 MHz, full Nb=0.13, 160 MHz, Nb/Cu , 160 MHz,Nb/Cu , 160 MHz, Pb/Cu

 CR20 resonators are in ALPI since 1998 T are drilled from a billet of OFHC Cu, 99.95% No brazed joints The average operational accelerating field is 6 MV/m  Installed in CR20 and CR19  Very simple shape  External beam ports jointed by In gaskets  Rounded shorting plate  Capacitive coupler  =0.13; f= 160 MHz ALPI high  QWRs

 CR19 cavities installed ALPI in 2001, similar in inner shape to CR20 cavities made in SeCu circumferential brazed joint brazed collar and supports ALPI high  QWRs

CR19 and CR20 year [MV/m] CR19 and CR20  Better performance in CR20  Lower performance in CR19 (similar shape but different construction technology)  2 cavities to be repaired because of a stuck coupler and rf line damage, High  QWRs

 Brazed joints (especially the ones in the outer resonator surface)  Flat shorting plate  Beam ports shape  Inductive coupler (hole in high current region) ALPI  = MHz Limited the reached performance to a lower level than the ones of high  resonators. ALPI medium  QWRs Originally Pb plated; Nb sputtered in between Pb Nb

Q CR7 and CR8 CR9 and CR10 CR12 and CR13 MV/m CR16 and CR17 CR18 Q-curves of medium  cavities installed in ALPI cryostats Q MV/m

[MV/m] CR7 and CR8 CR9 and CR10 CR12 and CR13 CR14 and CR15 CR16 and CR17 CR18 year Operational Ea in QWRs of medium  cryostats [MV/m] rinsing year

, Iimprovements maintaining old substrates  More accurate “Lifting ” of the old Cu substrate (the opening of all the trapped enclaves was not well performed in the first produced resonators)  Better tuning plate contact to avoid Indium joint (by modifying the end plate and doubling its fixing screws)  HPW resonator rinsing  Cleaner assembling condition before and after sputtering  Longer high power rf conditioning

 We have To align the resonators with their beam port open to air. To close the cryogenic circuits after the resonator assembling  It would surely help: – Avoid cryostat venting to air (because of cryogenic circuits leaks) – Perform high pressure rinsing after resonator alignment (possible if we have not the In joint) – Longer rf and He conditioning (5 MV/m 7W in old substrates) Drawbacks /possible improvements

Nb/Cu Average 4.83MV/m Nb/Cu Operational Ea : 4.70 MV/m Pb/Cu Average Ea: 2.48 MV/m * 2000* 1999* * Nb/Cu ALPI QWR Performance 1998 * Recent cryostat maintenance Cryostat installation year

old New medium  QWRs We have 4 new cavities ready with – New beam port design – A rounded shorting plate – A capacitive coupler – Without holes in high current regions – Without brazing in the outer resonator body

New medium  QWR performance 4 READY  4 cavities produced (MBD2 sputtered twice)  Improvement due to cathode optimization  Tested up to 3MV/m in laboratory  Ea between 5.5 and 6.5 expected on line  Better results possible but we prefer to install them in CR15 as soon as possible

 Since 2001 most of the ALPI equivalent voltage (  V) is provided by Nb/Cu cavities  Operation at Ea determined by the available cryogenic power  No frequency tracking or fast tuning required  No degradation with time; average fields is still improving  Low  have to be locked at Ea <3.5 MV/m in ALPI  Higher operational Ea expected by increasing the rf driving power; new rf cryostat lines and a L.N cooled coupler required L Cavities at work W=energy gain q=State of charge

16  Nb, 80 MHz,  =0.056, 12+(4) resonators  Excellent performance: 6.7 7W  Installed in between  Mechanical dampers effectively reduce their sensitivity to acoustic vibrations  Sensitivity to He bath pressure drifts (1Hz/mbar) made the cavity locking tricky when the resonators were cooled by the very noisy ALPI cryogenic system  Operating up to 3.5 MV/m in ALPI;4.2 MV/m in PIAVE; 2/3 out of work  Upgraded tuners, amplifiers, bottom plates…  New L.N 2 cooled couplers coming soon  Expected 5 MV/m in lock condition Low  section

HIAT Pressure excursions in ALPI cryostats

Surface finishing and chemical treatments.  Frequency adjustment by electro- polishing  Electro-polishing (20  m, 2 hours, phosphoric acid +butanol, computer controlled)  Rinsing (water, ultrasonic water, HPR)  Chemical polishing (10  m, 4 min, SUBU5)  Passivation (sulphamic acid)  Rinsing (water, ultrasonic water, HPR)  Drying (ethanol, nitrogen)

Biased Nb sputtering Good vacuum Backing No discharges High substrate temperature Cathode: Nb tube Cu base Sputtering chamber Sputtering performed in about 12 steps of 15’ Production cycle asks for 9 days

Nb sputtering advantages  Mechanical stability (mechanical vibrations are not an issue)  Frequency not affected by changes He bath (  p <0.01Hz/mbar, no frequency tracking)  Reduced over-coupling (smaller amplifier, coupler do not need cooling, rf lines have reduced size and limited rf dissipation)  High thermal stability (less prone to hot spots, conditioning easier)  Stiffness (in case of loss of isolation vacuum leak…)  Absence of Q-disease (less demand on cryogenic system cooling velocity and reliability)  Insensitivity to small magnetic fields (no magnetic shielding)  High Q of the N.C. cavity (easier coupling in N.C state, better multipactor conditioning)  Lower X-ray production (lower power available for field emission)  Absence of In vacuum joints (vacuum leaks less probable)  Price (both material and construction)

Conclusion  The Nb sputtering technology showed to be very effective in producing reliable resonators, which have high performance, are very steadily phase locked and are easy to put into operation.  Even better results were obtained using suitable substrates.  The high number of produced and operational resonators and the reliability of the sputtering. Thanks for your attention!

A.M.Porcellato, Lea Workshop, Padua April 7 th Cryostat maintenance Change of the leaking cryogenic valve (external actuator) Viton sealing in the cryostat beam line valves, from resonator integral conditioning (changed + shielded through stainless steel rings) Gaskets in the He circuits (changed + fixed by silver plated screws) Leaks on the cryostat upper thermal shield RF lines (Mechanical adjustments + Cu re-plating)