ANL/FNAL/UC Collaboration meeting 27 June 2008 SRF Materials: First Acceleration Test of Coated Cavities Pellin 1, Zasadzinski 2, Proslier 1,2, Norem 3,

Slides:



Advertisements
Similar presentations
Prospect of High Gradient Cavity H. Hayano, Tohoku Forum for Creativity 2013.
Advertisements

Point contact tunneling spectroscopy and Atomic layer deposition for superconducting rf cavities Thomas Prolier, Mike Pellin, Jim Norem, Jeff Elam. Collaboration:
The Continuing Role of SRF for AARD: Issues, Challenges and Benefits SRF performance has been rising every decade SRF installations for HEP (and other.
Superconducting Materials R&D: RRCAT-JLAB Collaboration S B Roy Materials & Advanced Accelerator Science Division RRCAT, Indore Collaborators: M. K. Chattopadhyay,
An ab-initio Study of the Growth and the Field Emission of CNTs : Nitrogen Effect Hyo-Shin Ahn §, Tae-Young Kim §, Seungwu Han †, Doh-Yeon Kim § and Kwang-Ryeol.
Fundamental Studies on SRF Materials – Interfacial Oxidative Chemistry of Niobium Progress Report July 2007 to June 2008.
Presented by Grigory Eremeev Grigory Eremeev. Presented by Grigory Eremeev Outline: - Cavities and Fields; - Results; - Tricks of the Trade: new shapes;
Atomic Layer Deposition for SCRF RF in the MTA 11/15/10 J. Norem ANL/HEP.
PEALD/CVD for Superconducting RF cavities
SRF Materials Workshop; MSU, October 29-31, 2008 Recent Progress with Atomic Layer Deposition T.Proslier 1,2, J.Norem 1 J.Elam 3, M.Pellin 4, J.Zasadzinski.
SRF Materials R&D Alex Gurevich 1 & Pierre Bauer 2 1 Applied Superconductivity Center, UW/NHMFL 2 Fermi National Accelerator Laboratory AARD Meeting Fermilab,
RF background, analysis of MTA data & implications for MICE Rikard Sandström, Geneva University MICE Collaboration Meeting – Analysis session, October.
MUCOOL RF Program Derun Li Center for Beam Physics Lawrence Berkeley National Laboratory MUTAC Review at BNL April 18, 2007.
Superconducting RF Materials University Collaboration STATUS Lance Cooley June 07, 2010.
Rong-Li Geng Jefferson Lab High Efficiency High Gradient Cavities - Toward Cutting Down ILC Dynamic Heat Load by Factor of Four R.L. Geng, ALCW2015,
Status of RFCC-Module Development Derun Li Center for Beam Physics Lawrence Berkeley National Laboratory MICE Collaboration Meeting at INFN-LNF, Frascati,
201 MHz NC RF Cavity R&D for Muon Cooling Channels
Cooley – Main Linac ILCTA 1 Summary of the SRF Materials Workshop held October at Michigan State Univ. hosted by MSU, NSCL, and Fermilab
Rong-Li Geng Toward Higher Gradient and Q 0 LCWS2013, U. of TokyoNov , 2013, R.L. Geng1.
R EVIEW ON Q - D ROP M ECHANISM B ernard V ISENTIN International Workshop on Thin Films 9 th - 12 th October 2006.
Summary SRF project at Argonne National Laboratory (started 11/09) Investigators: Th. Proslier, J. Klug, N. Becker, M. Kharitonov, H. Claus, J.Norem, M.
Update on SRF Activities at Argonne Mike Kelly, Peter Ostroumov, Mark Kedzie, Scott Gerbick (PHY) Tom Reid, Ryan Murphy (HEP) Thomas Proslier, Jeff Klug,
FNAL/ANL/UC SRF R&D Collaborations Lance Cooley – new SRF Materials Group Leader at FNAL.
EuCARD Task 10.4 Sergio Calatroni. Sub-task New and improved techniques for the production of Nb sputtered Quarter Wave (QW) cavities (CERN, INFN-LNL)
Structure of the task 12.2 Claire Antoine Eucard2 WP12 DESY
CLIC Workshop – CERN, October / 17 DC breakdown experiments for CLIC CERN, TS-MME Antoine Descoeudres, Trond Ramsvik, Sergio Calatroni, Mauro Taborelli.
1Claire AntoineCEA/Saclay - Fermilab (Innovative) Processing of materials SRF materials Workshop Fermilab May 23-24, 2007 Today’s process is long, complex,
High Q R&D at JLab G. Ciovati, P. Dhakal, R. Geng, P. Kneisel, G. Myneni TTC Topical Meeting on CW SRF Cornell Univ., June 12 th -14 th, 2013.
RF breakdown in multilayer coatings: a possibility to break the Nb monopoly Alex Gurevich National High Magnetic Field Laboratory, Florida State University.
R.L. Geng, 5/27-31,2013 ECFA LC2013, DESY 1 Update on Raising Q0 at Ultra-High Gradient via Large-Grain Niobium Material Rongli Geng Jefferson Lab ECFA.
S.M. Deambrosis*^, G. Keppel*, N. Pretto^, V. Rampazzo*, R.G. Sharma°, D. Tonini * and V. Palmieri*^ Padova University, Material Science Dept * INFN -
Q-Slope at High Gradients ( Niobium Cavities ) Review about Experiments and Explanations Bernard VISENTIN CEA - Saclay.
RF studies at Fermilab MuCool Test Area Fermilab MuCool Test Area MuCool Test Area (MTA) at Fermilab is a dedicated facility at the end of the LINAC built.
Passivation of HPGe Detectors at LNL-INFN Speaker: Gianluigi Maggioni Materials & Detectors Laboratory (LNL-INFN) Scientific Manager: Prof. Gianantonio.
1 Vacuum chambers for LHC LSS TS Workshop 2004 Pedro Costa Pinto TS department, MME group Surface Characterization & Coatings Section.
Update on S0 Work in the Americas Region Mark Champion 17 June 2008.
Advances in Development of Diffused Nb3Sn Cavities at Cornell
Origin of unusual Ag diffusion profiles in CdTe 1 J. Lehnert, M. Deicher, K. Johnston, Th. Wichert, H. Wolf Experimentalphysik, Universität des Saarlandes,
CLIC09 WG4 RF Structure1 Engineering Perspectives on Quadrants (2) CLIC09 Workshop KEK Y.Higashi.
ALCPG2011, 3/19- 23, SRF Group Institute of Heavy Ion Physics, Peking University ALCPG /3/19-23, Eugene, Oregon, USA RF superconducting Cavity.
Updates and status on the next generation of Superconducting RF cavities 7 th of March 2013 Argonne National Laboratory DOE Review 2013 Speaker: Thomas.
Experiments to probe the inverse Spin-Hall Effect in GaAs U. Pfeuffer, R. Neumann, D. Schuh, W. Wegscheider, D. Weiss 7. June 2008 University of Regensburg.
Scanning Tunneling Microscopy Studies of Single-Crystal Niobium Oxidation Natalie A. Kautz, Yichen Yu, Kevin D. Gibson.
Annual Meeting CERN - November 2005 Bernard V ISENTIN.
Atomic-scale characterization of Nb for SRF cavities using UV
Point Contact Tunneling as a Surface Superconductivity Probe of bulk Nb and (Nb 1-x Ti x )N Thin Films Chaoyue Cao Advisor: J. Zasadzinski ANL N. Groll,
This work is supported by the US DOE/HEP and also by the ONR AppEl, and CNAM. Comparison Between Nb and High Quality MgB 2 Films for Their Mesoscopic Surface.
MIT Lincoln Laboratory 1 Magnesium Diboride Films for SRF Cavity Applications Y. D. Agassi Naval Surface Warfare Center, Carderock Division, Bethesda MD.
Niobium RRR and Ta specifications for SRF cavities: a critical review G. Ciovati, P. Kneisel and G. Myneni 7 th SRF Materials Workshop, July 16 th 2012.
Anne-Marie VALENTE-FELICIANO On behalf of the HEPTHF Collaboration.
RF Superconducting Materials Workshop at Fermilab, May 23 & 24, 2007 Advanced Nb oxide surface modification by cluster ion beams Zeke Insepov, Jim Norem.
Rongli Geng ILC Cavity Group Meeting October 25, 2011
Ultimate gradient limitation in Nb SRF cavities: the bi-layer model and prospects for high Q at high gradient Mattia Checchin TTC Meeting, CEA Saclay,
Superconducting NbN Thin Films Synthesized by Atomic Layer Deposition
Pulsed Energetic Condensation of Nb Thin Film Cavities at JLab
ILC-SCRF Test Facilities considerations
New Cavity Techniques and Future Prospects
JLab infusion and LG flux expulsion update
for the FNAL/ANL, JLab, and Cornell cavity teams
Main Linac EDR Planning: Cavity Fabrication Discussion W. Funk / H
Peng Sha Institute of High Energy Physics, CAS
High Q via N infusion R&D at Jefferson Lab
S0 Status report from KEK
A COMMON R&D ON THE HIGH GRADIENT Nb CAVITIES
Materials, Advanced Accelerator Science & Cryogenics Division
SRF Surface Studies and the High Field Q-slope Mystery
Quench Studies in Single and Multicell N-Doped Cavities
SRF Science and Technology
JLab Work on Low Temperature Near-Surface Diffusion aka “Infusion”
Infusion R&D at DESY TTC Meeting at TRIUMF –
Presentation transcript:

ANL/FNAL/UC Collaboration meeting 27 June 2008 SRF Materials: First Acceleration Test of Coated Cavities Pellin 1, Zasadzinski 2, Proslier 1,2, Norem 3, Cooley 4, Kneisel, Rimmer 5 1.Materials Science Division, ANL 2.Department of Biological, Chemical and Physical Sciences, IIT 3.High Energy Physics, ANL 4.Technical Division, FNAL 5.JLab ANL-LDRD

ANL/FNAL/UC Collaboration meeting 27 June 2008 XPS a Surface Probe of Nb Oxidation Nb 2 O 5 Nb NbO x Dielectric Nb 2 O 5 Nb 2 O 5- , NbO 2-  are magnetic NbO x (0.2 < x < 2),metallic NbO x precipitates (0.02 < x < 0.2) Scattering off magnetic interfaces or precipitates gives rise to Shiba states inside the gap. These cause dissipation (lowering Q). Nb samples supplied by FNAL!

ANL/FNAL/UC Collaboration meeting 27 June 2008 Point Contact Tunneling (PCT) Reveals the presence of dissipative Cooper pair breaking layers on the surface of cavity grade, processed Nb samples. Likely Source? Magnetic layers (Nb 2 O 5-  ) among the complex oxidized Nb surface Appl. Phys. Lett. 92, / Cavity grade Nb (Measured) Fit Assuming Idealized BCS Superconductor Fit Assuming BCS + Pair Breaking Surface Layer

ANL/FNAL/UC Collaboration meeting 27 June 2008 Point Contact Tunneling (PCT) Reveals the presence of dissipative Cooper pair breaking layers on the surface of cavity grade, processed Nb samples. Likely Source? Magnetic layers (Nb 2 O 5-  ) among the complex oxidized Nb surface Appl. Phys. Lett. 92, / Cavity grade Nb (Measured) Fit Assuming Idealized BCS Superconductor Fit Assuming BCS + Pair Breaking Surface Layer

ANL/FNAL/UC Collaboration meeting 27 June 2008 A Solution? Atomic Layer Deposition -> non-dissipative dielectric layer 1.Use ALD to synthesize a dielectric diffusion barrier on the Nb surface 2.Bake to “dissolve” the O associated with the Nb layer into the bulk

ANL/FNAL/UC Collaboration meeting 27 June 2008 Point Contact Tunneling (PCT) + ALD  (1.55meV = Nb).  (pair breaking) -> 500 C bake should significantly reduce dissipation Appl. Phys. Lett. in prep 

ANL/FNAL/UC Collaboration meeting 27 June 2008 Cavity Experimental Plan 1.Obtain a Single Cell Cavity from JLab a)“good” performance b)Tested several times 2.Coat cavity with 10 nm’s Al 2 O 3, 3 nm Nb 2 O 5 a)Niobia to reproduce original cavity surface b)Dust, clean room care 3.Acceleration Test at J Lab a)First test of ALD on cavities b)Check for “stuck” dust, high pressure rinse difficulties, material incompatibilities, etc. c)Goal: No performance loss Fermi, JLab (in progress)

ANL/FNAL/UC Collaboration meeting 27 June 2008 J Lab Cavity: Best Previous Performance Strong field emission for last 5 MV/m

ANL/FNAL/UC Collaboration meeting 27 June 2008 J Lab Cavity: Last Acceleration Test (Cluster Cleaning) Cavity “as received” for ALD Cavity Treatment

ANL/FNAL/UC Collaboration meeting 27 June 2008 J Lab Cavity: After ALD Synthesis (10 nm Al 2 O nm Nb 2 O 5 ) Only last point shows detectable field emission. 2 nd test after 2 nd high pressure rinse. (1 st test showed field emission consistent with particulates)

ANL/FNAL/UC Collaboration meeting 27 June 2008 Conclusions ALD is a compatible method for SCRF Cavity Processing. No significant multipactoring. –Alumina underlayer does not enhance –Other surface choices? Many better choices than Nb 2 O 5 are available. Field Emission reduction (dielectric improvement). –Alumina is a much better dielectric than than Nb 2 O 5 –Is 10 nm optimum? Thicker, two step coating, etc. Improved Performance from last result. –200 C during layer synthesis + surface reduction Improved performance vs previous best –3x improvement in Q, slight gradient enhancement –Anneal? Cavity Annealing Coating is proceeding.