Electron Stimulated Desorption of OFE Copper Chiara Pasquino, Politecnico di Milano 9th March 2011, RF Structure Meeting.

Slides:



Advertisements
Similar presentations
RHIC electron cloud and vacuum pressure rise characteristics P.He, H.C.Hseuh, W.Fischer, U.Iriso, D.Gassner, J.Gullotta, R.Lee, L.Smart, D.Trbojevic, L.F.Wang.
Advertisements

11-13/10/2007 ILC BDS Kick-Off Meeting, SLAC, US 1 BDS Vacuum System Dr. Oleg B. Malyshev ASTeC Daresbury Laboratory.
High gradient studies in simple setups (for discussion) T. Higo.
Parametric Study of the Ignition of Metal Powders by Electric Spark Graduate Mentor: Ervin Beloni Faculty Mentor: Prof. Edward Dreizin Bhavita Patel July.
L.B. Begrambekov Plasma Physics Department, Moscow Engineering and Physics Institute, Moscow, Russia Peculiarities, Sources and Driving Forces of.
Progress on investigation of dynamic vacuum (RF structures only) Sergio Calatroni With Cedric Garion, Chiara Pasquino, Pedro Costa Pinto, Mauro Taborelli.
How e-cloud effect affects the ILC DR Vacuum System Dr. Oleg B. Malyshev ASTeC Daresbury Laboratory.
Holger Kollmus - VBE-UHV 1 SIS100_1 ERDA Measurements ERDA – Measurements: Understanding of Ion Beam-Loss Induced Desorption.
Low SEY Engineered Surface for Electron Cloud Mitigation
Experimental breakdown studies – breakdown diagnostics Linking simulation and experiment Jan W. Kovermann, CERN, RWTH Aachen SLAC workshop July 2009.
Dark current measurement at KEK M. Gerbaux, S. Döbert, T. Higo, S. Matsumoto, K. Yokoyama.
Safety Review: RF Issues Derun Li Absorber Safety Review December 9-10, 2003 Lawrence Berkeley National Laboratory Berkeley, CA
Holger Kollmus - VBE-UHV 1 SIS100_1 ERDA Measurements ERDA – Measurements: Understanding of Ion Beam-Loss Induced Desorption.
High Gradient and High Q R&D Topics 1- Explore Q > for TESLA parameter flexibility –higher luminosity through higher rep rate, longer rf pulse… 2-
MuCool RF Status MICE Collaboration Meeting June 7-10, 2006, Fermilab A. Moretti June 9, 2006.
VASCO (VAcuum Stability COde) : multi-gas code to calculate gas density profile and vacuum stability in a UHV system Adriana Rossi General equation VASCO.
BISMV & H 0 -H - PSB INJECTION VACUUM REQUIREMENTS LIU - PSB meeting 29th October 2012 C. Pasquino, P. Chiggiato, J. Hansen.
Vacuum, Surfaces & Coatings Group Technology Department Vacuum tests for CLIC module prototypes 6 November 2013 C. Garion2 Outline: Reminder: specification.
E-CLOUD VACUUM OBSERVATIONS AND FORECAST IN THE LHC Vacuum Surfaces Coatings Group 03/07/2011 G. Bregliozzi On behalf of VSC Group with the contributions.
DC breakdown measurements Sergio Calatroni Present team: Jan Kovermann, Chiara Pasquino, Rocio Santiago Kern, Helga Timko, Mauro Taborelli, Walter Wuensch.
CLIC Breakdown Workshop – CERN, May / 13 Delay Times in Breakdown Triggering CERN, TS-MME Antoine Descoeudres, Sergio Calatroni, Mauro Taborelli.
DC breakdown experiments M.Taborelli, S.Calatroni, A.Descoeudres, Y.Levinsen, J.Kovermann, W.Wuensch CERN Ranking of materials Cathode mechanism Field.
DC breakdown measurements Sergio Calatroni Present team: Gonzalo Arnau Izquierdo, Jan Kovermann, Chiara Pasquino, Rocio Santiago Kern, Helga Timko, Mauro.
W. Wuensch, rf development meeting Considerations on running normal conducting cavities cold.
Vacuum system in the main Linacs C. Garion CERN/TE/VSC CLIC09 workshop, October.
26 January 07 Trond Ramsvik TS / MME DC Spark Test System for CLIC.
CERN DC Spark System Capabilities Anders Korsbäck, BE-RF-LRF University of Helsinki.
Metal photocathodes for NCRF electron guns Sonal Mistry Loughborough University Supervisor: Michael Cropper (Loughborough University) Industrial Supervisor:
26-28 August 2008 Final EUROTeV Scientific Workshop, Uppsala University, Sweden 1 ILC DR vacuum system related problems and solutions Oleg B. Malyshev.
13/09/2005Vacuum Systems for Synchrotron Light Sources Workshop, Barcelona, Spain 1 Gas Flow Modelling in Design of the Vacuum System for of the Synchrotron.
Accelerating structure test results and what’s next Walter Wuensch CTF3 collaboration meeting
18-20/12/2007 ILC Damping Ring R&D Mini-workshop, KEK, Japan Vacuum Design vs. e-cloud Oleg B. Malyshev ASTeC Daresbury Laboratory.
20-21 January 2009, RAL Joint DL-RAL Accelerator Workshop 1 INVESTIGATION OF NON- EVAPORABLE GETTER FILMS O. B. Malyshev, K.J. Middleman, A. Hannah and.
Fabrication of accelerator structures for CLIC study CLIC Workshop Oct , CERN T. Higo, KEK.
Antti Meriläinen 1, Ivan Kassamakov 1,2, Kenneth Österberg 1,2 and Edward Hæggström 1 1) Department of Physics, University of.
LRT2004 Sudbury, December 2004Igor G. Irastorza, CEA Saclay NOSTOS: a spherical TPC to detect low energy neutrinos Igor G. Irastorza CEA/Saclay NOSTOS.
CLIC Workshop – CERN, October / 17 DC breakdown experiments for CLIC CERN, TS-MME Antoine Descoeudres, Trond Ramsvik, Sergio Calatroni, Mauro Taborelli.
An RF & High-Speed Acquisition Systems for High-Gradient Tests at CLIC Test Facility Raquel Fandos.
Experimental part: Measurement the energy deposition profile for U ions with energies E=100 MeV/u - 1 GeV/u in iron and copper. Measurement the residual.
2009/1/16-18 ILD09 Seoul 1 Notes for ILD Beam Pipe (Technical Aspect) Y. Suetsugu, KEK Parasitic loss Vacuum pressure profile Some comments for beam pipe.
ESD SYSTEM OVERVIEW Sample Holder plate Bias Filament Cu Sample 1 2 B-A gaugeRGA Bias Sample Electrometer Butterfly valve Pumping group Conductance Gas.
Status of the Photocathode R&D for ATF RFgun N.Terunuma (KEK)
MTA RF Status 01/31/ 2007 NF&MCC Meeting UCLA A. Moretti.
Walter WuenschLCWS October 2012 Workshops on X-band and high gradients: collaboration and resource.
The CLIC accelerating structure development program Walter Wuensch CARE05 23 November 2005.
1 Vacuum chambers for LHC LSS TS Workshop 2004 Pedro Costa Pinto TS department, MME group Surface Characterization & Coatings Section.
DC Spark Test System for CLIC
Dynamic vacuum zero-order Dynamic vacuum requirement H 2 and CO 2 partial pressures < 1 nTorr (G. Rumolo and D. Schulte) BD meeting1Sergio Calatroni -
Orsay, May 5th 2011EuCARD- WP IN2P3 Les deux infinis IN2P3 Les deux infinis Orsay, May 5 th 2011 EuCARD Meeting WP10.8: Plasma Discharge Cleaning.
CLIC09 WG4 RF Structure1 Engineering Perspectives on Quadrants (2) CLIC09 Workshop KEK Y.Higashi.
Status of high gradient experiments at Nextef Kazue Yokoyama, Toshiyasu Higo, Yasuo Higashi, Shuji Matsumoto, Shigeki Fukuda Accelerator Laboratory, KEK.
THIN FILMS FOR CLIC ELEMENTS Outline Motivation The role of MME-CCS DB and MB transfer lines Main beam Main beam quadrupoles Other issues conclusions CLIC.
Some information from Nextef For poster session in IWLC T. Higo.
Estimates of residual gas pressure in the LHC Adriana Rossi AT-VAC Workshop on Experimental Conditions and Beam Induced Detector Backgrounds April.
Studies on 2.45 GHz microwave ion sources Abhishek Nag IISER, KOLKATA Presented By: G.O. Rodrigues IUAC, New Delhi Supervised By:
COPPER PHOTOCATHODES DEVELOPMENTS AT ASTEC R. Valizadeh Accelerator Science and Technology Centre Science & Technology Facility Council, UK.
13 th ESLS RF Meeting – 1 st October 2008 DAMPY Cavity 1/20 80 kW at Dampy Francis Perez.
Leak Detection method for Vacuum Systems Alexander Permogorov
Mg Films Grown by Pulsed Laser Deposition as Photocathodes: QE and surface adsorbates L. Cultrera INFN – National Laboratories of Frascati.
Progress on investigation of dynamic vacuum (RF structures only)
Electrostatic deflector development at RWTH Aachen
Breakdown experiments
Degradation and Recovery of Cavity Performance
Vacuum Problems in the ILC Damping Ring
Pulsed DC System Facilities
DOE Plasma Science Center Control of Plasma Kinetics
Participation IAP NAS of Ukraine in understanding of vacuum breakdown phenomena Iaroslava Profatilova, V.Baturin, O. Karpenko.
Effort to identify the critical issues for high gradient
Characterisation of technical surfaces at cryogenic temperature under electron bombardment. Bernard HENRIST, CERN TE/VSC 5/6/2018.
Pressure distribution calculations for the PETS
Presentation transcript:

Electron Stimulated Desorption of OFE Copper Chiara Pasquino, Politecnico di Milano 9th March 2011, RF Structure Meeting

Dynamic Vacuum: an issue for CLIC accelerating structures 9th March 2011, RF Structure Meeting  Static Vacuum: mbar [G.Rumolo, C.Garion]  Dynamic Vacuum: CO 2, H 2 < mbar 2 Technical Note, EDMS

Dynamic vacuum sources due to the High Gradient 9th March 2011, RF Structure Meeting  Breakdowns: during the discharge a gas burst is always detected;  Dark Currents: FE currents that don’t lead to a breakdown impinge on the Copper surface causing the ESD Effect. 3 FAST ION – BEAM INSTABILITIES

Dynamic Vacuum studies : Breakdowns 9th March 2011, RF Structure Meeting4  2*10 2 H 2 or CO molecules released [ exp. Data DC “spark test” reported in PRST-AB12, (2009) ];  Uniform pressure along the structure after ~ 3ms;  Background pressure recovered after 20 ms, no dynamic vacuum problems. [C.Garion]

Dynamic Vacuum studies : ESD 9th March 2011, RF Structure Meeting5 e - on faraday cup e - are uniformly distributed inside the cell e - on faraday cup S. Calatroni Faraday Cup measurement - T18_VG24_Disk_2 – KEK [T. Higo] ESD measurement on unbaked Copper [ N. Hilleret, CAS Vacuum School G. Vorlaufer CERN-Thesis (2002)]  H 2 PP = 1.12E-8 mbar 10 times higher  CO 2 PP = 3.37E-9 mbar 3 times higher NEW ESD EXPERIMENTAL DATA ON UNBAKED OFE COPPER AT HIGH ELECTRON ENERGY NEEDED!

Dynamic Vacuum studies: theoretical models 9th March 2011, RF Structure Meeting6 Gortel Fully Quantum Mechanical Model MGR Model e- Antoniewicz e-

Desorption Yield 9th March 2011, RF Structure Meeting7 Steady State Condition

Sample Campaign 9th March 2011, RF Structure Meeting8 3 Cleaning Procedures : w/o etching, passivation & SLAC etching Several Thermal Treatment : Vacuum, Argon, H or 820 °C

H 2 Diffusion Profiles :SLAC bonding 9th March 2011, RF Structure Meeting9 H2 Cu – H is an endothermic system! equal C s at both surfaces

H 2 Diffusion Profiles: SLAC bonding 9th March 2011, RF Structure Meeting10 THE ANNEALING TIME CAN BE DECREASED !!!

ESD Experimental Set-Up 9th March 2011, RF Structure Meeting11

ESD Experimental Set-Up 9th March 2011, RF Structure Meeting12 A A V V +15 V 2-3 A 35 KV

Measurement Scheme 9th March 2011, RF Structure Meeting13  ~ 20 s of desorption pulse;  precise check of the background pressure;  train of measurement continuous check of the pressure through the dual gauge read by Labview [thanks Rocio!!];  steady state condition useful experimental data.

Experimental 10 KeV: Cu spare samples 9th March 2011, RF Structure Meeting14

Experimental 10 KeV: 19_PCV082C 9th March 2011, RF Structure Meeting15 Experimental Error Analysis

Energy Correlation: Stopping Powers 9th March 2011, RF Structure Meeting16

Energy Correlation: Experimental Data 9th March 2011, RF Structure Meeting17  Increase up to 2.5 KeV, then a small decrease;  From 5 to 15 KeV, no dependence!  Something to be studied in the future!

Conclusions 9th March 2011, RF Structure Meeting18  A new experimental set – up has been built in order to provide ESD experimental data for unbaked copper at higher electron energy, as required;  The experimental set – up has been improved and it’s correctly working;  Further investigations about SLAC procedure are needed;  Further investigations on the energy correlation are required as well.

9th March 2011, RF Structure Meeting19 Many thanks to: Sergio, Mauro, Walter, Rocio, Helga, Jan, Markus, Ivo, Donat, Pawel, Luigi, Paul, Wil, Holger!!!