3 rd INSTALLATION: chicane magnetic field tests PEP-II e+ ring 1 st and 2 nd Feb 2008 Electron cloud installation studies at SLAC ILC tests - SLAC Cherrill.

Slides:



Advertisements
Similar presentations
KEK Update on the status of the electron cloud studies at KEKB Contents Brief review of our studies Updates Clearing electrode Groove structure SEY measurement.
Advertisements

Upgrade Plan of KEKB Vacuum system Pre-kickoff KEK1 Y. Suetsugu KEKB Vacuum Group Contents Challenges for vacuum system Designs for.
Study of a Clearing Electrode at KEKB - First beam test - Y. Suetsugu, H. Fukuma (KEK), M. Pivi, W. Lanfa (SLAC) 2008/3/3-61TLC08 Sendai.
R&D Plan on Clearing Electrode using the KEKB LER Y. Suetsugu and H. Fukuma, KEKB M. Pivi and L. Wang, SLAC at KEK.
KEK Recent results of beam tests on clearing electrode and grooves 2010/1/191ILC DR WebEx Meeting Y. Suetsugu, KEK.
Review of Electron Cloud R&D at KEKB 1.Diagnostics 1.Beam Size Blow-up 2.Beam Instabilities 3.Electron Density 4.SEY (Secondary Electron Yield) 2.Mitigation.
2006/09/25-28 ILCDR06, Cornell University 1 Experimental Study on Suppression of Electron Cloud Effect at the KEKB Positron Ring Contents Introduction.
9-12 April 2007 International Linear Collider DR electron cloud R&D effort 1 st part: Tests in PEP-II M. Pivi L. Wang, D. Arnett, G. Collet, R. Kirby,
Latest ILC DR wiggler simulations M. Pivi, T. Raubenheimer, L. Wang (SLAC) July, 2005.
R. Cimino COULOMB’05, Senigallia, Sept 15, Surface related properties as an essential ingredient to e-cloud simulations. The problem of input parameters:
45 th ICFA Beam Dynamic Workshop June 8–12, 2009, Cornell University, Ithaca New York Modeling Cyclotron Resonances in ECLOUD Jim Crittenden Cornell Laboratory.
Super-B Factory Workshop January 19-22, 2004 Super-B IR design M. Sullivan 1 Interaction Region Design for a Super-B Factory M. Sullivan for the Super-B.
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.
Sep 29 – Oct 3, 2009 LCWA 09 Linear Collider Workshop of the Americas Sept 29 – Oct 4, 2009 Damping Ring R&D updates SLAC Mauro Pivi SLAC Allison Fero.
DR Vacuum Component Overview April 25, 2012 Joe Conway.
Electron Clouds at SLAC Johnny Ng ILC Damping Rings Collaboration Meeting March 4, 2009.
Electron Cloud Studies for Tevatron and Main Injector Xiaolong Zhang AD/Tevatron, Fermilab.
Webex Electron Cloud Evaluations for ILC DR Mauro Pivi on behalf of the ILC Electron Cloud Working Group - by Webex - KILC12 – Daegu Korea April 25, 2012.
ILC damping ring Workshop, Dec 19, 2007, KEK, L. WANG Ecloud simulation 2007 ILC Damping Rings Mini-Workshop December, 2007 Lanfa Wang, SLAC.
SuperKEKB Vacuum System - for the positron ring - Y. Suetsugu KEKB Vacuum Group Outline Design and production status of key components Beam pipes for arc.
ILC08 Chicago November 2008 Summary of Recent Results from SLAC M. Pivi, J. Ng, D. Arnett, G. Collet, T. Markiewicz, D. Kharakh, R. Kirby, F. Cooper,
March 23, 2010 CMAD a tracking and e-cloud beam instability parallel code (M.Pivi SLAC) Taking MAD(X) optics file at input, thus tracking the beam in a.
1 CERN 1 Mar E-CLOUD Build-up in Grooved Chambers Marco Venturini Center for Beam Physics, LBNL ECL2 -- CERN, 1-2 March 2007.
Electron cloud in the wigglers of ILC Damping Rings L. Wang SLAC ILC Damping Rings R&D Workshop - ILCDR06 September 26-28, 2006 Cornell University.
ILC MDI workshop January 6-8, 2004 PEP-II IR M. Sullivan 1 Interaction Region of PEP-II M. Sullivan for the ILC MDI workshop January 6-8, 2005.
Study Plan of Clearing Electrode at KEKB Y. Suetsugu, H. Fukuma (KEK), M. Pivi, W. Lanfa (SLAC) 2007/12/191 ILC DR Mini Work Shop (KEK) Dec.
June 13, 2007 Global Design Effort 1 ILC Effort at SLAC RDR > EDR Nan Phinney SLAC/GDE.
October 13,2010 WG Meeting Cornell U. Recommendation for Electron Cloud Mitigations in the ILC Damping Ring ILC DR Working Group October 13, 2010 Cornell.
2008/7/281 ILCDR08 Report - Electron Cloud Session – Univ. Y. Suetsugu, KEK.
Compare options: simulations recent history Cloud density near (r=1mm) beam (m -3 ) before bunch passage, values are taken at a cloud equilibrium density.
Compare options: simulations recent history Cloud density near (r=1mm) beam (m -3 ) before bunch passage, values are taken at a cloud equilibrium density.
ILC DR Workshop - KEK December, A new resonance in wiggler simulations: Christine Celata Use POSINST code.
Electron Cloud Growth & Mitigation: In-Situ SEY Measurements Retarding Field Analyzer Studies W. Hartung, J. Calvey, C. Dennett, J. Makita, V. Omanovic.
Nov 17, 2009 Webex Assessing the 3.2 km Ring feasibility: Simulation parameters for electron cloud Build-up and Instability estimation LC DR Electron Cloud.
Recent Electron-Cloud Mitigation Studies at KEK E-cloud mitigation mini-workshop on November at CERN Kyo Shibata (for KEKB Group)
SKEKB Mini Work SKEKB Vacuum System – Arc Section – Contents Y.Suetsugu KEKB Vacuum Group 1.Beam Chambers 2.Pumps: Pump, Pressure,
CesrTA Vacuum System Conversion and Operational Experiences Yulin Li for the CesrTA Team Cornell Laboratory for Accelerator-based ScienceS and Education.
Prepared by M. Jimenez AT Dept / Vacuum Group, ECloud’04 Future Needs and Future Directions Maximizing the LHC Performances J.M. Jimenez …when Nature persists.
Electron cloud in Final Doublet IRENG07) ILC Interaction Region Engineering Design Workshop (IRENG07) September 17-21, 2007, SLAC Lanfa Wang.
FCC-hh: First simulations of electron cloud build-up L. Mether, G. Iadarola, G. Rumolo FCC Design meeting.
SPS coating studies 28 February, 2016TE-VSC1 Present situation of the development of e-cloud mitigation methods -MD 2011 results -Carbon coating of dipoles.
ILC GDE - ILCDR08 Cornell 8-11 July 2008 Electron Cloud Mitigation R&D at SLAC M. Pivi, D. Arnett, G. Collet, T. Markiewicz, D. Kharakh, R. Kirby, J. Seeman,
AEC09, CERN Mauro Pivi, SLAC TiN chambers and SEY measurements in PEP-II M. Pivi J. Ng, T. Markiewicz, D. Kharakh, R. Kirby, F. Cooper, C. Spencer, B.
Electron cloud measurement in Cu/Al chambers with/without TiN coating at KEKB positron ring ILC DR Working Group Meeting Kyo Shibata (KEK)
Electron Cloud R&D at SLAC Johnny Ng SLAC DOE HEP Review July 7 – 9, 2008.
E-cloud Remedies and PS2 vacuum design J.M. Jimenez AT Department – Vacuum Group CARE-HHH-APD BEAM’07 Thursday 04 October Session 2: PS2 E-cloud.
2nd International Particle Accelerator Conference September 4–9, 2011, San Sebastián, Spain LEPP, the Cornell University Laboratory for Elementary-Particle.
U. Iriso CELLS, Barcelona, Spain Electron Cloud Mitigation Workshop 2008 Nov st, 2008 Electron Cloud Simulations for ANKA in collaboration with.
R&D GOALS AND MILESTONES TOWARDS A TECHNICAL DESIGN REPORT TDR (2008) First Intnl. Teleconference Ecloud, Impedance/Instabilities - M. Pivi, SLAC 31 October.
Possible solutions for the e- cloud problem – SPS upgrade meeting - Frank Zimmermann, 21 March possible solutions for the electron-cloud problem  suppress.
Updates of EC Studies at KEKB 1.EC studies at KEKB 2.Recent results 1.Clearing Electrode 2.Groove surface 3.TiN coating 4.Measurement of EC in solenoid.
Recent ECLOUD07 Workshop in Daegu, S. Korea (~50 participants) –Highlights: Measurements of the surface Secondary Electron Yield (SEY) of samples inserted.
ECLOUD’12 (the 5 th electron-cloud workshop) Kyo Shibata (on behalf of KEKB Vacuum Group) SuperKEKB Vacuum System KEK Tsukuba site SuperKEKB Linac.
Electron Cloud Studies at DAFNE Theo Demma INFN-LNF Frascati.
Electron Cloud in the International Linear Collider ILC Mauro Pivi work performed while at SLAC and the ILC Damping Ring Working Group High.
Benchmarking simulations and observations at the LHC Octavio Domínguez Acknowledgments: G. Arduini, G. Bregliozzi, E. Métral, G. Rumolo, D. Schulte and.
2007/03/1-2 ECL2, CERN 1 SEY and Clearing Studies at KEKB Contents Contents Introduction Studies Beam duct with Ante-chambers Coatings with Low SEY Clearing.
Recent Studies on Electron Cloud at KEKB 1.EC studies at KEKB 2.Recent results –Clearing Electrode –Groove surface –EC measurement in Q and solenoid field.
PEP-II test chambers installation
CERN Grooved Chamber Review
International Linear Collider R&D on electron cloud (SLAC)
Groove Mitigation and Plans
Electron Cloud Effects in SuperB
Electron Cloud R&D for Future Linear Colliders
Impedance & SEY of grooved Surface Ecloud in Quadpole
RECENT DEVELOPMENTS IN MODELING
Work In January 2007, we installed 5 chambers in a straight Field Free region of PEP-II Low Energy Ring (LER). Closest bend at ~18 meters upstream: 1 stainless.
Impedance of grooved surface
Electron Clouds at SLAC
R&D GOALS AND MILESTONES TOWARDS A TECHNICAL DESIGN REPORT TDR (2008)
Presentation transcript:

3 rd INSTALLATION: chicane magnetic field tests PEP-II e+ ring 1 st and 2 nd Feb 2008 Electron cloud installation studies at SLAC ILC tests - SLAC Cherrill Spencer

ILC DR Workshop - KEK “Ecloud1” SEY test station in PEP-II SLAC Transfer system at 0 o PEP-II LER e+  Transfer system at 45 o 2 samples facing beam pipe are irradiated by SR Isolation valves ILC tests, M. Pivi et al. – SLAC

ILC DR Workshop - KEK Results of TiN conditioning in PEP-II e+ beam line SEY of Tin-samples measured before and after 2-months conditioning in the beam line. 2 samples inserted respectively in the synchrotron radiation fan plane (0 o position) and out of this plane (45 o ). ILC tests, M. Pivi et al. – SLAC Before installation in beam line After beam conditioning e- dose > 40mC/mm**2 Similar low SEY recently measured in situ in KEKB beam line S. Kato, Y. Suetsugu et al.

LER#1 XPS Before installationXPS After exposure in PEP-II LER for 2 months (e dose 40mC/mm^2) Carbon content is strongly reduced after exposition to PEP-II LER  synchrotron radiation + electron + ion conditioning. This is a different result if compared to electron (only) conditioning in laboratory set-up where carbon crystals growth has been observed by many laboratories. Surface analysis: Carbon content decrease TiN samples: X-ray Photon Spectroscopy. ILC tests, M. Pivi et al. – SLAC

Results of NEG conditioning in PEP-II e+ beam line ILC tests – SLAC NEG as received After beam conditioning March 2008 After NEG heating

KEK, Feb 2008

Clearing electrodes in KEKB magnetic free region Y. Suetsugu, KEK

11 March, 2008 SPS meeting. Mauro Pivi SLAC Gianluigi Arduini, Elena Chapochnikova, Paolo Chiggiato, Miguel Jimenez, Mauro Taborelli (CERN) Mauro Pivi, Lanfa Wang, Frank Cooper, Munro Morrison (SLAC) Marco Venturini, Miguel Furman (LBNL) SPS Groove Chamber Tests Collaborators

Secondary electron yield (SEY) estimate: SPS Groove Height=2mmHeight=1mm In this simulation the groove height is taken to be the effective total height from top to valley Lanfa Wang, SLAC

Simulation of electron cloud build up Groove height =1mm In the following simulations hg=1mm is the fixed height of the groove triangle (roundness reduces effective height). SEY= bunches per batch. Chamber cross section: 152x45 mm Other relevant parameters: E=450 GeV, B =2 T Grooves either on one or both sides of chamber

Marco Venturini, LBNL electron cloud build-up as a function of time for 1mm deep grooves with angle alpha =80 deg, for various choices of the groove tip radius. Groove on bottom and top sides. In these simulations hg=1mm is the height of the groove triangle. Simulation of electron cloud build up

Max. e-cloud linear density vs. groove tip radius (SEY=1.3) For flat surfaces the max. linear density is ~ 1.5 nC/m). In the SPS tests, grooves on top and bottom side. In these simulations hg=1mm is the height of the groove triangle. Marco Venturini, LBNL Simulation of electron cloud build up

Roundness of tips and valley is important Manufacture Tolerances on roundness are rather tight for 1mm grooves Few more work on simulations: –In the SPS, would it be more realistic to assume initial SEY=1.5 (?!), since no photon scrubbing. –Define tolerance roundness to obtain SEY<1 –For small 1mm groove important to consider the effective groove height (after roundness)

munro16 TRIANGULAR GROOVE CHAMBER MFG January, 2008

Requirements Triangular Grooves Groove Width 0.35 mm Groove Depth 1 mm Overall Depth 2 mm Groove Length 0.5 M Taper Angle 20 degrees Radius at Top & Bottom 0

Basic Problems Very small grooves are difficult to fab Sharp radii at base & top of grooves unattainable by normal mfg methods Mfg options are to either have grooves as part of vac chamber, or fab grooves as separate item & then attach to vac chamber.

Mfg Options Extrusion: Very small radii at top & bottom of grooves are difficult to mfg Machining: Mill multiple slots in solid material Metal Folding: Form multiple folds EDM: Small radii are beyond normal tolerances Brazed-up Assembly: Use individual razor type foil blades Isostatic Pressing or Metal Injection Molding: Uses powdered metal & binders which would probably would not be suitable for vacuum usage. Also have difficulty in forming small radii

Groove Options Manufactured Series of aluminum extrusions fabricated Grooves all around chamber (2 different groove profiles) Grooves at top & bottom of chamber Separate linear extrusion for insertion into existing stainless vacuum chamber

Cost Considerations Assuming long sections required, the extrusion approach is by far the least expensive. Limited to aluminum material Copper may be possible, but could not find vender

Aluminum triangular grooves by ALMAG. Original design for the SPS: 2mm depth, limited by the groove sharpness. SLAC 2008

Aluminum triangular groove: depth 1.9mm, angle 20deg, radius top 0.095mm, radius valley 0.140mm

With final geometry The real geometry: radius of tip=0.095mm radius of valley =0.14mm Lanfa Wang, SLAC

Manufacturing Options depth 1mm: Metal Folding Metal Folding: Form multiple folds. [EMEGA Company, USA]

Manufacturing Options depth 1mm: Razor Blades

Brazed-up Assembly: Use individual razor type foil blades Manufacturing Options depth 1mm: Razor Blades