CERN, LIU-SPS ZS Review, 20/02/2013 1 Brief review on electron cloud simulations for the SPS electrostatic septum (ZS) G. Rumolo and G. Iadarola in LIU-SPS.

Slides:



Advertisements
Similar presentations
PyECLOUD G. Iadarola, G. Rumolo Thanks to: F. Zimmermann, G. Arduini, H. Bartosik, C. Bhat, O. Dominguez, M. Driss Mensi, E. Metral, M. Taborelli.
Advertisements

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.
Heat load due to e-cloud in the HL-LHC triplets G. Iadarola, G. Rumolo 19th HiLumi WP2 Task Leader Meeting - 18 October 2013 Many thanks to: H.Bartosik,
BUILD-UP SIMULATIONS FOR DAFNE WIGGLER W/ ELECTRODES Theo Demma.
Summary of the two-stream instability session G. Rumolo, R. Cimino Based on input from the presentations of G. Iadarola, H. Bartosik, R. Nagaoka, N. Wang,
Electron-cloud instability in the CLIC damping ring for positrons H. Bartosik, G. Iadarola, Y. Papaphilippou, G. Rumolo TWIICE workshop, TWIICE.
Fusion Physics - Energy Boon or Nuclear Gloom? David Schilter and Shivani Sharma.
Review of 2011 studies and priorities for 2012 LIU-SPS-BD.
LHC e - cloud simulations C.Octavio Domínguez, Giovanni Rumolo, Frank Zimmermann 17 th January e - cloud simulations.
Preliminary results and ideas for the SPS upgrade MDs on LHC beams in 2011 G. Rumolo on behalf of all the MD team (Elena, Thomas, Karel, Christina, Holger,
Vacuum, Surfaces & Coatings Group Technology Department 04/12/2014 R. Salemme – COLDEX results during SPS Scrubbing Run I Electron Cloud Meeting #18,
SPS scrubbing run in 2014 H. Bartosik, G. Iadarola, G. Rumolo LHC Performance Workshop (Chamonix 2014), 22/9/2014 Many thanks to: G. Arduini, T. Argyropoulos,
BE-ABP-HSC Electron cloud simulations in the LHC MKI Electron Cloud meeting A. Romano, G. Iadarola, G. Rumolo Many thanks to: M. Barnes, M. Taborelli.
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.
Giovanni Rumolo, G. Iadarola and O. Dominguez in LHC Beam Operation workshop - Evian 2011, 13 December 2011 For all LHC data shown (or referred to) in.
Simulations on the EC detector in MU98 A. Romano, G. Iadarola, G. Rumolo LIU-PS Meeting 28 April 2015 Many thanks to: M. Taborelli, C. Yin Vallgren.
March 2, 2007ELC Experience with clearing voltages and solenoids at SPS damper pick-ups W. Hofle Acknowledgements PS-OP, SL-OP, SL-BI LHC-VAC, SL-HRF.
AB-ABP/LHC Injector Synchrotrons Section CERN, Giovanni Rumolo 1 Final results of the E-Cloud Instability MDs at the SPS (26 and 55 GeV/c) G.
SPS scrubbing experience: electron cloud observables L. Mether on behalf of the LIU-SPS e-cloud team LIU SPS scrubbing review, September 8, 2015.
LHC Scrubbing Runs Overview H. Bartosik, G. Iadarola, K. Li, L. Mether, A. Romano, G. Rumolo, M. Schenk, G. Arduini ABP information meeting 03/09/2015.
First measurements of longitudinal impedance and single-bunch effects in LHC E. Shaposhnikova for BE/RF Thanks: P. Baudrenghien, A. Butterworth, T. Bohl,
LHC beams in the SPS in 2014 H. Bartosik, G. Rumolo, G. Iadarola With the help from K. Kornelis, V. Kain and SPS OP crew.
PS (electron cloud?!) instability at flat top Mauro Pivi Gianni Iadarola, Giovanni Rumolo, Simone Gilardoni, Hannes Bartosik, Sandra Aumon 27/06/2012 ICE.
Design and operation of existing ZS B.Balhan, J.Borburgh, B.Pinget B.BalhanDesign and operation of existing ZS SPS ZS Electrostatic Septum Upgrade Review.
G. Rumolo, G. Iadarola, H. Bartosik, G. Arduini for CMAC#6, 16 August 2012 Many thanks to: V. Baglin, G. Bregliozzi, S. Claudet, O. Dominguez, J. Esteban-
C. Fischer – LHC Instrumentation Review – 19-20/11/2001 Gas Monitors for Transverse Distribution Studies in the LHC LHC Instrumentation Review Workshop.
1 CERN 1 Mar E-CLOUD Build-up in Grooved Chambers Marco Venturini Center for Beam Physics, LBNL ECL2 -- CERN, 1-2 March 2007.
4. Summary and outlook 4. Summary and outlook Electron cloud evolution can be modeled using polynomial maps whose coefficients are functions of beam and.
Production of bunch doublets for scrubbing of the LHC J. Esteban Muller (simulations), E. Shaposhnikova 3 December 2013 LBOC Thanks to H. Bartosik, T.
Physics of electron cloud build up Principle of the multi-bunch multipacting. No need to be on resonance, wide ranges of parameters allow for the electron.
LIU-SPS ZS Electrostatic Septum Upgrade Review held on M.J. Barnes & T. Kramer.
Discussion and preliminary conclusions LIU-SPS ZS Electrostatic Septum Upgrade Review M.J. Barnes.
Improved electron cloud build-up simulations with PyECLOUD G. Iadarola (1),(2), G. Rumolo (1) (1) CERN, Geneva, Switzerland, (2) Università di Napoli “Federico.
Some ideas for/from the SPS LIU-SPS team. Scrubbing (only) for ecloud in SPS? aC coating remains baseline..... –but scrubbing has many potential advantages.
Progress on electron cloud studies for HL-LHC A. Axford, G. Iadarola, A. Romano, G. Rumolo Acknowledgments: R. de Maria, R. Tomás HL-LHC WP2 Task Leader.
Simulation of multipacting thresholds G. Iadarola and A. Romano on behalf of the LIU-SPS e-cloud team LIU SPS scrubbing review, 8 September, 2015.
Electron cloud in the LHC: lessons learnt from 2015 experience with 25 ns beams G. Iadarola, H. Bartosik, K. Li, L. Mether, A.Romano, G. Rumolo, M. Schenk.
Heat load analysis for Inner Triplet and Stand Alone Modules H. Bartosik, J. Hulsmann, G. Iadarola and G. Rumolo LBOC meeting 28 October 2014 Based on.
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.
BE-ABP-HSC Non convex chamber in PyECLOUD Electron Cloud meeting G. Iadarola, A. Romano, G. Rumolo.
Elias Métral, LHC Beam Commissioning Working Group meeting, 30/11/2010 /241 PRELIMINARY FINDINGS FROM INSTABILITY MEASUREMENTS DURING THE 75ns AND 50ns.
Technology Department. ZS Ion Trap Development G. Raffaele and R.A. Barlow Acknowledgements: B. Balhan, M.J. Barnes and B. Pinget 21/04/2015 TCM: ZS Ion.
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.
Prepared by M. Jimenez AT Dept / Vacuum Group, ECloud’04 ELECTRON CLOUDS AND VACUUM EFFECTS IN THE SPS Experimental Program for 2004 J.M. Jimenez Thanks.
End-of-year talk LIU-SPS BD WG meeting Our meetings in 2015 O During year - 9 meetings of LIU-SPS BD WG (as in 2013, but 10 in 2014 and 12 in.
Comparison of stainless steel and enamel clearing electrodes E. Mahner, F. Caspers, T. Kroyer Acknowledgements to G. Arduini, H. Damerau, S. Hancock, B.
Simulation of the new PS EC detector: implementation and results A. Romano, G. Iadarola, G. Rumolo LIU-PS Student Day 20 April 2015.
Vacuum specifications in Linacs J-B. Jeanneret, G. Rumolo, D. Schulte in CLIC Workshop 09, 15 October 2009 Fast Ion Instability in Linacs and the simulation.
RF measurements during floating MD in Week 40 3 rd of October 2012 LIU-SPS BD WG 25/10/2012 Participants: T. Argyropoulos, H. Bartosik, T. Bohl, J. Esteban.
Progress on e-cloud effects (PS and SPS) G. Iadarola, H.Bartosik, G. Rumolo, M. Taborelli, C. Yin Vallgren Many thanks to: G. Arduini, T. Argyropoulos,
Fast Ion Instability Study G. Rumolo and D. Schulte CLIC Workshop 2007, General introduction to the physics of the fast ion instability Fastion.
MTE commissioning status S. Gilardoni, BE/ABP With C. Hernalsteens and M. Giovannozzi.
Electron cloud measurements in Cesr-TA during the July-August run for the SPSU Study Team, report by S. Calatroni and G. Rumolo thanks to J.
Benchmarking Headtail with e-cloud observations with LHC 25ns beam H. Bartosik, W. Höfle, G. Iadarola, Y. Papaphilippou, G. Rumolo.
Benchmarking simulations and observations at the LHC Octavio Domínguez Acknowledgments: G. Arduini, G. Bregliozzi, E. Métral, G. Rumolo, D. Schulte and.
Update on RF parameters A.Lachaize11 th HPPS design meeting04/09/13.
HP-PS beam acceleration and machine circumference A.LachaizeLAGUNA-LBNO General meeting Paris 18/09/13 On behalf of HP-PS design team.
AB-ABP/LHC Injector Synchrotrons Section CERN, Giovanni Rumolo 1 Preliminary results of the E-Cloud Instability MDs at the SPS G. Rumolo, in.
Two-beam instabilities in low emittance rings Lotta Mether, G.Rumolo, G.Iadarola, H.Bartosik Low Emittance Rings Workshop INFN-LNF, Frascati September.
Two beam instabilities in low emittance rings Lotta Mether, G.Rumolo, G.Iadarola, H.Bartosik Low Emittance Rings Workshop INFN-LNF, Frascati September.
SPSU M.Taborelli Results from MD week 45 Views of extracted liners and RF shields M. Taborelli for SPSU team.
Sparking of SPS electrostatic septa in presence of e-cloud
Machine Coordinators: G. Arduini, J. Wenninger
Possible causes for SPS ZS2 misalignment
Proposals of new electron cloud monitor in the PS
Scrubbing progress - 10/12/2012
ELENA Extra Low ENergy Antiproton Ring
Beam dynamics requirements after LS2
Scrubbing progress - 08/12/2012
Presentation transcript:

CERN, LIU-SPS ZS Review, 20/02/ Brief review on electron cloud simulations for the SPS electrostatic septum (ZS) G. Rumolo and G. Iadarola in LIU-SPS ZS Review, 20/02/2013 ZS with LHC-type beams Study of electron cloud build up thresholds in a ZS-like geometry with LHC25 beams: –Without external fields –With the voltage from the ion traps Some conclusions New simulations run with PyECLOUD with the correct model/geometry

Some practical information on the ZS 20mm V=-220kV -6kV -3kV Anode Cathode Ion-traps 2 From J. Wenninger, Introduction to Slow Extraction to the North Targets 2000 W.75 Re.25 septum wires. Wire diameter 50  m (first ZS) to 100  m. Wire spacing 1.5 mm.

Instructions when high intensity LHC beams are in the SPS:  Retracted girder (not anymore after 2010 to allow || MDs & conditioning)  HV 0 kV (not anymore after 2010, kV applied, reduces outgassing)  Ion traps on Observations at the ZS with 25 ns high intensity beam (see also talks from Bruno and Karel):  Above certain intensities (nominal beam, more than 1 batch injected) vacuum spike in the ZS observed  The increased vacuum levels can provoke a vacuum interlock, which stops the ion traps and hence the beam in the machine. In this sense, “ZS limits the LHC beam”  By increasing the bunch length the vacuum does not degrade.  Sparking occasionally occurs (ramp, ejection) Ion trap voltage drop and current measured off the plates Does not appear to be the principal problem, rate decreasing ⇒ Some hints that e-cloud could build up in the ZS, even if the presence of a voltage should clear electrons…. ZS during SPS operation with high intensity LHC beams 3

In absence of voltage from the ion traps  significant electron cloud builds up for  max > 1.5  the electron cloud between bunches is uniformly distributed over the chamber cross section Electron cloud simulations the ZS geometry without external fields 4 ec = e - /m 46 mm 140 mm

Assuming a voltage of 3 kV between the bottom and top plates  the electron cloud is suppressed at least up to  max =2.0 (different build up curves are all below the one for  max =2.0) Electron cloud simulations including the voltage from the ion traps 5 E ec = 10 3 e - /m 46 mm 140 mm

Assuming a voltage of 3 kV between the bottom and top plates  the electron cloud is suppressed at least up to  max =2.0 (different build up curves are all below the one for  max =2.0)  the electrons are fully cleared between subsequent bunches and there is no visible dependence on the SEY of the plate. Electron cloud simulations including the voltage from the ion traps 6 E 46 mm 140 mm Zoom of previous plot in the first 0.3  s

For V=100 V the SEY threshold lies also around 1.5 Assuming  max =1.7 and scanning the voltage between the bottom and top plate  the electron cloud is found to be fully suppressed for 500 V ≤ V < 4 kV  V=100 V is not sufficient and a strong electron cloud is formed (with a faster rise time than V=0 but a faster decay, too, due to the clearing voltage) Electron cloud simulations scanning the voltage values 7 V = 100 V

Changing the voltage, we actually change the clearing efficiency  electrons are cleared more efficiently (i.e. more quickly) with higher voltages  However, if the voltage becomes too low (<500 V), the intra-bunch clearing is insufficient and multipacting cannot be avoided  the quoted clearing voltage values also depend on having assumed in the model a maximum SEY at E max =230 eV and R 0 =0.7 Electron cloud simulations scanning the voltage values 8  max =1.7, zoom on the first 50 ns

Electron cloud simulations electron dynamics and distribution 9 No voltage applied

Electron cloud simulations electron dynamics and distribution 10 V = 3 kV

All the simulations have been re-run with the PyECLOUD, which allows for the use of the correct chamber shape (both correct geometric and electromagnetic boundary conditions) The geometry of the ZS is confirmed to be prone to electron cloud build up with LHC25 beams at nominal intensity → in absence of the voltage from the ion traps, there is electron cloud build up for maximum SEY above 1.5 A difference of potential between top and bottom plate is certainly effective to clear the electrons from residual gas ionization between bunches  voltage should be at least a few hundreds V (100V certainly not enough) Summary and conclusions 11