Electron Cloud in ilcDR: Update

Slides:



Advertisements
Similar presentations
BUILD-UP SIMULATIONS FOR DAFNE WIGGLER W/ ELECTRODES Theo Demma.
Advertisements

Electron-cloud instability in the CLIC damping ring for positrons H. Bartosik, G. Iadarola, Y. Papaphilippou, G. Rumolo TWIICE workshop, TWIICE.
Latest ILC DR wiggler simulations M. Pivi, T. Raubenheimer, L. Wang (SLAC) July, 2005.
Using Tune Shifts to Evaluate Electron Cloud Effects on Beam Dynamics at CesrTA Jennifer Chu Mentors: Dr. David Kreinick and Dr. Gerry Dugan 8/11/2011REU.
E-Cloud Effects in the Proposed CERN PS2 Synchrotron M. Venturini, M. Furman, and J-L Vay (LBNL) ECLOUD10 Workshshop, Oct Cornell University Work.
ECLOUD Calculations of Field Gradients During Bunch Passage Jim Crittenden Cornell Laboratory for Accelerator-Based Sciences and Education Electron Cloud.
LEPP, the Cornell University Laboratory for Elementary-Particle Physics, has joined with CHESS to become the Cornell Laboratory for Accelerator-based Sciences.
Electron Cloud Modeling for CesrTA Daniel Carmody Mentors: Levi Schächter, David Rubin August 8th, 2007.
R. Cimino COULOMB’05, Senigallia, Sept 15, Surface related properties as an essential ingredient to e-cloud simulations. The problem of input parameters:
ECLOUD Calculations of Coherent Tune Shifts for the April 2007 Measurements - Study of SEY Model Effects - Jim Crittenden Cornell Laboratory for Accelerator-Based.
LEPP, the Cornell University Laboratory for Elementary-Particle Physics, has joined with CHESS to become the Cornell Laboratory for Accelerator-based Sciences.
Electron Cloud in ilcDR: Update T. Demma, INFN-LNF.
ECLOUD Calculations of Coherent Tune Shifts for the April 2007 Measurements - This presentation limited to resolving drift/dipole weighting question -
45 th ICFA Beam Dynamic Workshop June 8–12, 2009, Cornell University, Ithaca New York Jim Crittenden Cornell Laboratory for Accelerator-Based Sciences.
45 th ICFA Beam Dynamic Workshop June 8–12, 2009, Cornell University, Ithaca New York Recent Studies with ECLOUD Jim Crittenden Cornell Laboratory for.
ECLOUD Calculations of Coherent Tune Shifts for the April 2007 Measurements - Thanks to Marco for clarifying the drift/dipole weighting - - Thanks to Gerry.
ECLOUD Simulations for CESR Witness Bunch Tune Shift Measurements Jim Crittenden Cornell Laboratory for Accelerator-Based Sciences and Education.
E-cloud studies at LNF T. Demma INFN-LNF. Plan of talk Introduction ECLOUD Simulations for the DAFNE wiggler ECLOUD Simulations for build up in presence.
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.
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.
NEW COMMENTS TO ILC BEAM ENERGY MEASUREMENTS BASED ON SYNCHROTRON RADIATION FROM MAGNETIC SPECTROMETER E.Syresin, B. Zalikhanov-DLNP, JINR R. Makarov-MSU.
Electron cloud simulations for SuperKEKB Y.Susaki,KEK-ACCL 9 Feb, 2010 KEK seminar.
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.
E-cloud studies at LNF T. Demma INFN-LNF. Plan of talk Introduction New feedback system to suppress horizontal coupled-bunch instability. Preliminary.
Cesr-TA Simulations: Overview and Status G. Dugan, Cornell University LCWS-08.
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.
Electron cloud measurements and simulations at CesrTA G. Dugan, Cornell University 4/19/09 TILC09 4/18/09.
Recent Electron-Cloud Mitigation Studies at KEK E-cloud mitigation mini-workshop on November at CERN Kyo Shibata (for KEKB Group)
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.
Electron Cloud Studies Theo Demma INFN-LNF Frascati.
U. Iriso CELLS, Barcelona, Spain Electron Cloud Mitigation Workshop 2008 Nov st, 2008 Electron Cloud Simulations for ANKA in collaboration with.
3 February 2010 ILC Damping Ring electron cloud WG effort Mauro Pivi SLAC on behalf of ILC DR working group on e- cloud ILC DR Webex Meeting Jan 3, 2010.
Electron Cloud Studies at DAFNE Theo Demma INFN-LNF Frascati.
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.
Electron Cloud in the International Linear Collider ILC Mauro Pivi work performed while at SLAC and the ILC Damping Ring Working Group High.
LEPP, the Cornell University Laboratory for Elementary-Particle Physics, has joined with CHESS to become the Cornell Laboratory for Accelerator-based Sciences.
Synrad3D Photon propagation and scattering simulation G. Dugan, D. Sagan CLASSE Cornell University Ithaca, NY USA.
Status of ECLOUD Simulations for the Shielded Button Measurements
Electron Cloud & IBS Update
Electron Cloud, IBS, and Fast Ion Update
Update to ECLOUD Calculations for the
Electron Cloud Effects in SuperB
Electron Cloud R&D at Cornell ILCDR08--7/8/08
Observations and Predictions for DAFNE and SuperB
R. Cimino LNF-INFN Frascati (Roma) Italy.
Measurement of Electron Cloud in KEKB LER with RFA
RECENT DEVELOPMENTS IN MODELING
Electron cloud and collective effects in the FCC-ee Interaction Region
Physics Scope and Work Plan for the Shielded-Pickup Measurements -- Synchrotron Radiation Photon Distributions Photoelectron Production Parameters.
First Look at the New SYNRAD3D Results
RECENT DEVELOPMENTS IN MODELING
Physics Scope and Work Plan for the Shielded-Pickup Measurements -- Synchrotron Radiation Photon Distributions Photoelectron Production Parameters.
Ecloud in quadrupole & Sextupole
J.A.Crittenden, Y.Li, X.Liu, M.A.Palmer, J.P.Sikora (Cornell)
CESRTA Measurement of Electron Cloud Density by TE Wave and RFA
Electron Cloud in ilcDR: Update
SuperB General Meeting June , Perugia (Italy)
ILC DR instability simulations
Status of Ecloud Build-Up Simulations for the ILC DR’s
ILC DR instability simulations
ILC DR Working Group on Collective Effect: Electron Cloud
ILC Damping Ring electron cloud WG effort
Electron Cloud Build-up in ilcDR
Electron Cloud Update US LHC Accelerator Research Program
CINVESTAV – Campus Mérida Electron Cloud Effects in the LHC
A Mapping Approach to the Electron Cloud for LHC
ILC DR instability simulations
Presentation transcript:

Electron Cloud in ilcDR: Update T. Demma, INFN-LNF

Electron cloud buildup simulation Cloud buildup was calculated by code “ECLOUD” developed at CERN. Assumptions: - Round Chambers - A fraction R of the primary electrons are uniformly produced on chamber wall. - A reduced number of primary electrons is artificially used in order to take into account the reduction of electron yield by the ante-chamber: where: dn/ds is the average number of emitted photons per meter per e+, Y is the quantum efficiency, and  is the percentage of photons absorbed by the antechambers.

Estimation of antechamber protection in ILC-DR In order to calculate the number of photons that remain inside the chamber, we must integrate the fundamental spectrum of synchrotron radiation The calculation is done by numerical integration taking into account the geometry of the chamber and the curvature of the orbit (extrapolated from mad lattice files: https://wiki.lepp.cornell.edu/ilc/bin/view/Public/DampingRings/WebHome). Very preliminary estimate for ILC-DR DCO4 lattice indicate that only ~2% of the radiated photons remain inside the chamber (to be double checked)

Build Up Input Parameters for ECLOUD ilc-DR 6.4 Km, 6 ns bunch spacing*. Bunch population Nb 2.1x1010 Number of bunches 45 x 8 trains Bunch gap Ngap 15 Bunch spacing Lsep[m] 1.8 Bunch length σz [mm] 6 Bunch horizontal size σx [mm] 0.26 Bunch vertical size σy [mm] 0.006 Photoelectron Yield Y 0.1 Photon rate (e-/e+/m) dn /ds 0. 204 Antechamber protection  90%; 97% 99% Fraction of uniformely dist photelectrons R 15% 20% 25% Max. Secondary Emission Yeld δmax 0.9 1.2 1.4 Energy at Max. SEY Εm [eV] 300 SEY model Cimino-Collins ((0)=0.5) *https://wiki.lepp.cornell.edu/ilc/pub/Public/DampingRings/WebHome/DampingRingsFillPatterns.xls

Average e-cloud density in ILC-DR dipole (SEY=0.9;1.2;1.4) =90% R=25% =97% R=25% =99% R=15% =90% R=15% =97% R=15% =99%

e-cloud “distribution” SEY=0.9 SEY=1.2 SEY=1.4 Snapshot of the cloud distribution “just before” the passage of the last bunch for: R=25%, =90%

Average e-cloud density SEY=1.2 =90%; =97%; =99% R=25% =90%; =97%; =99%

Average e-cloud density SEY=1.2, R=20% =90%; =97%; =99%

Average vs central density SEY=1.2, R=20%,=90% t[sec] Red dots mark e-cloud density near the beam (+ -10 sig.) evaluated “just before” the passage of each bunch.

Comparison with bruns Average Central Dopo il passaggio di 150 bunches consecutivi con pey=10-4, sey=1.1, R=99.9%, bunch spacing=0.94 m. Lui si trova una densità di 2*1011, ci siamo vicini soprattuto con la central. Comunque aspetto che finisca la simulazione mi mancano ancora 150 bunches. Le gap nel treno sono importanti!!!!