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Parameters for electron cloud build-up and
instability simulations 2012
ILC DR Electron Cloud Working Group
Feb 29, 2012
February 15, 2012 ILC DR Working Group
Link to 3.2 km DR files
ILC Damping Ring wiki website:
5Hz lattice (baseline) files:
• https://wiki.lepp.cornell.edu/ilc/bin/view/Public/Dampi
ngRings/#TDP_II_Baseline_Lattice_Vers_AN1
10Hz lattice files:
• https://wiki.lepp.cornell.edu/ilc/bin/view/Public/Dampi
ngRings/#TDP_II_Baseline_Lattice_Version
Lattice design by David Rubin, Cornell U.
February 15, 2012 ILC DR Working Group
David Rubin, Cornell U.
February 15, 2012 ILC DR Working Group
wiggler arc arc injection /
extraction
February 15, 2012 ILC DR Working Group
February 15, 2012 ILC DR Working Group
Magnets
Wigglers strength 1.5T at 5 Hz and 2.16T at 10Hz
max
February 15, 2012 ILC DR Working Group
Build-Up Simulations 3.2 km DR
Section Vacuum
chamber radius
(from RDR)
Antechamber
full height
Beam sizes
sx,sy
(mm)
Surface +
mitigation
peak SEY
Arc Dipole 25 mm 10 mm 215, 6.9 TiN + Grooves 1
Arc Quadrupole 25 mm 10 mm 290, 6 TiN 1
Arc Sextupole 25 mm 10 mm 290, 6 TiN 1
Arc Drift 25 mm 10 mm 290, 6 TiN + solenoid 1
Quadrupole in straigth 25 mm none 110, 6.4 TiN 1.2
Drift in straigth 25 mm none 110, 6.4 TiN + solenoid 1.2
Wigglers 23 mm 20 mm 80, 5.5 Cu + clearing
electrodes
1.22
Quadrupole in wiggler
region
23 mm 20 mm 80, 5.5 TiN 1
Drift in wiggler region 23 mm 20 mm 80, 5.5 TiN + solenoid 1
Electron cloud build-up simulation parameters:
arc
s
str
aig
hts
w
igg
ler
February 15, 2012 ILC DR Working Group
Cloud Density
From build-up simulation, we need to extract the
value of the cloud density:
1. After build-up and several bunch passes, when
cloud density reaches an equilibrium value
2. Cloud density JUST BEFORE electron cloud
pinching (at the head of the bunch)
3. Cloud density “near the beam” (20 sx, 20 sy)
February 15, 2012 ILC DR Working Group
Fill pattern
February 15, 2012 ILC DR Working Group
Secondary emission yield for TiN and Copper
surfaces to assume in simulations
• Our mitigation recommendation plan for most of the
ring to be coated with TiN (on Al substrate)
• Wiggler regions consists of Cu and clearing
electrodes
• Selected TiN and Cu samples from in-situ
measurements at KEK-B, CesrTA and PEP-II:
– processed TiN from CesrTA (SEY peak ~1)
– processed Cu from PEP-II (SEY peak ~1.2)
February 15, 2012 ILC DR Working Group
SEY for processed TiN film coating
email Walter Hartung ([email protected]) or Joe Calvey ([email protected]) for data files
TiN CesrTA - “horizontal sample” 0 degree
February 15, 2012 ILC DR Working Group
TiN with peak SEY~1.2 to simulate regions with less conditioning only: i.e. drift and
quadrupole in straights
(Note: drift and quadrupole in wiggler regions should use instead TiN with SEY~1).
SEY for non-fully processed TiN film coating
Fitting the low energy
part of the spectrum
might be improved …
TiN CesrTA - 45 degree sample
February 15, 2012 ILC DR Working Group
SEY for processed Copper surface
Peak 1.22, Energy at peak ~ 570 eV
C:\\ P
hys
ics S
EY
\\ Mauro
_F
red _
SE
Y _
Data
_ 2
003-2
008\\ A
SC
II TR
AN
SLA
TE
D F
ILE
S \\ 0
06061.D
AT
PEP-II beam parameters
Beam Energy, E (GeV) 3.1
Relativistic Factor, g 6066.5
Nominal Beam Current, I (A) 4.7
Dipole Magnet Field, B (Tesla) 0.765
Critical Energy, Ecrit (keV) 4.8
Dipole Magnet Arc Section, Dq (mrad) 32.7
Dipole Arc Section of photons hitting sample, Dq (mrad) 7.5 10-6
Distance of last bend magnet to SEY station location, (m) 10.1
Bunch length (mm) 12
Spacing between bunches (ns) 4.2
Transverse beam size at the sample (x/y) (μm) 228/840
zoom at 10-300 eV energy
email: [email protected] for data file
February 15, 2012 ILC DR Working Group
Fitting data with POSINST model to SEY of
“processed TiN” coating
Walter Hartung Cornell U.
The fitted parameters for the horizontal
sample are:
delta hat ts = 0.73
E hat ts = 370 eV
s = 1.32
and the fitted parameters for the 45
degree sample are:
delta hat ts = 0.95
E hat ts = 330 eV
s = 1.25
February 15, 2012 ILC DR Working Group
Photon Distribution and Photoelectric Yield Models
• The photon distribution in the ILC DR is supplied by
Synrad3D simulations (see attached Gerry Webex
presentation February 29, 2012.)
Link to photon distribution data: …
contact Gerry for more information
• Photoelectric yield (PY) model is similar in ECLOUD and
POSINST codes.
– Low energy truncated Gaussian distribution available to
both codes (Cornell version of POSINST) or Lorentzian with
high energy tail. CesrTA tune data not very sensitive to
different models.
– CLOUDLAND needs to include similar PY model
Wiggler Chamber with Clearing Electrode
• Thermal spray tungsten electrode and Alumina insulator
• 0.2mm thick layers
• 20mm wide electrode in wiggler
Joe Conway – Cornell U.
Dipole Chamber with Grooves
• 20 grooves (19 tips)
• 0.079in (2mm) deep with 0.003in tip radius
• 0.035in tip to tip spacing
• Top and bottom of chamber
Joe Conway – Cornell U.
SEY of Grooved Surface in Dipole magnet(b=2.28kG)
-2 -1 0 1 20
0.2
0.4
0.6
0.8
1
1.2
1.4
1.6
1.8
X (mm)
Y (
mm
)
Groove shape used in simulation
0 500 1000 1500 20000
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
Energy (eV)
SE
Y o
f g
roo
ve s
urf
ace
0=1.8
0=1.0
Simulated SEY of Grooved Surface
1st case: Sey0=1.0, emax=570eV; (Processed TiN);
2nd case: Sey0=1.8, emax=250eV; (Un-processed TiN ,before installation in CesrTA)
Lanfa Wang, SLAC
Simulation of grooved surface
February 15, 2012 ILC DR Working Group
Instability Simulations
• Use cloud density from build-up simulations
• Beam-cloud interactions:
- First use 40 interaction points/turn
- Then use a realistic MAD lattice at input
• Deliverable: define the emittance increase and growth rate
for cloud density extracted by the build-up simulations with
mitigations implemented.
February 15, 2012
Electron cloud assessment for TDR
Global Design Effort 20
ILC DR simulations ACTION ITEM 2012:
• Provide ILC DR "wall" file for Synrad3D - Ongoing
• Validate ILC DR "wall" input file for Synrad3D - Gerry Dugan, Laura Boon
• Benchmark Synrad3D with data - Jim Crittenden; end of January
• Photoelectron ILC DR Synrad3D simulations - Gerry Dugan, Laura Boon, mid-Feb
• Post DTC03 lattice and parameters list - David Rubin, ASAP
• Provide beam parameters and SEY models for simulations - Mauro Pivi, by mid-February
• Build-up simulations BEND with TiN and GROOVES - Venturini / Furman, mid-March
• Build-up simulations DRIFT: 1) fully & 2) partially conditioned - Jim Crittenden, by mid-March
• Build-up simulations QUADRUPOLE and SEXTUPOLE - Jim Crittenden, by mid-March
• Benchmark build-up simulations for QUADRUPOLE - Lanfa Wang, by mid-March
• Build-up simulations WIGGLER (as BEND) with cl. ELECTRODES- Lanfa Wang, by mid-March
• Instability simulations for DTC03 - Mauro Pivi, by mid-March
• Write up simulation results for TDR: total (3) paragraphs - All, by mid-April
February 15, 2012
Supporting slides …
February 15, 2012
• Preliminary CESRTA results and simulations suggest the possible presence of
sub-threshold emittance growth - Further investigation required
- May require reduction in acceptable cloud density a reduction in safety margin
• An aggressive mitigation plan is required to obtain optimum performance from
the 3.2km positron damping ring and to pursue the high current option
ILC Working Group Baseline Mitigation Recommendation
Drift* Dipole Wiggler Quadrupole*
Baseline
Mitigation I TiN Coating
Grooves with
TiN coating
Clearing
Electrodes TiN Coating
Baseline
Mitigation II
Solenoid
Windings Antechamber Antechamber
Alternate
Mitigation NEG Coating TiN Coating
Grooves with TiN
Coating
Clearing Electrodes
or Grooves
*Drift and Quadrupole chambers in arc and wiggler regions will incorporate antechambers
Summary of Electron Cloud Mitigation Plan
Global Design Effort 22
Mitigation Evaluation conducted at ILC DR Working Group Workshop meeting
M. Pivi, S. Guiducci, M. Palmer, J. Urakawa on behalf of the ILC DR Electron Cloud Working Group
February 15, 2012
Electron cloud ILC Damping Ring
simulations for Technical Design Report
TDR 2012
Global Design Effort 23
• The goal is to validate mitigations for the ILC DR.
• Build-up simulations should include “Baseline
Mitigation I” and “Baseline Mitigation II” as in
previous slide
• For the TDR, we will assume defined SEY values
for TiN and Copper, i.e. (given the tight deadlines
for delivering the results to the TDR) we will not
scan the SEY as it was done in the previous
simulation campaign.
February 15, 2012 ILC DR Working Group
February 15, 2012 ILC DR Working Group
Beam Sizes
wiggler arc arc injection /
extraction straight
February 15, 2012 ILC DR Working Group
February 15, 2012 ILC DR Working Group
Peak
SEY
before
Peak
SEY
after
Sample
position
respect to
SR fan
Electron
dose De
[mC/mm2
]
Photon
dose Dph
[ph/mm2]
Time
frame in
the -II
beam line
Equivalent
Integrated
beam current
[A hour]
Additional
Notes
TiN/Al 1.77 0.95 0 degree 910 8.45E+20 22Dec06 to
26Mar07
2198 Still SEY < 1
after 1000h
stand-by in
vacuum
TiN/Al 1.71 0.92 45 degree 910 - - - 22Dec06 to
26Mar07
2198 SEY < 1 after
1000h stand-by
in vacuum
NEG
TiZrV/Al
1.33* 1.09 0 degree 1183 1.06E+21 04Dec07 to
27Feb08
2767 *sample was
heated before
installation
Cu 1.8 1.22 0 degree 902 6.92E+20 27Feb08 to
08Apr08
1799
Stainless
steel
1.85 1.3* 45 degree 1667.5 - - - 15Jun07 to
24Sep07
3388 *measured 500h
after beam stop
Al 3.5 2.4 45 degree 2085 - - - 24Sep07 to
08Apr08
4566
PEP-II samples in-situ conditioning. Summary:
Will use the processed copper sample data from Pep-II
SEY for processed Cu surface - DR wiggler region
M. Pivi et al. Nuclear Instruments and Methods in Physics Research A 621 (1-3), 47–56, (2010).