9-12 April 2007

International Linear Collider DR electron cloud R&D effort1st part: Tests in PEP-IIM. Pivi

L. Wang, D. Arnett, G. Collet, R. Kirby, F. King, T. Markiewicz, B. McKee, M. Munro, N. Phinney, T. Raubenheimer, J. Seeman (SLAC), F. Le Pimpec (PSI)

ECLOUD 07Daegu

S. Korea

Courtesy P. Garbincius

• Effort started in 2003 with extensive simulations of electron cloud

build-up in DR including quadrupole and wigglers regions, and

simulations to characterize the single-bunch instability threshold

• International collaboration R&D effort: 2005-2006 simulation

campaign culminating in the recommendation for the damping ring

circumference reduced from 17 km to 12km [electron cloud safe],

then further reduced to 6km [red flag for electron cloud].

• Although an electron cloud is expected in the 6km positron Damping

Ring, simulations give increased confidence on possible remedies as

clearing electrodes and grooves.

• Substantial R&D effort is needed to confirm possible mitigation

techniques.

ILC DR Electron cloud simulation historyILC DR Electron cloud simulation historyILC DR Electron cloud simulation historyILC DR Electron cloud simulation history

Compare options: simulations historyCompare options: simulations historyCompare options: simulations historyCompare options: simulations history

Cloud density near (r=1mm) beam (m-3) before bunch passage, values are taken at a cloud equilibrium density. Solenoids decrease the cloud density in DRIFT regions, where they are only effective. Compare options LowQ and LowQ+train gaps. All cases wiggler aperture 46mm.

Global ILC R&D programIn progress:- At KEKB: in situ Secondary Electron Yield (SEY) measurements, ante-

chamber, Cu, TiN and NEG chambers. PLANNED: Clearing electrodes in wiggler.

- At SLAC: SEY of samples in accelerator beam line, rect. groove chambers, TiN chambers.

PLANNED: Clearing electrodes and grooves in bends.

Planned:- SPS and PS: LHC pre/injectors. Scrubbing runs and several mitigation

techniques are under evaluation.- Daphne: positron ring limited in current. TiN in aluminum wiggler

sections.

Proposed:- CesrTA: suppression techniques in wigglers (ILC damping ring

wigglers). Electron cloud build-up and instability with ultra-low emittancies close to the ILC DR.

- KEKB: Low emittance operation for electron cloud tests

• R&D Goals:– Estimate e-cloud build-up and single-bunch instability thresholds– Reduce surface secondary electron yield (SEY) below electron cloud

threshold for ILC DR: SEY ≤ 1.2

• Surface approaches– Thin film coatings– Electron and photon surface conditioning– Clearing electrodes– Grooved surfaces

• Projects:– ONGOING: conditioning TiN and NEG coatings in PEP-II straights– ONGOING: rectangular groove chambers in PEP-II straights– PLANNED: clearing electrode chamber in magnets– PLANNED: triangular groove chamber in magnets

E-cloud and SEY R&D Program SLAC

SEY GROOVE 1 GROOVE 2FLAT 1 FLAT 2

COLLECTORSENERGY ANALYZER

THERMOCOUPLES

GROOVE CHAMBERS EXPERIMENTSEY TEST STATION

PEP-II test chambers installationPEP-II test chambers installationPEP-II test chambers installationPEP-II test chambers installation

SEY station can be used to expose samples to PEP-ii beam environment and then measure samples in lab (transport in load-lock)

Grooved and Flat chambers installed to measure performance inPEP-ii beam environment

TiN/Al sample exposed to SR

PEP-II LER sideRF seal location

SEY TESTS TiN and NEGSEY TESTS TiN and NEGSEY TESTS TiN and NEGSEY TESTS TiN and NEG

Expose samples to PEP-II LER synchrotron radiation and electron conditioning. Then, measure Secondary Electron Yield (SEY) in laboratory. Samples transferred under vacuum.

Complementary at SPS and KEK studies

20mm

Project 2: chamber with coating samples.

e+

sample supports and transferring systems

45o position

0o position

PEP-II

SEY test station in PEP-II LERSEY test station in PEP-II LERSEY test station in PEP-II LERSEY test station in PEP-II LER

45o position

0o position

SEY test station in PEP-II LERSEY test station in PEP-II LERSEY test station in PEP-II LERSEY test station in PEP-II LER

45o position

0o position

SEY chamber instrumentation: SEY chamber instrumentation: e- energy analyzere- energy analyzerSEY chamber instrumentation: SEY chamber instrumentation: e- energy analyzere- energy analyzer

R. Kirby and M. P. SLAC, based on K.Harkay and R.Rosenberg design

p.14

Design- Fin ExtrusionsDesign- Fin Extrusions

FIN TIPS= I.D. OF CHAMFAN HITS HERE FIRST

LIGHT PASSES THRU SLOTS BETW FINSBECAUSE FAN IS “THICKER” THAN FIN

FAN EVENTUALLY HITS “BOTTOM” OF SLOT FOR FULL SR STRIKE

VIEW IS ROTATED 90 CCW FROM ACTUAL FAN ORIENTATION

p.15

Design- Fin ChamberDesign- Fin Chamber

Chambers are constructed of Al extrusions machined to length with end preps for masks & flanges.

Al extrusions were chosen for their economy and ease of manufacture

Bonus - cooling is integral to the cross section, not welded to the outside

Flanges are bi-metal Atlas flanges that are welded directly to chamber

Insufficient space between the chamber and the flange knife edge for a bi-metal transition

Bottom sides of chambers are perforated at the ports Inside surfaces are TiN coated

Reduce thermal outgassing & PSD Reduce secondary electron yield

Fin chamber weight ~ 32 lbs

p.16

Design- Port DetailDesign- Port Detail

4” port shown here, 500 holes, 25 x 20, holes 1.6 mm

1.5” port hole pattern is 50 holes, 10x5, holes 1.6 mm

Instrumentation: collector plate inside portInstrumentation: collector plate inside portInstrumentation: collector plate inside portInstrumentation: collector plate inside port

Chamber samples: SEY after TiN coating Chamber samples: SEY after TiN coating before installation in PEP-II before installation in PEP-II Chamber samples: SEY after TiN coating Chamber samples: SEY after TiN coating before installation in PEP-II before installation in PEP-II

Installation in PEP-II LERInstallation in PEP-II LERInstallation in PEP-II LERInstallation in PEP-II LER

Fin chamber

Flat chamber

p.20

Design – Existing Ring LayoutDesign – Existing Ring Layout

LER DIRECTION

ELEVATION VIEW

PLAN VIEW

BEND B1

AISLE SIDE

TIN/Al GROOVE/FLAT CHAMBERS HERESEY CHAMBER HERE

SEY test chamber samples: SEY before installation in PEP-II

LER #1 and #2 samples are then inserted in the PEP-II stainless steel chamber respectively in the plane of the synchrotron radiation fan (0o position) and out of this plane (45o position)

Secondary Yields after two months in PEP-II LER

LER#1

XPS Before installation After exposure in PEP-II LER for 2 months (e dose 100mC/mm^2)

Different from electron conditioning in laboratory setup where carbon crystals grows! Carbon is strongly reduced if exposed to beam. Same for LER #1 and #2 samples.

Surface analysis: Carbon content decrease

+214 hours at 1.1e-9 torr, 10:1 H2:COAfter 2 months conditioning in PEP-II

SEY after exposure to vacuum

(214 = 52 hours in PEP-II no beam +162 in laboratory setup)

Measured electron energy distribution

Compare vacuum chamber e- currents

Measured e- current in TiN/Al fin/flat chambers << StSt chamber. PEP-II LER current still raising (2.7A 4A).

groove1 groove2 flat2 flat1

18 March 2007

Solenoid ON at fin/flat chambers location

Switched external solenoid winding ON (10A Bz=20 Gauss). Ibeam = 2.2A. Note: at ~20 Gauss, photoelectrons should dominate with respect to secondary electrons..

10 15 20 250

0.2

0.4

0.6

0.8

1

1.2

1.4

1.6

1.8

2x 10

14

S (m)

Ph

oto

n d

ensi

ty (

ph

oto

ns

m-1

s-1)

Photon Density for 1mA beam

G1

G1

F1

F2

0 500 1000 1500 2000 25000

0.5

1

1.5

2

2.5

3

3.5

4

4.5

5

Beam Current (mA)

Ele

ctro

n C

urr

ent

(10

-6A

/cm

2)

TiN Groove 1TiN Groove 2TiN Flat 1TiN Flat 2Stainless Steel

Photon electron dominant ?

Preliminary benchmark with CLOUDLAND

0

0.5

1

1.5

2

2.5

0 0.5 1 1.5 2 2.5 3

Ib(A)

Ie

SEY=1.3, R=0.001 SEY=1.2, R=0.001 Flat 2

SEY=1.3,R=0.001 SEY=1.2, R=0.0005

0

0.5

1

1.5

2

2.5

0 0.5 1 1.5 2 2.5 3

Ib (A)

Ie

SEY=1.2, R=0.001 SEY=1.1 R=0.001 Flat 1

SEY=1.3, R=0.001 SEY=1.2 SEY=0.0005

Flat 1 Flat 2

In simulation, the SEY and the number of photon electrons are varied

For the Flat chamber, the SEY is around 1.1~1.2

L.Wang SLAC

Flat chamber

0

0.5

1

1.5

2

2.5

3

0 0.5 1 1.5 2 2.5 3 3.5

I (A)

Ie

SEY=1.2 SEY=1.1 Flat 2 SEY=1.3

This plot only show the SEY effect, R=0.001 for all of them

(R=e/p/m)

Simulation: - Uniform photoe- distribution- Electron current at the wall

Grooved chamber

0

0.5

1

1.5

2

2.5

3

3.5

4

0 0.5 1 1.5 2 2.5 3

I (A)

Ie

Groove 1 Groove 2 SEY=1 R=0.004 SEY=1 R=0.005

For the grooved chamber, the SEY is ~1

Simulation: - Uniform photoe- distribution- Electron current at the wall

SEY estimation

500 1000 1500 2000 2500 30000

2

4

6

8

10

12

14

Beam Current (mA)

No

rmal

ized

Ele

ctro

n C

urr

ent

TiN Groove 1TiN Groove 2TiN Flat 1TiN Flat 2

0 500 1000 1500 2000 25000

0.5

1

1.5

2

2.5

3

3.5

4

4.5

5

Beam Current (mA)

Ele

ctro

n C

urr

ent

(10

-6A

/cm

2)

TiN Groove 1TiN Groove 2TiN Flat 1TiN Flat 2Stainless Steel

Raw data

...)(sec ondaryrmnonlinerteII bphotone

Ratio of Secondary to photoelectronsTotal electrons

Grooved Chamber has more photon electrons for some reason, but Flat Chamber has more secondary electrons, hence a higher SEY. This agree with simulation.

0

0.5

1

1.5

2

2.5

0 0.5 1 1.5 2 2.5 3

I (A)

Ie

New Model

Y. Suetsugu, APAC07

0 500 1000 1500 2000 25000

0.5

1

1.5

2

2.5

3

3.5

4

4.5

5

Beam Current (mA)

Ele

ctro

n C

urr

ent

(10

-6A

/cm

2)

TiN Groove 1TiN Groove 2TiN Flat 1TiN Flat 2Stainless Steel

PEPII Exp.

KEKB Exp.

Simulation closer to the experimental setup:- Photo e- on the chamber side-Collector on bottom chamber

Need more detail study

Work in progressWork in progressWork in progressWork in progress

• Electron signal in flat & fin chambers is much lower than stainless steel chamber.

• Electron signal in flat chambers is lower than fin chambers:– Photoelectron dominant in fins?– Fin chambers efficient photon absorbers?

• Simulation campaign starting:– Fitting stainless steel data to parameterize SEY– Fitting to flat & fin chamber data:

• Low SEY in flat chambers and grooved chambers between 0.9~1.2

• Appear to have higher photo e- rate in fin chambers

– Need ray tracing of photons to understand fin chamber

More input would be welcome

Plan for future workPlan for future workPlan for future workPlan for future work

Simulations:

• Systematic simulation effort starting • Further code benchmarking will be done

Experimental

• Conditioning and recontamination studies

• Insertion in beam line of non-evaporable getter NEG samples

• Insertion of samples with different materials: Cu, Stst, Al

• Study asymptotic conditioning effect: coating the stainless steel chamber with TiN (and NEG).

• Testing of chambers with NEG and clearing electrodes

Outstanding e-cloud questions Outstanding e-cloud questions Outstanding e-cloud questions Outstanding e-cloud questions Simulations

• Are the build-up codes sufficiently developed and benchmarked?

• Are the instability code sufficiently developed and benchmarked?

• What is the SEY threshold in the ILC DR configuration 3ns bunch spacing? – More code benchmarking needed

• In the presence of an electron cloud: is the dynamic aperture preserved at injection? – Large beam sizes no instability, but incoherent tune shift, ..

• Incoherent emittance growth below threshold, is it a real effect?

Remedies

• Is TiN thin film resistant after long term exposure?

• How to minimize vacuum recontamination (SEY) effects?

• What coating: TiN or NEGs (TiZrV)

• Do we need ultra-small emittance facilities to run electron cloud tests? CesrTA/KEKB

• Dependence of the SEY with NEG activation cycles? (highly requested by CERN!)

• Do we need to test clearing electrodes to suppress the electron cloud?

• Is TiN coating sufficient in wigglers?

• Measured trapping and accumulation of electrons in quadrupoles (sextupoles)? Is this an issue per se?

41

Milestones to the ILC Engineering Design Report (EDR)

1. Characterize electron-cloud build-up. (Very High Priority)

2. Develop electron-cloud suppression techniques. (Very High Priority)

Priority: characterize coating techniques and testing of conditioning and recontamination in situ.

Clearing electrodes concepts by installation of chambers in accelerators. Characterization of impedance, HOM and power load deposited to the electrodes.

Groove, slots and other concepts. Characterization of impedance, and HOM.

3. Develop modeling tools for electron-cloud instabilities. (Very High Priority)

4. Determine electron-cloud instability thresholds. (Very High Priority)

Characterization the electron cloud instability: various codes in use PETHS, HEAD-TAIL, WARP/POSINST, CMAD

SummarySummarySummarySummary

• Installed 5 chambers in PEP-II in January 2007

• Directly measured secondary electron yield of ~0.9 of TiN samples after exposure to beam. [Steering the ILC R&D effort in the direction of fully characterizing coating mitigation techniques..]

– Recontamination studies ongoing

• Electron signal in Fin & Flat chambers is much lower than stainless steel chamber

• Initial simulations: consistent with high SEY in Stainless steel chamber and low SEY in Fin & Flat TiN/Al chambers

– Systematic simulation effort ongoing to parameterize fin & flat chambers results

Thanks To contributors and collaborators: L. Wang, T. Raubenheimer,

D. Arnett, G. Collet, R. Kirby, N. Kurita, B. Mckee, M. Morrison, G. Stupakov, N. Phinney, J. Seeman (SLAC), M. Palmer, D. Rubin, D. Rice, L. Schachter, J. Codner, E. Tanke, J. Crittenden (Cornell), J. Gao (HIPEP), A. Markovic et al. (Rostock Univ.), M. Zisman, S. De Santis, C. Celata, M. Furman, J.L. Vay, S. De Santis (LBNL), K. Ohmi, Y. Suetsugu (KEK), F. Willeke, R. Wanzenberg (DESY), J.M. Laurent, A. Rossi, E. Benedetto, F. Zimmermann, G. Rumolo, J.M. Jimenez, J-P. Delahaye (CERN), A. Wolski (Cockroft Uniiv.), B. Macek (LANL), C. Vaccarezza, S. Guiducci, R. Cimino, P. Raimondi (Frascati), et many other colleagues…