1claire antoinecea/saclay - fermilab (innovative) processing of materials srf materials workshop...
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1Claire Antoine CEA/Saclay - Fermilab
(Innovative) Processing of materials
SRF materials Workshop Fermilab May 23-24, 2007
Today’s process is long, complex, expensive … and not very efficient
2Claire Antoine CEA/Saclay - Fermilab
Why do we need to process the cavities ?
1) Getting a “good” superconductor
OOPS !? What is a good SC ?
Empirically inferred with time:
Good thermal conductivity (need to use high RRR material)
EB-welding, in very good vacuum (Nb = good getter!)
Low interstitials (don’t anneal in poor vacuum, avoid hydrogen…)
No damage layer ? (need to chemically remove 100 -200 m of
the surface before achieving “good performances”)
No inclusion (metallic inclusion = hot spot for sure !)
Smooth surface ? (EP better than BCP)
…. ?
Other suspects : surface oxides, chemical residues, grain boundaries,
adsorbed layers,…
3Claire Antoine CEA/Saclay - Fermilab
Damage layer:100-200 m Origin: previous mechanical history (rolling, deep drawing/spinning…)
Not controlled yet, batch to batch variations Various recipes tried:
Chemical etching (BCP) Quick, efficient, reproducible… but rough surfaces But : stuck @ ~ 30 MV/m Problem = roughness near the weld area ?Alternative solutions: monoXstals, hydroforming (no welding seam, no roughness!)
Electropolishing (EP) Slow, expensive, higher risk of H contamination Gives the best results:40mV/m Lack of reproducibility (aging of solution, chemical residues… ?) Alternative EPs under study …
BCP+ EP: need to remove ~ 100 m (EP) to achieve smooth surface
Barrel polishing (mechanical) + BCP/EP: need to remove ~ 100 m (EP) to get rid of the damage layer…
Ideal surface processing: • removes 200 m of internal surface • no damage layer, no roughness• no chemical contamination (e.g. hydrogen)…
4Claire Antoine CEA/Saclay - Fermilab
Why do we need to process the cavities ?
2) Get a dust free surface to prevent filed emission (high electric field regions = cavities’ irises)
• Emitting sites = dusts, scratches
• Dust particles gather and weld together and to surface
• Local enhancement of E =>E
Field emission is the main practical limitation in accelerator operation
~ 3
~ 100-500
Ni particles
5Claire Antoine CEA/Saclay - Fermilab
Detail of the usual process (1/2)
FormingFormingWHY COMMENT
EB weldingEB welding Clean weldingNb = getter. Degraded RRR @ weld => Q0/10
Ti purificationTi purification
Deep etchingDeep etching
Increase RRR RRR 300-400 now commercially available
BCP
EP
Remove damage layer (100-200 µm)
BCP limited to ~ 30MV/m; EP => >40 mV/m but lack of reproducibility
800°C annealing800°C annealing Remove Hydrogen contamination
hydrogen source : wet processesHydrogen segregates at the surface and form hydrides (poor SC)
Diffusion layer < ~1µmLight etchingLight etching Remove diffusion layer (O, C, N)
6Claire Antoine CEA/Saclay - Fermilab
Detail of the usual process (2/2)
WHY COMMENT
HPRHPR
HF, H2O2, ethanol, degreasing,…
Fight field emission gt rid of S (after EP)……Special rinseSpecial rinse
……Light etchingLight etching
Get rid of dust particles Most convenient, but not sufficient
Ancillaries: couplers antennas…
In clean room. But re-contamination still possible
Baking, 120°C, 48hBaking, 120°C, 48h Get rid of the high field losses (Q-drop)
Mechanism not understood, concerns the first 10 nm of the material
assemblyassembly
Post processingPost processing Get rid of dust particlesDue to assembly
Under developmentEx: dry ice cleaning, plasma
RF testRF test
He processing, HPPHe processing, HPP Field emission Field emission: SRF accelerator plague !
7Claire Antoine CEA/Saclay - Fermilab
High pressure rinsing (HPR) 1/2
ultra pure H2O, ultra filtered, 80-100 bars
MPa 14 2
v
2f
MPa 250
vu fs
(Droplets)
(Flow)
Fe
vf ~ 160 m/s
Fe
100 bars
Size
(m)
Fe
(N)
Fad
(N)
0.1 10-9 10-9
1 10-6 10-8
10 10-4 10-6
Particles are displaced when Fe > Fad
8Claire Antoine CEA/Saclay - Fermilab
High pressure rinsing (HPR) 2/2
• HPR is due to mechanical effect of the droplets
• Fe is high enough to deform Nb (l Nb ~ 150-200 MPa)
• post contamination after HPR is still possible
• HPR is not very efficient on S particles after EP (S embedded in organic material ?)
Before HPR
After HPR
[M. Luong, PhD, 1998]
9Claire Antoine CEA/Saclay - Fermilab
RF post processing : He processing & HPPP
Helium processing
Developed mainly @ CERN
Helium gaz + RF => plasma
Low efficiency, mainly low field
High Peak Power processing (HPP)
Concept developed @ Cornell: burning out particles at high field
Pulsed RF to prevent quench
High power klystron or adjustable coupling (expensive)
High risks: limitations of the couplers, creation of stable emitters
Advantage: in situ,after assembly
[H.Padamsee et al., RF superconductivity for accelerators, 1998]
10Claire Antoine CEA/Saclay - Fermilab
High Peak Power processing (HPP)
[1] A. Boechner et al., Proc. of EPAC06, p413, 2006[2] W-D. Moeller et al., Proc. of EPAC96, p2013, 1996
HPP in a Cryomodule at ELBE, Rossendorf [1] HPP for C19 at DESY [2]
For ILC: 10MW (1.565mS) klystron and 1MW power coupler. Qext = 3.5x10-6
Power could be available but needs re-configuration of RF distribution (expensive!!!)
HPP power and field in Tesla 9-cell cavity
SC=>long pulses to compensate filling time
Need for high power or adjustable couplers
Need for high power Klystron
Was never tested for field higher than 25 MV/m (no power source available until recently)
Reliability and thermal load issues
11Claire Antoine CEA/Saclay - Fermilab
Other post processingAdvantage: applicable in situ, after assembly
Dry ice cleaning
Developed @ DESYCarbonic snow => residuals = CO2
Mechanical effect, similar to HPR
Applicable on horizontal cavities
In situ ECR plasma cleaning
Developed @ FNALApplicable on equipped cavities: usual antennas, RF source
Need for a valve + external magnet, no internal parts
Cleaning of particles/surface layers by plasma
Possible post/ (dry) oxidation to protect surfaces
ECR = electron cyclone resonance
m
eB
[courtesy of D.Reschke, DESY]
[courtesy of G. Wu, FNAL]
12Claire Antoine CEA/Saclay - Fermilab
Coating as a bulk niobium cavity treatment
1. M. J. Sadowski et al., The Andrzej Soltan Institute2. A-M. Valente et al., JLAB3. S. Calatroni, CERN
Standard Nb coating methods:
Electron cyclotron resonance plasma deposition 2
Vacuum Arc deposition 1
Concept: overlay bulk Nb defects by a “good”, very pure Nb layer, no wet process.
Drawback : thin layers are usually less good than bulk Nb
Advantage: substrate = Nb => annealing (recrystallization) = possible
Other drawback : post contamination still possible (complex assembly/re-assembly process)
Biased magnetron sputtering 3
13Claire Antoine CEA/Saclay - Fermilab
Other possible processing methods:
Laser, electron or ion beam irradiation:Recrystallization of the surface, vaporization of defects, particles
Non-HF wet chemical etching, polishing, other recipes…To replace EP
Alternative rinsing (for S, organic contamination, EP specific)US degreasing
Ethanol rinsing
H2O2
UV ozone
Plasma processing/etchingElectrohydrodynamic cleaning (corona plasma)
Ion beam
Ion cluster beam etching…
Ultrasonic, megasonic Better cleaning of sub micron particles
Field emission +
14Claire Antoine CEA/Saclay - Fermilab
Conclusion
Deep etching cannot be prevented, but better definition/specifications of the material could help to reduce it.
Final treatment should produce smooth surface and be able to get rid of chemical residues as well as dust particles.
In situ post processing should be developed since recontamination during assembly is still possible.
Processing of ancillaries parts should also be addressed.
New ideas are awaited