ECLOUD´12 Novel Types of Anti-e Cloud Surfaces · SEY of graphene oxide Critical experimental...
Transcript of ECLOUD´12 Novel Types of Anti-e Cloud Surfaces · SEY of graphene oxide Critical experimental...
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Novel Types of Anti-e Cloud Surfaces
I. Montero1, V. Nistor2, L.Aguilera1, L.Galán2, D. Raboso3, L.A.
González2, M.E. Dávila1, P. Costa Pinto4, M.Taborelli4 and
F.Caspers4
1ICMM-CSIC 2UAM, 3ESA, 4CERN
ECLOUD´12
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• Main goals
• Basic Objectives and Concepts
• Critical Experimental Activities
• Anti-ecloud-Multipactor Coatings:
SEY Research
• Summary and Conclusions
Isabel Montero, ICMM-CSIC ECLOUD’12
Outline
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Main goals
To mitigate:
1. The electron cloud
and its adverse consequences
2. The multipactor effect
in space-related
high-power
RF hardware
Isabel Montero, ICMM-CSIC
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Development of coatings with
low secondary electron
emission yield (SEY)
p
sample
Basic Objectives and Concepts
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by surface material of low SEY
by surface roughness of high aspect ratio and density
Very low SEY
Very low RF
surface resistance
► by optimization of depth
of surface roughness
Very slow aging in air by stable surface material
MAIN OBJECTIVES:
Basic Objectives and Concepts
Isabel Montero, ICMM-CSIC
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Very low SEY
Very low RF
surface resistance
►
Very slow aging in air
MAIN OBJECTIVES:
Basic Objectives and Concepts
like Au / roughAg
max < 1.5
E1 > 200 eV
Stability one year
close to Ag
Rs< 3x Rsurf(Ag)
Isabel Montero, ICMM-CSIC
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Critical experimental activities
MAIN CONCEPTS: Multilayer coating
roughness layer
conductive
layer
low-SEY layer
Multilayer coating
Isabel Montero, ICMM-CSIC
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Ag, Cu, Au roughness layer
conductive
layer
low-SEY layer
Ag, Cu
Rh, TiN, …,
Au, Rh, Ir,
TiN, BC,… 50 – 1000 nm
5 – 20 μm
50 – 500 nm
5 – 50 nm
Material Thickness
Critical experimental activities
MAIN CONCEPTS: Multilayer coating
SEY suppression increases with roughness shape
(aspect ratio, density, profile)
RF surface resistance increases with roughness size
Multilayer coating
Isabel Montero, ICMM-CSIC
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Critical experimental activities
MAIN CONCEPTS: Multilayer coating
SEY and Roughness
to be optimized
Ag, Cu, Au roughness layer
conductive
layer
low-SEY layer
Ag, Cu
Rh, TiN, …,
Au, Rh, Ir,
TiN, BC,… 50 – 1000 nm
5 – 20 μm
50 – 500 nm
5 – 50 nm
Material Thickness Multilayer coating
Isabel Montero, ICMM-CSIC
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Critical experimental activities
ITI Innovation Triangle Initiative
Optimization of Surface Roughness of Anti-Multipactor
Coatings for Low Insertion Losses and Secondary
Emission Suppression for High Power RF Components in
Satellite Systems
ESA PROJECT
Departamento de
Física Aplicada
Departamento de
Física Aplicada
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Anti-Multipactor Coatings
Two different kinds tested
Critical experimental activities
Aluminum
Nickel Silver etched
Au 2 µm
Magnesium
device
MgO
5 µm
Au, Ag
2 µm
2 µm
1µm Rr /Rs = 2.2 @ 9.5 GHz 1µm Rr /Rs = 2.4 @ 12 GHz
Gold-coated anomag Gold-coated etched silver
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1/e
skin depth
silver 2
1 gold
silver 1
vacu
um
Bu
lk
Al
Critical experimental activities
Insertion losses /surface rough. is a crucial issue
Ni
z
At sufficient high ω, the induced Is are confined by the skin
effect to a surface region of poor because of surface
roughness
Isabel Montero, ICMM-CSIC
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fo
dc
fo
dc
f πμ
ρ δ
o
dc
Critical experimental activities
f R dc o
dc
s
1
surface region formed by a coating of thickness dcoat over a substrate,
A Layered Model for RF Surface Resistance Calculation
-0.5
0.0
0.5
1.0
0 0.5 1 1.5 2 2.5 3
Distance along flat surface x /p
Heig
t over
flat
surf
ace h
/p rough surface
0.9
0.8
0.7
0.6
0.5
0.4
0.3
0.2
0.1
RF current
A: Factor of increased current path at
depth z due to roughness
Rs = RF SURFACE RESISTANCE
Resonant circuit
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Anti-ecloud Coatings
0 ·
11dze
AR
z
0 ·
11dze
AR
z
0 ·
11dze
AR
z
0 ·
11dze
AR
z
1.0
1.5
2.0
0 2 4 6 8 10 12
Normalized Roughness Heigh h o /
R /
Ro
Our model
Filipovic (2007)
ho/p = ½3
/p = ¼ ho/p
=
R/R
o
Using this function with three fitting parameters it is possible
to fit the results of Filopovic or Matsushima
M V Lukic, D S Filipovic:; IEEE, 55, 518-525 (2007)
A. Matsushima and K. Nakata: Elect. Commun. Jpn. 89 (1) 1 (2006).
ho/
A Layered Model for RF Surface Resistance Calculation
h p -- Matshusima (2006)
_ _ _ _ Our model
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Liquid
Chemical Bath
Deposition
Chemical Etching
Gas (UHV)
Evaporation
Sputtering
Anodization Ion implantation
Physical Vapor
Deposition
Solid
Particle
Deposition
Anti-Multipactor Coatings
Deposition Methods
Anti-ecloud Coatings
Isabel Montero, ICMM-CSIC
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RF ion gun control units
pressure gauge and microAmp
turbo pump
RF ion gun
spherical prep chamber
UHV preparation chamber with RF ion gun for
deposition of anti-multipactor coatings
Departamento de
Física Aplicada
Departamento de
Física Aplicada
Anti-ecloud Coatings
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Selected materials
• Silver
• Gold
• NEG
• Graphene like coatings
• Magnetic and dielectric/metal
composites:
particulated surfaces
Anti-ecloud Coatings
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Selected materials
• Silver
Anti-ecloud Coatings
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Al bulk
Ni
Ag
SEY Characteristics
of Mo-Masked, Ion-Textured Silver
Al bulk
Ni
Ag 40 µm
10 µm
Al bulk
Method for producing
1. uniform,
2. highly textured surface
on high-conductivity Ag
Device
Anti-ecloud Coatings
Mo cone Ar ion beam
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Al bulk
Ni
Ag
Ar ion beam
Mo cone
SEY Characteristics
of Mo-Masked, Ion-Textured Silver
Al bulk
Ni
Ag 40 µm
10 µm
Al bulk
Method for producing
1. uniform,
2. highly textured surface
on high-conductivity Ag
Device
Anti-ecloud Coatings
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SEM of Ag treated coating
Surface roughness depends on
1. Ion density
2. Ion energy
3. Time
Anti-ecloud Coatings
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The purpose was to develop a basicaIly Ag surface having
very low-SEY characteristics.
SEY of Ag plating after treatment and exposure to the air.
Its untreated
surface
displays
relatively
very high
levels of
SEY
SEY of Ag treated coating
Anti-ecloud Coatings
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Anti-ecloud Coatings
HEATER
SAMPLE
Growing rough Ag coating CBD Chemical Bath Deposition Method
electrodes
Electrical
Contact
Preparation conditions
Growth Temperature 50ºC
TEA
AgNO3
SnClx
With and without Efield
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Selected materials
• Gold
Anti-ecloud Coatings
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Nanometric Au layer to prevent aging process
to decrease SEY
ALUMINIUM
SILVER
NICKEL
GOLD
Anti-ecloud Coatings
Isabel Montero, ICMM-CSIC
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Au coated CuO nanowires
Anti-ecloud Coatings
First
stadies of
NW
growth
XPS
NW
0 200 400 600 800 10000.0
0.5
1.0
1.5
2.0
SE
Y
Primary Electron Energy (eV)
Cu foil +Au
CuO 500ºC-2h +Au
CuO 500ºC-4h +Au
CuO 500ºC-6h + Au
CuO 500ºC-8h + Au
CuO 500ºC-10h +Au
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SEY experimental measurements Au coated CuO nanowires
Anti-ecloud Coatings
SEY of Nano-structured Materials
aspect ratio 1:1000
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Selected materials
• NEG
Non-Evaporable Getter
Anti-ecloud Coatings
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Substrate: Rough Al
Etching time (s)
SEY results
Correlation between SEY and Ra
Anti-ecloud Coatings
Isabel Montero, ICMM-CSIC
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Aluminium etched, HCl
profilometry measurements
t
Anti-ecloud Coatings
Isabel Montero, ICMM-CSIC
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Anti-Multipactor Coatings
EDC curves for Al
Anti-ecloud Coatings
Isabel Montero, ICMM-CSIC
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NEG coated rough Al
SEM
NEG
Al
Anti-ecloud Coatings
Isabel Montero, ICMM-CSIC
AFM image
NEG/flat Al
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Critical experimental activities
SEY of Rough NEG
Rough NEG, before activation Rough NEG, after activation
Isabel Montero, ICMM-CSIC
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Selected materials
• Graphene like coatings
Critical experimental activities
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0 200 400 600 800 1000 1200 1400 1600 18000.0
0.2
0.4
0.6
0.8
1.0
Al foil-aC
Al 60s-aC
Al 120s-aC
Al 150s-aC
Al 210s-aC
Al 300s-aC
Al 360s-aC
SE
Y
Primary Electron Energy (eV)
SEY <1
Critical experimental activities
Introduction: a-C coated rough Al
AFM image
aC/flat Al
SEM image
aC/roughAl
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Graphite and Graphene Oxide (GO)
Critical experimental activities
The results reveal that the GO sheets are rough and the
structure is predominantly amorphous due to distortions from
the high fraction of sp3 C−O bonds. Isabel Montero, ICMM-CSIC
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SEY of graphene oxide
Critical experimental activities
Isabel Montero, ICMM-CSIC
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Critical experimental activities
SEY of graphene oxide
Isabel Montero, ICMM-CSIC
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Selected materials
• Magnetic particulated
surfaces: ferrites
Critical experimental activities
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Critical experimental activities
SEY OF MAGNETIC PARTICULATED
SURFACES: ferrites
the surface coating
including a multitude of
particles sized
Reexamining the effects of
magnetized surfaces on the SEY
properties
primary
Isabel Montero, ICMM-CSIC
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Selected materials
• Composites: dielectric/metal
Critical experimental activities
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Critical experimental activities
New Insights into metal/dielectric particulated
surfaces and their SEY properties composite
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Critical experimental activities
New Insights into metal/dielectric particulated
surfaces and their SEY properties
Composite
Alumina/aluminium
Isabel Montero, ICMM-CSIC
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Critical experimental activities
New Insights into metal/dielectric particulated
surfaces and their SEY properties
+ +
+ + + + + + +
+ + + + +
substrate
Secondary
electrons
Primary
electrons SEY<<1
Dielectric
metal
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SUMMARY
Anti-eCloud coatings exposed to the air.
Critical experimental activities
SE
Y
Rough
Surfaces Flat
Surfaces
Isabel Montero, ICMM-CSIC
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Summary and Conclusions
Future work
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This work is directed to providing surfaces
having extremely low secondary electron
emissions.
The molybdenum-masked, ion-textured
silver surface wiII be a promising material for
inhibiting multipactor.
Extremely reduction of SEY is observed in
different particulated metal/dielectric systems.
Summary and Conclusions
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As far as the achievement of low SEY coatings
should rely heavily on surface morphologies with
roughness of high aspect ratio, insertion losses due
to surface resistance become a crucial issue.
It is necessary the optimization of surface
roughness of anti-multipactor coatings for low
insertion losses and secondary emission
suppression for high power RF components in
satellite systems
.
Summary and Conclusions
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