new opportunities in plasma-surface interactions for functionalization of surfaces* ananth bhoj,...
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NEW OPPORTUNITIES IN PLASMA-SURFACE INTERACTIONS FOR FUNCTIONALIZATION OF
SURFACES*
Ananth Bhoj, Natalie Babaeva, Rajesh Dorai and Mark J. Kushner
Iowa State University104 Marston HallAmes, IA [email protected]
http://uigelz.ece.iastate.edu
May 2005
*Work supported by National Science Foundation, 3M Inc.
DAMOP_0505_01
Iowa State University
Optical and Discharge Physics
AGENDA
Plasmas for modification of surfaces
Functionalization of polymers
Challenges for adapting commodity processes for high value materials.
Opportunities for AMO
Concluding Remarks
DAMOP_0505_02
Iowa State University
Optical and Discharge Physics
PLASMAS FOR MODIFICATION OF SURFACES
Plasmas are ideal for producing reactive species (radicals, ions) for modifying surface properties to achieve desired mechanical or chemical functionality.
Plasma processing that adds or remove molecules from surfaces to achieve this functionality span orders of magnitude in conditions:
.
Etching for micro-electronics fabrication (<100’s mTorr)…. Peter Ventzek…prior talk.
Functionalization of polymers (atmospheric pressure)
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Low pressure Low throughput High precision Grow expensive
materials High tech
High pressure High throughput Low precision Modify cheap
materials Commodity
Web Treatment of Films
$0.05/m2 $1000/cm2
Microelectronics
EXTREMES IN CONDITIONS, VALUES, APPLICATIONS
Iowa State UniversityOptical and Discharge PhysicsDAMOP_0505_04
Can commodity processes be used to fabricate high value materials?
Iowa State UniversityOptical and Discharge Physics
CREATING HIGH VALUE: COMMODITY PROCESSES
$0.05/m2 $1000/cm2?
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Where will, ultimately, biocompatible polymeric films fit on this scale? Artificial skin for $0.05/cm2 or $1000/cm2?
What are the opportunities for AMO physics to build the knowledge base to meet this challenge?
LOW COST, COMMODITY FUNCTIONALIZATION OF POLYMERS
DAMOP_0505_06
Iowa State University
Optical and Discharge Physics
SURFACE ENERGY ANDFUNCTIONALITY OF POLYMERS
Most polymers, having low surface energy, are hydrophobic.
For good adhesion and wettability, the surface energy of the polymer should exceed of the overlayer by 2-10 mN m-1.
0
10
20
30
40
50
60
PT
FE
Pol
ypro
pyle
ne
Pol
yeth
ylen
e
Pol
ysty
rene
SU
RF
AC
E E
NE
RG
Y (
mN
m-1
)
POLYMER0
10
20
30
40
50
60
Prin
ting
inks
UV
adh
esiv
es
Coa
tings
Wat
erba
sed
adhe
sive
s
UV
inks
Wat
erba
sed
inks
SU
RF
AC
E T
EN
SIO
N (
mN
m-1
)
LIQUID
DAMOP_0505_07
Iowa State University
Optical and Discharge Physics
PLASMA SURFACE MODIFICATION OF POLYMERS
To improve wetting and adhesion of polymers atmospheric plasmas are used to generate gas-phase radicals to functionalize their surfaces.
Untreated PP
Plasma Treated PP
M. Strobel, 3M
Polypropylene (PP)
He/O2/N2 Plasma
Massines et al. J. Phys. D 31, 3411 (1998).
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Hydrophilic
Hydrophobic
Iowa State University
Optical and Discharge Physics
POLYMER TREATMENT APPARATUS
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HIGH-VOLTAGEPOWER SUPPLY
FEED ROLLGROUNDEDELECTRODE
COLLECTORROLL
PLASMA
~
SHOEELECTRODE
POWERED
TYPICAL PROCESS CONDITIONS:
Gas gap : a few mm
Applied voltage : 10-20 kV at a few 10s kHz
Energy deposition : 0.1 - 1.0 J cm-2Residence time : a few sWeb speed : 10 - 200 m/min
Filamentary Plasma 10s – 200 m
Iowa State University
Optical and Discharge Physics
COMMERCIAL CORONA PLASMA EQUIPMENT
Tantec, Inc.
Sherman Treaters
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N2
O2
H2O
N N2(A)
e
e O
H OH
e
O2
NO
O2,
OH
HNO2
OH
NO2O3, HO2
OHNO3
OHN2
N
O3
HO2
OH
OH
O2
O2(1)
HO2
O2HO2
H2O2
N2O5
NO3OH
Iowa State UniversityOptical and Discharge Physics
REACTION MECHANISM FOR HUMID-AIR PLASMA
Initiating radicals are O, N, OH, H
Gas phase products include O3, N2O, N2O5, HNO2, HNO3.
DAMOP_0505_11
Iowa State University
Optical and Discharge Physics
REACTION PATHWAY
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C C C C C C C C C
C C C C C C C C C C
O
H
OH
O||
OH, O
C C C C C C C C C C C
LAYER 1
LAYER 2
LAYER 3
H
OH, H2O
OH
OHO2
O2
HUMID-AIR PLASMA
BOUNDARY LAYER
POLYPROPYLENE
H2O
e e
H OH
N2
e e
N NO2
O O
e e
O2O3
O2NO
NO
Iowa State University
Optical and Discharge Physics
FUNCTIONALIZATION OF THE PP SURFACE
Untreated PP is hydrophobic.
Increases in surface energy by plasma treatment are attributed to the functionalization of the surface with hydrophilic groups.
Carbonyl (-C=O)
Alcohols (C-OH)
Peroxy (-C-O-O)
Acids ((OH)C=O)
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• Boyd, Macromol., 30, 5429 (1997).
Polypropylene, Air corona
The degree of functionalization depends as gas mix, energy deposition and relative humidity (RH).
Iowa State University
Optical and Discharge Physics
POLYPROPYLENE (PP) POLYMER STRUCTURE
The surface energy of polypropylene [C2H3(CH3)]n is increased by hydrogen abstraction (ions, radicals photons) followed by passivation by O atoms, in this case forming peroxy groups.
DAMOP_0505_13A
Iowa State University
Optical and Discharge Physics
SITE SPECIFIC REACTIVITY
Three types of carbon atoms in a PP chain:
Primary – bonded to 1 C atom Secondary – bonded to 2 C atoms Tertiary – bonded to 3 C atoms
The reactivity of an H-atom depends on the type of C bonding. Reactivity scales as:
HTERTIARY > HSECONDARY > HPRIMARY
C C C C C C
H H H H H H
H H HCH3 CH3CH31
2 31 - Primary C
2 - Secondary C
3 - Tertiary C
DAMOP_0505_14
Iowa State University
Optical and Discharge Physics
PP SURFACE REACTION MECHANISM: INITIATION
The surface reaction mechanism has initiation, propagation and termination reactions.
INITIATION: O and OH abstract H from PP to produce alkyl radicals; and gas phase OH and H2O.
~CH2 C CH2~
CH3
~CH2 C CH2~
CH3
H O(g)
OH(g), H2O(g)
(ALKYL RADICAL)(POLYPROPYLENE)
OH(g)
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~CH2 C CH2~
CH3
(ALKYL RADICAL)
O(g), O3 (g)
(ALKOXY RADICAL)
O2 (g)
O
~CH2 C CH2~
CH3
~CH2 C CH2~
CH3
OO
(PEROXY RADICAL)Iowa State University
Optical and Discharge Physics
PP SURFACE REACTION MECHANISM: PROPAGATION
PROPAGATION: Abundant O2 reacts with alkyl groups to produce “stable” peroxy radicals. O3 and O react to form unstable alkoxy radicals.
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~CH2 C CH2
CH3
OO
C CH2~
CH3
H
~CH2 C CH2
CH3
OO
C CH2~
CH3
H
+ O2 (g)
~CH2 C CH2
CH3
OO
C CH2~
CH3
HO
O
Iowa State UniversityOptical and Discharge Physics
PP SURFACE REACTIONS: PROPAGATION / AGING
PROPAGATION / AGING: Peroxy radicals abstract H from the PP chain, resulting in hydroperoxide, processes which take seconds to 10s minutes.
DAMOP_0505_17
Iowa State University
Optical and Discharge Physics
PP SURFACE REACTION MECHANISM: TERMINATION
TERMINATION: Alkoxy radicals react with the PP backbone to produce alcohols and carbonyls. Further reactions with O eventually erodes the film.
CH2~
O
~CH2 CCH3
+
(ALKOXY RADICAL)
O
~CH2 C CH2~
CH3
(CARBONYL)
OH
~CH2 C CH2~
CH3
H(s)
(ALCOHOLS)
O(g) CO2 (g)
DAMOP_0505_18
Iowa State University
Optical and Discharge Physics
GLOBAL_KIN AND SURFACE KINETICS
Reaction mechanisms in pulsed atmospheric air plasma treatment of polymers have been investigated with global kinetics and surface models.
POLYPROPYLENE
BOUNDARYLAYER ~ mfp
BULK PLASMA
DIFFUSION REGIME
O OH CO2
GLOBAL_KIN
2-Zone homogeneous plasma chemistry (bulk plasma, boundary layer)
Plug flow Multilayer surface site
balance model Circuit module Boltzmann derived f()
DAMOP_0505_19
Iowa State University
Optical and Discharge Physics
BASE CASE: ne, Te
Ionization is dominantly of N2 and O2,
e + N2 N2+ + e + e,
e + O2 O2+ + e + e.
After a few ns current pulse, electrons decay by attachment (primarily to O2).
Dynamics of charging of the dielectrics produce later pulses with effectively larger voltages; residual preionization and metastables also persist.
N2/O2/H2O = 79/20/1, 300 K 15 kV, 9.6 kHz, 0.8 J-cm-2
Web speed = 250 cm/s (460 pulses)
DAMOP_0505_20
Iowa State University
Optical and Discharge Physics
GAS-PHASE RADICALS: O, OH
Electron impact dissociation of O2 and H2O produces O and OH. O is consumed primarily to form O3; OH is consumed by both bulk and surface processes.
After 100s of pulses, radicals attain a periodic steady state.
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O OH N
Iowa State University
Optical and Discharge Physics
PP SURFACE GROUPS vs ENERGY DEPOSITION
Surface concentrations of alcohols, peroxy radicals are near steady state with a few J-cm-2.
Alcohol densities decrease at higher J-cm-2 energy due to decomposition by O and OH to regenerate alkoxy radicals.
Air, 300 K, 1 atm, 30% RH
Ref: L-A. Ohare et al., Surf. Interface Anal. 33, 335 (2002).
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Increasing RH produces OH which react with PP to form alkyl radicals, which are rapidly converted to peroxy radicals by O2.
PP-H + OH(g) PP + H2O(g) PP + O2(g) PP-O2
Alcohol and carbonyl densities decrease due to increased consumption by OH to form alkoxy radicals and acids.
Iowa State UniversityOptical and Discharge Physics
HUMIDITY: PP FUNCTIONALIZATION BY OH
PP-OH+ OH(g)PP-O + H2O(g) , PP=O + OH(g) (OH)PP=O
DAMOP_0505_23
Iowa State University
Optical and Discharge Physics
COMMODITY TO HIGH VALUE
Control of O to O3 ratio using He/O2 mixtures can be used to customize surface functionalization.
1 atm, He/O2, 15 kV, 3 mm, 9.6 kHz, 920 pulses.
As the material value increases (cents to dollars /cm2?) higher process refinement is justified to customize functionalization.
DAMOP_0505_24
Iowa State University
Optical and Discharge Physics
COMMODITY TO HIGH VALUE
1 atm, He/O2/ H2O, 15 kV, 3 mm,9.6 kHz, 920 pulses.
Additional “tuning” of functionalization can be achieved with sub-mTorr control of water content.
Small water addition “tuning” of functionalization can be achieved with sub-mTorr control of water content.
H and OH reduce O3 while promoting acid formation.
DAMOP_0505_25
THE CHALLENGE: COMMODITY PROCESSING FOR HIGH VALUE
MATERIALS
DAMOP_0505_26
Iowa State University
Optical and Discharge PhysicsDAMOP_0505_27
THE ROLE OF PLASMAS IN BIOSCIENCE
Plasmas, to date, have played important but limited roles in bioscience.
Plasma sterilization
Plasma source ion implantation for hardening hip and knee replacements.
Modification of surfaces for biocompatibility (in vitro and in vivo)
Artificial skin
The potential for commodity use of plasmas for biocompatibility is untapped.
Low pressure rf H2O2 plasma (www.sterrad.com)
Iowa State University
Optical and Discharge Physics
“HIGH VALUE” PROCESSING - CELL MICROPATTERNING
DAMOP_0505_28
Low pressure “microelectronics-like” plasmas are used to pattern selective substrate regions with functional groups for cell adhesion.
These processes have costs commensurate with microlectronics: high value, high cost.
1Andreas Ohl, Summer School, Germany (2004).
PEO - polyethyleneoxide
pdAA – plasma deposited acrylic acid
Iowa State University
Optical and Discharge PhysicsDAMOP_0505_29
ATMOSPHERIC PRESSURE PLASMAS:THE CHALLENGE
Controlling functional groups on polymers through fundamental understanding of plasma-solid interactions will enable engineering large area biocompatible surfaces.
10,000 square miles of polymer sheets are treated annually with atmospheric pressure plasmas to achieve specific functionality. Cost: < $0.05 /m2
Low pressure plasma processing technologies produce biocompatible polymers having similar functionalities. Cost: up to $100’s /cm2 ($1000’s/cm2 for artificial skin)
Can commodity, atmospheric pressure processing technology be leveraged to produce high value biocompatible films at low cost? The impact on health care would be immeasurable.
$0.05/m2 $1000/cm2?
Iowa State University
Optical and Discharge Physics
The surface modification of polymers (such as PP) by atmospheric pressure corona DBDs is a geometrically complex but cheap process.
The plasma is filamentary non-uniformly producing reactants The surface is at best rough and at worst a mesh of strands.
Can these surfaces be functionalized to meet high value standards?
POLYMER PROCESSING BY CORONA DBDs
DAMOP_0505_30
Iowa State University
Optical and Discharge Physics
Continuity (sources from electron and heavy particle collisions, surface chemistry, photo-ionization, secondary emission), fluxes by modified Sharfetter-Gummel with advective flow field.
Poisson’s Equation for Electric Potential:
Electron energy equation:
Photoionization, electric field and secondary emission:
ii St
N
SV
DESCRIPTION OF nonPDPSIM: CHARGED PARTICLE, SOURCES
2
3
4
exp)()(
)(rr
rdrr
rNrN
rSjiji
Pi
DAMOP_0505_31
e
ieiie
e qj,T2
5NnEj
t
n
Iowa State University
Optical and Discharge Physics
CAN COMMODITY PROCESSES PRODUCE HIGH VALUE MATERIALS
Demonstration: corona-rod, 2 mm gap, 15 kV pulse, N2/O2/H2O =79.5 / 19.5 / 1, 1 atm Tantec, Inc.
DAMOP_0505_32
E/N, Te, SOURCES, ELECTRON DENSITY Pulse is initiated with electron emission from tip of cathode.
Development of plasma streamer deforms potential producing large electric field. Pulse is terminated with dielectric charging.
N2/O2/H2O =79.5 / 19.5 / 1, 1 atm,-15 kV, 0-15 ns
E/N
MIN MAX
Animation Slide
DAMOP_0505_33
Te Net Ionization Te
[e]
Iowa State University
Optical and Discharge Physics
POST PULSE RADICAL DENSITIES
Radical and ion densities at end of pulse are as high as 10s ppm. Temperature rise is nominal due to short pulse duration.
O O2(1)
MIN MAX
N2/O2/H2O =79.5 / 19.5 / 1, 1 atm,15 kV, 0-15 ns
N2(A)
DAMOP_0505_34
H, OH
Iowa State University
Optical and Discharge Physics
Electrons penetrate surface features on the polymer to a limited extent due to surface charging.
SURFACE INTERACTIONS: ELECTRON DENSITY
-15 kV, 760 Torr, N2/O2/H2O=79.5/19.5/1
MIN (log scale) MAX1.35 ns 1.40 ns
2x109- 2x1011
2x1011- 2x1013
1.45 ns
2x1010- 2x1012
1.5 ns
1x1011- 5x1013
1.65 ns
[e] cm-3
10 mDAMOP_0505_35
Iowa State University
Optical and Discharge Physics
Radicals striking the surface penetrate into the features by diffusion.
Unlike charged species, with time, the density of radicals such as [O], increases inside these features.
SURFACE INTERACTIONS: [O] DENSITY
-15 kV, 760 Torr, N2/O2/H2O=79.5/19.5/1
1x109- 1x1012
1x1011- 1x1014
1.65 ns
5x1010- 5x1013
4.0 ns 7.0 ns
MIN (log scale) MAX
[O] cm-3
1.5 ns1.4 ns
10 m
DAMOP_0505_36
Iowa State University
Optical and Discharge Physics
FUNCTIONAL GROUP DENSITIES ON POLYPROPYLENE
1 atm, N2/O2/H2O=79.5/19.5/1, 1.5 ms, 10 kHz.DAMOP_0505_37
Iowa State University
Optical and Discharge Physics
FUNCTIONALIZATION OF SCAFFOLDING
DAMOP_0505_38
Functionalization of scaffolding-like surfaces for cell adhesion.
Can uniformity be maintained over micro-and macroscopic lengths.
Use 1 atm, He/O2/H2O mixtures to optimize.
Iowa State University
Optical and Discharge Physics
FUNCTIONALIZING PP SCAFFOLDING: HIGH O2 (He/O2/H2O = 69/30/1)
DAMOP_0505_39
High O2 produces O3 and rapid alkoxy formation.
Reactivity of O3 limits transport and produces long- and short-scale nonuniformities.
1 atm, He/O2/H2O = 69/30/1
Iowa State University
Optical and Discharge Physics
FUNCTIONALIZING PP SCAFFOLDING: LOW O2 (He/O2/H2O = 89/10/1)
DAMOP_0505_40
Lower O2 produces less O3 and limits alkoxy formation.
Overall uniformity becomes reaction limited, producing smoother functionalization.
1 atm, He/O2/H2O = 89/10/1
Iowa State University
Optical and Discharge Physics
REMINDER: LOCAL STRUCTURE MATTERS
DAMOP_0505_41
The reactivity of =C-H to gas phase species depends and with other surface species on their local bonding and orientation on surface.
1 atm, N2/O2/H2O = 79.5/19.5/1
C C C C C C
H H H H H H
H H HCH3 CH3CH31
2 31 - Primary C
2 - Secondary C
3 - Tertiary C
Experimental evidence suggest reactivity scales as:
HTERTIARY > HSECONDARY > HPRIMARY
Iowa State University
Optical and Discharge Physics
COVERAGE OF PEROXY [=C-O-O] BY BONDING AT 10 ms
DAMOP_0505_42
Primary and secondary sites with large view angles are rapidly functionalized to peroxy.
Alkyl tertiary sites lag and are susceptible to OH, O3 passivation
1 atm, N2/O2/H2O = 79.5/19.5/1
C C C C C C
H H H H H H
H H HCH3 CH3CH31
2 31 - Primary C
2 - Secondary C
3 - Tertiary C
Iowa State University
Optical and Discharge Physics
COVERAGE OF PEROXY [=C-O-O] BY BONDING AT 140 ms
DAMOP_0505_43
Long term production of O3 and reactions between surface species favor secondary and tertiary sites.
Uniformity improves (mostly).
1 atm, N2/O2/H2O = 79.5/19.5/1
C C C C C C
H H H H H H
H H HCH3 CH3CH31
2 31 - Primary C
2 - Secondary C
3 - Tertiary C
Iowa State University
Optical and Discharge Physics
PROCESSING COMPLEX SHAPES
DAMOP_0505_44
Functionalization of parts with complex shapes with dimensions larger than reaction length of radicals requires plasma to penetrate into structure.
Demonstration case: grooved disk with 30 m slots.
Iowa State University
Optical and Discharge Physics
PROCESSING COMPLEX SHAPES: PLASMA PENETRATION
DAMOP_0505_45
Plasma penetrates through grooves but shadow some surfaces.
Charging of surface steers plasma
Electron density (max = 1014 cm-3)
Animation Slide-GIF
1 atm, N2/O2/H2O = 79.5/19.5/1, 2 ns
MIN MAX
Iowa State University
Optical and Discharge Physics
PROCESSING COMPLEX SHAPES: O ATOM DENSITY
Plasma penetrates through grooves but shadow some surfaces.
Charging of surface steers plasma
O atom density (max = 1015 cm-3)
DAMOP_0505_46
1 atm, N2/O2/H2O = 79.5/19.5/1, 2 ns
MIN MAX
Animation Slide-GIF
Iowa State University
Optical and Discharge Physics
COMMENTS: PHOTONS AND CHARGING
Unlike neutral radicals that eventually diffuse into nooks-and-crannies, shadowing (photons) and local electric fields (surface charging) produce highly non-uniform profiles.
What affect does UV illumination and charging have on reactivity?
DAMOP_0505_47
1 atm, N2/O2/H2O = 79.5/19.5/1, 2 ns
MIN MAX
Iowa State University
Optical and Discharge Physics
THE CHALLENGE
Can established AMO theory and measurement techniques developed for gas phase species be extended to produce reaction probabilities on the surfaces of solid polymers?
Can scaling laws be developed for going from molecules to surfaces?
For example, how different are…..
DAMOP_0505_48
Iowa State University
Optical and Discharge Physics
OPPORTUNITIES AND CONCLUDING REMARKS
The interaction of plasma produced species with polymer surfaces is an exceedingly rich field of study.
The are very (very [very]) few fundamental studies capable of producing reaction probabilities of even simple systems such as O atoms on polypropylene or polyethylene.
Probabilities for reactions between surface species are only now becoming quantified. (Session C1: “Interaction of Slow Electrons with Biomolecules”)
Photon and charging effects on rates……unknown.
Improving our fundamental understanding and predictive capability (and leveraging commodity techniques) will revolutionize fields such as health products.
DAMOP_0505_49