NEW%20OPPORTUNITIES%20IN%20PLASMA-SURFACE%20INTERACTIONS%20FOR%20FUNCTIONALIZATION%20OF%20SURFACES* - PowerPoint PPT Presentation

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NEW%20OPPORTUNITIES%20IN%20PLASMA-SURFACE%20INTERACTIONS%20FOR%20FUNCTIONALIZATION%20OF%20SURFACES*

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Title: NEW%20OPPORTUNITIES%20IN%20PLASMA-SURFACE%20INTERACTIONS%20FOR%20FUNCTIONALIZATION%20OF%20SURFACES*


1
NEW OPPORTUNITIES IN PLASMA-SURFACE INTERACTIONS
FOR FUNCTIONALIZATION OF SURFACES Ananth Bhoj,
Natalie Babaeva, Rajesh Dorai and Mark J.
Kushner Iowa State University 104 Marston
Hall Ames, IA 50011 mjk_at_iastate.edu http//uigelz.
ece.iastate.edu May 2005 Work supported by
National Science Foundation, 3M Inc.
DAMOP_0505_01
2
AGENDA
  • Plasmas for modification of surfaces
  • Functionalization of polymers
  • Challenges for adapting commodity processes for
    high value materials.
  • Opportunities for AMO
  • Concluding Remarks

Iowa State University Optical and Discharge
Physics
DAMOP_0505_02
3
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 (lt100s
    mTorr). Peter Ventzekprior talk.
  • Functionalization of polymers (atmospheric
    pressure)

Iowa State University Optical and Discharge
Physics
DAMOP_0505_03
4
EXTREMES IN CONDITIONS, VALUES, APPLICATIONS
Web Treatment of Films
Microelectronics
  • High pressure
  • High throughput
  • Low precision
  • Modify cheap materials
  • Commodity
  • Low pressure
  • Low throughput
  • High precision
  • Grow expensive materials
  • High tech

Iowa State University Optical and Discharge
Physics
DAMOP_0505_04
5
CREATING HIGH VALUE COMMODITY PROCESSES
  • Can commodity processes be used to fabricate high
    value materials?
  • 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?

Iowa State University Optical and Discharge
Physics
DAMOP_0505_05
6
LOW COST, COMMODITY FUNCTIONALIZATION OF POLYMERS
DAMOP_0505_06
7
SURFACE ENERGY AND FUNCTIONALITY 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.

Iowa State University Optical and Discharge
Physics
DAMOP_0505_07
8
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.
  • Massines et al. J. Phys. D 31, 3411 (1998).

Iowa State University Optical and Discharge
Physics
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9
POLYMER TREATMENT APPARATUS
  • Filamentary Plasma 10s 200 mm

Iowa State University Optical and Discharge
Physics
DAMOP_0505_09
10
COMMERCIAL CORONA PLASMA EQUIPMENT
  • Sherman Treaters
  • Tantec, Inc.

Iowa State University Optical and Discharge
Physics
DAMOP_0505_10
11
REACTION MECHANISM FOR HUMID-AIR PLASMA
  • Initiating radicals are O, N, OH, H
  • Gas phase products include O3, N2O, N2O5, HNO2,
    HNO3.

Iowa State University Optical and Discharge
Physics
DAMOP_0505_11
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REACTION PATHWAY
Iowa State University Optical and Discharge
Physics
DAMOP_0505_12
13
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 (-CO)
  • Alcohols (C-OH)
  • Peroxy (-C-O-O)
  • Acids ((OH)CO)
  • The degree of functionalization depends as gas
    mix, energy deposition and relative humidity
    (RH).
  • Boyd, Macromol., 30, 5429 (1997).
  • Polypropylene, Air corona

Iowa State University Optical and Discharge
Physics
DAMOP_0505_13
14
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.

Iowa State University Optical and Discharge
Physics
DAMOP_0505_13A
15
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 gt HSECONDARY gt HPRIMARY

Iowa State University Optical and Discharge
Physics
DAMOP_0505_14
16
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.

Iowa State University Optical and Discharge
Physics
DAMOP_0505_15
17
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.

Iowa State University Optical and Discharge
Physics
DAMOP_0505_16
18
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.

Iowa State University Optical and Discharge
Physics
DAMOP_0505_17
19
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.

Iowa State University Optical and Discharge
Physics
DAMOP_0505_18
20
GLOBAL_KIN AND SURFACE KINETICS
  • Reaction mechanisms in pulsed atmospheric air
    plasma treatment of polymers have been
    investigated with global kinetics and surface
    models.
  • GLOBAL_KIN
  • 2-Zone homogeneous plasma chemistry (bulk plasma,
    boundary layer)
  • Plug flow
  • Multilayer surface site balance model
  • Circuit module
  • Boltzmann derived f(?)

Iowa State University Optical and Discharge
Physics
DAMOP_0505_19
21
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)

Iowa State University Optical and Discharge
Physics
DAMOP_0505_20
22
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.
  • O
  • OH
  • N

Iowa State University Optical and Discharge
Physics
DAMOP_0505_21
23
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).

Iowa State University Optical and Discharge
Physics
DAMOP_0505_22
24
HUMIDITY PP FUNCTIONALIZATION BY OH
  • 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.

PP-OH OH(g)?PP-O? H2O(g) , PPO? OH(g)
? (OH)PPO
Iowa State University Optical and Discharge
Physics
DAMOP_0505_23
25
COMMODITY TO HIGH VALUE
  • As the material value increases (cents to dollars
    /cm2?) higher process refinement is justified to
    customize functionalization.
  • 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.

Iowa State University Optical and Discharge
Physics
DAMOP_0505_24
26
COMMODITY TO HIGH VALUE
  • 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.
  • 1 atm, He/O2/ H2O, 15 kV, 3 mm,
  • 9.6 kHz, 920 pulses.

Iowa State University Optical and Discharge
Physics
DAMOP_0505_25
27
THE CHALLENGE COMMODITY PROCESSING FOR HIGH
VALUE MATERIALS
DAMOP_0505_26
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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
DAMOP_0505_27
29
HIGH VALUE PROCESSING - CELL MICROPATTERNING
  • PEO - polyethyleneoxide
  • pdAA plasma deposited acrylic acid
  • 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).
Iowa State University Optical and Discharge
Physics
DAMOP_0505_28
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ATMOSPHERIC PRESSURE PLASMASTHE 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 lt 0.05 /m2
  • Low pressure plasma processing technologies
    produce biocompatible polymers having similar
    functionalities. Cost up to 100s /cm2
    (1000s/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.

Iowa State University Optical and Discharge
Physics
DAMOP_0505_29
31
POLYMER PROCESSING BY CORONA DBDs
  • 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?

Iowa State University Optical and Discharge
Physics
DAMOP_0505_30
32
DESCRIPTION OF nonPDPSIM CHARGED PARTICLE,
SOURCES
  • Continuity (sources from electron and heavy
    particle collisions, surface chemistry,
    photo-ionization, secondary emission), fluxes by
    modified Sharfetter-Gummel with advective flow
    field.
  • Poissons Equation for Electric Potential
  • Electron energy equation
  • Photoionization, electric field and secondary
    emission

Iowa State University Optical and Discharge
Physics
DAMOP_0505_31
33
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.

Iowa State University Optical and Discharge
Physics
DAMOP_0505_32
34
E/N, Te, SOURCES, ELECTRON DENSITY
Animation Slide
  • 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.
  • Te
  • Net Ionization
  • Te
  • e
  • E/N
  • N2/O2/H2O 79.5 / 19.5 / 1, 1 atm,
  • -15 kV, 0-15 ns

DAMOP_0505_33
35
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?)
  • N2(A)
  • H, OH
  • N2/O2/H2O 79.5 / 19.5 / 1, 1 atm,
  • 15 kV, 0-15 ns

Iowa State University Optical and Discharge
Physics
DAMOP_0505_34
36
SURFACE INTERACTIONS ELECTRON DENSITY
2x109- 2x1011
2x1010- 2x1012
? Electrons penetrate surface features on the
polymer to a limited extent due to surface
charging.
? -15 kV, 760 Torr, N2/O2/H2O79.5/19.5/1
e cm-3
MIN (log scale) MAX
1.45 ns
1.5 ns
1.65 ns

2x1011- 2x1013
1x1011- 5x1013
Iowa State University Optical and Discharge
Physics
10 mm
DAMOP_0505_35
37
SURFACE INTERACTIONS O DENSITY
1x109- 1x1012
5x1010- 5x1013
? 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.
? -15 kV, 760 Torr, N2/O2/H2O79.5/19.5/1
1.5 ns
1.4 ns
4.0 ns
1.65 ns
7.0 ns

O cm-3
MIN (log scale) MAX
10 mm
1x1011- 1x1014
Iowa State University Optical and Discharge
Physics
DAMOP_0505_36
38
FUNCTIONAL GROUP DENSITIES ON POLYPROPYLENE
  • 1 atm, N2/O2/H2O79.5/19.5/1, 1.5 ms, 10 kHz.

Iowa State University Optical and Discharge
Physics
DAMOP_0505_37
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FUNCTIONALIZATION OF SCAFFOLDING
  • ? 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
DAMOP_0505_38
40
FUNCTIONALIZING PP SCAFFOLDING HIGH O2
(He/O2/H2O 69/30/1)
  • 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
DAMOP_0505_39
41
FUNCTIONALIZING PP SCAFFOLDING LOW O2
(He/O2/H2O 89/10/1)
  • 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
DAMOP_0505_40
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REMINDER LOCAL STRUCTURE MATTERS
  • The reactivity of C-H to gas phase species
    depends and with other surface species on their
    local bonding and orientation on surface.
  • Experimental evidence suggest reactivity scales
    as
  • HTERTIARY gt HSECONDARY gt HPRIMARY

? 1 atm, N2/O2/H2O 79.5/19.5/1
Iowa State University Optical and Discharge
Physics
DAMOP_0505_41
43
COVERAGE OF PEROXY C-O-O? BY BONDING AT 10 ms
  • Primary and secondary sites with large view
    angles are rapidly functionalized to peroxy.
  • Alkyl tertiary sites lag and are susceptible to
    OH, O3 passivation

Iowa State University Optical and Discharge
Physics
? 1 atm, N2/O2/H2O 79.5/19.5/1
DAMOP_0505_42
44
COVERAGE OF PEROXY C-O-O? BY BONDING AT 140 ms
  • Long term production of O3 and reactions between
    surface species favor secondary and tertiary
    sites.
  • Uniformity improves (mostly).

Iowa State University Optical and Discharge
Physics
? 1 atm, N2/O2/H2O 79.5/19.5/1
DAMOP_0505_43
45
PROCESSING COMPLEX SHAPES
  • 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
DAMOP_0505_44
46
PROCESSING COMPLEX SHAPES PLASMA PENETRATION
  • 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
Iowa State University Optical and Discharge
Physics
DAMOP_0505_45
47
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)

Animation Slide-GIF
? 1 atm, N2/O2/H2O 79.5/19.5/1, 2 ns
Iowa State University Optical and Discharge
Physics
DAMOP_0505_46
48
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?

? 1 atm, N2/O2/H2O 79.5/19.5/1, 2 ns
Iowa State University Optical and Discharge
Physics
DAMOP_0505_47
49
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..

Iowa State University Optical and Discharge
Physics
DAMOP_0505_48
50
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 ratesunknown.
  • Improving our fundamental understanding and
    predictive capability (and leveraging commodity
    techniques) will revolutionize fields such as
    health products.

Iowa State University Optical and Discharge
Physics
DAMOP_0505_49
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