complex materials group peter f. green department of chemical engineering and texas materials...
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Complex Materials Group
Peter F. Green
Department of Chemical Engineering and Texas Materials Institute
The University of Texas at Austin
• Conventional applications: – Coatings– Membranes – Lubrication
• Processing: – Self assembly– Lithography
• Device technologies– Light emitting diodes– Organic photodiodes– Sensors
Motivation for research : problems at the nanoscale in polymer based systems
thin film transistor
(T. Kawase, et. al. Digest of Technical Papers 2001)
Polymer is the active material
component
Particles of Nanoscale dimensions
h~1-50 nm
Polymer thin films (h~1-100 nm) exhibit properties that differ from the bulk (new phenomena)
• Confinement (entropic), enthalpic (polymer-polymer) interactions and interfacial interactions influence properties
– Surface induced ordering of block copolymers
– phase stability (change in Tc)
– Dynamics (Viscosity, chain diffusion)
– Glass transition temperature Tg
– Instabilities and pattern formation
OrderedDisordered
Topics of Interest: Self-Organization, Dynamics and Wetting
• Polymer-nanoparticle systems (bulk and thin film)
• Glass Transition temperature of thin films
• Chain dynamics and miscibility in confined geometries
• Instabilities in thin films (mixtures and homopolymers)
• Wetting and nano-scale organization of structured liquids
• Polymer thin film/CO2 systems (with Johnston group)
Polymer-based Nanocomposites
• Properties at the nanoscale are of broad interest, cross-cutting many disciplines… diverse technical issues (e- transport and single-molecule transistors to mechanical properties and automobile bumpers)
• Polymer-based nanocomposites: polymers+ nanoscale particles (fullerenes, layered silicates, nanoparticles, nanotubes)-new pathways to “tailor” properties of materials
20-50 nm
Thin film
Polymer coil Rg~2-20 nm
Self Organization of chains on a surface determined by film thickness, temperature, substrate topography
h1
h2h3
LEffects of temperature and film thickness
The Glass transition temperature of nanocomposite thin films
- Background: The glass transition temperature of polymer thin films
Influence of - i) single walled carbon nanotubes, - (ii) C60 fullerenes (“buckyballs”) and - (iii) mica-type layered silicate inorganic clays
on the Tg of thin polymer films in the nanometer thickness range
20-50 nm
Polymer coil Rg~2-20 nm
from mmptdpublic.jsc.nasa.gov/jscnano/
The Glass transition of Polymer thin film nanocomposites
• C60, and carbon nanotubes have a similar effect
85
90
95
100
105
110
115
120
125
0 50 100 150 200 250
h (nm)
PS
PS+1wt% layered silicate clay
PS+5 wt% layered silicate clay
3/1
1)(
h
aThT gg
PS: =9Nanocomposite: =4
Decrease in reflects the increase in fraction of the slowly relaxing domains
The effect of nanoparticles is to increase the effective fraction of slowly relaxing domains in the sample
37
36
35
34
Film
Thi
ckne
ss (
nm)
25020015010050
Temperature (o C)
Dynamic processes in confined environmentsNeutron scattering experiments
Relaxation processes affect scattering intensity as well as change d <u2>/dt
0
0.5
1
1.5
2
2.5
3
0 100 200 300 400 500 600
MS
D (
A2)
Temperature (K)
Phase Separation
Glass Transition
Temperature (K)
Red
uced
Int
ensi
ty
0.25
0.3
0.35
0.4
100 200 300 400 500
Dewetting of Thin Films
• Mechanisms (determined by the nature of the intermolecular interactions)
Nucleation: Heterogeneous and homogeneous
Spinodal Dewetting: Spontaneous amplification of capillary waves
Droplets
film
substrate
Misc. Info about the group
• Current Funding: National Science Foundation (DMR, STC), Robert A. Welch Foundation, Sematech
• Facilities used: Atomic force microscopy, spectroscopic ellipsometry, X-ray Scattering, TEM, neutron scattering, dynamic mechanical analysis, rheology
• Collaborations: Johnston, Ganesan, Sanchez, Yacaman
Loo, Bonnecaze, Korgel
• Distribution of Researchers during last 12 months: 9 PhD Students (2 co-advised), visiting scientist, undergraduates, shared post-doc (Johnston group)