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Education
Ph.D.,
Materials Science, Massachusetts Institute of Technology, 1996
B. S. , Mechanical Engineering, University of California, Santa
Barbara, 1990
Dr.
Foulger graduate work was performed under the guidance of Prof.
Gregory Rutledge and explored the structural characteristics
of the disordered state of liquid crystalline polymers through
molecular simulation. Prior to joining the faculty of Clemson
University, he served as a polymer scientist in the Division
of Research, Development & Engineering of the Italian company
Pirelli Tyres / Cables & Systems.
Research
Materials
science researchers have been striving over the last decade
to develop a full repertoire of dielectric, semiconductor, and
metallic nanomaterials and characterize their size dependent
electronic and optical properties. These particles are of interest
not only because they can be used to make very small structures,
but also because the commonly understood properties of ordinary
bulk materials are dramatically different at the nano-length
scale. Transitioning this knowledge from the realm of basic
science into a technology that can be exploited in the development
of novel optical & electronic devices will require a multidisciplinary
approach. To this end, our group is composed of people with
backgrounds spanning the scientific and engineering disciplines.
Self-assembly.

Since
the original proposal that three dimensional periodic dielectric
structures could exhibit a photonic bandgap (PBG), considerable
attention has been focused on developing these materials into
a form which is suitable for use in photonic applications. Unfortunately,
the general exploitation of visible photonic crystals as devices
has been hindered by the difficulties in creating 3D periodic
dielectric structures with a feature size comparable to the
wavelength of visible light, as well as achieving dielectric
contrasts that result in a forbidden gap that overlaps in all
directions within the Brillouin zone. Though a number of groups
have made progress applying conventional microlithographic techniques
to this end, this objective remains a challenge employing these
techniques. Focus has now turned to systems which undergo self
organization at a nanometer length scale, such as colloidal
crystals.
Two
self-assembly approaches to generating photonic crystals have
emerged. One approach involves the assembly of nanoparticles
into close-packed arrays through sedimentation and typically
relies on non-specific particle-particle repulsion to induce
order. Particle assembly via this method is attractive in terms
of both simplicity and versatility. Because close packed order
typically involves concentrating particles into a confined space,
these studies often involve hard spheres (e.g., ceramic, metal,
dense polymer) that undergo little deformation upon packing.
The second approach involves the longer range electrostatic
repulsive interactions of suspended colloidal spheres bearing
a high surface charge and arranged in ordered arrays.
Our
group has focused on crystalline colloidal arrays. A crystalline
colloidal array is a three dimensionally ordered lattice of
self-assembled monodisperse colloidal particles, most commonly
amorphous silica or a polymer latex, dispersed in aqueous or
non-aqueous media. At high particle concentrations, long-range
electrostatic interactions between particles result in a significant
inter-particle repulsion which yields the adoption of a minimum
energy colloidal crystal structure with either BCC or FCC symmetry.
The ordering of the particles in the media results in spatial
periodicities that range from ca. 100-1000 nm, often resulting
in optical bandgap effects.
Unfortunately,
the low elastic modulus exhibited by a liquid dispersion results
in weak shear, gravitational, electric field, or thermal forces
having the propensity to disturb the crystalline order and is
a severe drawback to the practical application of these arrays
in photonic devices. Our group has devised ways to encapsulate
the ordered arrays in water-free, robust matrixes, resulting
in PBG composites. The devised route to encapsulation offers
the material designer the ability to tune the glass transition
of the composite through a judicious choice in the encapsulation
monomer(s) and allows for a wide range of coupled optical and
mechanical properties, such as the variation of the stop band
with stress (i.e., mechanochromic response).
Nanoparticle Synthesis

Photonic
crystals are usually fabricated from dielectric materials with
relatively frequency independent refractive indexes, though
a number of experiments and theoretical calculations have demonstrated
that materials with significant index contrast and frequency
dependent refractive indexes can be used to construct PBG composite
materials with unique features, and possibly with a complete
photonic bandgap. To increase the refractive index contrast
between spheres and matrix, as well introduce optical nonlinearities
into the crystals, a number of approaches are being pursued
in the group, such as the synthesis of metal & synthetic
metal particles, as well combining different materials in a
core-shell topology.

The
exploitation of a core-shell topology results in the appearance
of particles that exhibit new properties. Our group is active
in developing ways to combine dissimilar materials in one particle
to enhance the physical or optical performance of a self-assembled
structure composed of the core-shell particles. Examples (highlighted
in the previous figure) include the synthesis of monodisperse
polystyrene particles coated with the intrinsically conducting
polymer (ICP) poly(3,4-ethylenedioxythiophene) (PEDOT) .
An
Eye towards the device

A
main point of concentration in our group is on formulating approaches
to fabricating device-ready PBG composites for direct integration
with opto-electronic components. Our emphasis on the integration
of nanoscale materials with established device fabrication routes
is an effort to establish the scientific principles that govern
the design, performance, and integration of these materials
into optical and sensory components. One technique exploited
within the group is soft lithography, a technique developed
by George Whitesides of Harvard University to allow for the
rapid prototyping of microfluidic devices. The previous figure
presents the optical characteristics at various viewing angles
of a polymerized crystalline colloidal array templated via soft
lithography into a Clemson University tiger paw ensignia: a.
blue photonic crystal at ca. 20° viewing angle; b. green
photonic crystal at ca. 15° viewing angle; c. green-red
photonic crystal at ca. 10° viewing angle; and d. red photonic
crystal at ca. 0° viewing angle.
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Recent
Publications and Awards
1.H.
Bao, G. Chumanov, R. Czerw, D. L. Carroll, and S. H. Foulger,
“Synthesis of Core-Shell Silver Colloidal Particles by
Surface Immobilization of an Azo-Initiator”, Colloid &
Polymer Science, in press (2005).
2.
P. Jiang, J. Ballato, D. W. Smith, and S. H. Foulger, “Multicolor
Pattern Generation in Photonic Bandgap Composites”, Advanced
Materials, 17, 179 (2005). (Note: image featured on the cover)
3.
J. Ballato, S. H. Foulger, and D. W. Smith, “Optical properties
of perfluorocyclobutyl polymers. II. Theoretical and Experimental
Attenuation”, Journal of the Optical Society of America
B-Optical Physics, 21, 958 (2004).
4.
M. Han and S. H. Foulger, “Preparation of poly(3,4-ethylenedioxythiophene)
(PEDOT) coated silica core-shell particles and PEDOT hollow
particles”, Chemical Communications, 19, 2154 (2004).
5.
M. Han and S. H. Foulger, “Crystalline Colloidal Arrays
Composed of Poly(3,4-ethylenedioxythiophene) Coated Polystyrene
Particles with a Stop Band in the Visible Regime”, Advanced
Materials, 16, 231 (2004).
6.
S. Chen, Z. L. Wang, J. Ballato, S. H. Foulger, and D. L. Carroll,
“Monopod, Bipod, Tripod, Tetrapod Gold Nanocrystals”,
Journal of the American Chemical Society, 10, 1021 (2003).
7.
J. Ballato, S. H. Foulger, and D. W. Smith, “Optical Properties
of Perfluorocyclobutyl Polymers”, Journal of the Optical
Society of America B-Optical Physics, 20, 1838 (2003).
8.
M. W. Perpall K. P. U. Perera J. DiMaio, J. Ballato, S. H. Foulger,
and D. W. Smith, “Novel Network Polymer for Templated
Carbon Photonic Crystal Structures”, Langmuir, 19, 7153
(2003).
9.
Z. Xu, Z. Wang, M. E. Sullivan, D. J. Brady, S. H. Foulger,
A. Adibi, “Multimodal Multiplex Spectroscopy Using Photonic
Crystals” Optics Express, 11 2126 (2003).
10.
S. H. Foulger, P. Jiang, A. Lattam, J. Ballato, D. W. Smith,
Jr. D. Dausch, S. Grego, and B. Stoner, “Photonic Bandgap
Composites with Reversible High-Frequency Stop Band Shifts,”
Advanced Materials, 15, 685 (2003).
11.
D. W. Smith, Jr., S. Chen, S. Kumar, J. Ballato, C. Topping,
and S. H. Foulger, “Pefluorocyclobutyl (PFCB) Copolymers
for Microphotonics,” Advanced Materials, 14, 1585 (2002).
12.
H. Zengin, W. S. Zhou, J. Y. Jin, R. Czerw, D. W. Smith, L.
Echegoyen, D. L. Carroll, S. H. Foulger, and J. Ballato, “Carbon
Nanotube Doped Polyaniline”, Advanced Materials, 14, 1480
(2002).
13.
K. Perera, H. V. Shah, S. H. Foulger, and D. W. Smith, Jr.,
“Substituent Effects on Bergman Cyclopolymerization Kinetics
of Bis-Ortho-Diynylarene (BODA) Monomers by Dynamic Scanning
Calorimetry”, Thermochima Acta 1-2, 371-375 (2002).
14.
S. H. Foulger, P. Jiang, Y. Ying, A. Lattam, J. Ballato, and
D. W. Smith, Jr., “Photonic Bandgap Composites,”
Advanced Materials, 13, 1898-1901 (2001).
15.
S. H. Foulger, A. Lattam, P. Jiang, D. W. Smith, Jr., and J.
Ballato, “Optical and Mechanical Properties of Poly(ethylene
glycol) Methacrylate Hydrogel Encapsulated Crystalline Colloidal
Arrays,” Langmuir 17, 6023-6026 (2001).
National Science
Foundation CAREER Award - MPS/DMR, Clemson University Award
for Faculty Achievement in the Sciences, Clemson University
Board of Trustees Faculty Excellence Award, National Textile
Center Scientific Excellence Award, 3M Corporation Pre-tenured
Faculty Award.
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