high refractive index polythiophene for 3-d photonic crystals with complete band gaps shi jin, matt...
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High Refractive Index Polythiophene for 3-D High Refractive Index Polythiophene for 3-D Photonic Crystals with Complete Band GapsPhotonic Crystals with Complete Band Gaps
Shi Jin, Matt Graham, Frank W. Harris
and Stephen Z. D. Cheng
Maurice Morton Institute and Department of Polymer Science The University of Akron
Timothy J. Bunning, Richard A. Vaia and Barry L. Farmer
AFRL Materials and Manufacturing Directorate
Collaborative Center in Polymer Photonics between AFRL Collaborative Center in Polymer Photonics between AFRL Materials and Manufacturing Directorate Materials and Manufacturing Directorate
and The University of Akronand The University of Akron
Polymer Photonics WorkshopPolymer Photonics Workshop
Photonics, Photonic Crystal and Photonics, Photonic Crystal and Photonic Band GapPhotonic Band Gap
• Photonics: “The technology of generating and harnessing light and other forms of radiant energy whose quantum unit is the photon.”1
• Photonic Crystals: (photonic band gap materials), are materials with periodic variation of refractive index. A photonic crystal can control the flow of electromagnetic waves, if its periodicity is comparable to their wavelengths.
• Photonic band gap: a frequency band in which electromagnetic waves are forbidden.
1. Photonic Dictionary at www.photonics.com
Applications of PhotonicsApplications of Photonics
Fiber optics
Optical switches
Light emitting diodes
PhotovoltaicsOptical amplifiers
Applications of Photonic CrystalsApplications of Photonic Crystals
Waveguides
Thresholdless Lasers
Photonic Computers
Signal Filters
Loss-less Mirrors
Dimensionality of Photonic CrystalsDimensionality of Photonic Crystals
Periodic in one dimension
Periodic in two dimensions
Periodic in three dimensions
Joannopoulos, D. D. et al. Photonic Crystals, Princeton University, 1995.
Different colors represent different refractive indices.How does the degree of refractive index variation affect the property of a photonic crystal?
2
2
1
2
2
1
2
1
1
N
N
nnnn
R
R: peak reflectivity in the band gapN: multilayer number: wavelength in the center of
photonic band gap: bandwidth of band gap
ni, ti are refractive indices and thicknesses of corresponding layers.
Assuming n1 > n2 and n1t1 = n2t2 = /4:
21
211
/1
/1sin
4
nn
nn
n1/n2 (refractive index contrast) is important for both R and !
n1
n2
One-dimensional Photonic Band Gap-One-dimensional Photonic Band Gap-Layered Dielectric StructureLayered Dielectric Structure
Yeh, P. Optical Waves in Layered Media, John Wiley & Sons: New York, 1988.
3D Complete Photonic Band Gap3D Complete Photonic Band Gap
• Complete photonic band gap: a frequency band in which electromagnetic waves propagation is forbidden along all directions.
• Complete photonic band gaps can only be opened up under favorable circumstances: – Right structures– Sufficient (threshold) refractive index
contrast
Yablonovitch, E. J. Phys.: Condens. Matter 1993, 5, 2443.
Threshold RI Contrasts for Complete Band Threshold RI Contrasts for Complete Band Gaps in 3-D Photonic CrystalsGaps in 3-D Photonic Crystals
Diamond:1.87
Single Gyroid: 2.28
HCP: 3.10
Inversed Opal: 2.80
Inversed Square Spiral: 2.20
• 3-D photonic crystals with complete band gaps were fabricated using Ge, Si (inversed opal).
• These inorganic materials are brittle and difficult to process.
• Polymers are desired for better physical properties.• Inorganic nano-particles were incorporated to improve
refractive indices of polymers • Can we have polymers with high refractive indices?
Refractive Indices of MaterialsRefractive Indices of Materials
Ge (633 nm) 5.5
Si (633 nm) 3.8
Air 1
Polysulfone (589 nm) 1.63
Polystyrene (589 nm) 1.59
Polypropylene (589 nm) 1.51
Refractive Index and Molecular StructureRefractive Index and Molecular Structure
n – Refractive IndexNA – Avogadro’s constantMw – Molar weight – Density – Molecular polarizability
w
A
MN
n
34
1
322
• Higher higher n• Higher higher n• What kinds of polymers are expected to show high
values?
Yang; C., Jenekhe, S. Chem. Mater. 1995, 7, 1276
Conjugated Polymers: Conjugated Polymers: A Source of Achieving Higher RI ContrastA Source of Achieving Higher RI Contrast
Conjugated polymers possess higher polarizability than classical polymers, thus higher refractive indices are expected.• They are often referred to as conducting polymers.• Most of them are semiconductors in pristine state.• They become conducting upon doping (partial
oxidation/reduction).• Higher conductivity better conjugation higher RI• Unsubstituted conjugated polymers are preferred over
their functionalized analogues.
n
polyacetylene(PA)
S
S
n
polythiophene(PT)
n
polyphenylenevinylene(PPV)
Predicted Refractive Indices of Predicted Refractive Indices of Conjugated PolymersConjugated Polymers
Polymer n700nm n1064nm n2500nm
trans-PA 2.47 2.44
PPV 2.28 2.04 1.95
PT 3.90 3.04 2.77
According to calculation, polythiophene has the refractive index comparable to inorganic materials!
Predicted Refractive Indices
Yang; C., Jenekhe, S. Chem. Mater. 1995, 7, 1276
Refractive Indices: Refractive Indices: Calculations versus ExperimentsCalculations versus Experiments
Polymer npred. nexp.
trans-PA 2.442.5 m 2.331
PPV 2.28700 nm 2.09633 nm2
PT* 3.9700 nm 1.4633 nm3
However, 6T shows n633nm = 2.154!What are the problems with electrochemically synthesized polythiophene films?
*Electrochemically synthesized1. Yang; C., Jenekhe, S. Chem. Mater. 1995, 7, 12762. Burzynski, R.; Prasad, P. N.; Karasz, F. E. Polymer 1990, 31, 6273. Hamnett, A.; Hillman, A. R. J. Electrochem. Soc. 1988, 135, 25174. Yassae, A. et al. J. Appl. Phys. 1992, 72, 15
Why Electrochemical Synthesis?Why Electrochemical Synthesis?
• Unsubstituted polythiophene is preferred for maximizing refractive index.
• Most of other methods only can produce polythiophene powders.
• Advantages of electrochemical synthesis:
• Direct grafting of the doped conducting polymer films onto the electrode surface
• Easy control of the film thickness by the deposition charge
Polythiophene ParadoxPolythiophene Paradox
• Electro-polymerization must begin with the electro-oxidation of thiophene monomers;
• The electro-oxidation of thiophene occurs at potentials higher than 1.6 V vs. SCE in conventional solvents;
• Over-oxidation of formed polythiophene occurs at potentials above 1.4 V vs. SCE;
• Polythiophene degrades at potentials that are required to synthesize it, a paradox.
• Conjugation is rather limited in polythiophene films electro-synthesized in conventional solvents. Refractive indices are thus low.
Roncali, J. Chem. Rev. 1992, 92, 711
Lewis Acid-assisted Lewis Acid-assisted Low-potential PolymerizationLow-potential Polymerization
Ct = 0.1 mole/L
The oxidation potential of thiophene was lowered to 1.3 V, degradation of polymer can be avoided!
BF3•Et2O
CH3CN
3 mole/L AlCl3/CH3CN
Borontrifluoridediethyl ether
Proton-free Low-potential Proton-free Low-potential Polymerization of ThiophenePolymerization of Thiophene
• Elimination of protons– Protons have a negative impact to the structural
integrity. – Lewis acid is needed to avoid degradation of formed
polymers.– A proton scavenger that exclusively reacts with
protons could solve the problem.
N
2,6-di-tert-butylpyridine (DTBP)
Spectroscopic Characterization of Spectroscopic Characterization of Polythiophene FilmsPolythiophene Films
With DTBP
Without DTBP
Amount of saturated units was greatly reduced.
Red-shift of max indicates a more extended conjugated structure.
10 15 20 25 30 35
with DTBP without DTBP
2 (°)
Wide-angle X-ray Scattering of Wide-angle X-ray Scattering of Polythiophene FilmsPolythiophene Films
S
S
S
S
S
S
S
S
S
S
S
S
0.5 nm
0.35 nm
0.5 nm
0.35 nm
Packing was improved with introducing proton scavenger.
=1.512 g cm-3
=1.495 g cm-3
• Conductivity: up to 1300 S cm-1
– Comparable to regio-regular poly(3-alkyl-thiophenes)– Compare with ~100 S cm-1 without DTBP– High refractive indices are expected.
• Mechanical properties– Tensile strength: ~135 MPa– Tensile modulus: 4 GPa– Elongation at break: 4%
Electric and Mechanical PropertiesElectric and Mechanical Properties
Refractive Index Dispersion of a Highly Refractive Index Dispersion of a Highly Conjugated Polythiophene FilmConjugated Polythiophene Film
Courtesy of AFRL Materials and Manufacturing Directorate
Threshold RI Contrasts for Complete Threshold RI Contrasts for Complete Band Gaps in 3-D Photonic CrystalsBand Gaps in 3-D Photonic Crystals
Diamond:1.87
Single Gyroid: 2.28
HCP: 3.10
Inversed Opal: (FCC) 2.80
Inversed Square Spiral: 2.20
Electrochemical Fabrication of a PT Electrochemical Fabrication of a PT Inversed Opal Photonic CrystalInversed Opal Photonic Crystal
Addition of monomer
Electro-synthesis of polythiophene
Removal of colloid spheres
FCC single crystal Partial fusion of colloids
Dedoping of polythiophene
n1 = 2.9 n2 = 1
FCC and HCPFCC and HCP
Volume fraction = 0.7405Coordination # = 12Sequence = ABCABC
Volume fraction = 0.7405Coordination # = 12Sequence = ABAB
FCC HCPG = 0.005kBT per particle
Bolhuis, P. B.; Frenkel, D.; Mau, S. and Huse, D. Nature 1997, 388, 235
FCC is more stable than HCP with a very small energy difference.
Colloid CrystallizationColloid Crystallization
50 m
Polystyrene colloid, d = 269 nm
FCC:refl. 640 nm
HCP:refl. 600 nm
HCP
FCC
Mechanical AnnealingMechanical Annealing
Colloid crystal
Piezoelectric element
Oscillator
Phase Flipping Phase Flipping with Mechanical Annealingwith Mechanical Annealing
HCP FCC conversion was achieved by mechanical annealing.
50 m50 m
Phase Structure of an Inversed Opal Phase Structure of an Inversed Opal Photonic CrystalPhotonic Crystal
SummarySummary
• Oxidation potential of thiophene monomer was lowered by a Lewis acid system so that degradation of the polymer is avoided.
• Acid-initiated addition polymerization was suppressed by introducing a proton trap.
• Highly conjugated polythiophene films were obtained with the refractive index comparable to dielectric inorganics.
• HCP FCC conversion was successfully carried out via mechanical annealing.