Presentation is loading. Please wait.

Presentation is loading. Please wait.

High Refractive Index Polythiophene for 3-D Photonic Crystals with Complete Band Gaps Shi Jin, Matt Graham, Frank W. Harris and Stephen Z. D. Cheng Maurice.

Similar presentations


Presentation on theme: "High Refractive Index Polythiophene for 3-D Photonic Crystals with Complete Band Gaps Shi Jin, Matt Graham, Frank W. Harris and Stephen Z. D. Cheng Maurice."— Presentation transcript:

1 High Refractive Index Polythiophene for 3-D Photonic 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 Materials and Manufacturing Directorate and The University of Akron Polymer Photonics Workshop

2 Photonics, Photonic Crystal and Photonic 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

3 Applications of Photonics Fiber optics Optical switches Light emitting diodes Photovoltaics Optical amplifiers

4 Applications of Photonic Crystals Waveguides Thresholdless Lasers Photonic Computers Signal Filters Loss-less Mirrors

5 Dimensionality of Photonic Crystals Periodic in one dimension Periodic in two dimensions Periodic in three dimensions Joannopoulos, D. D. et al. Photonic Crystals, Princeton University, Different colors represent different refractive indices. How does the degree of refractive index variation affect the property of a photonic crystal?

6 R: peak reflectivity in the band gap N: multilayer number : wavelength in the center of photonic band gap  :bandwidth of band gap n i, t i are refractive indices and thicknesses of corresponding layers. Assuming n 1 > n 2 and n 1 t 1 = n 2 t 2 = /4: n 1 /n 2 (refractive index contrast) is important for both R and  ! n1n1 n2n2 One-dimensional Photonic Band Gap- Layered Dielectric Structure Yeh, P. Optical Waves in Layered Media, John Wiley & Sons: New York, 1988.

7 3D 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.

8 Threshold RI Contrasts for Complete Band Gaps in 3-D Photonic Crystals Diamond: 1.87 Single Gyroid: 2.28 HCP: 3.10 Inversed Opal: 2.80 Inversed Square Spiral: 2.20

9 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 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

10 Refractive Index and Molecular Structure n – Refractive Index N A – Avogadro’s constant M w – Molar weight  – Density  – Molecular polarizability 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

11 Conjugated Polymers: A 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. polyacetylene (PA) polythiophene (PT) polyphenylenevinylene (PPV)

12 Predicted Refractive Indices of Conjugated Polymers Polymern 700nm n 1064nm n 2500nm trans-PA PPV PT According to calculation, polythiophene has the refractive index comparable to inorganic materials! Predicted Refractive Indices Yang; C., Jenekhe, S. Chem. Mater. 1995, 7, 1276

13 Refractive Indices: Calculations versus Experiments Polymern pred. n exp. trans-PA  m 2.33  1 PPV nm nm 2 PT* nm nm 3 However, 6T shows n 633nm = ! What are the problems with electrochemically synthesized polythiophene films? *Electrochemically synthesized 1.Yang; C., Jenekhe, S. Chem. Mater. 1995, 7, Burzynski, R.; Prasad, P. N.; Karasz, F. E. Polymer 1990, 31, Hamnett, A.; Hillman, A. R. J. Electrochem. Soc. 1988, 135, Yassae, A. et al. J. Appl. Phys. 1992, 72, 15

14 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

15 Polythiophene 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

16 Lewis Acid-assisted Low-potential Polymerization C t = 0.1 mole/L The oxidation potential of thiophene was lowered to  1.3 V, degradation of polymer can be avoided! BF 3Et 2 O CH 3 CN 3 mole/L AlCl 3 /CH 3 CN Borontrifluoride diethyl ether

17 Proton-free Low-potential Polymerization 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. 2,6-di-tert-butylpyridine (DTBP)

18 Spectroscopic Characterization of Polythiophene Films With DTBP Without DTBP Amount of saturated units was greatly reduced. Red-shift of max indicates a more extended conjugated structure.

19 Wide-angle X-ray Scattering of Polythiophene 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

20 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 Properties

21 Refractive Index Dispersion of a Highly Conjugated Polythiophene Film Courtesy of AFRL Materials and Manufacturing Directorate

22 Threshold RI Contrasts for Complete Band 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

23 Electrochemical Fabrication of a PT Inversed Opal Photonic Crystal Addition of monomer Electro-synthesis of polythiophene Removal of colloid spheres FCC single crystal Partial fusion of colloids Dedoping of polythiophene n 1 = 2.9 n 2 = 1

24 FCC and HCP Volume fraction = Coordination # = 12 Sequence = ABCABC Volume fraction = Coordination # = 12 Sequence = ABAB FCCHCP  G = 0.005k B T 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.

25 Colloid Crystallization 50  m Polystyrene colloid, d = 269 nm FCC: refl.  640 nm HCP: refl.  600 nm HCP FCC

26 Mechanical Annealing Colloid crystal Piezoelectric element Oscillator

27 Phase Flipping with Mechanical Annealing HCP  FCC conversion was achieved by mechanical annealing. 50  m

28 Phase Structure of an Inversed Opal Photonic Crystal

29 Summary 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.


Download ppt "High Refractive Index Polythiophene for 3-D Photonic Crystals with Complete Band Gaps Shi Jin, Matt Graham, Frank W. Harris and Stephen Z. D. Cheng Maurice."

Similar presentations


Ads by Google