Title: Physics of Degenerate Defect Modes in Photonic Crystal Bandgaps
1Physics of Degenerate Defect Modes in Photonic
Crystal Bandgaps
Sahand Mahmoodian1
Ross McPhedran1, Martijn de Sterke1, Kokou
Dossou2, Chris Poulton2, Lindsay Botten2 1 -
University of Sydney, 2 - University of
Technology Sydney
2Photonic Crystals
- Photonic Crystals (PCs) spatially periodic
refractive index - Man-made also exist in nature (butterflies,..)
- 1D, 2D and 3D PCs
2D
1D
3D
3Bandgaps
- Periodicity Bragg reflection
- Bragg reflection adds coherently at particular
frequencies. - Light cannot propagate in PC bandgap
4Photonic Crystal Devices
- Perturbations or defects in
- periodic lattice used for PC devices.
- Require good understanding of defects and their
modes
5Outline
- Overview of PC theory
- Defect Modes
- Degenerate Modes
- Coupling of Degenerate Modes
- Outlook and Conclusion
6(Photonic) Crystal Overview
- Periodicity ? Blochs Thm ? form of modes
Reciprocal Lattice
PC Lattice
Lattice Vectors R
Reciprocal Lattice Vectors G
Fourier
Transform
Brillouin Zone
7Bands and Brillouin Zone
- Non-redundant set of wave-vectors in First
Brillouin zone. - Bands and
- Bandgaps
- Irreducible Brillouin
- Zone (BZ) edge
Square Lattice Photonic Crystal
8Origin of Bandgaps
- Variational Theorem ? Modes maximize electric
energy (minimizing frequency) and are orthogonal
to lower modes.
9Defect Modes in Bandgaps
- Defect by changing index of single cylinder
- ve index change ? lower freq.
- -ve index change ? higher freq.
n1.8
Bandgap
10Degenerate Defect Modes
- X and Y points in BZ have degenerate
- Bloch modes.
- Defect modes also
- degenerate
- Modes have different symmetry
11Where now
- Looked at single defect
- Need understanding of multiple defects to
construct devices (eg. waveguide) - Use single defect info for multiple defects?
12Two Defects
- Coupling ? frequency split
Red points Two Defects four periods aparts
Blue line One Defect
13Tight-Binding Treatment of Defects
- Treat coupling using a tight-
- binding (supermodes) method
- Similar to coupled waveguides
14Tight Binding Photonic Crystals
- Two identical defects infinite PC
- Ez polarisation
- Supermode via Tight-Binding
Periodic Permittivity
Governs Single Isolated Defect
Change in permitivitty
Overall Frequency
Governs Both Defects
15Tight Binding
- Tight-binding ansatz in governing equation.
- Multiply by Ezi and integrate over space.
- K, J, I are overlap integrals, N is
normalisation.
16Tight-Binding Treatment
- Solutions of 4x4 matrices
- tend to be messy.
- But many elements vanish
- because
- Defects are arranged in symmetric fashion.
- No cross coupling.
Modes have different symmetry
17Tight Binding Treatment
- Solutions are now simple
- Fields are odd and even superpositions of
isolated modes with same symmetry.
18Tight-Binding Treatment
Red points Two Defects four periods aparts
Cyan Two Defects Tight Binding calculation
Blue line One Defect
19Symmetry
- Applies to defects on any symmetry plane
- Treatment extends to hexagonal lattices
20Conclusion
- Analysed coupling of degenerate defects.
- Degeneracy doesnt cause cross-coupling when
defects are positioned symmetrically - Treatment OK for both polarisations
- Symmetry arguments applies, provided defects
preserve symmetry of lattice.