Title: Photonic Crystal and its Application: A Basic Understanding
1Photonic Crystal and its Application A Basic
Understanding
- Cheung Chi Shing Stephen
- Lai Ho Fung
2Photonic Crystal Some History
- 1887 Lord Rayleighs study of Bragg Diffraction
of 1-D PC - - propose of 1-D photonic bandgap(stop band)
3Photonic Crystal Some History
- At 1987(100 years later!!!)
- -Eli Yablonovitch
- control of spontaneous emission of materials
in PC - -Sajeev John
- defected high-D PC give rise to strong
localization of light
4Some daily examples - Butterflies
5Some daily examples shells
6Some daily examples
- A scan by SEM of the butterfly wing (blue)
7Photonic Crystals Definition
- Periodic structures with alternating refractive
index (dielectric constant)
8Photonic Crystals Definition
- 1-D multi-layer membrane
- 2-D air columns in dielectric material
- 3-D stacking structure
9Photonic Crystals Definition
- Crucial property
- Photonic bandgap-
- Range of lights frequencies which the light
cannot pass throught PCWHY? - because
- BRAGG DIFFRACTION!
10Photonic Crystals Definition
Constructive interference 2d sin? n?. ( O(d)
O(?) )
11Photonic Crystals Definition
- eGaAs 13, eGaAlAs12, eAir1
- ??e?, range of photonic bandgap ?
12Computational method
- So, how do we know the PBG of a certain PC?
- EM waves travelling in PC are described by
Maxwell Eqs. -
13Computational method
- 1. Plane-wave expansion method
- Assume plane wave solutions, i.e.,
-
14Computational method
- The two curl equation can be rewritten as
15Computational method
- Where the first one is just like a
- Schrödinger equation with
- being the operator
- (?(k)/c)2 being the corresponding
eigenvalue
16Computational method
- Hence given the boundary conditioins, i.e., the
structure of the PC and e(r), H(r) and E(r) can
be found - Hk(r) ei(k.r) uk(r)
17Computational method
- An analogy to electronic bandgap in semiconductor
18Computational method
- 2. FDTD (Finite-difference time domain) method
- Consider again the two curl equations
19Computational method
- They can be expanded into
20Computational method
An electromagnetic wave interaction structure is
mapped into the space lattice by assigning
appropriate values of permittivity to each
electric field component, and permeability to
each magnetic field component.
21Physical Phenomena
- 1. Photonic bandgap(PBG)
- Bragg diffraction -gt destructive interference in
PC -gt Photonic badgap - 1-D PC only in one direction
- Because periodicity becomes different if the
wave enters in a different direction
22Physical Phenomena
- 2-D PC 2-D PBG
- 3-D PC possibility of PBG in all direction
23Physical Phenomena
- 2. Strong localization of light
- If defects are introduced to the PC, light can
be trapped within the defect.
24Physical Phenomena
25Physical Phenomena
26 Applications
- Photonic crystal fiber ( PCF )
- Laser
- Future development
27 Photonic crystal fiber ( PCF )
- Benefits
- high transmission speed
- not much interaction between photons
- ? low energy loss
28 Photonic crystal fiber ( PCF )
29 Photonic crystal fiber ( PCF )
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31 Photonic crystal fiber ( PCF )
- Range of wavelength 440nm 2000nm
- Best reported loss
-
- 13dB/km over 100m _at_1.5µm
- wavelength
32Photonic crystal fiber ( PCF )
- Holey-assisted fiber
- Holey cladding
- (low refractive index)
- Core (high refractive
index)
33Photonic crystal fiber ( PCF )
- As the refractive index of the central defect
core is relative higher than the holey cladding
materials - ? wave is rather confined and transmits in the
core
34Photonic crystal fiber ( PCF )
- Group dispersion is reduced to minimium
- Core area is 10 times greater than that of optic
fiber - Single mode maintains within a large range of
wavelength
35Laser
- Pumping / Exciting
- Population inversion
- Spontaneous
Stimulated - emission
emission - Energy loss
Resonator
36Laser
- Probability of an atom in excited state is given
by
37Laser
- One may think increasing the temperature can
increase the population of excited atoms -
- ? Blackbody radiation
38Laser
39Laser
- However, blackbody radiation cannot produce
intensive and monochromatic radiation - One may try to reduce energy loss by using
Photonic crystal as the resonator shielder
40Laser
- Relation between photonic band gap and
semiconductor laser
41Laser
42Laser
- Spontaneous emission of excited electrons are
inhibited - Probability of electrons maintaining in the
excited states ? - Population inversion of laser ?
- Simulated emission ?
- Power loss ?
43Future development
- Size in micro- order devices
- Largely reduce the size of communication system
to 1000 times
44Photonic crystal and its applications