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Layered media and photonic crystals Cord Arnold / Anne L’Huillier

Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

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Page 1: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

Layered media and photonic crystals

Cord Arnold / Anne L’Huillier

Page 2: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

A photonic crystal is a periodic arrangement

of a dielectric material that exhibits strong

interaction with light

Variation of refractive index on the scale of the wavelength λ

Photonic Crystals; J.D. Joannopoulos

Definition

Page 3: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

Artificial photonic crsytals

1D: Bragg Reflector

J. Serbin

LZH

2D: Si pillar crystal

3D: Colloidal crystal

3D: Wood pile

diameter of the rods 200 nm,

spacing in-between 250 nm

Page 4: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

Natural Examples

Natural opalsNatural opals

http://www.viewsfromscience.com/documents/webpages/natural_photonics_p1.html

Page 5: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

Multilayer Optics

Page 6: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

How to analyze a multilayer system

Scattering MatrixWave-Transfer Matrix

Si � Mi MΣ � S Σ

Analysis of multilayer optical system

Conversion

Page 7: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

Cascaded system - Airy formulas

Page 8: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

Examples: Homogeneous medium

Page 9: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

Examples: Partially reflective mirror (beamsplitter)

Page 10: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

Examples: Single dielectric boundary

Page 11: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

Off-axis waves in layered media

• Reflections become angle-dependent

• Reflections become polarisation dependent

• The phase is obtained from a projection on the optical axis

• The angle is different in different refractive index media

Page 12: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

Off Axis Waves in Layered Media

Single boundary

Page 13: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

Fabry-Perot Etalon (Mirror)

Free spectral range

Page 14: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

Dielectric Slab as a Fabry-Perot Etalon

Page 15: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

Off-Axis Transmittance of FPE

Page 16: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

Bragg grating

Page 17: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

Dielectric Bragg grating

( ) πϕϕ mdndnk =+=+ 2211021

Condition

The accumulated phase shift must add to π, λ/2

Page 18: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

Off-axis high-reflection mirrors

Page 19: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

Examples for 1-dimensional multilayer structures

Dielectric multi-layer mirror:

- Alternating stack of high and low refractive index materials (n1>n2) with

optical thickness of lambda/4 in each layer.

- Reflectivity >99.999% for narrow bands, >99% for very broad bands

Typical coating materials:

- Magnesium fluoride n~1.3

- Silicone dioxide n~1.45

- Tantalum pentoxide n~2

- Zinc sulfide n~2.3

- Titanium dioxide n~2.4

Image source: Wikipedia

n1 n2

Page 20: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

Examples for 1-dimensional multilayer structures

Chirped dielectric mirror:

- The layer thickness changes as function of depth into the mirror. Blue

wave lengths are reflected at the surface, red in the depth.

- Chirped mirrors are used to cancel dispersion in ultrashort pulse

oscillators.

- They form the basis of today’s femtosecond laser technology.

- Reflectivity >99% for 500-1000nm.

Page 21: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

Examples for 1-dimensional multilayer structures

Fiber Bragg grating (FBG):

- Wavelength filtering and multiplexing

- Single frequency fiber lasers

- Stretching, compression, dispersion compensation with chirped FBGs

- Sensing, e.g. temperature and pressure

Image source: Wikipedia

Page 22: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

A short introduction into photonic crystals

Page 23: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

Dispersion relation K(ω) and wave localization for a 1d photonic

crystal made from alternating dielectric layers

Page 24: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

Dispersion relation K(ω) for a 1d photonic crystal made from

alternating dielectric layers

Page 25: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

Phase and group velocity

eff

pn

cv 0=Phase velocity

Group velocity

eff

gN

cv 0=

Slo

w r

egio

n

Page 26: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

Photonic band gaps at off-axis propagation

Internal off-axis waves External off-axis propagation coupled into

the structure

Page 27: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

Two-dimensional photonic crystals

Rectangular lattice

Triangular lattice

Page 28: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

Photonic Crystal in Two Dimensions

Band Gap for TM modes

Page 29: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

2D PhC, Complete (!) 2D Band Gap

Triangular lattice of holes! , a , r ~λ

Page 30: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

3D Photonic Crystals: Yablonovite

Historically 1st 3D Band

Gap Crystal

Page 31: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

3D PhC Woodpile structure

Page 32: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

Defect modes

Page 33: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

Defect modes

By introducing a “defect” in the

highly periodic environment as

for example removing one rod

or simply changing the radius

of one or a few roods, the

periodicity is broken and

“defect modes” can exist in the

forbidden gap!

This e.g. allows for laser

cavities with dimensions of the

order of one wave length!

Page 34: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

Bending light in 2D PhC

Page 35: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

PhC Add-Drop Splitter

λ1 >λ2 >λ3 λ1 >λ3

λ2

NB: Add-drop filter with wavelength selectivity of ca 1% having dimensions of ca.

one wavelength

Page 36: Layered media and photonic crystals - Atomic Physics · Off-axis waves in layered media • Reflections become angle-dependent • Reflections become polarisation dependent • The

End Of Lecture