aos metamaterial 29-10-2010 weeklyseminar

31
Photonics in Engineering GROUP Metamaterials Aos Al-waidh Photonics in Engineering Research Group General Engineering Research Institute Liverpool John Moores University E-mail: [email protected]

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Page 1: Aos Metamaterial 29-10-2010 WeeklySeminar

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Metamaterials

Aos Al-waidh

Photonics in Engineering Research Group

General Engineering Research Institute

Liverpool John Moores University

E-mail: [email protected]

Page 2: Aos Metamaterial 29-10-2010 WeeklySeminar

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Outlines• Introduction to metamaterials

• Classification of materials

• Photonic Crystal

• Realisation of Metamaterials

• Unit Cell Size

• Metamaterial Application

• Cloaking

• Conclusions

Page 3: Aos Metamaterial 29-10-2010 WeeklySeminar

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Introduction To Metamaterials

Metamaterials are periodic or quasi-periodic, sub-wavelength metal structures. The electro-magnetic material properties are derived from its structure rather than inheriting them directly from its material composition.

Based on definition of J.Pendry 2000

empty glass

regular water, n = 1.3

“negative” water, n = -1.3

Page 4: Aos Metamaterial 29-10-2010 WeeklySeminar

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GROUP Positive refraction index Negative refraction index

Introduction To Metamaterials

This term is particularly used when the resulting material has properties that are not found in naturally formed substances as indicated by the prefix “meta”.

Page 5: Aos Metamaterial 29-10-2010 WeeklySeminar

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1

2

ENERGY

PHASEVELOCITY

Air

Materiallike glass

Metamaterial

Yes as a backward wave

Page 6: Aos Metamaterial 29-10-2010 WeeklySeminar

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μ

ε

PropagatingStandard optical

materialsEvanescent

Metals (UV – Optical)

EvanescentNatural magnetic

materials (up to GHz)

PropagatingMetamaterials

(−, +) (+, +)

(−, −) (+, −)

OR

Negative Phase

PositivePhase

Backward Waves

ForwardWaves

n n

1

1

n<1

Classification of materials

Page 7: Aos Metamaterial 29-10-2010 WeeklySeminar

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μ

ε

Classification of materials

(DNG) ε < 0, μ < 0Not found in nature

(MNG) ε > 0, μ < 0Gyrotropic

(DPS) Dielectrics

(ENG) ε < 0, μ > 0Plasma

ABSORPTION

ABSORPTION

POSITIVE REFRACTION

NEGATIVE REFRACTION!!

( )( )n

Page 8: Aos Metamaterial 29-10-2010 WeeklySeminar

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DPSENGMNG

Classification of materials

DNG

Cloak

Page 9: Aos Metamaterial 29-10-2010 WeeklySeminar

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Realisation of Metamaterials

Negative ε• Thin metallic wires are arranged periodically• Effective permittivity takes negative values below plasma

frequencyNegative μ• An array of split-ring resonators (SRRs) are arranged

periodically

Page 10: Aos Metamaterial 29-10-2010 WeeklySeminar

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EyHx

ISRR

IROD

y x

z

Magnetic resonance

(Negative μ)

Electric resonance

(Negative ε)

Realisation of MetamaterialsEmbedding a metal split-ring and a metal rod creates left-handedness

Page 11: Aos Metamaterial 29-10-2010 WeeklySeminar

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• Another example of composite material with negative refraction index is the photonic crystal:

• Photonic crystals may behave as if they possess a negative refractive effect without actually having a negative refractive index. Additionally, and μ are not defined for photonic crystals as they are not homogeneous systems at their operational wavelength.

Photonic Crystal

Page 12: Aos Metamaterial 29-10-2010 WeeklySeminar

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/a0 1

a <<< a a >>

vs. a

Effective mediumdescription using Maxwell equations with µ and Example:Metamaterials

Properties determinedby diffraction andInterference Example:Photonics crystals

Properties describedusing geometrical optic and ray tracing Example:Lens systemShadows

Page 13: Aos Metamaterial 29-10-2010 WeeklySeminar

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Not this one0,0 kHE

,,

The right hand rule

Page 14: Aos Metamaterial 29-10-2010 WeeklySeminar

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Not this oneIf then is a left set of vectors:

0,0 kHE

,,

The left hand rule !

Page 15: Aos Metamaterial 29-10-2010 WeeklySeminar

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a

a

w

w

schematics of the elementary cell.

d•A simple calculation can be carried out to verify the UV laser capability to create the required size.

•Mostly the open ring resonator can be considered as an LC circuit where the capacitance can described by the usual textbook formula.

Unit Cell Size

Page 16: Aos Metamaterial 29-10-2010 WeeklySeminar

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•For a large capacitor with the separation between the plates is small compared to the dimensions of the plates, to ensure a uniform distribution of the field over plate’s area:•C ∝ plate area/distance •And the inductance by the formula for a coil with N windings: •L ∝ coil area/length (for N = 1)

a

a

w

w

schematics of the elementary cell.

d

Unit Cell Size

Page 17: Aos Metamaterial 29-10-2010 WeeklySeminar

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For simplicity, we can consider the width of the metal is equal to the distance between the capacitor plates (a)C = oc ad/a where:c = the effective permittivity of the material in between the plates andd= the metal thicknessL = o w2/d where:W= width = length of the coil

a

a

w

w

schematics of the elementary cell.

d

Unit Cell Size

Page 18: Aos Metamaterial 29-10-2010 WeeklySeminar

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LC-resonance frequency:

LC = 1/ =

Where c =

And the LC-resonance wavelength

LC =

Lcc

cw 1

00

1

cLC

wc 22

a

a

w

w

schematics of the elementary cell.

d

Unit Cell Size

Page 19: Aos Metamaterial 29-10-2010 WeeklySeminar

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•For relevant parameters c ≈ 3.5 this yield LC ≈ 10 ×w. •Thus, for microwave wavelength of ≈ 10 mm, the linear dimension of the coil would need to be on the order of w = 1 mm, implying minimum feature sizes around 200.

a

a

w

w

schematics of the elementary cell.

d

Unit Cell Size

Page 20: Aos Metamaterial 29-10-2010 WeeklySeminar

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Negative phase velocity, reversal of Doppler Effect and Backward Cerenkov radiation are interesting novel physical properties emerging from left-handed metamaterials phenomena.

The Perfect Lens

Metamaterial Application

Page 21: Aos Metamaterial 29-10-2010 WeeklySeminar

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Cloaking deviceIs it real, how?Can I borrow your cloak to get my PhD ?

Metamaterial Application

Page 22: Aos Metamaterial 29-10-2010 WeeklySeminar

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Its not that simple

No tricks No

Cloaking device

Page 23: Aos Metamaterial 29-10-2010 WeeklySeminar

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Another approachvirtual invisibilityRetro-reflective Projection Technology, Optical Camouflage

Cloaking device

Page 24: Aos Metamaterial 29-10-2010 WeeklySeminar

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What we are locking for ?

Cloaking device

True invisibility

Page 25: Aos Metamaterial 29-10-2010 WeeklySeminar

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The idea is to create a region that is inaccessible

To be realised by creating a new material

We need to manipulate space

Page 26: Aos Metamaterial 29-10-2010 WeeklySeminar

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-6 -4 -2 0 2 4 6-6

-4

-2

0

2

4

6

-6 -4 -2 0 2 4 6-6

-4

-2

0

2

4

6

-6 -4 -2 0 2 4 6-6

-4

-2

0

2

4

6

-6 -4 -2 0 2 4 6-6

-4

-2

0

2

4

6

-6 -4 -2 0 2 4 6-6

-4

-2

0

2

4

6

-6 -4 -2 0 2 4 6-6

-4

-2

0

2

4

6

-6 -4 -2 0 2 4 6-6

-4

-2

0

2

4

6

-6 -4 -2 0 2 4 6-6

-4

-2

0

2

4

6

-6 -4 -2 0 2 4 6-6

-4

-2

0

2

4

6y’

x’

y

x

Constant x:

Constant y:

Forbidden:

Purely geometrical distortion of space: No material yet

Hole in space

Page 27: Aos Metamaterial 29-10-2010 WeeklySeminar

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Transformation of a region

Preserve form of Maxwell’s equations

Predict form of permittivity and permeability to use in the original frame

for cloaking

Realisation

Page 28: Aos Metamaterial 29-10-2010 WeeklySeminar

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Fill the original empty space with this material

Now we have a cloaking device

The cloak

Page 29: Aos Metamaterial 29-10-2010 WeeklySeminar

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LIGHTSOURCE

OBJECT

METAMATERIAL

LIGHTRAYS

A 3D Possibility

Page 30: Aos Metamaterial 29-10-2010 WeeklySeminar

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• Meta-materials have been shown to have remarkable applications

• LHM s and negative materials can be used to overcome diffraction limit and construct a super-lens

• A super-lens enables ultra-deep sub-surface imaging

• Very new field, lots of work to do (theory and experiments)

Conclusions

Page 31: Aos Metamaterial 29-10-2010 WeeklySeminar

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Thanks for your attention.