aos metamaterial 29-10-2010 weeklyseminar
DESCRIPTION
metamaterialsTRANSCRIPT
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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]
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Outlines• Introduction to metamaterials
• Classification of materials
• Photonic Crystal
• Realisation of Metamaterials
• Unit Cell Size
• Metamaterial Application
• Cloaking
• Conclusions
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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
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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”.
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1
2
ENERGY
PHASEVELOCITY
Air
Materiallike glass
Metamaterial
Yes as a backward wave
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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
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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
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DPSENGMNG
Classification of materials
DNG
Cloak
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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
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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
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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
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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
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Not this one0,0 kHE
,,
The right hand rule
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Not this oneIf then is a left set of vectors:
0,0 kHE
,,
The left hand rule !
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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
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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
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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
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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
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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
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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
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Cloaking deviceIs it real, how?Can I borrow your cloak to get my PhD ?
Metamaterial Application
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Its not that simple
No tricks No
Cloaking device
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Another approachvirtual invisibilityRetro-reflective Projection Technology, Optical Camouflage
Cloaking device
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What we are locking for ?
Cloaking device
True invisibility
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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
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-6 -4 -2 0 2 4 6-6
-4
-2
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-6 -4 -2 0 2 4 6-6
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-6 -4 -2 0 2 4 6-6
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-6 -4 -2 0 2 4 6-6
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-6 -4 -2 0 2 4 6-6
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-6 -4 -2 0 2 4 6-6
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-6 -4 -2 0 2 4 6-6
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-6 -4 -2 0 2 4 6-6
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-6 -4 -2 0 2 4 6-6
-4
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6y’
x’
y
x
Constant x:
Constant y:
Forbidden:
Purely geometrical distortion of space: No material yet
Hole in space
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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
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Fill the original empty space with this material
Now we have a cloaking device
The cloak
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LIGHTSOURCE
OBJECT
METAMATERIAL
LIGHTRAYS
A 3D Possibility
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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
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Thanks for your attention.