2. Talk Outline
What is a metamaterial?
How to get negative µ and ε
Technical Challenges
Applications
3D Metamaterials
Slow Light
Superlens
Chiral Metamaterials
Metamaterial Cloak
3. Classifying Materials
based on electromagnetic response (µ,ε)
ε<0, µ>0
Metals ,Doped
Semiconductors
Evanescent waves
ε>0, µ> 0
Most Dielectrics
Propagating Waves
ε<0, µ<0
No natural
Materials
Propagating Waves
ε>0, µ<0
Some ferrites
Evanescent waves
ε
µ III
III IV
4. What is a metamaterial ?
‘Meta’ means Beyond
Metamaterial is an artificially engineered composite of
periodic or non-periodic structures with exotic
macroscopic properties that are not found in Nature.
5. Where do metamaterials fit
in Optical Engineering ?
a<< λ
Effective medium
Approximation with
Maxwell Equations
a~λ
Structure dominates
Properties
determined by
diffraction and
interference
a>>λ
Properties
described by
geometrical optics
and ray tracing
Examples
Optical Crystals
Metamaterials
Examples
Photonic Crystals
X Ray diffraction
Radar Systems
Examples
Lens Systems
Shadows
a/λ0 1 ∞
6. )1)(1( iin )()1( i
2
)(
1
i
t
D
jHD
t
B
EB
,.
,0.
In 1968,
Victor Veselago theoretically proved that we can have material
with
Maxwell’s equations
2
n
i
i
Real part is negative,
Generally imaginary parts are >0
since they characterizes light absorption
Imaginary part of n has to be positive for any passive material.
Therefore minus sign must be chosen
Both ε´ < 0 and μ´ < 0 is possible ,
But not the only approach to achieving a negative n
Equation ε´|μ| + μ´|ε| < 0 must be obeyed to get negative n
Simultaneously negative ε and μ
8. Poynting Vector S: The direction of the
energy is determined by the real part of
the vector
Reversed
Doppler shift
EHk
HEk
ε<0,μ<0
E,H,K form a left-
handed triplet
ε>0,μ>0
E,H,K form a right-
handed triplet
HES
2
1
Left or Right ?
9. How to Get ε<0 Noble metals
Assuming Drude Model for permittivity Silver parameters
Plasma frequency
depends on geometry
rather than on material
properties
A periodic array of thin
metal wires with
r<<a<<λ
can acts as a low
frequency plasma
ε<0
10. How to get μ < 0 : Split Ring Resonator
Bulk metal has
no magnetism
in optics
A metal ring : weak
magnetic response
Current induced by H
A Split ring : magnetic
resonance due to LC
Double Split ring :
Enhanced magnetic
resonance
L
C
LC
res
1
Hind
Hext
12. Technical Challenges
Optical Metamaterials
3D Metamaterials
Loss Compensation in Metamaterials
Incorporate Gain Media
Coupling Effects in Meta-atoms
Metamolecules?
Slow Light
Fano Resonances
14. What we will focus on…
Optical Metamaterials
3D Metamaterials
Slow Light
Cloaks
Chiral Metamaterials
Superlens
15. How low can you go ? Scaling Limit of SRRs
• Saturation of resonance frequency with scaling
• Reason Loss in metal giving rise to kinetic inductance
• Finite electron mobility
;coilL size
1
kineticL
size
;total coil kineticL L L
total sizeC
2
1 1 1
( . / ).( . )total total
res
L C A size A size C size size const
16. Fishnet Structure : ε<0, μ<0
Nanostrip pair (TM):
Magnetic field applied along the
nanostrip. µ < 0 (resonant)
Nanostrip pair (TE):
Electric field applied along the
nanostrip. ε < 0 (non-resonant)
Fishnet - Combination of
Nanostrip pair in TM and TE:
µ < 0 and ε < 0
H
E
K
Nanostrip consists of 2 layers of
metal separated by a dielectric
spacer layer.
Dielectric Metal
24. In conclusion
• Traditionally Question: Which material has
desired optical properties ?
• New Question: How to engineer/design
materials to achieve desired optical
properties ?
– Answer: Metamaterials
• Dispersion engineering(Tamper ε and μ)
– Change how light interacts with matter
– Slow Light, Cloaking, Superlensing,
Thank You ALL, Q?A!
25. Divide and Rule
• Kain Lu LowChiral
• Zhang Taishi Slow light
• Shuvan Prashant3D Meta
• Zhao WenWen Cloak
• Naomi
Nandakumar
Super
Lens
26. References
• General
– Veselago, Soviet Physics Uspekhi 10 509, (1968)
– Liu & Zhang, Chem. Soc. Rev ., 40, 2 494–2507, (2011)
– Optical Metamaterials, Wenshan Cai and Vladimir Shalaev, 1st Edition,
Springer.(2010) and references therein.
– Shalaev, Nature Photonics, 1 ,41(2007)
• 3D Metamaterials
– Soukoulis and Wegener, Nature Photonics Published online, doi:
10.1038/nphoton.2011.154, (2011) and references therein
• Slow Light and Fano Resonances
– Lukyanchuk et al , Nature Materials, doi: 10.1038/nmat2810, (2010)
– Papasimakis et al, Optics and Photonics News, 20(10), 22-27 (2009)
• Cloaks
– Chen et al, Nature Materials, doi: 10.1038/nmat2743 2010
– Tolga, Ergin et al Science 328, 337(2010)
• Chiral Metamaterials
– Gansel et al, Science 325, 1513(2009)
– Plum et al, Physical Review B 79, 035407 (2009)
– Radke et al, Advanced Materials23(27), 3018-3021, (2011)
• Superlens
– Zhang & Liu, Nature Materials 7,435, (2008)
its man-made artifical atoms which has its own fuequency
Chiral Metamaterial is composed of particles that cannot be superimposed on their mirror image.
Left and right-handed circularly polarized light propagating in a chiral medium, the refractive index is : Hence, refractive index can be negative for sufficiently large Κ. It provides alternative route to realize the negative refractive index.
Slow light is light with reduced group velocity. Group velocity determines how fast the wave packet travels, or energy transmits, it’s dependent on both material refractive index as well as how fast refractive index changes with frequency, or dispersion. So to achieve slow light, drastic change of refractive index over short spectrum is needed.
Ref: 2007_nature_MM slow light; 2010_NMaterial_Fano Resonances in plasmonic NS and MMs