chapter 6. photonic crystals, plasmonics, and...
TRANSCRIPT
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Chapter 6.
Photonic Crystals, Plasmonics,
and Metamaterials
Reading: Saleh and Teich Chapter 7
Novotny and Hecht Chapter 11 and 12
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1. Photonic Crystals
http://optoelectronics.eecs.berkeley.edu/photonic_crystals.htmlhttps://alexandramjurgens.wordpress.com/tag/ens-cachan/
1D 2D 3D
Periodic photonic structures
Period ๐ ~ ๐
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Natural Photonic Crystals
http://optoelectronics.eecs.berkeley.edu/photonic_crystals.html
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Photonic Crystal Optical Fibers
Photonic Bandgap Fibers for Precision Surgery and Cancer Therapy
http://optoelectronics.eecs.berkeley.edu/photonic_crystals.html
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Photonic Crystal Enhanced LED
Photonic Integrated Circuits
http://optoelectronics.eecs.berkeley.edu/photonic_crystals.html
Photonic Crystal Waveguide
http://spie.org/x104683.xml
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A photonic crystal of dielectric media has a periodic lattice structure whose constituent media have distinctive dielectric constants:
๐๐ ๐ซ = ๐๐ ๐ซ + ๐ฎ
for all Bravais lattice vectors, ๐ฎ = ๐1๐๐ + ๐2๐๐ + ๐3๐๐
The electromagnetic modes in the photonic crystal take the form,
๐ ๐ซ, ๐ก = ๐ ๐ซ ๐โ๐๐๐ก , ๐ ๐ซ, ๐ก =๐
๐๐0๐๐ ๐ซ๐ป ร ๐ ๐ซ, ๐ก
where the spatial mode function ๐ ๐ซ is determined by the wave equation
๐ป ร1
๐๐ ๐ซ๐ป ร ๐ ๐ซ =
๐2
๐2๐ ๐ซ
Wave Equation in a Photonic Crystal
๐๐ค ๐ซEigenmodes
Eigenvalues ๐ ๐ค
3D
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๐๐๐๐ง
๐๐๐โ๐๐๐ง
Bragg ReflectionIncident light
๐
๐
The total reflection coefficient ๐ from a semi infinite structure:
๐๐ = ๐ + ๐๐2๐๐๐ + ๐๐4๐๐๐ + ๐๐6๐๐๐ +โฏ =
๐
1 โ ๐2๐๐๐
Light cannot propagate in a crystal, when the frequency of the incident light satisfies the Bragg condition.
Origin of the photonic bandgap
Diverges if ๐2๐๐๐ = 1 โ ๐ =๐
๐Bragg condition
Constructive interference
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e(x) = e(x+a)a
e1
Any 1d Periodic System has a Gap
w
0 ฯ/a
sin
ax
cos
ax
x = 0
Treat it asโartificiallyโ periodic
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e(x) = e(x+a)a
e1 e2 e1 e2 e1 e2 e1 e2 e1 e2 e1 e2w
0 ฯ/a
Add a smallโrealโ periodicity๐2 = ๐1 + ฮ๐
sin
ax
cos
ax
x = 0
Any 1d Periodic System has a Gap
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band gap
w
0 ฯ/a
sin
ax
cos
ax
e(x) = e(x+a)a
e1 e2 e1 e2 e1 e2 e1 e2 e1 e2 e1 e2
x = 0
Splitting of degeneracy:state concentrated in higher index (๐2) has lower frequency
Any 1d Periodic System has a Gap
Add a smallโrealโ periodicity๐2 = ๐1 + ฮ๐
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1D Photonic Crystal
๐ ๐ง = ๐ ๐ง + ฮ
๐ป ๐ง = ๐ป๐ ๐ง ๐๐๐๐ง
๐ =2๐
ฮDispersion relation: cos 2๐
๐
๐= Re
1
๐ก ๐
cos 2๐๐
๐=
1
๐ก12๐ก21cos ๐
๐
๐๐ตโ ๐12
2 cos ๐๐๐
๐๐ต
๐ก12๐ก21 =4๐1๐2๐1 + ๐2
2 ๐122 =
๐2 โ ๐12
๐1 + ๐22
๐๐ต =๐๐
เดค๐ฮเดค๐ =
๐1๐1 + ๐2๐2ฮ
๐ =๐1๐1 โ ๐2๐2๐1๐1 + ๐2๐2
Bragg frequency
๐1 ๐2
ฮ
๐1 ๐2
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๐
2๐๐ต
๐๐ต
โ๐
2
๐
2๐
๐ โ ๐
photonic bangap
photonic bangap
cos 2๐๐
๐=
1
๐ก12๐ก21cos ๐
๐
๐๐ตโ ๐12
2 cos ๐๐๐
๐๐ตBand structure:
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Y. Akahane et. al. Nature 425, 944 (2003)
Photonic Nanocavities
Photonic cavities strongly confine light.
Applications โข Coherent electronโphoton
interactions โข Ultra-small optical filtersโข Low-threshold lasers โข Photonic chipsโข Nonlinear optics and
quantum information processing
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PC Waveguide: High transmission through sharp bends
A. Mekis et al, PRL, 77, 3786 (1996)
Highly efficient transmission of light around sharp corners in photonic bandgap waveguides
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Tunneling through localized resonant state
S. Fan et. al., PRL 80, 960 (1998).
Complete transfer can occur between the continuums by creating resonant states of different symmetry, and by forcing an accidental degeneracy between them.
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2. Surface Plasmons
K. Yao and Y. Liu, Nanotech. Rev. 3, 177 (2014)
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Recall the inhomogeneous wave equation:
Electromagnetic Waves in Conductors
๐2๐
๐๐ง2โ1
๐2๐2๐
๐๐ก2= ๐0
๐2๐
๐๐ก2
The equation of motion based on the forced oscillator model is
Polarization ๐ when there are free electrons:
๐2๐ฅ ๐ก
๐๐ก2= ๐พ
๐๐ฅ ๐ก
๐๐ก+๐๐ธ0๐๐
๐๐๐๐ก
resistive force by scattering
force due to the incident light field
From this, we found the polarization:
๐ ๐ก = ๐๐๐ฅ ๐ก = โ๐๐2/๐๐๐2 + ๐๐๐พ
๐ธ(๐ก)
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We now plug this in for the polarization term in the wave equation.
Plasma Frequency
Polarization in conductor: ๐ ๐ก = โ๐๐2/๐๐๐2 + ๐๐๐พ
๐ธ(๐ก)
Define a new constant, the โplasma frequencyโ ๐๐:
๐๐2 =
๐๐2
๐0๐๐
Thus ๐ ๐ก = โ๐0๐๐2
๐2 + ๐๐๐พ๐ธ(๐ก)
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So this must be the (complex) refractive index for a metal.
Back to the wave equation
๐2๐ธ
๐๐ง2โ1
๐2๐2๐ธ
๐๐ก2= ๐0
๐2๐
๐๐ก2= โ๐0๐0
๐๐2
๐2 + ๐๐๐พ
๐2๐ธ
๐๐ก2
๐2๐ธ
๐๐ง2โ1
๐21 โ
๐๐2
๐2 + ๐๐๐พ
๐2๐ธ
๐๐ก2= 0
This is the wave equation for a wave propagating in a uniform medium, if we define the refractive index of the medium as:
๐2 ๐ = ๐๐ ๐ = 1 โ๐๐2
๐2 + ๐๐๐พ
๐2๐ธ
๐๐ง2โ๐2
๐2๐2๐ธ
๐๐ก2= 0
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Optical properties in the low-frequency limit, ๐ โช ๐ธ
๐ ๐ = ๐0 1 โ๐๐2
๐2 + ๐๐๐พโ ๐0 1 + ๐
๐๐2
๐๐พDielectric function:
๐ ๐ = ๐0 1 + ๐๐0๐0๐
In the Drude model, ๐ฝ = ๐0๐ธ ๐0 =๐๐2๐
๐๐=๐๐2
๐๐๐พwhere
From Drude theory, that ๐~10โ14 sec, so ๐พ = 1/๐ ~1014 Hz.
For a typical metal, ๐๐ is 100 or even 1000 times larger.
(corresponding to the frequency of infrared light)
(corresponding to the frequency of ultraviolet light)
In the high-frequency limit, ๐ โซ ๐ธ ๐ ๐ โ ๐0 1 โ๐๐2
๐2
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A plot of Re ๐ and Im ๐ for illustrative values:
โข Imaginary part gets very small for high frequenciesโข Real part has a zero crossing at the plasma frequency
0 2000 4000 6000 8000 10000
0
-1
-2
-3
-4
-5
1
2
3
4
5
Frequency (cm-1)
๐๐/๐
0
Re ๐Im ๐
linear scale
๐๐ = 4000 cm-1
๐พ = 40 cm-1
๐๐
10-3
10-1
101
103
105
๐๐/๐
0100 101 102 103 104
Frequency (cm-1)
log scale
๐๐
Re ๐
โRe ๐
Im ๐
10510-5
๐ ๐ = ๐0 1 โ๐๐2
๐2 + ๐๐๐พDielectric function of metals:
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Drude theory at optical frequencies
large and negative (below ๐๐)
small and positive
Re{๐}
๐0
Im{๐}
๐0
๐ ๐
๐0= 1 โ
๐๐2
๐2 + ๐๐๐พ
โ 1 โ๐๐2
๐2+ ๐
๐พ
๐
๐๐2
๐2
๐๐ > ๐ โซ ๐พ
IR visible
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In the regime where ๐ > ๐พ,
โข For frequencies below the plasma frequency, ๐ is complex, so the wave is attenuated and does not propagate very far into the metal.
โข For high frequencies above the plasma frequency, ๐ is real. The metal becomes transparent! It behaves like a non-absorbing dielectric medium.
Reflectivity drops abruptly at the plasma frequency.
This is why x-rays can pass through metal objects.
๐ ๐ =๐ ๐
๐0= 1 โ
๐๐2
๐2
High frequency optical properties
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The uppermost part of the atmosphere, where many of the atoms are ionized. There are a lot of free electrons floating around here.
For ๐~1012 mโ3, the plasma frequency is:
Radiation above 9 MHz is transmitted, while radiation at lower frequencies is reflected back to earth.
Thatโs why AM radio broadcasts can be heard very far away.
Radio Waves in Ionosphere
๐๐ =๐๐2
๐0๐๐= 2๐ ร 9 MHz
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๐๐ = 15000 cmโ1
๐พ = 40 cmโ1
For real metals, there is a very broad range of frequencies for which Im ๐ ~0 and Re ๐ < 0.
0 4000 8000 12000 16000 20000
0
-4-8
-12
-16
-20
4
8
12
16
20
Frequency (cm-1)
e(w
)/e 0
Re ๐
Im ๐
linear
scale
๐๐
This has interesting implications!!!
Dielectric Function of Real Metals
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Consider a wave at the interface between two semi-infinite non-magnetic media (๐1 = ๐2 = ๐0).
Is there a solution to Maxwellโs equations describing a wave that propagates along the surface?
๐บ๐ ๐บ๐
๐ง
๐ฅ
๐ง = 0
This propagates along the interface, and decays exponentially into both media.
(Note: this is not a transverse wave, but thatโs OK.)
Waves trapped at an interface
We can guess a solution of the form for media 1 and 2:
๐๐ = ๐ธ1๐ฅ , 0, ๐ธ1๐ง ๐โ๐ ๐ ๐ง ๐๐ ๐๐ฅโ๐๐ก
๐๐ = 0, ๐ต1๐ฆ , 0 ๐โ๐ ๐ ๐ง ๐๐ ๐๐ฅโ๐๐ก
๐ = 1,2
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In order to exist, the wave must satisfy Maxwellโs equations:
Since ๐ 1 and ๐ 2 are always positive, this shows that interface waves only exist if ๐1 and ๐2 have opposite signs.
In a metal, ๐ < 0 for frequencies less than ๐๐.
๐๐ 1๐ต1๐ฆ = ๐1๐
๐2๐ธ1๐ฅ
๐๐ 2๐ต2๐ฆ = โ๐2๐
๐2๐ธ2๐ฅ
and also the continuity boundary conditions at ๐ง = 0:
๐ต1๐ฆ ๐ง = 0 = ๐ต2๐ฆ ๐ง = 0 ๐ธ1๐ฅ ๐ง = 0 = ๐ธ2๐ฅ ๐ง = 0
It is easy to show that these conditions can only be satisfied if:๐1๐ 1
+๐2๐ 2
= 0
Interface Waves
๐ป ร ๐ = ๐๐๐๐
๐๐ก
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Surface Plasmon Polariton (SPP) - a surface wave moving along the interface between a metal and a dielectric (e.g., air)
The electrons in the metal oscillate in conjunction with the surface wave, at the same frequency. In fact, an SPP is both an electromagnetic wave and a collective oscillation of the electrons.
Surface Plasmon Polaritons
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SPP Dispersion Relation
๐ 1๐1+๐ 2๐2
= 0
๐ธ = ๐ธ0๐โ๐ ๐ง ๐๐ ๐๐ฅโ๐๐ก
๐2 + ๐ ๐2 = ๐๐
๐
๐
2
SPP Electric field:
and ๐ = 1,2
Dispersion relation:
๐ =๐
๐
๐1๐2๐1 + ๐2
1/2
๐1 ๐ = 1 โ๐๐2
๐2For
๐๐ ๐ =๐๐
1 + ๐2
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Surface plasmonsare very sensitive to molecules on the metal surface.
Surface plasmon sensors
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Instead of considering a semi-infinite piece of metal, what if the metal object is small?
e.g., a metal nanosphere
We can still excite a plasmon, but in this case it does not propagate! The electrons just collectively slosh back and forth.
excess negative charge
excess positive charge
There is a restoring force on the electron cloud! Once again, we encounter something like a mass on a spring, with a resonanceโฆ
Surface plasmons on small objects
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2.8 nm copper nanoparticles
Pedersen et al., J Phys Chem C (2007)
The sloshing electrons interact with light most strongly at the resonant frequency of their oscillation.
gold nanoparticles give rise to the red colors in stained glass
windows
Surface plasmon resonance
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Controlling the surface plasmon resonance
gold nano-shells
The frequency of the plasmon resonance can be tuned by changing the geometry of the metal nano-object.
Halas group, Rice U.
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3. Metamaterials
L. Billings, Nature 500, 138 (2013)
Negative refractive index
K. Yao and Y. Liu, Nanotech. Rev. 3, 177 (2014)
Metadevices
N. I. Zheludev and Y. S. Kivshar, Nature Mat. 11, 917 (2012)
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Is an invisibility cloak magic or reality?
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Invisibility Skin Cloak for Visible Light
Ni et. al. Science 349, 1310 (2015).
AFM Cloak on Cloak off
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๐ โซ ๐, ๐
a b
Electromagnetic Metamaterial
Physics Today Jun 2004 Physics Today Feb 2007
Negativerefraction
Invisibility
Meta-atom
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Y. Liu and X. Zhang, Chem. Soc. Rev. 40, 2494 (2011)
Material Parameter Space by ๐บ and ๐
๐2 = ๐๐๐๐
๐ = ยฑ ๐๐ ๐๐
๐ค ร ๐ = ๐๐๐
๐ค ร ๐ = โ๐๐๐๐ = ๐0๐๐, ๐ = ๐0๐๐ ๐ = ๐ ร ๐
๐ โฅ ๐ค
๐ โฅ โ๐ค
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Y. Liu and X. Zhang, Chem. Soc. Rev. 40, 2494 (2011)
Basic metamaterial structures to implement artificial electric and magnetic Responses
Periodic Wires
Split RingResonators(SRR)
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Smith et. al., PRL14, 234 (2000)
First Negative Index Material
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Negative Refraction and Perfect Focusing
RHM LHM
๐ ๐
๐๐ > 0
๐๐ < 0
๐ = 1 ๐ > 1 ๐ = 1 ๐ < 1
sin ๐ = ๐ sin ๐๐
pointsource
imageInternalfocus
evanescent waves
๐ = 1 ๐ = 1๐ = โ1
Fang et. al. Science 308, 534 (2005)
FIB 40nm
AFM with superlens
AFM w/o superlens
Shelby et. al. Science 292, 77 (2001)
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Y. Liu and X. Zhang, Chem. Soc. Rev. 40, 2494 (2011)
Invisibility Cloak