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• it is more like solid-state physics in the sense that it might tell us much of great interest about the strange phenomena that occur in complex situations.
• Why cannot we write the entire 24 volumes of the Encyclopaedia Britannica on the head of a pin?
• What good would it be to see individual atoms distinctly?
• it would be interesting in surgery if you could swallow the surgeon. You put the mechanical surgeon inside the blood vessel and it goes into the heart and “looks”around.
• Why can’t we manufacture very small computers? Why can’t we drill holes, cut things, solder things, stamp things out, mold different shapes all at an infinitesimal level? What I would like to suggest is the possibility of training an ant to train a mite to do this.
• 1. Nanotechnology involves research and technology development at the 1nm-to-100nm range.
• 2. Nanotechnology creates and uses structures that have novel properties because of their small sizes (at this level atoms leave the realm of classical physical properties behind, and venture into the world of quantum Mechanics).
• 3. Nanotechnology builds on the ability to control or manipulate at the atomic scale.
scanning tunneling microscope (STM)
• The “tunneling” of electrons (quantum tunneling) between the tip and the substance being viewed creates a current (flow of electrons). The strength of the current and how it changes over time can be used to create an image of the surface of the substance.
• Among other things, they can be used to move atoms around and arrange them in a preferred order.
atomic force microscope (AFM)
• uses a tiny tip that moves in response to the electromagnetic forces between the atoms of the surface and the tip. As the tip moves up and down, the motion is recorded and an electronic image of the atomic surface is formed.
Atom-by-Atom Assembly
• it can be done but don’t necessarily have practical application because the process is expensive and slow.
Lithography is a Beast[ S. Kawata et al., Nature 412, 697 (2001) ]
2µm
λ = 780nm
resolution = 150nm
7µm
(3 hours to make)
One-PhotonHolographic Lithography
[ D. N. Sharp et al., Opt. Quant. Elec. 34, 3 (2002) ]
huge volumes, long-range periodic, fcc lattice…backfill for high contrast
10µm
Mass-production: Colloids
microspheres (diameter < 1µm)silica (SiO2)
(evaporate)
sediment by gravity intoclose-packed fcc lattice!
In Order To Forma More Perfect Crystal…meniscus
silica250nm
Heat Source
80C
65C1 micron silica spheresin ethanol
evaporate solvent
• Capillary forces during drying cause assembly in the meniscus
• Extremely flat, large-area opals of controllable thickness
[ figs courtesyD. Norris, UMN ]Inverse Opals
fcc solid spheres do not have a gap…
…but fcc spherical holes in Si do have a gap
Infiltration
sub-micron colloidal spheres
Template(synthetic opal)3D
Remove Template
“Inverted Opal”
complete band gap
~ 10% gap between 8th & 9th bandssmall gap, upper bands: sensitive to disorder
Inverse-Opal Photonic Crystal[ fig courtesy
D. Norris, UMN ]
[ Y. A. Vlasov et al., Nature 414, 289 (2001). ]
The Lycurgus Cup (glass; British Museum; 4th century A. D.)
When illuminated from outside, it appears green. However, whenIlluminated from within the cup, it glows red. Red color is due to very small amounts of gold powder (about 40 parts per million) embedded in the glass, which have an absorption peak at around 520 nm.
Trasmitted light is redSurface scattered light is green
What are PLASMONS?
• Coupled oscillations of charge carrier density and electromagnetic field (plasmon polariton)
• Solutions of Maxwell’s equation for metals
•Bulk plasmon modes•Surface plasmon modes
Plasmon coupling: Surface Plasmons
• Surface plasmons can propagate along a periodic chain of metallic nanoparticles
• Solution of Maxwell’s equation for a dielectric/metal interface
Metamaterials and their applications
• Metamaterial– From Greek metà (beyond) + Latin materia
(material)– To-the-letter meaning: material that doesn’t
exist in nature– Physics meaning: material with negative
refractive index
Nano Solar Cells
• The researchers added single-walled carbon nanotubes to a film made of titanium-dioxide nanoparticles, doubling the efficiency of converting ultraviolet light into electrons when compared with the performance of the nanoparticles alone.
From Principles of Quantum Mechanics :
electrons are waves 1
waves in a periodic medium can propagate without scattering:
Bloch’s Theorem (1d: Floquet’s)
2
The foundations do not depend on the specific wave equation.
شبكه الكتروني يك بعديروش ترسيم يك ياخته ويگنر سايتس دوبعدي
( ) ( ) ikx
k
x C k eψ =∑
( ) [ ( )] ( ) ( ) ( )x P U x x xm c
ωψ ψ ψΗ = + =2 212
( )( ) ( ) ( )ikx i k G x ikxG
k G k k
k C k e U C k e C k em
ε++ =∑ ∑∑ ∑2
2
2
( ) ( ) ( )k GG
C k U C k Gλ ε− + − =∑ 0 kkm
λ =2 2
2
( ) ( )( ) ( )
( ) ( )( ) ( )( ) ( )
k g
k g
k
k g
k g
U U C k g C k gU U U C k g C k gU U U U C k C k
U U U C k g C k gU U C k g C k g
λλ
ελλ
λ
−
−
+
+
⎛ ⎞ ⎛ ⎞ ⎛ ⎞⎜ ⎟ ⎜ ⎟ ⎜− −⎜ ⎟ ⎜ ⎟ ⎜⎜ ⎟ ⎜ ⎟ ⎜− −⎜ ⎟ ⎜ ⎟ ⎜
=⎜ ⎟ ⎜ ⎟ ⎜⎜ ⎟ ⎜ ⎟ ⎜+ +⎜ ⎟ ⎜ ⎟ ⎜
+ +⎜ ⎟ ⎜ ⎟ ⎜⎜ ⎟ ⎜ ⎟ ⎜⎝ ⎠ ⎝ ⎠ ⎝
2 1 2
1 1 2
2 1 1 2
2 1 1
2 1 2
0 0 2 20
00 0 2 2
⎟⎟⎟⎟⎟⎟⎟⎟⎟⎠
k g
k g
k
k g
k g
U UU U UU U U U
U U UU U
λ ελ ε
λ ελ ε
λ ε
−
−
+
+
−−
− =−
−
2 1 2
1 1 2
2 1 1 2
2 1 1
2 1 2
0 00
000 0
Electronic and Photonic Crystalsatoms in diamond structure
wavevector
elec
tron
ene
rgy
Per
iodi
cM
ediu
mB
and
Dia
gram
dielectric spheres, diamond lattice
wavevector
phot
on f
requ
ency
Blo
ch w
aves
:
interacting: hard problem non-interacting: “easy” problem
{ }E
E
__
L̂ ( )
L̂ ( , ) ( , ) ( , )( )
eigen vectoreigen value
operator
E r t E r t E r tcrω
ε= ∇× ∇× =
2
2
1
}H
H
__
L̂ ( )
L̂ ( , ) ( , ) ( , )( )
eigen vectoreigen value
operator
H r t H r t H r tcrω
ε⎧
= ∇ × ∇ × =⎨⎩
2
2
1
[( ). ]( ) ( ) i k G rkn kn
G
E r E G e +=∑
Photonic Crystals(are micro/nano structures)
periodic electromagnetic media
1887 1987
with photonic band gaps: “optical insulators”
2-D
periodic in two directions
3-D
periodic in three directions
1-D
periodic in one direction
(need a more
complex topology)
Photonic Crystals in Nature
wing scale:
Morpho butterfly
6.21µm
[ L. P. Biró et al., PRE 67, 021907
(2003) ]
Peacock feather
[J. Zi et al, Proc. Nat. Acad. Sci. USA,100, 12576 (2003) ]
[figs: Blau, Physics Today 57, 18 (2004)]
(Waveguides don’t really need a complete gap)
Fabry-Perot waveguide:
We’ll exploit this later, with photonic-crystal fiber…
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Help!
A Linear Nonlinear Filter
in out
Linear response:Lorenzian Transmisson shifted peak
+ nonlinearindex shift
References:
1- “2002 Photonics Design & Applications Handbook”, Writers: [email protected] Plasmon applications in PhC,Metamaterials and superfocusing effectsDaniele Masciarelli25 July 20073- Photonic Crystals:Principles and Applications, Steven G. JohnsonMIT Applied Mathematics4- S. G. Johnson and J. D. Joannopoulos, Photonic Crystals: The Road from Theory to Practice (Kluwer, 2002).
5- K. Sakoda, Optical Properties of Photonic Crystals (Springer, 2001).6- Nanoscale Assembly, WilhelmT.S.Huck, 2005 Springer.