nanophotonics course material-2012 for students 110112
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Nano-photonics Course material
Reference:
1. Nanophotonic by Paras N. Prasad, Wiley Interscience, 2004, USA2. Photonic Crystals: Molding the flow of Lightby John D. Joannopoulos,
Steven G. Johnson, Joshua N.Winn, Robert D. Meade April 17, 2007
3. Nanooptics By Sotoshi Kawata, Motichi Ohtsu, Masahiro Irie, Springer Verlag
20024. Optical Nanotechnologyby J. Tominga and DP Tsai, Springer 2003
5. Principles of Nano-Opticsby Lukas Novotny, BertHecht, Cambridge
University Press 2006.6. Electromagnetic Metametrials: Transmission Line Theory by Christoophe
Caloz, Tatsuo Itoh, Wiley IEEE Press 2005
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WHAT DIFFERENTIATES ELECTRONfrom PHOTON
1. Electron is a Charged particle
2. Photon is a Non-charged particle
3. Electron has mass associated with it.
4. Photon is a mass-less particle
5. Both behave as a Particle and as Wave.
6. Both are governed by EM theory but their behaviors are different
7. Electron Wave is a Vector propagation under field and thereforehas vector field while Photon is a Scalar Propagation therefore has
Vector field associated with it and both move in 3-D.
8. Electron is defined by 3 components viz. frequency orwavelength, amplitude (as voltage or current) and phase.
9. Photon has 4 components viz. frequency or wavelength,
amplitude (as power), phase and polarization.
10.Electron wave up to 300GHZ is bipolar and after that it becomes
unipolar. When it becomes unipolar it is called Electronic Photon.
11.Photon is always Unipolar.
12.Electrons posses SPIN, and their distributions are defined by
FERMI-DIRAC Statistics and therefore are called FERMIONS
13.Photons do not have SPIN therefore their distribution is governedby Bose Einstein statistics and are therefore called BOSONS.
14.Electrons being charged particles get guided within vacuum or any
media only under electric field, while photons being non-chargedparticle, need a dielectric medium for guidance.
15. Electron hassmallerDe-Broglie wave-length and Photon has a
longerDe-Broglie wave-length.
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5 B1
r` a
fffffffffff5 B B r
` a=
c
fffffe2
B r` a
for optical wave
O F = C F where C is an eigen value and is given by
c
fffffe2
and O is the Eigen function
THE DENSITY OF STORAGE ACHIEVABLE WITH Nanophotonicsdevices
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NANOPHOTONICS works BEYOND the DIFFRACTION LIMIT or is
DIFFRACTION FREE, where the x< and kx 1 and k is the
UNCERTAINITY in the wave number k . It is this characteristics that
enable HIGH RESOLUTION and HIGH FREQUENCY OPERATIONS.
When the incident light radiation
WAVELENGTH is greater than thePARTICLE SIZE Electric Dipoles are formed at
every diffraction point which explains the
DIFFRACTION FREE transmission as
OPTICAL NEAR FIELD Radiation.
1. The radiated NEAR FIELD isindependent of the phase of the
incoming incident light.
2. Therefore the SPATIALDISTRIBUTION and DECAY
LENGTH of the Optical Near FieldEnergy does not depend on the
WAVELENGTH of the incident light
but on the size, conformation and the
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REVIEW OF ELECTROMAGNETICS andMAXWELLs EQUATIONS
The basic set of FOUR Maxwells equations for Propagation
through Dielectric Medium when written in the CGS units are asfollows:
5 AB =0
5 AD =4
5 xE +1
c
ffffj k D
t
ffffffffff=0 ..(1)
5 xH@1
c
ffffj kD
t
ffffffffff=0
Eand Hare the Electric and Magnetic Field Vectors, D and B are the
Electric and Magnetic Flux Density Vectors and cis the velocity of light
in vacuum. is the charge density. Assuming that the ElectromagneticEnergy is propagating in the medium with fluctuating dielectric constant and there are no sources of light within the Dielectric Medium then =0 .
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The medium is linear for small field strengths and dielectric constant
also remains same. Further assuming a loss in isotropic medium, isconsidered real and a scalar quantity. It is independent of the operating
frequency. With these assumptions, the Electric Field Eand Electric Flux
Density D are related as
D r = r E r ..(2)
Thus is a function of space within the Micro-structured systems. Formost of the dielectrics the magnetic permeability is very close to unity
and hence
B =H ..(3)
The 1st Equation above can be written as
5 AH r,t =0
5 A ra
E r,t =0
5 xE r,tb c
+1
c
ffffj kH r,t
t
ffffffffffffffffffffffffffff=0 ..(4)
5 xH r,tb c
@ r
` a
c
ffffffffffffffj kE r,t
t
fffffffffffffffffffffffffflj
mk =0
In this, the field vectors E and H are assumed to be the functions oftime and space, i.e. t and r. Let the time dependency be denoted by an
exponential function such as
H r,t = H raejwt
E r,t = E r ,t e jwt .(5)
Substituting the above in the previous equation we have
5 AH r = 05 A r E r =0
5 xE r` a
+
j
cffffffffj k H r
` a=0 .(6)
5xH r` a@
j
c
ffffffffj k E r` a
=0
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The last TWO equations of (6) in the above set of four equations can bemanipulated to decouple each other to get equations entirely in H(r) or
E(r) as follows
5 x
1
r` a
ffffffffffffff
5 xH r
` a
J K =
c
fffff g2
L
J
M
KH r
` a
(7)
E r` a
=@jc
r` a
ffffffffffffffffffffJ K5 xH r` a
.(8)
Equation (7) above is a complex differential equation which gives the
harmonic mode in a mixed dielectric medium. If the operation of takingthe Curl, dividing by r and again taking the Curl is attributed to a
complex operation defined as operator ,then
H r` a
=
c
ffffV W2
H r` a
..(9)
Thus the result of operator H(r) with is leaving it as it is and
multiplying it by a constant
c
ffffV W2
as it Eigen Vector.
IN DIELECTRIC MEDIA
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