Bhupendra Subedi– University of Missouri Kansas City 
Kansas City, MO 64111 
bsr34@mail.umkc.edu
Antenna: converts radiation energy to 
localized energy and vice versa 
analogous to 
phenomena in the surface of the metallic 
nanostructures (optical frequency) called 
Localized Surface Plasmon Resonance 
(LSPR). 
So any plasmonic nanostructures can be 
considered as nanoantennas (not very rigid)
[1] Javier Aizpurua, "Quantum kisses between optical nanoantennas”, mappingignorance 
(2013). 
Wave strikes metal nanostructures, energy is transferredto electrons 
and resonance occurs when mom. of photons = mom of polaritons
ε2 
θ 
y 
ε1 
E0 x 
F = F (r,q ,j ),scalar _ potential 
E1 = -Ñ F 1andÑ 2F 1 = 0 
E2 = -Ñ F 2andÑ 2F 2 = 0 
We need to solve Laplace Equation
Electric Field in x direction is given by: 
F 0 = - E0x = - E0rcosq ,andF 2 = F scatter + F 0
Applied _ Field = E0 
Fdipole = p 
4pe2 
e1 
-e2 
e1+2e2 
cosq 
r2 = -E0r cosq 
a3 cosq 
r2 
E0 
x 
y 
ε2 
ε1 
Shows: Field outside = Field due to dipole + Applied_Field
# Areas of Application Appli.cation and devices 
1. Nanophotonics detectors, filters and lasers eg. maskless optical 
lithography, NSOM 
2. Plasmonic Solar Cells rectennas using ALD technology 
3. Metamaterials optical/EM sheilding and invisibility cloaks 
4. Chemical and bio/medical 
sensing and optical devices 
super lenses for medical sensing, medical 
cancer treatment; gases and radiation sensors 
5. On-Chip Interconnect on-chip nanoantennas 
So nanoantennas cover wide spectrum of 
applications
Conventional Antennas Nanoantennas 
• Fed by real current, EM 
resonance causes waves 
• Fed by localized current, Surface 
Plasmon Polaritons causes waves 
• Demands classical treatment • Demands QM treatment 
• Dissipated power related to 
voltage and current 
• Dissipated power related to Green’s 
function tensor and Local density of 
state (LDOS) 
Need for different infrastructures such as modeling 
software and fabrication engineering
• Long lifetime of exiton polariton 
causes recombination 
P0 = 
I 2 
3 ph 
Dl 
l0 
• Large ohmic losses and relative finite 
skin depth decreasing efficiency and 
unfocussed radiation pattern 
Need for optimized antenna element and 
skin depth
h =1- Tcold 
Thot 
Simple idea: Recycling of the wasted 
heat from the cold sink
Hotter Sink 
gets more 
hotter 
Increases 
efficiency 
Colder Sink gets 
more colder
1. Absorbing antenna as 
close to Cold sink as possible 
Say ¼ wave distance 
=>short-circuit (unbalanced 
Voltage condition) 
Solution: 
Coupling capacitance
Coupling Capacitance, A. Boswell, “amasci” 
Tuned capacitive 
Coupling 
Improves power 
Radiation by 100 
folds 
Avoids short-circuit; ehhances absorption
Nano-rectifiers 
Not easy to channel heat radiations 
These waves are vibrating in infra red or even THz frequency 
that todays commercial rectifiers can’t handle 
Nano-rectifiers 100-1,000 X smaller rectifiers needed
P0 = 
I 2 
3 ph 
Dl 
l0
Graphene based absorbing antenna 
Fabry –Perot Resonance 
Chamber (LSPR) 
[Stamatios A. Et. Al] 
Can be tuned to absorb certain 
wavelength
P0 = 
I 2 
3 ph 
Dl 
l0 
[16] Maciej Klemm. "novel directional nanoantennas for single-emitter sources and 
wireless nano-links". International Journal of Optics, 2012(2012), 2012.
Basically an idea, 
I would do Modelling, FEKO Simulation, Implementation and what 
not. 
P0 = 
I 2 
3 ph 
Dl 
l0 
[1] Circuit implementation 
[2] efficiency improvement 
[3] good absorbing and radiating elements/ improvisation
[1] Javier Aizpurua, "Quantum kisses between optical 
nanoantennas”, mappingignorance (2013). 
[2] Javier Aizpurua, “Lecture given at 2 
SSOP Porquerolles, Sept. 
2009 
I Dl 
P= 
ph 
0 [3] Maciej Klemm. "novel directional 3 nanoantennas for single-emitter 
l0 
sources and wireless nano-links". International Journal of 
Optics, 2012(2012), 2012 
[4] A. Boswell, “amasci 
Thank you
bsr34@mail.umkc.edu

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Carnot - efficiency based Nanoantenna Systems

  • 1. Bhupendra Subedi– University of Missouri Kansas City Kansas City, MO 64111 bsr34@mail.umkc.edu
  • 2. Antenna: converts radiation energy to localized energy and vice versa analogous to phenomena in the surface of the metallic nanostructures (optical frequency) called Localized Surface Plasmon Resonance (LSPR). So any plasmonic nanostructures can be considered as nanoantennas (not very rigid)
  • 3. [1] Javier Aizpurua, "Quantum kisses between optical nanoantennas”, mappingignorance (2013). Wave strikes metal nanostructures, energy is transferredto electrons and resonance occurs when mom. of photons = mom of polaritons
  • 4. ε2 θ y ε1 E0 x F = F (r,q ,j ),scalar _ potential E1 = -Ñ F 1andÑ 2F 1 = 0 E2 = -Ñ F 2andÑ 2F 2 = 0 We need to solve Laplace Equation
  • 5. Electric Field in x direction is given by: F 0 = - E0x = - E0rcosq ,andF 2 = F scatter + F 0
  • 6. Applied _ Field = E0 Fdipole = p 4pe2 e1 -e2 e1+2e2 cosq r2 = -E0r cosq a3 cosq r2 E0 x y ε2 ε1 Shows: Field outside = Field due to dipole + Applied_Field
  • 7. # Areas of Application Appli.cation and devices 1. Nanophotonics detectors, filters and lasers eg. maskless optical lithography, NSOM 2. Plasmonic Solar Cells rectennas using ALD technology 3. Metamaterials optical/EM sheilding and invisibility cloaks 4. Chemical and bio/medical sensing and optical devices super lenses for medical sensing, medical cancer treatment; gases and radiation sensors 5. On-Chip Interconnect on-chip nanoantennas So nanoantennas cover wide spectrum of applications
  • 8. Conventional Antennas Nanoantennas • Fed by real current, EM resonance causes waves • Fed by localized current, Surface Plasmon Polaritons causes waves • Demands classical treatment • Demands QM treatment • Dissipated power related to voltage and current • Dissipated power related to Green’s function tensor and Local density of state (LDOS) Need for different infrastructures such as modeling software and fabrication engineering
  • 9. • Long lifetime of exiton polariton causes recombination P0 = I 2 3 ph Dl l0 • Large ohmic losses and relative finite skin depth decreasing efficiency and unfocussed radiation pattern Need for optimized antenna element and skin depth
  • 10. h =1- Tcold Thot Simple idea: Recycling of the wasted heat from the cold sink
  • 11. Hotter Sink gets more hotter Increases efficiency Colder Sink gets more colder
  • 12. 1. Absorbing antenna as close to Cold sink as possible Say ¼ wave distance =>short-circuit (unbalanced Voltage condition) Solution: Coupling capacitance
  • 13. Coupling Capacitance, A. Boswell, “amasci” Tuned capacitive Coupling Improves power Radiation by 100 folds Avoids short-circuit; ehhances absorption
  • 14. Nano-rectifiers Not easy to channel heat radiations These waves are vibrating in infra red or even THz frequency that todays commercial rectifiers can’t handle Nano-rectifiers 100-1,000 X smaller rectifiers needed
  • 15. P0 = I 2 3 ph Dl l0
  • 16. Graphene based absorbing antenna Fabry –Perot Resonance Chamber (LSPR) [Stamatios A. Et. Al] Can be tuned to absorb certain wavelength
  • 17. P0 = I 2 3 ph Dl l0 [16] Maciej Klemm. "novel directional nanoantennas for single-emitter sources and wireless nano-links". International Journal of Optics, 2012(2012), 2012.
  • 18. Basically an idea, I would do Modelling, FEKO Simulation, Implementation and what not. P0 = I 2 3 ph Dl l0 [1] Circuit implementation [2] efficiency improvement [3] good absorbing and radiating elements/ improvisation
  • 19. [1] Javier Aizpurua, "Quantum kisses between optical nanoantennas”, mappingignorance (2013). [2] Javier Aizpurua, “Lecture given at 2 SSOP Porquerolles, Sept. 2009 I Dl P= ph 0 [3] Maciej Klemm. "novel directional 3 nanoantennas for single-emitter l0 sources and wireless nano-links". International Journal of Optics, 2012(2012), 2012 [4] A. Boswell, “amasci Thank you