5. Metamaterial is an arrangement of periodic
structures of unit cells in which the average
size of a unit cell should be much smaller
than the impulsive wavelength of the light.
5
6. It was seen that wave propagation in metamaterial was in
opposite direction than the naturally occurring materials.
Materials with negative permittivity such as ferroelectrics
were available in nature but materials with negative
permeability did not exist in nature.
6
7. For simultaneous change of sign of
permittivity and permeability, the
direction of energy flow is not affected..
For left-handed system, n is negative,
thus the phase velocity is negative.
Hence the direction of energy flow and
the wave will be opposite resulting in
backward wave propagation
7
8. For right handed system, n is
positive, thus the phase velocity will
be positive. Therefore, energy and
wave will travel in same direction
resulting in forward wave
propagation
8
10. Artificial Dielectrics
Artificial dielectrics are the
structures having negative
permittivity but positive
permeability.
An array of cylinders displays
negative permittivity below
plasma frequency
10
12. Artificial Magnetics
Artificial magnetics are the
structures having negative
permeability but positive
permittivity.
Artificial magnetics exhibits
negative permeability below
plasma frequency.
12
13. Negative-Index Material
The materials with simultaneous negative permittivity
and permeability are called Negative-index materials
(NIM).
These are also called left handed materials.
The combination of alternating layers of thin metallic
wires and circular split rings, Omega shaped, S shaped
structures , Double H shaped structures etc. exhibits
negative index of refraction.
13
15. The combination of alternating layers of thin metallic wires and circular split rings,
Omega shaped , S shaped structures etc. exhibits negative index of refraction.
15
16. NZIM
Near Zero Index Material
CATEGORY
epsilon-near-zero and
mu-very-large media
mu-near-zero (MNZ) &
epsilon-very-large (EVL)
media
double-zero media (DZR)
16
18. Reference Paper
1
Gain Enhancement of Microstrip
Patch Antenna using Near-zero
Index Metamaterial (NZIM) Lens
Hemant Suthar
Debdeep Sarkar
Kushmanda Saurav
Kumar Vaibhav Srivastava
18
19. Reference Patch Antenna
Schematic diagram of coax fed microstrip patch antenna:
(a) Top view. (b) Side view; Lp= 16.5 mm, W p= 12.6 mm,
Ls= 60 mm, Ws= 50mm,
Coaxial Feed
Operation Frequency 5.2 Ghz
Impedance bandwidth of 4.25%
(5.08 GHz - 5.3 GHz)
Peak realized gain of 5.6 dBi.
19
20. Unit Cell
NZIM unit cell: (a) Top surface, (b) Bottom surface;
ax= ay=4.5 mm, L1 = 4.2 mm, L2 = 1.725 mm, L3 = 1.2 mm
W1 = 4.3 mm, W2 = 3.5 mm, W = 0.25 mm.
Structure printed on both sides
Substrate FR4 thickness 0.8mm
It’s a NZIM near zero index
material
Enhances the gain of the reference
antenna 7.65dB
20
22. Extracted real and imaginary part of refractive
index for the proposed NZIM unit cell
|S11| v/s frequency for the reference patch
antenna and proposed antenna with single layer
NZIML. (b) Gain v/s frequency
22
23. Extracted real and imaginary part of permittivity
and permeability for the proposed NZIM unit cell
Simulated radiation pattern of reference patch
antenna and patch antenna loaded with single
layer NZIML (a) E-plane. (b) H-plane.
23
24. Reference Paper
2
A Compact Gain Enhancement Patch
Antenna Based On NZIM Superstrate.
Jinxin li
Tayab A
Qingsheng Zeng
24
25. Reference Patch Antenna
Schematic diagram of coax fed microstrip patch
antenna: Top view and side view ; L= 59.7 mm, W =
39.8 mm, Ls= 150mm, Ws=150mm, hs=12mm.
Coaxial Feed
Operation Frequency 2.44 Ghz
Impedance bandwidth of 3.25%
(2.42 GHz - 2.46 GHz)
Peak realized gain of 2.3 dBi.
25
26. ● This structure is designed to act as near zero refractive
index metamaterial at 2.44 GHz
● Superstrate diagram
● Unit cell diagram
NZIM UNIT CELL DESIGN
26
27. STRUCTURE UNIT CELL AND SUPERSTRATE
Unit-cell dimension of unit cell:
● a= 140mm, b= 105mm
● Length of each side of unit cell is 35mm.
● The thickness of layer is 1.575 mm.
● Substrate is RT/duroid 5880 (εr= 2.2).
27
28. Patch Antenna Based On NZIM Superstrate
• Compact high-gain patch antenna based on near-zero index metamaterial
(NZIM) superstrate lens operating at 2.44 GHz is proposed.
• A single layer NZIM superstrate with unit-cell periodicity of 3 × 4 is designed and
suspended above a patch antenna at a very close distance of 0.097 λ.
• The proposed single layer NZIM superstrate provides a gain enhancement of 2.3
dB at 2.44 GHz to a conventional patch antenna.
28
30. ● Simulation results show that the NZIM superstrate could converge the
electromagnetic wave radiated by the antenna to enhance the radiation
gain
30
31. Reference Paper
3
Microstrip Antenna Gain
Enhancement by Metamaterial
Radome with More Subwavelength
Holes
Kai-Shyung Chen,
Ken-Huang Lin,
Hsin-Lung Su
31
32. JERUSALEM CROSS STRUCTURE UNIT CELL
•This structure is designed to act as near zero refractive index
metamaterial at 3.5 GHz.
•Unit cell diagram:
32
33. JERUSALEM CROSS STRUCTURE UNIT
CELL
Unit-cell dimension of Jerusalem unit cell:
• a = 23 mm, b = 20 mm, c = 19 mm,
•d = 1mm. The thickness of each layer is 0.8 mm.
•Substrate is FR4 (εr= 4.4).
•the separation between each layer is 1.6mm.
33
35. JERUSALEM CROSS STRUCTURE UNIT CELL
•A large number of positive and negative charges assemble in the ends of the
metal strip.
•it would cause the E-field that is distributed as shown in Figure.
•E-field distribution phenomenon would form a vortex to collect the
electromagnetic wave and collimate the electromagnetic wave passing through
this subwavelength hole
35
39. JERUSALEM CROSS STRUCTURE UNIT CELL
Gain and directivity enhancement of the patch antenna using The Jerusalem
structure metamaterial radome which has 9 holes and 4 holes.
39
40. Reference Paper
4
BROADSIDE GAIN AND
BANDWIDTH ENHANCEMENT
OF MICROSTRIP PATCH
ANTENNA USING A MNZ-
METASURFACE
KWOK L. CHUNG
SARAWUTH CHAIMOOL
40
41. Unit-cell and 4 4 cells (p = 20, L1 = 18, L2 = 16, d = 1, unit: mm)
UNIT CELL
41
42. Side view of the metasurfaced patch antenna (h1 = 1.6, h2 = 6.0,
h3 = 0.8, unit: mm, FR4: P1 = P3 = 4.2) and top view of the patch
only (L = 28, W = 29, unit: mm)
Side View
42
Pendry showed that the negative permittivity could be achieved by aligning metallic wires along the direction of a wave whereas negative permeability by placing split ring with its axis along the direction of propagation of wave.
If a source is embedded in a substrate with zero index of refraction, then according to Snell's law, the exiting ray from substrate will be very close normal to the surface. Then, all the refracted rays will be in almost the same direction around the normal.
Through proper control of design parameters the near-zero index frequency region can be matched to the resonant frequency band of antenna
7*7 unit cell,
H is approximately λ0/2, where λ0 is the operating wavelength of the MPA.
Both results are after simulations after nzim peak gain is 7.65 dBi
Without it was 5.6dbiand if we use double layer it will come 8.26dbi
Both results are after simulations after nzim peak gain is 7.65 dBi
Without it was 5.6dbi
Electric permittivity (ε) and magnetic permeability (μ) are the two basic parameters of metamaterials.
GAIN BAND_IDTH AND IMPEDENCE BAND_IDTH NOT BEEN ACCOUNTED...
SNELLS LAW
2.45GHZ PATCH IS DESIGNED
3 TYPES OF NEAR ZERO
0.049lamda
ENHANCEMENT ON BROADSIDE DIRECTIVE AND BAND_IDTH OF PATCH ANTENNA
REDUCING BACK RADIATION
E’=17.4 U’=0.02 N’=0.77
8.1 Dbi 2.1 Dbi 6 db gain enhancement
10db band_idth is 2% increased to 15%
Gain of >7db is arranted in this range
Half po_er beam _idth
D=10log(30000/(______)
6.4 Dbi 9.5 Dbi
Refrative index = D(lambda)(square)/4(pi)A
Front to Backard radiation enhanced by 5.2 db.