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International Journal of Trend in Scientific Research and Development (IJTSRD)
Volume 5 Issue 5, July-August 2021 Available Online: www.ijtsrd.com e-ISSN: 2456 – 6470
@ IJTSRD | Unique Paper ID – IJTSRD43731 | Volume – 5 | Issue – 5 | Jul-Aug 2021 Page 4
The Novel Study of Metamaterial and Its Aspects
Manish Verma, SM Abbas
Scientist, DMSRDE, Kanpur, Uttar Pradesh, India
ABSTRACT
Stealth knowledge is used to make the object less observable and is
defined in terms of absorption of electromagnetic waves that is an
important research area used in defence research. Radar cross-section
is the proportion of the objective's capacity to reflect radar signals
toward the radar beneficiary. Some techniques such as shaping, radar
absorbing material (RAM), passive cancellation and active
cancellation have been used for RCS reduction purposes. For a long
time, radar absorbing material (RAM) has been actively pursued. For
RAM weight, design, thickness, mechanical strength and absorptivity
are key factors and therefore in the development of RAM, there is a
trade-off between weight and thickness of absorber material. Along
with this, an alternative to RAM is RAS and metamaterial are one of
the possible options. The metamaterial is lightweight and easy to use.
The Stealth property of metamaterial is based on material property
i.e., permittivity and permeability of material varying from small
positive to large negative values at a particular frequency. In this
paper, we hada novel study of metamaterial and its various aspects.
KEYWORDS: RCS, LO, Metamaterial, Absorber, RAM, Absorption,
Stealth
How to cite this paper: Manish Verma |
SM Abbas "The Novel Study of
Metamaterial and Its
Aspects" Published
in International
Journal of Trend in
Scientific Research
and Development
(ijtsrd), ISSN: 2456-
6470, Volume-5 |
Issue-5, August 2021, pp.4-7, URL:
www.ijtsrd.com/papers/ijtsrd43731.pdf
Copyright © 2021 by author(s) and
International Journal of Trend in
Scientific Research and Development
Journal. This is an
Open Access article
distributed under the
terms of the Creative Commons
Attribution License (CC BY 4.0)
(http://creativecommons.org/licenses/by/4.0)
I. INTRODUCTION
With WWII the Radar tracking and Surveillance
capability were developed to track and hit down
aircraft. Stealth is initially closely related to some
special form of low observable (LO) aircraft. This
was the beginning of Stealth in Defence [1,2]. As we
know the Radar is used to track aircraft on the
battlefield and they emit electromagnetic waves and
receive signals backscattered by the aircraft. Radar
cross-section (RCS) of aircraft is used to identify the
type of plane flying. The maximum detection range of
Aircraft by radar is proportional to the One-fourth
power of radar cross-section of aircraft. RCS [11] is
related to size, shape, material of aircraft and ratio of
incident and reflected power. On surveillance and
tracking a stealth Aircraft the radar measures reduced
radar cross-section (RRCS). Reduced Radar Cross
Section (RRCS) is obtained by methods such as
shaping, radar absorbing material, passive loading
and active loading. Initially shaping is used to
backscatter the radar signal. By shaping there is a
specular reflection of incident radiation from the
sharp edges and corners of aircraft. So, we use Radar
absorbing material (RAM) to absorb the incident
radiation to a certain extent (~ 90 % reflection loss).
For RAM weight, design, thickness, mechanical
strength and absorptivity are important factors [12-
16]. Moreover, by passive loading, passive materials
are aimed to modify the surface impedance to cancel
the scattered signal. Further in Active loading, active
material detects the incident radiation and emits a
signal of opposite phase and equal amplitude to
cancel the signal. In this paper metamaterial aspects
are being discussed.
The metamaterial is artificial engineered composite
materials. The history of metamaterial may be traced
back to 1898 by Sir J. C. Bose, who published work
on the rotation of the plane of polarisation by man-
made twisted structures. These man-made twisted
structures are called artificial chiral structures that
change the plane of polarisation. The metamaterial is
lightweight and easy to use and the metamaterial is an
engineered composite having properties not found in
nature. According to Veselago's theoretical
prediction, the permittivity and permeability of
artificial material are simultaneously negative. When
the electromagnetic wave travels in this medium then
the direction of the propagation vector is Left side
while in the conventional material propagation vector
is in the right direction. These materials are generally
known as Left-handed material (LHM). Thus, LHM
IJTSRD43731
International Journal of Trend in Scientific Research and Development @ www.ijtsrd.com eISSN: 2456-6470
@ IJTSRD | Unique Paper ID – IJTSRD43731 | Volume – 5 | Issue – 5 | Jul-Aug 2021 Page 5
has a pointing wave vector in a backward direction as
compared to right-handed materials. Due to its
specific properties, LHM has been of special interest
to defence applications, particularly stealth.
The present material shows that when a left-handed
material is used in an electromagnetic wave absorber,
more effective impedance matching can be done, and
absorption bandwidth can be expanded more. This
shows that left-handed material may be one of the
materials used to design electromagnetic wave
absorbers with good absorbability. Based on the
broad application of metamaterial from photovoltaic
to stealth, novel applications as metamaterial perfect
absorbers are also possible. For all metamaterial
absorbers studied so far are in the frequency of
operation in GHz/THz/IR, it can be used for defence
purposes too. In this paper, we are going to discuss a
few aspects of metamaterial in brief.
II. CONCEPT OF METAMATERIAL
The metamaterial is made of building blocks in the
same manner as the matter is made up of atoms. Also,
these building blocks are made up of conventional
materials. Metamaterial is usually lightweight and
easy to use and is the next level of the structural
hierarchy of atoms. The idea of metamaterial is
depicted in Figure 1.
Figure 1 Metamaterial with the many options
for inclusions [3,10].
From figure 1 metamaterial can have any shape and
size of its structural building blocks like split ring
resonator (SSR), hat resonator (HR), coupled ring
resonator (CRR) etc. Generally, metamaterial imply a
crucial case of a periodic lattice of identical elements
and thereby analogous for the crystal. The
metamaterial is an artificial engineered composite
material with properties not found in nature. The
metamaterial is having various properties like
reversed Doppler Effect, reversed Cerenkov radiation,
negative refractive index, super lenses, solar radiation
absorber.
III. THEORY OF METAMATERIAL
Metamaterial was first coined in the late 1990s[4,5].
Given Veselago's theoretical prediction that the
permittivity and permeability of metamaterial are
simultaneously negative. When an electromagnetic
wave propagates in this medium, then the direction of
the propagation vector is in the Left direction. He
establishes that in metamaterial the electric field
vector E. the magnetic field vector H and the
propagation wave vector k of a plane electromagnetic
waveform a left-handed system and these materials
are possible. The electromagnetic wave will convey
energy in the direction opposite to phase velocity.
Also, they obey the law of electrodynamics. These
materials are also known as Left-handed material.
Figure 2: Plane-wave in LHM
The Maxwell equation for the plane harmonic wave is
given as
(1)
Electric Field E, magnetic field H and propagation
vector k form a left-hand orthogonal system at close
to resonance frequency for material having real part
of electrical permittivity and magnetic permeability to
be negative. Medium possessing these values is a left-
handed medium (LHM) or DNG medium. In DPS
medium these vectors form right hand system[5,6].
The equation of energy density for DNG medium is
(2)
The necessary condition for energy density
simultaneous negative permittivity and permeability
is
(3)
This does not require ‘ε’ and ‘µ’ to be simultaneously
negative. But the DNG medium should necessarily be
dispersive [7].
IV. APPLICATIONS OFMETAMATERIALS
Metamaterials have shown several effects and devices
such as cloaking, superlenses, negative refraction,
etc., in which the µ, ε will be satisfied by periodic/
non-periodic arrays of magnetic or electric resonant/
International Journal of Trend in Scientific Research and Development @ www.ijtsrd.com eISSN: 2456-6470
@ IJTSRD | Unique Paper ID – IJTSRD43731 | Volume – 5 | Issue – 5 | Jul-Aug 2021 Page 6
non-resonant. The idea of simultaneous negative
permeability and permittivity was given by Veselago
in 1968. The idea was realized by Smith et al [6] in
2000 demonstrating a composite medium based on a
periodic array of inter-gap conducting SRR and
continuous wires that shows frequency region in
microwave region with simultaneously negative
values of effective permeability and permittivity.
Based on the above notion, electromagnetic absorbers
have been suggested where the path of the
electromagnetic wave is controlled by introducing
spatial variation in permeability and permittivity
parameters. Absorbers are basically of two types
namely, (a) interference absorbers, where reflection
occurring at the front surface of absorbers are
cancelled by destructive interference with wave
entering the layers and subsequently emergence (b)
antireflection coatings, where the absorber material is
so designed that no reflection takes place at the front-
facing surface and the attenuation in the layer
extinguishes the, entering waves [8]. The
metamaterial absorbers are made of periodic sub-
wavelength resonators and are considered
homogeneous mediums. The absorption in the
capability of metamaterial-based structures is entirely
dependent on the thickness and various structural
parameters of the periodic patterns. Metamaterial
absorbers have shown an increase in reflection loss as
compared to absorbers without layers of the
metamaterial. As the number of layers of
metamaterial is increased it found that reflection loss
also increases as compared to simulated results. Tao
et al. [9] designed the absorbers for the terahertz
frequency region. The strong absorption coefficient
makes this metamaterial spectrally selective THz
absorber. This is used in RCS reduction technology at
terahertz frequency where estimation of RCS of the
bigger object is accurate possible. Thus, the THz
metamaterial absorbers are engineered composite that
may be used in stealth.
V. CONCLUSION
There are a lot of opportunities for metamaterial
absorbers in the microwave and THz frequencies.
Metamaterial has a great deal of research interest in
high-frequency absorber applications. Due to their
resonant nature most of the metamaterial operate over
a narrow spectral range, impetus has been on making
absorbers with high-frequency tenability and
broadband/ multiple functionalities that support
stealth uses. Several metamaterial absorbers
development and theory are put forward for further
applications. Thus, metamaterial absorbers are
electromagnetic wave absorbers that are lightweight
and easy to use and metamaterial absorbers are
engineered composite having varying degrees of
stealth properties. Thus, RCS reduction may be done
by Metamaterial.
ACKNOWLEDGEMENT
We are highly thankful to N.E.Prasad, Sc-‘H’.
Director DMSRDE, Kanpur for his support for this
research works on metamaterial and its relevance to
stealth. Also, we are thankful to Sarvesh Kumar, Sc-
'F', Bhavana Srivastava, TO- ‘A’ for their support and
valuable inputs in this research paper.
REFERENCES
[1] Stonier, Roger A. "Stealth Aircraft and
Technology from World-War-II to The Gulf. 2.
Applications and Design." Sampe Journal 27.5
(1991): 9-18.
[2] John, D., and M. Washington. "USAF unveils
stealth fighter." Aviat Week Space Technol
129.November 14 (1988): 28-29.
[3] Nanostructured Metamaterials brochure.
EUROPEAN COMMISSION. Editor in Chief
Anne F. de Baas.
[4] Lakhtakia, Akhlesh, Werner S. Weiglhofer, and
Ian J. Hodgkinson. "Complex mediums II:
Beyond linear isotropic dielectrics." Complex
Mediums II: Beyond Linear Isotropic
Dielectrics 4467 (2001).
[5] Cai, Wenshan, and Vladimir M. Shalaev.
Optical metamaterials. Vol. 10. No. 6011. New
York: Springer, 2010.
[6] Kumar, M. Ashok, N. P. Anusha, and Alok
Sharan. "FDTD Modelling of 1D Photonic
Crystal for Thermal Masking Application with
CPML Absorbing Boundary Condition."
Defence Science Journal 67.2 (2017).
[7] Smith, David R., et al. "Composite medium
with simultaneously negative permeability and
permittivity." Physical review letters 84.18
(2000): 4184.
[8] Chatterjee, S. K., and Rajeswari Chatterjee.
"Some Recent Advances in Microwaves A
Review." Defence Science Journal 40.1 (1990):
25.
[9] Tao, Hu, et al. "Highly flexible wide angle of
incidence terahertz metamaterial absorber:
Design,fabrication,and
characterization." physical review B 78.24
(2008): 241103.
[10] Zheludev, Nikolay I., and Yuri S. Kivshar.
"From metamaterials to metadevices." Nature
materials 11.11 (2012): 917-924.
[11] Verma, Manish, S. M. Abbas, and N. E. Prasad.
International Journal of Trend in Scientific Research and Development @ www.ijtsrd.com eISSN: 2456-6470
@ IJTSRD | Unique Paper ID – IJTSRD43731 | Volume – 5 | Issue – 5 | Jul-Aug 2021 Page 7
"RCS reduction in context of stealth
technology: Theoretical Aspects."
[12] Tripathi, K. C., et al. "Electromagnetic &
microwave absorption properties of Carbon
black/PU di-electric Nano-composite absorber."
IJSART 1.7 (2015).
[13] Tripathi, K. C., et al. "Microwave Absorption
Properties of Carbon Black Nano-filler in PU
based Nano-composites." IJARSET 3.2 (2016).
[14] Tripathi, K. C., et al. "Electromagnetic and
Microwave Absorption Properties of Ni0. 5
Zn0. 5 Fe2O4 Nano Ferrite/PU Based Nano-
Composite." (2015): 19-25.
[15] Tripathi, K. C., et al. "Preparation and EM
Absorption Properties of Gamma (γ) Nano-
Ferrite in Epoxy Based Nano-Composites."
[16] Tripathi, Krishna Chandra, et al. "Microwave
absorbing properties of MWCNT/Carbon
black-PU Nano-composites." 2017 IEEE
International Conference on Power, Control,
Signals and Instrumentation Engineering
(ICPCSI). IEEE, 2017.

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The Novel Study of Metamaterial and Its Aspects

  • 1. International Journal of Trend in Scientific Research and Development (IJTSRD) Volume 5 Issue 5, July-August 2021 Available Online: www.ijtsrd.com e-ISSN: 2456 – 6470 @ IJTSRD | Unique Paper ID – IJTSRD43731 | Volume – 5 | Issue – 5 | Jul-Aug 2021 Page 4 The Novel Study of Metamaterial and Its Aspects Manish Verma, SM Abbas Scientist, DMSRDE, Kanpur, Uttar Pradesh, India ABSTRACT Stealth knowledge is used to make the object less observable and is defined in terms of absorption of electromagnetic waves that is an important research area used in defence research. Radar cross-section is the proportion of the objective's capacity to reflect radar signals toward the radar beneficiary. Some techniques such as shaping, radar absorbing material (RAM), passive cancellation and active cancellation have been used for RCS reduction purposes. For a long time, radar absorbing material (RAM) has been actively pursued. For RAM weight, design, thickness, mechanical strength and absorptivity are key factors and therefore in the development of RAM, there is a trade-off between weight and thickness of absorber material. Along with this, an alternative to RAM is RAS and metamaterial are one of the possible options. The metamaterial is lightweight and easy to use. The Stealth property of metamaterial is based on material property i.e., permittivity and permeability of material varying from small positive to large negative values at a particular frequency. In this paper, we hada novel study of metamaterial and its various aspects. KEYWORDS: RCS, LO, Metamaterial, Absorber, RAM, Absorption, Stealth How to cite this paper: Manish Verma | SM Abbas "The Novel Study of Metamaterial and Its Aspects" Published in International Journal of Trend in Scientific Research and Development (ijtsrd), ISSN: 2456- 6470, Volume-5 | Issue-5, August 2021, pp.4-7, URL: www.ijtsrd.com/papers/ijtsrd43731.pdf Copyright © 2021 by author(s) and International Journal of Trend in Scientific Research and Development Journal. This is an Open Access article distributed under the terms of the Creative Commons Attribution License (CC BY 4.0) (http://creativecommons.org/licenses/by/4.0) I. INTRODUCTION With WWII the Radar tracking and Surveillance capability were developed to track and hit down aircraft. Stealth is initially closely related to some special form of low observable (LO) aircraft. This was the beginning of Stealth in Defence [1,2]. As we know the Radar is used to track aircraft on the battlefield and they emit electromagnetic waves and receive signals backscattered by the aircraft. Radar cross-section (RCS) of aircraft is used to identify the type of plane flying. The maximum detection range of Aircraft by radar is proportional to the One-fourth power of radar cross-section of aircraft. RCS [11] is related to size, shape, material of aircraft and ratio of incident and reflected power. On surveillance and tracking a stealth Aircraft the radar measures reduced radar cross-section (RRCS). Reduced Radar Cross Section (RRCS) is obtained by methods such as shaping, radar absorbing material, passive loading and active loading. Initially shaping is used to backscatter the radar signal. By shaping there is a specular reflection of incident radiation from the sharp edges and corners of aircraft. So, we use Radar absorbing material (RAM) to absorb the incident radiation to a certain extent (~ 90 % reflection loss). For RAM weight, design, thickness, mechanical strength and absorptivity are important factors [12- 16]. Moreover, by passive loading, passive materials are aimed to modify the surface impedance to cancel the scattered signal. Further in Active loading, active material detects the incident radiation and emits a signal of opposite phase and equal amplitude to cancel the signal. In this paper metamaterial aspects are being discussed. The metamaterial is artificial engineered composite materials. The history of metamaterial may be traced back to 1898 by Sir J. C. Bose, who published work on the rotation of the plane of polarisation by man- made twisted structures. These man-made twisted structures are called artificial chiral structures that change the plane of polarisation. The metamaterial is lightweight and easy to use and the metamaterial is an engineered composite having properties not found in nature. According to Veselago's theoretical prediction, the permittivity and permeability of artificial material are simultaneously negative. When the electromagnetic wave travels in this medium then the direction of the propagation vector is Left side while in the conventional material propagation vector is in the right direction. These materials are generally known as Left-handed material (LHM). Thus, LHM IJTSRD43731
  • 2. International Journal of Trend in Scientific Research and Development @ www.ijtsrd.com eISSN: 2456-6470 @ IJTSRD | Unique Paper ID – IJTSRD43731 | Volume – 5 | Issue – 5 | Jul-Aug 2021 Page 5 has a pointing wave vector in a backward direction as compared to right-handed materials. Due to its specific properties, LHM has been of special interest to defence applications, particularly stealth. The present material shows that when a left-handed material is used in an electromagnetic wave absorber, more effective impedance matching can be done, and absorption bandwidth can be expanded more. This shows that left-handed material may be one of the materials used to design electromagnetic wave absorbers with good absorbability. Based on the broad application of metamaterial from photovoltaic to stealth, novel applications as metamaterial perfect absorbers are also possible. For all metamaterial absorbers studied so far are in the frequency of operation in GHz/THz/IR, it can be used for defence purposes too. In this paper, we are going to discuss a few aspects of metamaterial in brief. II. CONCEPT OF METAMATERIAL The metamaterial is made of building blocks in the same manner as the matter is made up of atoms. Also, these building blocks are made up of conventional materials. Metamaterial is usually lightweight and easy to use and is the next level of the structural hierarchy of atoms. The idea of metamaterial is depicted in Figure 1. Figure 1 Metamaterial with the many options for inclusions [3,10]. From figure 1 metamaterial can have any shape and size of its structural building blocks like split ring resonator (SSR), hat resonator (HR), coupled ring resonator (CRR) etc. Generally, metamaterial imply a crucial case of a periodic lattice of identical elements and thereby analogous for the crystal. The metamaterial is an artificial engineered composite material with properties not found in nature. The metamaterial is having various properties like reversed Doppler Effect, reversed Cerenkov radiation, negative refractive index, super lenses, solar radiation absorber. III. THEORY OF METAMATERIAL Metamaterial was first coined in the late 1990s[4,5]. Given Veselago's theoretical prediction that the permittivity and permeability of metamaterial are simultaneously negative. When an electromagnetic wave propagates in this medium, then the direction of the propagation vector is in the Left direction. He establishes that in metamaterial the electric field vector E. the magnetic field vector H and the propagation wave vector k of a plane electromagnetic waveform a left-handed system and these materials are possible. The electromagnetic wave will convey energy in the direction opposite to phase velocity. Also, they obey the law of electrodynamics. These materials are also known as Left-handed material. Figure 2: Plane-wave in LHM The Maxwell equation for the plane harmonic wave is given as (1) Electric Field E, magnetic field H and propagation vector k form a left-hand orthogonal system at close to resonance frequency for material having real part of electrical permittivity and magnetic permeability to be negative. Medium possessing these values is a left- handed medium (LHM) or DNG medium. In DPS medium these vectors form right hand system[5,6]. The equation of energy density for DNG medium is (2) The necessary condition for energy density simultaneous negative permittivity and permeability is (3) This does not require ‘ε’ and ‘µ’ to be simultaneously negative. But the DNG medium should necessarily be dispersive [7]. IV. APPLICATIONS OFMETAMATERIALS Metamaterials have shown several effects and devices such as cloaking, superlenses, negative refraction, etc., in which the µ, ε will be satisfied by periodic/ non-periodic arrays of magnetic or electric resonant/
  • 3. International Journal of Trend in Scientific Research and Development @ www.ijtsrd.com eISSN: 2456-6470 @ IJTSRD | Unique Paper ID – IJTSRD43731 | Volume – 5 | Issue – 5 | Jul-Aug 2021 Page 6 non-resonant. The idea of simultaneous negative permeability and permittivity was given by Veselago in 1968. The idea was realized by Smith et al [6] in 2000 demonstrating a composite medium based on a periodic array of inter-gap conducting SRR and continuous wires that shows frequency region in microwave region with simultaneously negative values of effective permeability and permittivity. Based on the above notion, electromagnetic absorbers have been suggested where the path of the electromagnetic wave is controlled by introducing spatial variation in permeability and permittivity parameters. Absorbers are basically of two types namely, (a) interference absorbers, where reflection occurring at the front surface of absorbers are cancelled by destructive interference with wave entering the layers and subsequently emergence (b) antireflection coatings, where the absorber material is so designed that no reflection takes place at the front- facing surface and the attenuation in the layer extinguishes the, entering waves [8]. The metamaterial absorbers are made of periodic sub- wavelength resonators and are considered homogeneous mediums. The absorption in the capability of metamaterial-based structures is entirely dependent on the thickness and various structural parameters of the periodic patterns. Metamaterial absorbers have shown an increase in reflection loss as compared to absorbers without layers of the metamaterial. As the number of layers of metamaterial is increased it found that reflection loss also increases as compared to simulated results. Tao et al. [9] designed the absorbers for the terahertz frequency region. The strong absorption coefficient makes this metamaterial spectrally selective THz absorber. This is used in RCS reduction technology at terahertz frequency where estimation of RCS of the bigger object is accurate possible. Thus, the THz metamaterial absorbers are engineered composite that may be used in stealth. V. CONCLUSION There are a lot of opportunities for metamaterial absorbers in the microwave and THz frequencies. Metamaterial has a great deal of research interest in high-frequency absorber applications. Due to their resonant nature most of the metamaterial operate over a narrow spectral range, impetus has been on making absorbers with high-frequency tenability and broadband/ multiple functionalities that support stealth uses. Several metamaterial absorbers development and theory are put forward for further applications. Thus, metamaterial absorbers are electromagnetic wave absorbers that are lightweight and easy to use and metamaterial absorbers are engineered composite having varying degrees of stealth properties. Thus, RCS reduction may be done by Metamaterial. ACKNOWLEDGEMENT We are highly thankful to N.E.Prasad, Sc-‘H’. Director DMSRDE, Kanpur for his support for this research works on metamaterial and its relevance to stealth. Also, we are thankful to Sarvesh Kumar, Sc- 'F', Bhavana Srivastava, TO- ‘A’ for their support and valuable inputs in this research paper. REFERENCES [1] Stonier, Roger A. "Stealth Aircraft and Technology from World-War-II to The Gulf. 2. Applications and Design." Sampe Journal 27.5 (1991): 9-18. [2] John, D., and M. Washington. "USAF unveils stealth fighter." Aviat Week Space Technol 129.November 14 (1988): 28-29. [3] Nanostructured Metamaterials brochure. EUROPEAN COMMISSION. Editor in Chief Anne F. de Baas. [4] Lakhtakia, Akhlesh, Werner S. Weiglhofer, and Ian J. Hodgkinson. "Complex mediums II: Beyond linear isotropic dielectrics." Complex Mediums II: Beyond Linear Isotropic Dielectrics 4467 (2001). [5] Cai, Wenshan, and Vladimir M. Shalaev. Optical metamaterials. Vol. 10. No. 6011. New York: Springer, 2010. [6] Kumar, M. Ashok, N. P. Anusha, and Alok Sharan. "FDTD Modelling of 1D Photonic Crystal for Thermal Masking Application with CPML Absorbing Boundary Condition." Defence Science Journal 67.2 (2017). [7] Smith, David R., et al. "Composite medium with simultaneously negative permeability and permittivity." Physical review letters 84.18 (2000): 4184. [8] Chatterjee, S. K., and Rajeswari Chatterjee. "Some Recent Advances in Microwaves A Review." Defence Science Journal 40.1 (1990): 25. [9] Tao, Hu, et al. "Highly flexible wide angle of incidence terahertz metamaterial absorber: Design,fabrication,and characterization." physical review B 78.24 (2008): 241103. [10] Zheludev, Nikolay I., and Yuri S. Kivshar. "From metamaterials to metadevices." Nature materials 11.11 (2012): 917-924. [11] Verma, Manish, S. M. Abbas, and N. E. Prasad.
  • 4. International Journal of Trend in Scientific Research and Development @ www.ijtsrd.com eISSN: 2456-6470 @ IJTSRD | Unique Paper ID – IJTSRD43731 | Volume – 5 | Issue – 5 | Jul-Aug 2021 Page 7 "RCS reduction in context of stealth technology: Theoretical Aspects." [12] Tripathi, K. C., et al. "Electromagnetic & microwave absorption properties of Carbon black/PU di-electric Nano-composite absorber." IJSART 1.7 (2015). [13] Tripathi, K. C., et al. "Microwave Absorption Properties of Carbon Black Nano-filler in PU based Nano-composites." IJARSET 3.2 (2016). [14] Tripathi, K. C., et al. "Electromagnetic and Microwave Absorption Properties of Ni0. 5 Zn0. 5 Fe2O4 Nano Ferrite/PU Based Nano- Composite." (2015): 19-25. [15] Tripathi, K. C., et al. "Preparation and EM Absorption Properties of Gamma (γ) Nano- Ferrite in Epoxy Based Nano-Composites." [16] Tripathi, Krishna Chandra, et al. "Microwave absorbing properties of MWCNT/Carbon black-PU Nano-composites." 2017 IEEE International Conference on Power, Control, Signals and Instrumentation Engineering (ICPCSI). IEEE, 2017.