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Tianxia Zhao

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Title: Tianxia Zhao


1
Beauty and Application of Periodic Structures
Tianxia Zhao
2
Introduction
  • Periodic structures in nature have fascinating
    characteristics.
  • When these structures interact with
    electromagnetic waves many unique features result
    such as stop-band, pass-bands, and band-gaps.
  • Various terminology have been used to classify
    these structures depending on the domain of the
    applications in filter design frequency
    selective surface(FSS), photonic crystals and
    band-gaps(PBG), and meta-materials and
    Electromagnetic band-gaps(EBG).
  • Broadly speaking, EBG structures are 3-D periodic
    objects that prevent the propagation of the
    electromagnetic waves in a specified band of
    frequency for all angles of arrival and for all
    polarization states of EM waves.
  • Brief introduction for each terminology and some
    representative application will be given at each
    section.

3
Outline
  • Natural periodic structures
  • Periodic structures in EM
  • Phased array antenna
  • Leaky wave antenna
  • Frequency selective surface(FSS)
  • Photonic crystal(photonic band-gap PBG
    structures)
  • 1D PC
  • 2D PC
  • 3D PC
  • Metamaterials and EBG(electromagnetic band-gap
    structure)

4
Natural Periodic Structures
Crystal structure
Butterfly wings
Bee hive
5
Section I Periodic structures in
electromagnetic applications
  • Part 1. Phased array antenna
  • application in radar system and
    satellite TV or
  • communication
  • Part 2. Leaky wave antenna
  • leaky wave antenna changes a
    wave-guiding structure into a
  • radiating structure
  • Part 3. Frequency selective surface
  • FSS as band-pass, band-stop filters,
    and application in
  • radomes, thermovoltaic system

6
Part I What is Phased Array antenna
  • Phased-array antennas contain a multitude of
    radiating elements, typically arranged in a
    rectangular or triangular tessellation.
  • Array of Antenna element with phase ( and
    sometimes, the amplitude) of each element being a
    variable.
  • Phased Array antenna can control the radiation
    beam direction and pattern shape including side
    lobes.
  • When the phase change is accomplished by varying
    the frequency, its called frequency scanning
    arrays.

7
The structure of Phased array antenna
Single antenna element and its radiation pattern
Phased array antenna and its radiation pattern
8
Phased array antenna in radar application
  • Extreme beam agility
  • Mechenical scanning takes 1 second while
    electronic scanning takes less than 1 ms.
  • Reducing antenna radar cross section
  • Advanced beam forming capabilities
  • High reliability and Less structural intrusion

Radiation deflected from threat antenna
Stationary phased array antenna
Phased array antenna application in radar system
9
Phased array antenna Application in DBS
Big Ugly dish(BUD)
The planar microstrip antenna array
Direct broadcast satellites
10
Part II 2D Leaky-Wave Antenna
  • Guiding Stucture In electromagnetics and
    communication engineering and optics, a waveguide
    is a physical structure that guides any
    electromagnetic waves or light. Metallic,
    dielectric waveguide and planar transmission line
    are all wave guiding structures.
  • Leaky wave antenna changes a guiding
  • structure into a radiation structure.

Metallic Waveguide
Leaky wave antenna radiation from a guiding
structure
11
2D Periodic Leaky-Wave Antenna
y
z
x
x

h
b
W
a
L
2D LWA using metal patches
z
x
h
2D LWA using slots
12
Design principle of 2D LWA
  • The source launches a parallel-plate mode (n1)
    that is leaky due to radiation through the
    PRS.
  • The substrate thickness h controls the beam
    angle.
  • The PRS controls the beamwidth.

13
Radiation Pattern Slot LWA
Slot LWA
Hplane patterns for ?r 2.2 (Slot
LWA) changing substrate thickness f 12 GHz, l
0.6 cm, w 0.05 cm, a 1.0cm, b 0.3 cm
14
Applications of LWA
  • Leaky-wave application based on the higher order
    modes of planar transmission lines possess the
    advantage of higher gain, wider bandwidth,
    frequency scanning.
  • LWA can be made electronically steerable using a
    tunable ferroelectric material whose dielectric
    properties is controlled by a bias voltage
    applied to the traveling waveguide.
  • Leaky wave waveguide antenna used in vehicular
    radar antenna arrays that can be blended into
    surfaces curved in two dimensions.

15
Frequency Selective Surface(FSS)
  • What is FSS?
  • A FSS is any surface construction designed as a
    filter for plane waves
  • Angular/frequency dependence
  • Band pass/ band stop behavior
  • FSS characteristics
  • Typically narrow band
  • Periodic, typically in 2 dimensions
  • FSS Degrees of Freedom
  • Element type dielectric or metallic/circuit
  • Element size,shape and loading
  • Element spacing and orientation

16
printed dipole FSS structures
17
Complementary surfaces-slot FSS
18
Slot Vs Dipoles FSS
19
Applications of FSS
  • Traditional Applications
  • Radomes
  • Dichroic subreflectors
  • Reflect array lense
  • Recent Applications
  • RFID
  • Collision avoidance
  • RCS augmentation
  • Robotic guided paths
  • EMI protection
  • Photonic bandgap structures
  • Waveguide or cavity controlled coupling
  • Low-probability of intercept systems(e.g.
    stealth)

20
FSS applications- radome
Radome must be transparent at operating
frequency. Radome protects antenna from the
environment. Radome will affect the antenna
pattern by refraction from radome wall, loss from
radome materials and multiple reflection, and
increased sidelobes from multiple reflection.
21
FSS radome
Bandpass radome is constructed from one or more
metallic screens sandwiched between dielectric
slabs
22
Application of FSS with antenna
Surface wave elimination
23
application of FSS
Thermovoltaic system
24
Section II- PBG structure
Butterfly P. Nireus
The blue-green color on several species of
African butterflies is caused by the nanoscale
structure of the insects wings
25
Explaination for butterfly wings
  • Optical physicist studied the scales that make up
    the brightly colored regions of the creatures
    wings.
  • These scales contain a pigment that absorbs
  • light at wavelengths of around 420
    nanometers-
  • roughly sky blue- and radiates it at 505 nm
  • in the blue-green region where butterfly
  • eyes are particularly sensitive.
  • Underneath the pigment slab
  • are layers of reflective surfaces
  • natural versions of
  • distributed bragg reflector mirrors.
  • The butterfly's "mirrors" are tuned
  • to reflect blue-green light.

26
What is bragg reflector
  • What is distributed bragg reflector
  • In guided wave optics, a distributed Bragg
    reflector (DBR) is a structure formed from
    multiple layers of alternating materials with
    varying refractive index, or by periodic
    variation of some characteristic (such as height)
    of a dielectric waveguide, resulting in periodic
    variation in the effective refractive index in
    the guide. Each layer boundary causes a partial
    reflection of an optical wave, and for waves with
    optical wavelength such that the many reflections
    combine with constructive interference, a high
    quality reflector is formed.

Lights with different colors reflected by the
evenly-spaced data track of CD surface at
different angles
27
Explanation of butterfly wings
  • Just above the mirror, is a slab of material
    filled with hollow cylinders of air that run
    perpendicular to the mirror. These cylindrical
    holes channel the light away from the reflector,
    preventing it from getting trapped. The slab, is
    what optical physicists call a photonic crystal.
  • The combined effect of the reflectors and the
    structure of the slab, is a much brighter
    blue-green fluorescence than could be achieved
    with pigment alone.
  • The brighter wings allow the butterflies to
    better signal to each other.

28
photonic crystal(photonic bandgap structure)
  • Photonic crystals are periodic dielectric or
    metallo-dielectric nanostructures
  • PC or PBG structure affect the propagation of
    electromagnetic wave (EM) in the same way as the
    periodic potential in a semiconductor crystal
    affects the electron motion by defining allowed
    and forbidden electronic energy bands.
  • The absence of allowed propagating EM modes
    inside the structures, in a range of wavelengths
    called a photonic bandgap,
  • Optical phenomena such as inhibition of
    spontaneous emission, high-reflecting
    omnidirectional mirrors and low-loss-waveguiding
    among others.

29
1D photonic crystal
  • Application of 1D photonic crystal
  • Perfect dielectric mirror
  • The reflectivity of photonic crystals derives
    from their geometry and periodicity, not a
    complicated atomic-scale property (unlike
    metallic components mirror).
  • For the frequency range of interest, the
    material should be essentially lossless.
  • Such materials are widely available all the way
    from the ultraviolet regime to the microwave.

30
2D photonic crystal fiber
  • Photonic-crystal fiber, which use a nanoscale
    structure to confine light with radically
    different characteristics compared to
    conventional optical fiber for applications in
    nonlinear devices, guiding exotic wavelengths,
    and so on.

Conventional optical fiber
31
2D photonic crystal fiber
  • Hollow-core Bandgap Fibers

Photonic Crystal
32
Application of 2D photonic crystal
Waveguides and junctions
33
3D Photonic crystal
I.
II.
Experimental realization of the three-dimensional
layer-by-layer structure
34
light emitting diodes (LED)
  • Light-emitting diodes use semiconductor material
    that converts electrical current to light of a
    particular wavelength.
  • The improved design of ultra-high-efficiency
    light-emitting diodes can borrow from butterfly
    wings.
  • The butterfly wings Distributed Bragg reflectors
    are not perfect. Some light always becomes
    trapped on the surface of the reflector and is
    lost.
  • But in each scale, sitting just above the mirror,
  • cylindrical holes (photonic crystal.)
    channel the light away from the reflector,
    preventing it from getting trapped.
  • Light-emitting diodes based on this design
    principle would be much more efficient than
    today's models, which scatter light in all
    directions, causing much of the light they
    produce to be reabsorbed by the devices'
    material.

35
Section III- Metamaterials
  • a. Metamaterial is an artificial material whose
    permittivity and permeability are both negative.
  • b. Why it is artificial? Such materials possess
    engineered effective electromagnetic properties
    resulting from response functions not found in
    constituent materials and not readily observed in
    nature.

Negative refraction index
Positive refraction index
a. Based on definition of J.Pendry 2000
36
Introduction
  • Difference between PBG and meta-material
  • PBG exhibit stop bands as a result of Bragg
    reflection
  • and often implies structure in higher
    frequency regions (optics).
  • Metamaterial is a general electromagnetics
    term which covers
  • optics and photonics. It is an object
    that gains its (electromagnetic) material
    properties from its structure rather than
    inheriting them directly from the materials it is
    composed of. PBG materials are an example of an
    artificial visible light metamaterials.
  • Negative e already exist at optical frequencies,
    but less
  • explored at lower frequencies.
  • Natural material exist with a
    negative permittivity typically
  • ferroelectrics.
  • Negative permeability (µlt0) is the
    challenge.
  • Wires and SRR (split ring resonators) are
    conducting elements
  • that can be possible artificial
    structures, especially at lower
  • frequencies.

37
Metamaterial design- negative µ
SRR-split ring resonator
From Dana V. Radovic etc. XII telecom Forum
38
Metamaterial design- negative e
  • To obtain negative permittivity medium, thin
    metallic wires are arranged periodically.
    Effective permittivity takes negative plasma
    frequency.
  • Negative e and µ can be achieved simultaneously.

39
Metamaterial Application
Negative phase velocity, reversal of Doppler
Effect and Backward Cerenkov radiation are
interesting novel physical properties emerging
from left-handed metamaterials phenomena. Science
magazine listed metamaterial top ten
breakthrough in 2003
40
Summary
  • In this presentation, many applications based on
    periodic structures are introduced.
  • For phased array antenna, the control of phases
    from different array element will change the
    total radiation pattern.
  • For leaky wave antenna, the type of wave (wave
    number) is changed from guided mode to leaky
    radiation mode.
  • Inspired by some fascinating phenomenon from
    periodic structures new nanostructured devices at
    optical frequencies combines the electronic
    functions are being designed, PBG,EBG or
    metamaterials can lead to revolutionary optical
    components.

41
Thank you
42
Band-Structure(Brilloun Diagram)
a period, k0 2? / ?0 , ? 2 ? / ?g
?-1 a ?0 a - 2?
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