huygens’ metasurfacesfor antenna · pdf file · 2016-12-29huygens’...
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Huygens’ Metasurfaces for Antenna Applications
George V. Eleftheriades
The Edward S. Rogers, Sr. Department of Electrical and Computer EngineeringUniversity of TorontoCANADACANADA
29-Dec-16
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ACKNOWLEDGEMENTACKNOWLEDGEMENT Dr Ariel Epstein Dr. Ariel Epstein Michael Selvanayagam Joseph Wong Trevor Cameron Michael Chen Alex Wong Alex Wong Min Kim
229-Dec-16
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OVERVIEW Active Huygens’ Metasurfaces for
CloakingCloaking Scalar Passive Huygens’ Metasurfaces
R f ti M t f Refracting Metasurfaces Tensor and Chiral Huygens’ Metasurfaces Shaping the Radiation of Closeby Sources Reflectionless Huygens’ Metasurfaces Reflectionless Huygens Metasurfaces Optical Metasurfaces
Oth A t A li ti Other Antenna Applications Summary 3
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Stealth: Scattering re-directionStealth: Scattering re-direction Use shaped or engineered surfaces to
fl t EM i lreflect EM-waves in non-speculardirections
Examples:
Davenport, C.J.; Rigelsford, J.M., "Specularp , ; g , , pReflection Reduction Using Periodic Frequency Selective Surfaces," Antennas and Propagation, IEEE Transactions on , vol.62, no.9, pp.4518,4527, Sept. 2014 Can be detected with multistatic radar
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METAMATERIAL CLOAKINGMETAMATERIAL CLOAKING
Transformation: Fabrication: Measurement:
However cloak too bulky on the order of the size of the object
D. Schurig, J. J. Mock, B. J. Justice, S. A. Cummer, J. B. Pendry, A. F. Starr, and D. R. Smith, “MetamaterialElectromagnetic Cloak at Microwave Frequencies,” Science, vol. 314, no. 5801, pp. 977–980, 2006.
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ACTIVE CLOAKINGACTIVE CLOAKING(equivalence principle)
is EnM
ˆˆ
(c) The superposition of (a) and (b) such that the
(a) Scattering of a plane wave off of a
(b) An equivalent scenario where electric and magnetic
is HnJ ˆ
(a) and (b) such that the scattered and interior fields are cancelled out.
plane wave off of a cylindrical object.
gcurrent densities on the surface of the cylindrical object radiate the scattered field
M. Selvanayagam, G.V. Elefteriades, IEEE AWPL. 2012
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H ’ S U it C ll0 dB
H−Plane
Huygens’ Source Unit Cells
−24
−16
−8
0 dB
60o
30o−30o
−60o
H−PlaneE−Plane
−32
−24
90o
60−60
−90o
−120o 120o
JsMs
−150o
180o150o
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ACTIVE CLOAKINGACTIVE CLOAKING
J t d ( ) t l li d ithJust surround a (say) metal cylinder with magnetic dipoles (loop antennas) to createa magnetic current that cancels out the scattereda magnetic current that cancels out the scattered field.
M. Selvanayagam and G.V. Eleftheriades, IEEE AWPL, 2012
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CloakingCloakingCloak Design
12 total small loops to form an arra 12 total small loops to form an array
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CloakingCloakingCloak Design
Cloak consists of loop antennas (magnetic dipoles) Fed through phase shifters (outside waveguide)
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Measurement SetupMeasurement Setup
d d O t id W idInside Waveguide Outside Waveguide
M. Selvanayagam and G.V. Eleftheriades, Phys. Rev. X, 2013
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Fullwave SimulationFullwave SimulationWithout active cloak With active cloakWithout active cloak With active cloak
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MeasuredMeasured
Measured Fields: Scattering off of a t lli li d
Measured Cloak: note that the wavefrontsnow pass around themetallic cylinder.
Note the shadow region
now pass around the cylinder as if it was not there
M. Selvanayagam and G.V. Eleftheriades, Phys. Rev. X, 2013
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Cl ki M d WCloaking: Measured Waves
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Camouflage Results
Small Metallic Cylinder Disguise Dielectric Cylinder Disguise
Measured Scattering off of Measured Scattering off of disguised cylinder. Note how the
disguised cylinder. Note the smaller shadow region
g yshadow regions has been modified
Simulated dielectric cylinder (COMSOL)
Simulated smaller cylinder (COMSOL)
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Huygens’ MetasurfaceHuygens MetasurfaceDescription (equivalence principle)
[1] M. Selvanayagam and G.V. Eleftheriades, Optics Express, 2013[2] C Pfeiffer and A Grbic Physical Review Letters 2013
29-Dec-16
[2] C. Pfeiffer and A. Grbic, Physical Review Letters, 2013
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W f t Sh iWavefront Shaping
JSMS
y
xz
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Motivation: Thin Surfaces for Complete EM-control
(magnitude, phase, polarization; no or small reflections)
Traditional Transmit-arrayThin (/10) Huygens’ metasurfaceNo spurious Floquet modes
A. Epstein and G.V. Eleftheriades, ``Floquet-Bloch analysis of refracting metasurfaces ", Phys. Rev. B, 90, 235127 , Dec. (2014).
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Huygens’ MetasurfaceHuygens Metasurface DescriptionImpedance Boundary Condition:
Admittance Boundary Condition:
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Lattice Network Model Impedances:
Circuit Equations:
Field Boundary Cond.:
M. Selvanayagam and G.V. Eleftheriades, IEEE AWPL, 2013
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2D Refraction
29-Dec-16
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Impedance and Admittance pSpatial ProfileElectric Impedances:
Magnetic Admittances:
29-Dec-16 M. Selvanayagam and G.V. Eleftheriades, Optics Express, 2013
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2D Impedance Xse Profilep se
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Unit-Cell Geometryy
29-Dec-16
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A 2D-Refractive Metasurface
J.P.S. Wong, M. Selvanayagam and G.V. Eleftheriades, “Characterization of Huygens metasurfaces for 2D refraction”,IEEE Trans. on Microwave Theory and Techn., 2015.
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Experimental Setupp pWaveguide Probe Rexolite Lens
Huygens’ Metasurface Conical Horn
29-Dec-16
Huygens Metasurface
Rotary PostConical Horn
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Near-Field Isosurfacesz
y
x
29-Dec-16
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Far-Field Pattern
20 04°-20.04°
29-Dec-16
21.83°
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Far-Field Pattern Cuts @ 10GHz0
Far Field Pattern Cuts @ 10GHz
−20
−10
(dB
)
−30
−20
Am
plitu
de (
dB
−50
−40
A
Azimuth CutElevation Cut
−100 −80 −60 −40 −20 0 20−50
Angle (°)
Elevation Cut
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Measured EfficiencyMeasured Efficiency95
85
90 (
%)
75
80
Effi
cien
cy (
%
70
75E
−20 −10 0 10 20 30 40 5065
θi (°)
29-Dec-16 30
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2D Focusingg
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G i B F iGaussian-Beam Focusing
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TENSOR HUYGENS’ METASURFACESTENSOR HUYGENS’ METASURFACES
M. Selvanayagam and G.V. Eleftheriades, “Polarization control using tensor Huygens Surfaces”, IEEE Trans. on Antennas and Propagat. , vol. 62, no. 12, pp. 6155-6168, Dec. 2014.
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A 90 d P l i ti R t tA 90-degree Polarization Rotator
Cascaded and rotated metasurfaces create a bianisotropic effect
Y. Zhao, M. Belkin, and A. Al`u, “Twisted optical metamaterials for planarized ultrathin broadband circular polarizers,” Nature Communications, vol. 3, p. 870, 2012.
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M tMeasurement0° 30° 60°0 30 60
90° 120° 150°
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Circular Polarization SelectiveCircular Polarization Selective Surface (CPSS)For a circular polarization selective surface we need just three layersFor a circular polarization selective surface we need just three layers. Here our surface transmits right-handed CP while reflecting left-handed CP.
The three layers are shown here.The layers sit on a Rogers substrate and are separated by a λ/7 gap. The total thickness is < λ/2The total thickness is < λ/2. Compared to tradiotcal designs, that design required 7-layers and is 1.6λ thick.We can see that at 10GHz that right-handed CP is transmitted while left-handed CP is reflected.
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F b i t d CPSSFabricated CPSS
37
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4-Port Quasi-Optical Measurements4 Port Quasi Optical Measurements
LensDUT
OMT
Circular
Lens CircularHorn
DUT
VNA
HornOMT
M. Selvanayagam and G.V. Eleftheriades, ``Design and measurement of tensor impedance transmitarrays for chiral polarization control", IEEE Trans. on Microwave Theory and Techn., vol. 64, pp. 414-428, Feb. 2016.
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Measured Results
L ft h d d CP /Ri ht h d d CP i fl t d
39
Left-handed CP passes/Right-handed CP is reflected
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Measured Results
40
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Arbitrary sources to directiveArbitrary sources to directive radiation
zLongitudinal wavenumber
y
z
kwavenumber
x
ytk
Transverse
ε1ε2
inc 0,2 2
tjk yj ztx t
I dkE y z k f k e e
Source
Transverse wavenumber
PEC
ref 0,2 2
tjk yj ztx t t
I dkE y z k k f k e e
I dk
Source
Reflection
Transmission trans 0,
2 2tjk yj zt
x tI dkE y z k T k e e
Transmission
Degrees of FreedomDegrees of FreedomA. Epstein and G.V. Eleftheriades, ``Passive lossless Huygens metasurfaces for conversion of arbitrary source field to directive radiation ",IEEE Trans. on Antennas and Propagat. , vol. 62, no. 11, pp. 5681-5695, Nov. 2014.
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Passive and Lossless Designg
Local impedance Local impedance equalization kReflection =
outoutcos
Z
tkReflection
out
out
cosFresnel:cost
kkk
inc ref
inc refx x
y y
E y E yH y H y
Local power conservation 2,0W y
Aperture follows Transmission
* ,0x yE H y
incident power profile
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Huygens’ Metasurface (HMS) Designyg ( ) g
Source trans trans,E H
outcos sin, outjkz jkyW y z e e
Source, reflection, transmissiontransmission stipulated inc inc,E H
ref ref,E H
PhaseMagnitude
out
i f
,0 siny ky
out, 0 ,0cos cot
2 2
0 0
sm
y yY y j
inc ref,0 ,0 ,0x xy E y E y
out
, 0 ,0cot
2cos 2se
y yZ jy
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El t i Li SElectric Line Sourceoutθ = 0° outθ = 30° outθ = 60°
Finite-element simulation
out out out
simulation(“Implementation”)
y y y
z
Semi-analytical
y y y
ytheory
(Design)
y y y
z
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El t i Li SElectric Line Source
outθ = 0° outθ = 30° outθ = 60°
Fi i l i l i S i l i l hFinite-element simulation(“Implementation”)
Semi-analytical theory(Design)
A. Epstein and G.V. Eleftheriades, ``Passive lossless Huygens metasurfaces for conversion of arbitrary source field to directive radiation ",
IEEE Trans. on Antennas and Propagat. , vol. 62, no. 11, pp. 5681-5695, Nov. 2014.
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Electric Line Source and PECElectric Line Source and PEC
“Implementation”
Finite elements simulation
z
Design y
Semi-analytical
theory
z
y
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Cavity-excited HMS antenna (solves the aperture efficiency vs radiation efficiencyaperture efficiency vs radiation efficiency tradeoff in leaky-wave antennas)
Experiment
20GHzf
Experiment
Full-wave(Discretization
, losses)
88% 86% 87%
d 'z
Semianalytical97% 94% 95%
d
Semianalytical
A. Epstein, JPS Wong, GV Eleftheriades Nature Comm., Jan. 2016
L N
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Control of Radiation PatternControl of Radiation Pattern
Reduced side lobe level Direction of main beamReduced side-lobe level SLL= -20dB
(10dB reduction)
Direction of main beamθout=30°
(10dB reduction)
Full-wave(Discretization,
losses)81% 83% 85%
Semianalytical 92% 97% 93%y
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Switched beam Antenna20GHzf
Switched-beam AntennaAperture efficiency
Directivity [dBi]
3dB BeamwidthMain beamShift 20GHzf
M y
5
HMS
efficiency[dBi]Beamwidth
HFSSTheoryHFSSTheoryHFSSTheor
yHFSSTheory
sJ y sM y
32.4PEC
67%86%13.214.312.1°10.1°0°0°Δy=060%83%12.714.112.7°10.2°・9.8°・9.5°Δy=±0.6λ
59%72%12 413 312 7°10 7°・20 518 °Δ 1 2λ 59%72%12.413.312.7°10.7°20.5°・18.7°Δy=±1.2λ
Semianalytical Full-wave0 0
0dB
60
30-30
-60 60
30-30
-60
49
0dB
-90 90 -20dB
-10dB 0dB
-90 90 -20dB
-10dB
Switched-beam antenna Summary
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Ω‐Bianisotropic MetasurfacespHuygens’ metasurfaces
Ω-Bianisotropic metasurfaces
Electric impedance Magnetic admittance
Electric impedance Magnetic admittance Magnetoelectric Magnetoelectric
coupling
M
M
H sM
H sM
sJ
E
sJ
E sM
EsJ
Y. Ra’di, V. Asadchy and S. A. Tretyakov, IEEE Trans. Antennas Propag., 62, 7 (2014). J. Wong, A. Epstein, and GV Eleftheriades, IEEE Antennas Wireless Propag. Lett. , vol 15, (2016).
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Extreme Angle RefractionExtreme Angle RefractionRefraction Beam splitter
0° 80°Efficiency:
98 9%
0° 72°Efficiency:
99 5%
0° ±72°Efficiency: 98% (1:1)
98.9%(Huygens’: 50%)
99.5%(Huygens’: 73%)
* J. Wong, A. Epstein, and GV Eleftheriades, IEEE Antennas Wireless Propag. Lett. , (2016).* Epstein and Eleftheriades, accepted to APS/URSI Puerto Rico (2016).
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Floquet-Bloch (FB) analysis (arbitrary angle of incidence)
Refracting HMS in out Refracting HMS
Designated excitation
out in
out out
sin sin1 cot2 2
se smZ y Y yZ
jky
Y
in out
Designated excitationOnly two FB modes:
specular reflection and desirable refraction (the rest k I desirable refraction (the rest vanish, unlike grating)
Arbitrary ray excitationsR f ti ( 1) i
in incos sininc 0
cos sinref 0
,2
n n
jkz jkyx
jkz jky
k IE y z e e
k IE y z e e
R
in in
Refraction (n=1) is dominant over scattering to other directions (little sensitivity to angle of
cos sintrans 0
,2
,2
n n
xn
jkz jkyx
n
E y z e e
k IE y z e e
n
nT
R
in in sensitivity to angle of incidence)
2 n
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Floquet-Bloch AnalysisFloquet Bloch AnalysisRefractionEfficiency
Angle of incidence
Metasurface
ArbitraryHuygens’
2 2out0 1
in
cos 1 1cos
in in
DesignatedHuygens’
in2out
0in
cos 1cos
DesignatedΩ‐Bianisotropic 1p
in
A. Epstein and G.V. Eleftheriades, ``Floquet-Bloch analysis of refracting metasurfaces ", Phys. Rev. B, 90, 235127 , Dec. (2014).
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HMS Vs. Ω-BMS
20GHzf 20GHzf 20GHzf 20GHzf
Full-wave Full-wave
10mil
LFull-wave(Discretization,
losses)88% 100%
Full-wave(Discretization)apt L
effL
Semianalytical 97% 100% Semianalytical
2 /D effL
Arxiv:1604.0110100v1 10L 10L
1.61d 0.81d
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Advanced Pattern ControlAdvanced Pattern ControlBinomial virtual array(L=10λ)
Chebyshev virtual array (L=10λ SLL=-30dB)(L=10λ) (L=10λ, SLL=-30dB)
300
-30
300
-30
300
-30 300
-30
-20dB -10dB
0dB60-60
-20dB -10dB
0dB60-60
-20dB -10dB
0dB60-60
-20dB -10dB
0dB60-60
-90 90Full-wave (TLM)Semianalytical
-90 90Full-wave (TLM)Semianalytical
-90 90Full-wave (TLM)Semianalytical
-90 90Full-wave (TLM)Semianalytical
-150180
150
HPBWTLM=6.81[deg], DTLM = 16.9658[dB] HPBWanal=6.33[deg], Danal = 17.3539[dB]
-150180
150
HPBWTLM=6.81[deg], DTLM = 16.9658[dB] HPBWanal=6.33[deg], Danal = 17.3539[dB]
-150180
150
HPBWTLM=13.73[deg], DTLM = 13.7774[dB] HPBWanal=13.49[deg], Danal = 13.9864[dB]
-150180
150
HPBWTLM=13.73[deg], DTLM = 13.7774[dB] HPBWanal=13.49[deg], Danal = 13.9864[dB]
57
80 80
BMS modal refl. coeff.: MANY degrees of freedom!
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Optical Huygens’ Metasurfaces( l t h & it d t l)(complete phase & magnitude control)
Each unit-cell simultaneously employs both electric and magnetic resonances and mimics a Huygens’ source
M. Kim, A. Wong and G.V. Eleftheriades, Phys. Rev. X, Dec. 2014
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Optical Huygens’ MetasurfacesOptical Huygens Metasurfaces(complete phase & magnitude control)
5929-Dec-16
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Arbitrarily Reflecting Incident Field: Beam-Splitter
Able to re-direct incident light at any arbitrary direction Can be extended to the designs of exotic optical
fl t d f i l
M. Kim, A. Wong and G.V. Eleftheriades, Phys. Rev. X, Dec. 2014
reflectarrays and focusing lenses
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Optical Chebyshev PatternOptical Chebyshev Pattern
M. Kim, A. Wong and G.V. Eleftheriades, Phys. Rev. X, Dec. 2014
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Optical Reconfigurable MetasurfacesU i th Ph T iti f VO2Using the Phase Transition of VO2
Cross-sectional view:(for one unit cell)Top view ( )
Au
135nm
VO2
AuSiO2
Au245nm
SiO2 thickness: 10nmVO2 thickness: 50nm
Top Au thickness: 30nm
M. Kim, J. Jeong, J. Poon, GV Eleftheriades, JOSAB, May 2016
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Dynamic manipulation of reflectedDynamic manipulation of reflected wavefront Dynamic control of the reflected wavefront depending
on the digital voltage distribution (i.e., Vn on = 1 and Vnoff = 0) on the digital optical metasurface.off 0) on the digital optical metasurface.Voltage distribution #1:
000/111/000/111/…Voltage distribution #2:0000/1111/0000/1111/…
Voltage distribution #3:00000/11111/00000/11111/…
6329-Dec-16
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EXTENDING THE SCAN RANGE OF ARRAYS WITH METASURFACES
•Leaky-wave antenna scans beam as a function of frequency
METASURFACES
frequency•Etched on Rogers Duroid 5870
T.R. Cameron and G.V. Eleftheriades, IEEE Trans. on Antennas and Propagation. 63(9): 3928-3938, 2015.
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Experimental Validation:•Gain improvement beyond 45, as expected•Remarkable bandwidth•Minimal impact on cross-polarization levels
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Beam Squinting Reduction of Leaky-Wave q g yAntennas using Huygens’ Metasurfaces
v
h2nd row
3ndrow
ha
1st period
2nd period1strow
Port 1
6629-Dec-16 M. Mehdipour and G.V. Eleftheriades, IEEE Trans. On Antennas and Propagat., 2015
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Beam Squinting Reduction of Leaky-Wave q g yAntennas using Huygens’ Metasurfaces
Metasurface
Thick paper
(a)
Match load CPW-LWA
6729-Dec-16(b)
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Advantages of Huygens’ Metasurfaces Complete control of magnitude phase and Complete control of magnitude, phase and
polarization state (including chiral effects) Incident field can be a plane wave a Incident field can be a plane-wave, a
beam or a nearby sourceS b l th thi f Sub-wavelength thin surfaces
Controlled reflection coefficient Microwave, THz or optical implementation
possible p More with active/tuneable metasurfaces!