Tunable Terahertz Metamaterials by means of Piezoelectric
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Tunable Terahertz Metamaterials by means of Piezoelectric MEMS Actuators Antonios X. Lalas , Nikolaos V. Kantartzis, and Theodoros D. Tsiboukis Telecommunications Division Department of Electrical and Computer Engineering, Aristotle University of Thessaloniki, Thessaloniki GR-54124, GREECE
Tunable Terahertz Metamaterials by means of Piezoelectric
Slide 1Tunable Terahertz Metamaterials by means of Piezoelectric
MEMS Actuators
Antonios X. Lalas, Nikolaos V. Kantartzis, and Theodoros D.
Tsiboukis
Telecommunications Division Department of Electrical and Computer
Engineering,
Aristotle University of Thessaloniki, Thessaloniki GR-54124,
GREECE
META 2014, 20-23 May, Singapore
Motivation and objective.
Piezoelectric MEMS microgripper.
Reconfigurable THz metamaterial.
Conclusions and future aspects.
Motivation and objective
Motivation:
Metamaterials, exhibit extraordinary electromagnetic properties not
available in nature.
Real-life configurations are limited, mainly due to the lack of a
wide spectral bandwidth, especially in the THz regime.
RF-MEMS provide efficient solutions, acting as tuning mechanisms in
contemporary RF technology.
META 2014, 20-23 May, Singapore 4
Microelectromechanical systems (MEMS)
Structures exhibiting dimensions between 1μm and 1 mm, that combine
electrical and mechanical components to realize complex and
controllable functions.
They are considered as transducers, since they absorb energy in one
form and convert it to an other form.
Two main categories are denoted, i.e. sensors and actuators.
Several coupled physical phenomena must be considered, when
analyzing a MEMS device.
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A fragment of a piezoelectric material can be considered as a
voltage-driven actuator.
Piezoelectric MEMS microgripper
Design parameters: L1 = 2 μm, L2 = 8 μm,
L3 = 6 μm, w1 = w2 = 1 μm, g = 2 μm
Implementation Materials: Metal parts: Gold
Piezoelectric Material: Lead Zirconate Titanate (PZT-5H)
META 2014, 20-23 May, Singapore 6
Principle of operation
Electrical: An electrostatic field is created by setting a
potential difference between the edges of the piezoelectric
material.
Piezoelectric: A strain due to the piezoelectric effect is
generated resulting in piezoelectric expansion of the
actuator.
Structural: A deflection occurs owing to the actuator’s expansion
and thus the arms are deflected towards each other, resulting in
gripping procedure.
Piezoelectric MEMS microgripper
Reverse procedure: When the bias voltage is decreased, or reversed,
the contraction of the device releases an object.
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Total displacement distribution on the actuator (in μm) at the
actuation voltage of 200 V
Piezoelectric MEMS microgripper
Tip displacement vs actuation voltage
Maximum displacement ~ 0.162 μm @ 220 V
Minimum displacement ~ -0.165 μm @ -220 V
Piezoelectric MEMS microgripper
Reconfigurable THz metamaterial
Characterization of metamaterials
Our design approach focuses mainly on tunable MNG and ENG
marerials, but DNG configurations are, also, feasible.
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Similar performance to an equivalent LC network.
A robust homogenization method is utilized to retrieve the
constitutive effective parameters of the proposed
metamaterials.
To extract the S-parameters, a parallel-plate waveguide approach is
adopted, which requires the use of PEC and PMC boundary
conditions.
Conventional metamaterial unit cell
META 2014, 20-23 May, Singapore
• Piezoelectric actuators enable fine tuning.
• A bias network is also necessary for applying the actuation
voltage.
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Reconfigurable THz metamaterial
Design parameters: h1 = 5 μm, h2 = 3 μm, α = 18 μm, Gold layer’s
thickness = 0.4 μm,
PZT-5H layer’s thickness = 0.4 μm, Si3N4 substrate’s thickness = 2
μm
META 2014, 20-23 May, Singapore 12
Principle of operation
When a certain voltage is applied, the resulting piezoelectric
expansion or contraction, deforms the structure and the gaps are
shortened or enlarged, respectively.
A shortened or enlarged gap results in increased or decreased
capacitance and therefore a frequency swift is revealed.
Variations in voltage levels introduce tunable gaps and as a
consequence a programmable SRR.
Reconfigurable THz metamaterial
META 2014, 20-23 May, Singapore 13
As the actuation voltage increases from -200 V to 200 V, a shift at
the resonant frequency
is achieved.
Reconfigurable THz metamaterial
Similar deductions are drawn from the shift of the real part
of
the effective magnetic permeability.
Electric field snapshots
Reconfigurable THz metamaterial
Actuation Voltage (V)
Frequency Regions Start (THz) End (THz) BW (GHz)
-200 4.1807 4.1813 0.6 -100 4.1760 4.1770 1.0
0 4.1372 4.1389 1.7 100 4.1083 4.1104 2.1 200 4.0396 4.0424
2.8
The narrow bandwidth of 1.7 GHz, is artificially extended to 141.7
GHz, offering an improvement of 83 times magnification.
The maximum values occur in the vicinity of
the gap yielding an MNG performance.
Vact = -200 @ 4.181 THz Vact = 200 @ 4.041 THz
META 2014, 20-23 May, Singapore 15
Surface current distribution
200 V.
Reconfigurable THz metamaterial
The maximum value is obtained upon the surface of the SRR and
especially the inner part of the resonator, denoting the presence
of an MNG resonance.
META 2014, 20-23 May, Singapore 16
Rotated orientation of the complex medium
• The wave is rotated 90o in comparison to the initial
orientation.
• The electric field is perpendicular to the piezoelectric
actuators, while the magnetic field is perpendicular to the
loops.
An ENG THz resonance of the complex medium is associated with this
topology.
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As the actuation voltage increases from -200 V to 200 V, a shift at
the resonant frequency
is observed.
Rotated orientation of the complex medium
A bandwidth enhancement of the real part of the effective
electric
permittivity is also observed.
Electric field snapshots
Actuation Voltage (V)
Frequency Regions Start (THz) End (THz) BW (GHz)
-200 4.1842 4.2229 38.7 -100 4.1772 4.2263 49.1
0 4.1331 4.1899 56.8 100 4.1001 4.1598 59.7 200 4.0253 4.0832
57.9
The narrow bandwidth of 56.8 GHz, is artificially extended to 201
GHz, offering an improvement of 253.9%.
The maximum values are located at the half part of the resonator,
thus displaying the
ENG behavior.
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The maximum value is observed only upon the half portion of the
SRR. Thus, the unit cell acts as a metal
wire, sustaining an ENG resonance.
Rotated orientation of the complex medium
Surface current distribution
200 V.
Possible applications
The reconfigurable unit cells exhibit MNG behavior as well as ENG
performance depending on the orientation of the device.
The design of several implementations, such as tunable THz filters
and modulators is feasible.
Antenna configurations exploiting controllable ground planes or
reconfigurable reflectors are also possible.
META 2014, 20-23 May, Singapore
An elaborated multiphysics investigation concerning the performance
of the piezoelectric MEMS microgripper has been successfully
conducted.
A novel design incorporating the MEMS microgripper into
metamaterial unit cells has been proposed, achieving tunability and
overcoming bandwidth restrictions.
The response of the complex medium with a different orientation is
also examined.
Future investigation involves modeling of combined electrostatic
and electrothermal RF-MEMS as tuning components.
A detailed study extended in more complex metamaterial unit
cells.
Conclusions and future aspects