electromagnetics at ief - eth zalphard.ethz.ch/hafner/vorles/physicalmod/iefresearch2014.pdf ·...
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Institute of Electromagnetic Fields (IEF) Christian Hafner, [email protected] 03.09.2014 1 | |
Christian Hafner, [email protected]
Electromagnetics at IEF
Institute of Electromagnetic Fields (IEF) Christian Hafner, [email protected] 03.09.2014 2 | |
EM Overview
Traditional areas Electrostatics • Capacitors
• High voltage
Magnetostatics • Inductors
• Motors / Generators
Quasistatics • Sensors
• Electronic circuits
• Transmission lines
Electrodynamics • Antennas
• Wave propagation / scattering
• Gratings
• Guided waves
• Resonators...
«Modern areas» • Integrated optics
• Optical computers
• Nearfield optics
• Nano optics
• Photonic crystals
• Metamaterials
• Plasmonics
Mixed with other disciplines
• Semiconductors
• Lasers, LED, LCD
• Solar cells, Photovoltaics
• RF-MEMS
• (Nano-) Robots
• Bio/medical...
Institute of Electromagnetic Fields (IEF) Christian Hafner, [email protected] 03.09.2014 3 | |
Examples of IEF research
• Computational Electromagnetics (software development)
• Numerical Optimization (software development)
• Microwave and mm Wave Technology
• Electromagnetics in Medicine and Biology
• Metamaterials, Photonic Crystals, Plasmonics
• New: Photonic systems (Prof. Leuthold)
• Metamaterials for industrial applications
• Solar cell design
• Near field applications (SNOM, SNMM, TERS...)
• Electron emission / acceleration
• Photonic crystals and EBG structures
• Sensors and sensing
Institute of Electromagnetic Fields (IEF) Christian Hafner, [email protected] 03.09.2014 4 | |
Optimal Design: 2nd harmonic generation
COMSOL simulation
Various optimizers
Triple point problem!
Martin Spieser
Institute of Electromagnetic Fields (IEF) Christian Hafner, [email protected] 03.09.2014 5 | |
Metamaterials for magnetic field shielding
EWZ project
• Strong rules for maximum magnetic fields at 50Hz in Switzerland require additional shielding
• Extreme wavelength offers attractive opportunities (electronic circuits) for the metamaterial design →
tunable, active, NIC, Gyrator,... → «smart» metamaterials
Anisotropic, homogenous,
low μ metamaterial
Anisotropic, inhomogeneous
metamaterial
Experiment:
Homogenous
meta-layer
Improved metamaterial:
passive circuitry
Active circuits :
Heavy, expensive
Shielding performance: Upto 87% shielding
and suppressed undesired enhancement below resonance frequency
Source B Shielded B
Mustafa Boyvat
Meta-atoms for kHz and THz
ranges
Institute of Electromagnetic Fields (IEF) Christian Hafner, [email protected] 03.09.2014 6 | |
Wireless actuation of forces
LC resonators in external field:
Metamaterials and Wireless
Power Transfer
Strong fields close to high Q
resonance Strong forces
Controlling strength and
direction of forces and torques
via external magnetic field
frequency and magnitude
Easy wireless translational and
rotational motion control
Microrobotic Surgery
Coupled LC Resonators
Wireless Magnetic
Micro-Actuators
Institute of Electromagnetic Fields (IEF) Christian Hafner, [email protected] 03.09.2014 7 | |
Radar absorbing metamaterial: optimal design Arya Fallahi et al. IFH
Simulations using MoM + RCWA
Optimization: RHC ++
Goals (same as for solar cells!):
Lower reflection + Higher absorption +
Broader bandwidth + Better angular stability
All goals may be reached simultaneously!
Maybe surprising:
Metallic structures
on top
reduce reflection!
Institute of Electromagnetic Fields (IEF) Christian Hafner, [email protected] 03.09.2014 8 | |
Photonic structures for space applications Reflecting photonic system
(RPS)
Re-entry from
space
Radiative spectra of shock gas
layered media with roughness
Guided mode resonance structures
woodpiles
Porous reflectors
Inverse opals
Collaboration:
NASA, Material sciences
Nikolay Komarevskiy
Institute of Electromagnetic Fields (IEF) Christian Hafner, [email protected] 03.09.2014 9 | |
Advanced solar cell design
• Nanostructuring for
improving efficiency
• Space applications (low
light, low temperature
• Planned cooperation with
Grätzel + Fontcuberta
(EPFL)
Alexander Dorodnyy
Institute of Electromagnetic Fields (IEF) Christian Hafner, [email protected] 03.09.2014 10 | |
Fast chip to chip communication
x y
z
E-field
y
x
cylindrical holes
copper spacers
conical holes
GSG probe
on-chip excitation
0.45 dB insertion loss from chip-to-
waveguide (at 90GHz)
dipole
Replace metallic wires by dielectric EBG waveguides
Excite modes using on chip antennas
Collaboration with Jan Hesselbarth (Stuttgart)
Nemat Dolatsha
Institute of Electromagnetic Fields (IEF) Christian Hafner, [email protected] 03.09.2014 11 | |
Spatial power combining at 140 GHz
Power amplifier
(phase variable)
• High power
• High gain
• Beam forming (1-D scan)
• Active & passive lens
• Very efficient heat-sinking
Alternative:
2-D space scan;
1-D electronically,
1-D frequency scan
Rod antenna
(10-14 dBi gain)
Power
amplifier
(phase
variable
)
Leaky-wave
antenna
(12-17 dBi gain)
Institute of Electromagnetic Fields (IEF) Christian Hafner, [email protected] 03.09.2014 12 | |
Interaction of THz waves and proteins
Electrokinetically Enhanced THz Spectroscopy for Study of Uniformly Oriented Proteins, CB-SEED-13, Stanford Univ.
sensing at sub-THz frequencies. The length of the waveguide corresponds to several wavelengths (e.g., 14! ) at the center frequency of the operating bandwidth, which results in
several resonant peaks in the desired frequency range. It should be noted that the dynamic range and spectral resolution of the complex-domain electrical system (VNA) in DC-THz Lab are 110
dB and better than 10 Hz, respectively, which is far better than conventional optical techniques
for this part of the spectrum.
In order to extract information on the proteins, the obtained signal needs to be decomposed
into its separate contributions. To this end, a calibration approach comparing the pure liquid and
liquid with suspended proteins will be utilized to minimize interference due to background water.
This could be done by either making a differential measurement, or by sequentially measuring
the spectrum of buffer compared to protein suspended in buffer and dynamically subtracting the difference. The network analyzer setup allows for fast pulsed- measurements for this application
(down to 100 ns width).
(a) (b)
Fig. 1 (a) Conceptual schematic of the (sub) THz waveguide resonator applicable to determine the
complex permittivity of liquid samples. (b) A drawing of implementation of microfluidic channel on top
the (sub)THz waveguide. Inset: electric field distribution at the cross section of the waveguide with
strong electric field on top, exhibiting a good potential for material sensing.
(a) (b)
Fig. 2 (a) Measurement (solid) and simulation (dashed) transmission parameter of a prototype of the
resonator operating at 100 GHz. (b) Simulated transmission parameter with (dashed) and without (solid)
the biomaterial sample.
Microfluidic Channel and Protein Alignment: We aim to control the alignment of the proteins by selectively aligning the dipoles in a
single direction using a quasi- static field. This is necessary since our evanescent mode extends
On static
electric
field
Investigation of electrical properties
of proteins oriented in a certain
direction
Applying static electric field:
• Unipolar translation
• Dipolar orientation
Institute of Electromagnetic Fields (IEF) Christian Hafner, [email protected] 03.09.2014 13 | |
EMF‘s in Medical and Biological Research • Numerical and experimental tools
• Design of experimental setups
providing controlled conditions
• Applications in diagnosis, therapy
and safety assessment
• Clinical and in-vitro studies
Various collaborations
Jürg Fröhlich
Institute of Electromagnetic Fields (IEF) Christian Hafner, [email protected] 03.09.2014 14 | |
Smart sensors for smart phones
3D Magnetometer Applet
RF exposimeter Smart phone intensity on Google map
Projects for
EWZ
Armasuisse
...
Jürg Fröhlich
Marco Zahner