Chinese Optics Letters, Volume. 15, Issue 1, 011101(2017)
Flat mirror for millimeter-wave and terahertz imaging systems using an inexpensive metasurface
Fig. 1. Proposed reflector structure composed of an FR4 (glass epoxy) dielectric substrate with a ground plane on the back and printed metal patterns on the front. Each metal cell on the front is connected to the back ground plane by a via. The metal cells in the center are the largest, and they gradually decrease in size as they approach the edges of the FLAPS mirror. The FLAPS mirror cells can be described as an array of parallel LC resonance circuits.
Fig. 2. Top: Side view of parabolic mirror and parallel rays
Fig. 3. Simulation model.
Fig. 4. Top: Simulation results for S11 phase shift. Bottom: Simulation results for S11 magnitude. Each curve represents a different patch size.
Fig. 5. Experimental setup. Instead of one of the parabolic mirrors, the FLAPS mirror was tilted 20° relative to the optical axis to avoid optical aberrations, and in front of it, a track with a TK sensor was placed and replaced later by a Spiricon camera.
Fig. 6. Maximum response of the TK sensor for 94, 97, and 100 GHz was obtained for a distance of 65 cm from the FLAPS mirror.
Fig. 7. Energy scattering as observed on the Spiricon camera when it is located at the focal point of the FLAPS mirror. The bright color in the center is an indication of the maximum density spot, and the energy density becomes lower as the outer rings are approached. The photo size is
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Gil Litmanovitch, David Rrotshild, Amir Abramovich, "Flat mirror for millimeter-wave and terahertz imaging systems using an inexpensive metasurface," Chin. Opt. Lett. 15, 011101 (2017)
Category: Imaging Systems
Received: Jul. 8, 2016
Accepted: Nov. 11, 2016
Published Online: Jul. 26, 2018
The Author Email: Gil Litmanovitch (Gil.Litmanovitch@solaredge.com)