Research output: Chapter in Book/Report/Conference proceeding › Conference contribution › Research › peer-review
Manipulation with Terahertz Wave Fronts Using Self-Complementary Metasurfaces. / Lenets, V. A.; Kuznetsov, S. A.; Sayanskiy, A. D. et al.
2020 14th International Congress on Artificial Materials for Novel Wave Phenomena, Metamaterials 2020. Institute of Electrical and Electronics Engineers Inc., 2020. p. 294-296 9285140 (2020 14th International Congress on Artificial Materials for Novel Wave Phenomena, Metamaterials 2020).Research output: Chapter in Book/Report/Conference proceeding › Conference contribution › Research › peer-review
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TY - GEN
T1 - Manipulation with Terahertz Wave Fronts Using Self-Complementary Metasurfaces
AU - Lenets, V. A.
AU - Kuznetsov, S. A.
AU - Sayanskiy, A. D.
AU - Lazorskiy, P. A.
AU - Baena, J. D.
AU - Glybovski, S. B.
N1 - Funding Information: This work was supported by the Russian Science Foundation (Project 19-79-10260). Publisher Copyright: © 2020 IEEE. Copyright: Copyright 2021 Elsevier B.V., All rights reserved.
PY - 2020/9/27
Y1 - 2020/9/27
N2 - Here we numerically demonstrate the possibility to shape a wave front in the terahertz range using a self-complementary metasurface (SCMS) with spatial modulation. A circularly polarized incident wave passing through a SCMS causes two transmitted waves, a co- and cross-polarized. The co-polarized wave, in theory, has a complex transmission coefficient of 1/2 and keeps the same front shape as the incident wave, even if the metasurface is nonuniform. On the contrary, the cross-polarized wave obtains a phase, which can be locally controlled by geometric parameters of unit cells. We apply a phase holographic method to modify the shape of the cross-polarized wave in a desirable way while keeping the co-polarized wave unchanged.
AB - Here we numerically demonstrate the possibility to shape a wave front in the terahertz range using a self-complementary metasurface (SCMS) with spatial modulation. A circularly polarized incident wave passing through a SCMS causes two transmitted waves, a co- and cross-polarized. The co-polarized wave, in theory, has a complex transmission coefficient of 1/2 and keeps the same front shape as the incident wave, even if the metasurface is nonuniform. On the contrary, the cross-polarized wave obtains a phase, which can be locally controlled by geometric parameters of unit cells. We apply a phase holographic method to modify the shape of the cross-polarized wave in a desirable way while keeping the co-polarized wave unchanged.
UR - http://www.scopus.com/inward/record.url?scp=85099279507&partnerID=8YFLogxK
U2 - 10.1109/Metamaterials49557.2020.9285140
DO - 10.1109/Metamaterials49557.2020.9285140
M3 - Conference contribution
AN - SCOPUS:85099279507
T3 - 2020 14th International Congress on Artificial Materials for Novel Wave Phenomena, Metamaterials 2020
SP - 294
EP - 296
BT - 2020 14th International Congress on Artificial Materials for Novel Wave Phenomena, Metamaterials 2020
PB - Institute of Electrical and Electronics Engineers Inc.
T2 - 14th International Congress on Artificial Materials for Novel Wave Phenomena, Metamaterials 2020
Y2 - 27 September 2020 through 3 October 2020
ER -
ID: 27487077