Dual-band linear-to-circular and circular-to-linear polarization converter based on reflective metasurface

Abstract In this work, a dual-band polarization converter is proposed based on a reflective metasurface. The metasurface is an appropriate anisotropic structure with a pair of mutually perpendicular symmetric axes x and y, and the reflection phase difference under x- and y-polarized incidences is ve...
Ausführliche Beschreibung

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Autor*in:	Lin, Baoqin [verfasserIn] Huang, Wenzhun Guo, Jianxin Wang, Yanwei Ji, Xiang Ye, Hongjun

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2022

Schlagwörter:	Metasurface Polarization converter Circular polarization Axial ratio (AR)

Anmerkung:	© The Author(s), under exclusive licence to Springer-Verlag GmbH, DE part of Springer Nature 2022. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law.

Übergeordnetes Werk:	Enthalten in: Applied physics - Berlin : Springer, 1973, 128(2022), 11 vom: 29. Okt.
Übergeordnetes Werk:	volume:128 ; year:2022 ; number:11 ; day:29 ; month:10

Links:	Volltext

DOI / URN:	10.1007/s00339-022-06164-x

Katalog-ID:	SPR048491527

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245	1	0	\|a Dual-band linear-to-circular and circular-to-linear polarization converter based on reflective metasurface
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520			\|a Abstract In this work, a dual-band polarization converter is proposed based on a reflective metasurface. The metasurface is an appropriate anisotropic structure with a pair of mutually perpendicular symmetric axes x and y, and the reflection phase difference under x- and y-polarized incidences is very close to 90° in the two frequency ranges of 7.9–9.2 GHz and 12.4–25.2 GHz, so the metasurface can be used as a high-efficiency dual-band polarization converter to achieve both linear-to-circular (LTC) and circular-to-linear (CTL) polarization conversions in two separated frequency bands. The simulation and experimental results show that, when the dual-band polarization converter is under the incidence of u- and v-polarized waves, the reflected wave will be converted to a circular-polarized (CP) one in the two frequency bands of 7.78–9.38 GHz and 12.30–25.60 GHz, a dual-band LTC polarization conversion will be achieved with high-efficiency; in addition, under CP incidence, the reflected wave will be converted to a linear-polarized one in the two frequency bands of 7.76–9.39 GHz and 12.22–25.57 GHz, a dual-band CTL polarization conversion with almost the same working band and polarization conversion rate will be achieved. Therefore, the dual-band polarization converter has great potential application values in various polarization controlled devices.
650		4	\|a Metasurface \|7 (dpeaa)DE-He213
650		4	\|a Polarization converter \|7 (dpeaa)DE-He213
650		4	\|a Circular polarization \|7 (dpeaa)DE-He213
650		4	\|a Axial ratio (AR) \|7 (dpeaa)DE-He213
700	1		\|a Huang, Wenzhun \|4 aut
700	1		\|a Guo, Jianxin \|4 aut
700	1		\|a Wang, Yanwei \|4 aut
700	1		\|a Ji, Xiang \|4 aut
700	1		\|a Ye, Hongjun \|4 aut
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912			\|a GBV_ILN_63
912			\|a GBV_ILN_69
912			\|a GBV_ILN_70
912			\|a GBV_ILN_73
912			\|a GBV_ILN_74
912			\|a GBV_ILN_90
912			\|a GBV_ILN_95
912			\|a GBV_ILN_100
912			\|a GBV_ILN_101
912			\|a GBV_ILN_105
912			\|a GBV_ILN_110
912			\|a GBV_ILN_120
912			\|a GBV_ILN_138
912			\|a GBV_ILN_150
912			\|a GBV_ILN_151
912			\|a GBV_ILN_152
912			\|a GBV_ILN_161
912			\|a GBV_ILN_170
912			\|a GBV_ILN_171
912			\|a GBV_ILN_187
912			\|a GBV_ILN_206
912			\|a GBV_ILN_213
912			\|a GBV_ILN_224
912			\|a GBV_ILN_230
912			\|a GBV_ILN_250
912			\|a GBV_ILN_267
912			\|a GBV_ILN_281
912			\|a GBV_ILN_285
912			\|a GBV_ILN_293
912			\|a GBV_ILN_370
912			\|a GBV_ILN_602
912			\|a GBV_ILN_636
912			\|a GBV_ILN_702
912			\|a GBV_ILN_2001
912			\|a GBV_ILN_2003
912			\|a GBV_ILN_2004
912			\|a GBV_ILN_2005
912			\|a GBV_ILN_2006
912			\|a GBV_ILN_2007
912			\|a GBV_ILN_2008
912			\|a GBV_ILN_2009
912			\|a GBV_ILN_2010
912			\|a GBV_ILN_2011
912			\|a GBV_ILN_2014
912			\|a GBV_ILN_2015
912			\|a GBV_ILN_2020
912			\|a GBV_ILN_2021
912			\|a GBV_ILN_2025
912			\|a GBV_ILN_2026
912			\|a GBV_ILN_2027
912			\|a GBV_ILN_2031
912			\|a GBV_ILN_2034
912			\|a GBV_ILN_2037
912			\|a GBV_ILN_2038
912			\|a GBV_ILN_2039
912			\|a GBV_ILN_2044
912			\|a GBV_ILN_2048
912			\|a GBV_ILN_2049
912			\|a GBV_ILN_2050
912			\|a GBV_ILN_2055
912			\|a GBV_ILN_2056
912			\|a GBV_ILN_2057
912			\|a GBV_ILN_2059
912			\|a GBV_ILN_2061
912			\|a GBV_ILN_2064
912			\|a GBV_ILN_2065
912			\|a GBV_ILN_2068
912			\|a GBV_ILN_2088
912			\|a GBV_ILN_2093
912			\|a GBV_ILN_2106
912			\|a GBV_ILN_2107
912			\|a GBV_ILN_2108
912			\|a GBV_ILN_2110
912			\|a GBV_ILN_2111
912			\|a GBV_ILN_2112
912			\|a GBV_ILN_2113
912			\|a GBV_ILN_2118
912			\|a GBV_ILN_2119
912			\|a GBV_ILN_2122
912			\|a GBV_ILN_2129
912			\|a GBV_ILN_2143
912			\|a GBV_ILN_2144
912			\|a GBV_ILN_2147
912			\|a GBV_ILN_2148
912			\|a GBV_ILN_2152
912			\|a GBV_ILN_2153
912			\|a GBV_ILN_2188
912			\|a GBV_ILN_2190
912			\|a GBV_ILN_2232
912			\|a GBV_ILN_2336
912			\|a GBV_ILN_2446
912			\|a GBV_ILN_2470
912			\|a GBV_ILN_2472
912			\|a GBV_ILN_2507
912			\|a GBV_ILN_2522
912			\|a GBV_ILN_2548
912			\|a GBV_ILN_4035
912			\|a GBV_ILN_4037
912			\|a GBV_ILN_4046
912			\|a GBV_ILN_4112
912			\|a GBV_ILN_4125
912			\|a GBV_ILN_4126
912			\|a GBV_ILN_4242
912			\|a GBV_ILN_4246
912			\|a GBV_ILN_4249
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912			\|a GBV_ILN_4307
912			\|a GBV_ILN_4313
912			\|a GBV_ILN_4322
912			\|a GBV_ILN_4323
912			\|a GBV_ILN_4324
912			\|a GBV_ILN_4325
912			\|a GBV_ILN_4326
912			\|a GBV_ILN_4328
912			\|a GBV_ILN_4333
912			\|a GBV_ILN_4334
912			\|a GBV_ILN_4335
912			\|a GBV_ILN_4336
912			\|a GBV_ILN_4338
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author_variant	b l bl w h wh j g jg y w yw x j xj h y hy
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allfields	10.1007/s00339-022-06164-x doi (DE-627)SPR048491527 (SPR)s00339-022-06164-x-e DE-627 ger DE-627 rakwb eng Lin, Baoqin verfasserin (orcid)0000-0003-0966-368X aut Dual-band linear-to-circular and circular-to-linear polarization converter based on reflective metasurface 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer-Verlag GmbH, DE part of Springer Nature 2022. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract In this work, a dual-band polarization converter is proposed based on a reflective metasurface. The metasurface is an appropriate anisotropic structure with a pair of mutually perpendicular symmetric axes x and y, and the reflection phase difference under x- and y-polarized incidences is very close to 90° in the two frequency ranges of 7.9–9.2 GHz and 12.4–25.2 GHz, so the metasurface can be used as a high-efficiency dual-band polarization converter to achieve both linear-to-circular (LTC) and circular-to-linear (CTL) polarization conversions in two separated frequency bands. The simulation and experimental results show that, when the dual-band polarization converter is under the incidence of u- and v-polarized waves, the reflected wave will be converted to a circular-polarized (CP) one in the two frequency bands of 7.78–9.38 GHz and 12.30–25.60 GHz, a dual-band LTC polarization conversion will be achieved with high-efficiency; in addition, under CP incidence, the reflected wave will be converted to a linear-polarized one in the two frequency bands of 7.76–9.39 GHz and 12.22–25.57 GHz, a dual-band CTL polarization conversion with almost the same working band and polarization conversion rate will be achieved. Therefore, the dual-band polarization converter has great potential application values in various polarization controlled devices. Metasurface (dpeaa)DE-He213 Polarization converter (dpeaa)DE-He213 Circular polarization (dpeaa)DE-He213 Axial ratio (AR) (dpeaa)DE-He213 Huang, Wenzhun aut Guo, Jianxin aut Wang, Yanwei aut Ji, Xiang aut Ye, Hongjun aut Enthalten in Applied physics Berlin : Springer, 1973 128(2022), 11 vom: 29. Okt. (DE-627)235503231 (DE-600)1398311-8 1432-0630 nnns volume:128 year:2022 number:11 day:29 month:10 https://dx.doi.org/10.1007/s00339-022-06164-x lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 128 2022 11 29 10
spelling	10.1007/s00339-022-06164-x doi (DE-627)SPR048491527 (SPR)s00339-022-06164-x-e DE-627 ger DE-627 rakwb eng Lin, Baoqin verfasserin (orcid)0000-0003-0966-368X aut Dual-band linear-to-circular and circular-to-linear polarization converter based on reflective metasurface 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer-Verlag GmbH, DE part of Springer Nature 2022. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract In this work, a dual-band polarization converter is proposed based on a reflective metasurface. The metasurface is an appropriate anisotropic structure with a pair of mutually perpendicular symmetric axes x and y, and the reflection phase difference under x- and y-polarized incidences is very close to 90° in the two frequency ranges of 7.9–9.2 GHz and 12.4–25.2 GHz, so the metasurface can be used as a high-efficiency dual-band polarization converter to achieve both linear-to-circular (LTC) and circular-to-linear (CTL) polarization conversions in two separated frequency bands. The simulation and experimental results show that, when the dual-band polarization converter is under the incidence of u- and v-polarized waves, the reflected wave will be converted to a circular-polarized (CP) one in the two frequency bands of 7.78–9.38 GHz and 12.30–25.60 GHz, a dual-band LTC polarization conversion will be achieved with high-efficiency; in addition, under CP incidence, the reflected wave will be converted to a linear-polarized one in the two frequency bands of 7.76–9.39 GHz and 12.22–25.57 GHz, a dual-band CTL polarization conversion with almost the same working band and polarization conversion rate will be achieved. Therefore, the dual-band polarization converter has great potential application values in various polarization controlled devices. Metasurface (dpeaa)DE-He213 Polarization converter (dpeaa)DE-He213 Circular polarization (dpeaa)DE-He213 Axial ratio (AR) (dpeaa)DE-He213 Huang, Wenzhun aut Guo, Jianxin aut Wang, Yanwei aut Ji, Xiang aut Ye, Hongjun aut Enthalten in Applied physics Berlin : Springer, 1973 128(2022), 11 vom: 29. Okt. (DE-627)235503231 (DE-600)1398311-8 1432-0630 nnns volume:128 year:2022 number:11 day:29 month:10 https://dx.doi.org/10.1007/s00339-022-06164-x lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 128 2022 11 29 10
allfields_unstemmed	10.1007/s00339-022-06164-x doi (DE-627)SPR048491527 (SPR)s00339-022-06164-x-e DE-627 ger DE-627 rakwb eng Lin, Baoqin verfasserin (orcid)0000-0003-0966-368X aut Dual-band linear-to-circular and circular-to-linear polarization converter based on reflective metasurface 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer-Verlag GmbH, DE part of Springer Nature 2022. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract In this work, a dual-band polarization converter is proposed based on a reflective metasurface. The metasurface is an appropriate anisotropic structure with a pair of mutually perpendicular symmetric axes x and y, and the reflection phase difference under x- and y-polarized incidences is very close to 90° in the two frequency ranges of 7.9–9.2 GHz and 12.4–25.2 GHz, so the metasurface can be used as a high-efficiency dual-band polarization converter to achieve both linear-to-circular (LTC) and circular-to-linear (CTL) polarization conversions in two separated frequency bands. The simulation and experimental results show that, when the dual-band polarization converter is under the incidence of u- and v-polarized waves, the reflected wave will be converted to a circular-polarized (CP) one in the two frequency bands of 7.78–9.38 GHz and 12.30–25.60 GHz, a dual-band LTC polarization conversion will be achieved with high-efficiency; in addition, under CP incidence, the reflected wave will be converted to a linear-polarized one in the two frequency bands of 7.76–9.39 GHz and 12.22–25.57 GHz, a dual-band CTL polarization conversion with almost the same working band and polarization conversion rate will be achieved. Therefore, the dual-band polarization converter has great potential application values in various polarization controlled devices. Metasurface (dpeaa)DE-He213 Polarization converter (dpeaa)DE-He213 Circular polarization (dpeaa)DE-He213 Axial ratio (AR) (dpeaa)DE-He213 Huang, Wenzhun aut Guo, Jianxin aut Wang, Yanwei aut Ji, Xiang aut Ye, Hongjun aut Enthalten in Applied physics Berlin : Springer, 1973 128(2022), 11 vom: 29. Okt. (DE-627)235503231 (DE-600)1398311-8 1432-0630 nnns volume:128 year:2022 number:11 day:29 month:10 https://dx.doi.org/10.1007/s00339-022-06164-x lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 128 2022 11 29 10
allfieldsGer	10.1007/s00339-022-06164-x doi (DE-627)SPR048491527 (SPR)s00339-022-06164-x-e DE-627 ger DE-627 rakwb eng Lin, Baoqin verfasserin (orcid)0000-0003-0966-368X aut Dual-band linear-to-circular and circular-to-linear polarization converter based on reflective metasurface 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer-Verlag GmbH, DE part of Springer Nature 2022. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract In this work, a dual-band polarization converter is proposed based on a reflective metasurface. The metasurface is an appropriate anisotropic structure with a pair of mutually perpendicular symmetric axes x and y, and the reflection phase difference under x- and y-polarized incidences is very close to 90° in the two frequency ranges of 7.9–9.2 GHz and 12.4–25.2 GHz, so the metasurface can be used as a high-efficiency dual-band polarization converter to achieve both linear-to-circular (LTC) and circular-to-linear (CTL) polarization conversions in two separated frequency bands. The simulation and experimental results show that, when the dual-band polarization converter is under the incidence of u- and v-polarized waves, the reflected wave will be converted to a circular-polarized (CP) one in the two frequency bands of 7.78–9.38 GHz and 12.30–25.60 GHz, a dual-band LTC polarization conversion will be achieved with high-efficiency; in addition, under CP incidence, the reflected wave will be converted to a linear-polarized one in the two frequency bands of 7.76–9.39 GHz and 12.22–25.57 GHz, a dual-band CTL polarization conversion with almost the same working band and polarization conversion rate will be achieved. Therefore, the dual-band polarization converter has great potential application values in various polarization controlled devices. Metasurface (dpeaa)DE-He213 Polarization converter (dpeaa)DE-He213 Circular polarization (dpeaa)DE-He213 Axial ratio (AR) (dpeaa)DE-He213 Huang, Wenzhun aut Guo, Jianxin aut Wang, Yanwei aut Ji, Xiang aut Ye, Hongjun aut Enthalten in Applied physics Berlin : Springer, 1973 128(2022), 11 vom: 29. Okt. (DE-627)235503231 (DE-600)1398311-8 1432-0630 nnns volume:128 year:2022 number:11 day:29 month:10 https://dx.doi.org/10.1007/s00339-022-06164-x lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 128 2022 11 29 10
allfieldsSound	10.1007/s00339-022-06164-x doi (DE-627)SPR048491527 (SPR)s00339-022-06164-x-e DE-627 ger DE-627 rakwb eng Lin, Baoqin verfasserin (orcid)0000-0003-0966-368X aut Dual-band linear-to-circular and circular-to-linear polarization converter based on reflective metasurface 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer-Verlag GmbH, DE part of Springer Nature 2022. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract In this work, a dual-band polarization converter is proposed based on a reflective metasurface. The metasurface is an appropriate anisotropic structure with a pair of mutually perpendicular symmetric axes x and y, and the reflection phase difference under x- and y-polarized incidences is very close to 90° in the two frequency ranges of 7.9–9.2 GHz and 12.4–25.2 GHz, so the metasurface can be used as a high-efficiency dual-band polarization converter to achieve both linear-to-circular (LTC) and circular-to-linear (CTL) polarization conversions in two separated frequency bands. The simulation and experimental results show that, when the dual-band polarization converter is under the incidence of u- and v-polarized waves, the reflected wave will be converted to a circular-polarized (CP) one in the two frequency bands of 7.78–9.38 GHz and 12.30–25.60 GHz, a dual-band LTC polarization conversion will be achieved with high-efficiency; in addition, under CP incidence, the reflected wave will be converted to a linear-polarized one in the two frequency bands of 7.76–9.39 GHz and 12.22–25.57 GHz, a dual-band CTL polarization conversion with almost the same working band and polarization conversion rate will be achieved. Therefore, the dual-band polarization converter has great potential application values in various polarization controlled devices. Metasurface (dpeaa)DE-He213 Polarization converter (dpeaa)DE-He213 Circular polarization (dpeaa)DE-He213 Axial ratio (AR) (dpeaa)DE-He213 Huang, Wenzhun aut Guo, Jianxin aut Wang, Yanwei aut Ji, Xiang aut Ye, Hongjun aut Enthalten in Applied physics Berlin : Springer, 1973 128(2022), 11 vom: 29. Okt. (DE-627)235503231 (DE-600)1398311-8 1432-0630 nnns volume:128 year:2022 number:11 day:29 month:10 https://dx.doi.org/10.1007/s00339-022-06164-x lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_206 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_267 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 128 2022 11 29 10
language	English
source	Enthalten in Applied physics 128(2022), 11 vom: 29. Okt. volume:128 year:2022 number:11 day:29 month:10
sourceStr	Enthalten in Applied physics 128(2022), 11 vom: 29. Okt. volume:128 year:2022 number:11 day:29 month:10
format_phy_str_mv	Article
institution	findex.gbv.de
topic_facet	Metasurface Polarization converter Circular polarization Axial ratio (AR)
isfreeaccess_bool	false
container_title	Applied physics
authorswithroles_txt_mv	Lin, Baoqin @@aut@@ Huang, Wenzhun @@aut@@ Guo, Jianxin @@aut@@ Wang, Yanwei @@aut@@ Ji, Xiang @@aut@@ Ye, Hongjun @@aut@@
publishDateDaySort_date	2022-10-29T00:00:00Z
hierarchy_top_id	235503231
id	SPR048491527
language_de	englisch
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author	Lin, Baoqin
spellingShingle	Lin, Baoqin misc Metasurface misc Polarization converter misc Circular polarization misc Axial ratio (AR) Dual-band linear-to-circular and circular-to-linear polarization converter based on reflective metasurface
authorStr	Lin, Baoqin
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topic_title	Dual-band linear-to-circular and circular-to-linear polarization converter based on reflective metasurface Metasurface (dpeaa)DE-He213 Polarization converter (dpeaa)DE-He213 Circular polarization (dpeaa)DE-He213 Axial ratio (AR) (dpeaa)DE-He213
topic	misc Metasurface misc Polarization converter misc Circular polarization misc Axial ratio (AR)
topic_unstemmed	misc Metasurface misc Polarization converter misc Circular polarization misc Axial ratio (AR)
topic_browse	misc Metasurface misc Polarization converter misc Circular polarization misc Axial ratio (AR)
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title	Dual-band linear-to-circular and circular-to-linear polarization converter based on reflective metasurface
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title_full	Dual-band linear-to-circular and circular-to-linear polarization converter based on reflective metasurface
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author_browse	Lin, Baoqin Huang, Wenzhun Guo, Jianxin Wang, Yanwei Ji, Xiang Ye, Hongjun
container_volume	128
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author-letter	Lin, Baoqin
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title_sort	dual-band linear-to-circular and circular-to-linear polarization converter based on reflective metasurface
title_auth	Dual-band linear-to-circular and circular-to-linear polarization converter based on reflective metasurface
abstract	Abstract In this work, a dual-band polarization converter is proposed based on a reflective metasurface. The metasurface is an appropriate anisotropic structure with a pair of mutually perpendicular symmetric axes x and y, and the reflection phase difference under x- and y-polarized incidences is very close to 90° in the two frequency ranges of 7.9–9.2 GHz and 12.4–25.2 GHz, so the metasurface can be used as a high-efficiency dual-band polarization converter to achieve both linear-to-circular (LTC) and circular-to-linear (CTL) polarization conversions in two separated frequency bands. The simulation and experimental results show that, when the dual-band polarization converter is under the incidence of u- and v-polarized waves, the reflected wave will be converted to a circular-polarized (CP) one in the two frequency bands of 7.78–9.38 GHz and 12.30–25.60 GHz, a dual-band LTC polarization conversion will be achieved with high-efficiency; in addition, under CP incidence, the reflected wave will be converted to a linear-polarized one in the two frequency bands of 7.76–9.39 GHz and 12.22–25.57 GHz, a dual-band CTL polarization conversion with almost the same working band and polarization conversion rate will be achieved. Therefore, the dual-band polarization converter has great potential application values in various polarization controlled devices. © The Author(s), under exclusive licence to Springer-Verlag GmbH, DE part of Springer Nature 2022. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law.
abstractGer	Abstract In this work, a dual-band polarization converter is proposed based on a reflective metasurface. The metasurface is an appropriate anisotropic structure with a pair of mutually perpendicular symmetric axes x and y, and the reflection phase difference under x- and y-polarized incidences is very close to 90° in the two frequency ranges of 7.9–9.2 GHz and 12.4–25.2 GHz, so the metasurface can be used as a high-efficiency dual-band polarization converter to achieve both linear-to-circular (LTC) and circular-to-linear (CTL) polarization conversions in two separated frequency bands. The simulation and experimental results show that, when the dual-band polarization converter is under the incidence of u- and v-polarized waves, the reflected wave will be converted to a circular-polarized (CP) one in the two frequency bands of 7.78–9.38 GHz and 12.30–25.60 GHz, a dual-band LTC polarization conversion will be achieved with high-efficiency; in addition, under CP incidence, the reflected wave will be converted to a linear-polarized one in the two frequency bands of 7.76–9.39 GHz and 12.22–25.57 GHz, a dual-band CTL polarization conversion with almost the same working band and polarization conversion rate will be achieved. Therefore, the dual-band polarization converter has great potential application values in various polarization controlled devices. © The Author(s), under exclusive licence to Springer-Verlag GmbH, DE part of Springer Nature 2022. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law.
abstract_unstemmed	Abstract In this work, a dual-band polarization converter is proposed based on a reflective metasurface. The metasurface is an appropriate anisotropic structure with a pair of mutually perpendicular symmetric axes x and y, and the reflection phase difference under x- and y-polarized incidences is very close to 90° in the two frequency ranges of 7.9–9.2 GHz and 12.4–25.2 GHz, so the metasurface can be used as a high-efficiency dual-band polarization converter to achieve both linear-to-circular (LTC) and circular-to-linear (CTL) polarization conversions in two separated frequency bands. The simulation and experimental results show that, when the dual-band polarization converter is under the incidence of u- and v-polarized waves, the reflected wave will be converted to a circular-polarized (CP) one in the two frequency bands of 7.78–9.38 GHz and 12.30–25.60 GHz, a dual-band LTC polarization conversion will be achieved with high-efficiency; in addition, under CP incidence, the reflected wave will be converted to a linear-polarized one in the two frequency bands of 7.76–9.39 GHz and 12.22–25.57 GHz, a dual-band CTL polarization conversion with almost the same working band and polarization conversion rate will be achieved. Therefore, the dual-band polarization converter has great potential application values in various polarization controlled devices. © The Author(s), under exclusive licence to Springer-Verlag GmbH, DE part of Springer Nature 2022. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law.
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container_issue	11
title_short	Dual-band linear-to-circular and circular-to-linear polarization converter based on reflective metasurface
url	https://dx.doi.org/10.1007/s00339-022-06164-x
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author2	Huang, Wenzhun Guo, Jianxin Wang, Yanwei Ji, Xiang Ye, Hongjun
author2Str	Huang, Wenzhun Guo, Jianxin Wang, Yanwei Ji, Xiang Ye, Hongjun
ppnlink	235503231
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doi_str	10.1007/s00339-022-06164-x
up_date	2024-07-03T19:33:08.758Z
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Dual-band linear-to-circular and circular-to-linear polarization converter based on reflective metasurface

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