Wideband polarization-insensitive metamaterial perfect absorber based on bilayer graphene metasurface
Abstract In this article a polarization-insensitive broadband adjustable THz metamaterial absorber is proposed and examined. The absorber is constructed of a periodic array of patterned graphene elements that is like the star as unit cell, placed on a $ SiO_{2} $ dielectric layer and it is terminate...
Ausführliche Beschreibung
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| Autor*in: |
Khodadadi, Bahareh [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2022 |
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| Anmerkung: |
© The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2022. corrected publication 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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| Übergeordnetes Werk: |
Enthalten in: Optical and quantum electronics - Dordrecht [u.a.] : Springer Science + Business Media B.V, 1969, 54(2022), 11 vom: 16. Sept. |
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| Übergeordnetes Werk: |
volume:54 ; year:2022 ; number:11 ; day:16 ; month:09 |
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| DOI / URN: |
10.1007/s11082-022-04136-2 |
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SPR048123269 |
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| 520 | |a Abstract In this article a polarization-insensitive broadband adjustable THz metamaterial absorber is proposed and examined. The absorber is constructed of a periodic array of patterned graphene elements that is like the star as unit cell, placed on a $ SiO_{2} $ dielectric layer and it is terminated by a gold reflector. The simulation results display that the proposed absorber with single graphene layer has bandwidth of 1.96 THz for absorption above 90% with the peak absorption of 98.45% in 4.18 THz. This absorber with two graphene layers covers the frequency range of 2.99–6.16 THz for absorption > 90% with the highest absorption of 99.99% at 5.30 THz. The bandwidth for absorption above 99% is 0.72 THz. The absorption curves for TE and TM modes similar together. The electric fields and current surface of proposed absorber have been investigated on low and peak absorption frequency in TE and TM modes. This structure has features such as polarization independent for normal incident waves owing to its symmetric structure, good bearing angle of incident wave and adjustable by altering the Fermi level of graphene. Due to these properties, the broadband metamaterial perfect absorber is suitable for applications such as camouflage systems, imaging, detector, energy harvesting, and modulators. | ||
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| 650 | 4 | |a Polarization insensitive |7 (dpeaa)DE-He213 | |
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| 700 | 1 | |a Ghods, Vahid |4 aut | |
| 700 | 1 | |a Babaeinik, Majid |4 aut | |
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10.1007/s11082-022-04136-2 doi (DE-627)SPR048123269 (SPR)s11082-022-04136-2-e DE-627 ger DE-627 rakwb eng Khodadadi, Bahareh verfasserin aut Wideband polarization-insensitive metamaterial perfect absorber based on bilayer graphene metasurface 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2022. corrected publication 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 article a polarization-insensitive broadband adjustable THz metamaterial absorber is proposed and examined. The absorber is constructed of a periodic array of patterned graphene elements that is like the star as unit cell, placed on a $ SiO_{2} $ dielectric layer and it is terminated by a gold reflector. The simulation results display that the proposed absorber with single graphene layer has bandwidth of 1.96 THz for absorption above 90% with the peak absorption of 98.45% in 4.18 THz. This absorber with two graphene layers covers the frequency range of 2.99–6.16 THz for absorption > 90% with the highest absorption of 99.99% at 5.30 THz. The bandwidth for absorption above 99% is 0.72 THz. The absorption curves for TE and TM modes similar together. The electric fields and current surface of proposed absorber have been investigated on low and peak absorption frequency in TE and TM modes. This structure has features such as polarization independent for normal incident waves owing to its symmetric structure, good bearing angle of incident wave and adjustable by altering the Fermi level of graphene. Due to these properties, the broadband metamaterial perfect absorber is suitable for applications such as camouflage systems, imaging, detector, energy harvesting, and modulators. Terahertz (dpeaa)DE-He213 Metamaterial perfect absorber (dpeaa)DE-He213 Broadband (dpeaa)DE-He213 Polarization insensitive (dpeaa)DE-He213 Rezaei, Pejman (orcid)0000-0002-1266-3229 aut Ghods, Vahid aut Babaeinik, Majid aut Enthalten in Optical and quantum electronics Dordrecht [u.a.] : Springer Science + Business Media B.V, 1969 54(2022), 11 vom: 16. Sept. (DE-627)312693869 (DE-600)2000642-1 1572-817X nnns volume:54 year:2022 number:11 day:16 month:09 https://dx.doi.org/10.1007/s11082-022-04136-2 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_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_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_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 54 2022 11 16 09 |
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10.1007/s11082-022-04136-2 doi (DE-627)SPR048123269 (SPR)s11082-022-04136-2-e DE-627 ger DE-627 rakwb eng Khodadadi, Bahareh verfasserin aut Wideband polarization-insensitive metamaterial perfect absorber based on bilayer graphene metasurface 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2022. corrected publication 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 article a polarization-insensitive broadband adjustable THz metamaterial absorber is proposed and examined. The absorber is constructed of a periodic array of patterned graphene elements that is like the star as unit cell, placed on a $ SiO_{2} $ dielectric layer and it is terminated by a gold reflector. The simulation results display that the proposed absorber with single graphene layer has bandwidth of 1.96 THz for absorption above 90% with the peak absorption of 98.45% in 4.18 THz. This absorber with two graphene layers covers the frequency range of 2.99–6.16 THz for absorption > 90% with the highest absorption of 99.99% at 5.30 THz. The bandwidth for absorption above 99% is 0.72 THz. The absorption curves for TE and TM modes similar together. The electric fields and current surface of proposed absorber have been investigated on low and peak absorption frequency in TE and TM modes. This structure has features such as polarization independent for normal incident waves owing to its symmetric structure, good bearing angle of incident wave and adjustable by altering the Fermi level of graphene. Due to these properties, the broadband metamaterial perfect absorber is suitable for applications such as camouflage systems, imaging, detector, energy harvesting, and modulators. Terahertz (dpeaa)DE-He213 Metamaterial perfect absorber (dpeaa)DE-He213 Broadband (dpeaa)DE-He213 Polarization insensitive (dpeaa)DE-He213 Rezaei, Pejman (orcid)0000-0002-1266-3229 aut Ghods, Vahid aut Babaeinik, Majid aut Enthalten in Optical and quantum electronics Dordrecht [u.a.] : Springer Science + Business Media B.V, 1969 54(2022), 11 vom: 16. Sept. (DE-627)312693869 (DE-600)2000642-1 1572-817X nnns volume:54 year:2022 number:11 day:16 month:09 https://dx.doi.org/10.1007/s11082-022-04136-2 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_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_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_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 54 2022 11 16 09 |
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10.1007/s11082-022-04136-2 doi (DE-627)SPR048123269 (SPR)s11082-022-04136-2-e DE-627 ger DE-627 rakwb eng Khodadadi, Bahareh verfasserin aut Wideband polarization-insensitive metamaterial perfect absorber based on bilayer graphene metasurface 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2022. corrected publication 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 article a polarization-insensitive broadband adjustable THz metamaterial absorber is proposed and examined. The absorber is constructed of a periodic array of patterned graphene elements that is like the star as unit cell, placed on a $ SiO_{2} $ dielectric layer and it is terminated by a gold reflector. The simulation results display that the proposed absorber with single graphene layer has bandwidth of 1.96 THz for absorption above 90% with the peak absorption of 98.45% in 4.18 THz. This absorber with two graphene layers covers the frequency range of 2.99–6.16 THz for absorption > 90% with the highest absorption of 99.99% at 5.30 THz. The bandwidth for absorption above 99% is 0.72 THz. The absorption curves for TE and TM modes similar together. The electric fields and current surface of proposed absorber have been investigated on low and peak absorption frequency in TE and TM modes. This structure has features such as polarization independent for normal incident waves owing to its symmetric structure, good bearing angle of incident wave and adjustable by altering the Fermi level of graphene. Due to these properties, the broadband metamaterial perfect absorber is suitable for applications such as camouflage systems, imaging, detector, energy harvesting, and modulators. Terahertz (dpeaa)DE-He213 Metamaterial perfect absorber (dpeaa)DE-He213 Broadband (dpeaa)DE-He213 Polarization insensitive (dpeaa)DE-He213 Rezaei, Pejman (orcid)0000-0002-1266-3229 aut Ghods, Vahid aut Babaeinik, Majid aut Enthalten in Optical and quantum electronics Dordrecht [u.a.] : Springer Science + Business Media B.V, 1969 54(2022), 11 vom: 16. Sept. (DE-627)312693869 (DE-600)2000642-1 1572-817X nnns volume:54 year:2022 number:11 day:16 month:09 https://dx.doi.org/10.1007/s11082-022-04136-2 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_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_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_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 54 2022 11 16 09 |
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10.1007/s11082-022-04136-2 doi (DE-627)SPR048123269 (SPR)s11082-022-04136-2-e DE-627 ger DE-627 rakwb eng Khodadadi, Bahareh verfasserin aut Wideband polarization-insensitive metamaterial perfect absorber based on bilayer graphene metasurface 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2022. corrected publication 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 article a polarization-insensitive broadband adjustable THz metamaterial absorber is proposed and examined. The absorber is constructed of a periodic array of patterned graphene elements that is like the star as unit cell, placed on a $ SiO_{2} $ dielectric layer and it is terminated by a gold reflector. The simulation results display that the proposed absorber with single graphene layer has bandwidth of 1.96 THz for absorption above 90% with the peak absorption of 98.45% in 4.18 THz. This absorber with two graphene layers covers the frequency range of 2.99–6.16 THz for absorption > 90% with the highest absorption of 99.99% at 5.30 THz. The bandwidth for absorption above 99% is 0.72 THz. The absorption curves for TE and TM modes similar together. The electric fields and current surface of proposed absorber have been investigated on low and peak absorption frequency in TE and TM modes. This structure has features such as polarization independent for normal incident waves owing to its symmetric structure, good bearing angle of incident wave and adjustable by altering the Fermi level of graphene. Due to these properties, the broadband metamaterial perfect absorber is suitable for applications such as camouflage systems, imaging, detector, energy harvesting, and modulators. Terahertz (dpeaa)DE-He213 Metamaterial perfect absorber (dpeaa)DE-He213 Broadband (dpeaa)DE-He213 Polarization insensitive (dpeaa)DE-He213 Rezaei, Pejman (orcid)0000-0002-1266-3229 aut Ghods, Vahid aut Babaeinik, Majid aut Enthalten in Optical and quantum electronics Dordrecht [u.a.] : Springer Science + Business Media B.V, 1969 54(2022), 11 vom: 16. Sept. (DE-627)312693869 (DE-600)2000642-1 1572-817X nnns volume:54 year:2022 number:11 day:16 month:09 https://dx.doi.org/10.1007/s11082-022-04136-2 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_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_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_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 54 2022 11 16 09 |
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10.1007/s11082-022-04136-2 doi (DE-627)SPR048123269 (SPR)s11082-022-04136-2-e DE-627 ger DE-627 rakwb eng Khodadadi, Bahareh verfasserin aut Wideband polarization-insensitive metamaterial perfect absorber based on bilayer graphene metasurface 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2022. corrected publication 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 article a polarization-insensitive broadband adjustable THz metamaterial absorber is proposed and examined. The absorber is constructed of a periodic array of patterned graphene elements that is like the star as unit cell, placed on a $ SiO_{2} $ dielectric layer and it is terminated by a gold reflector. The simulation results display that the proposed absorber with single graphene layer has bandwidth of 1.96 THz for absorption above 90% with the peak absorption of 98.45% in 4.18 THz. This absorber with two graphene layers covers the frequency range of 2.99–6.16 THz for absorption > 90% with the highest absorption of 99.99% at 5.30 THz. The bandwidth for absorption above 99% is 0.72 THz. The absorption curves for TE and TM modes similar together. The electric fields and current surface of proposed absorber have been investigated on low and peak absorption frequency in TE and TM modes. This structure has features such as polarization independent for normal incident waves owing to its symmetric structure, good bearing angle of incident wave and adjustable by altering the Fermi level of graphene. Due to these properties, the broadband metamaterial perfect absorber is suitable for applications such as camouflage systems, imaging, detector, energy harvesting, and modulators. Terahertz (dpeaa)DE-He213 Metamaterial perfect absorber (dpeaa)DE-He213 Broadband (dpeaa)DE-He213 Polarization insensitive (dpeaa)DE-He213 Rezaei, Pejman (orcid)0000-0002-1266-3229 aut Ghods, Vahid aut Babaeinik, Majid aut Enthalten in Optical and quantum electronics Dordrecht [u.a.] : Springer Science + Business Media B.V, 1969 54(2022), 11 vom: 16. Sept. (DE-627)312693869 (DE-600)2000642-1 1572-817X nnns volume:54 year:2022 number:11 day:16 month:09 https://dx.doi.org/10.1007/s11082-022-04136-2 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_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_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_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 54 2022 11 16 09 |
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wideband polarization-insensitive metamaterial perfect absorber based on bilayer graphene metasurface |
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Wideband polarization-insensitive metamaterial perfect absorber based on bilayer graphene metasurface |
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Abstract In this article a polarization-insensitive broadband adjustable THz metamaterial absorber is proposed and examined. The absorber is constructed of a periodic array of patterned graphene elements that is like the star as unit cell, placed on a $ SiO_{2} $ dielectric layer and it is terminated by a gold reflector. The simulation results display that the proposed absorber with single graphene layer has bandwidth of 1.96 THz for absorption above 90% with the peak absorption of 98.45% in 4.18 THz. This absorber with two graphene layers covers the frequency range of 2.99–6.16 THz for absorption > 90% with the highest absorption of 99.99% at 5.30 THz. The bandwidth for absorption above 99% is 0.72 THz. The absorption curves for TE and TM modes similar together. The electric fields and current surface of proposed absorber have been investigated on low and peak absorption frequency in TE and TM modes. This structure has features such as polarization independent for normal incident waves owing to its symmetric structure, good bearing angle of incident wave and adjustable by altering the Fermi level of graphene. Due to these properties, the broadband metamaterial perfect absorber is suitable for applications such as camouflage systems, imaging, detector, energy harvesting, and modulators. © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2022. corrected publication 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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Abstract In this article a polarization-insensitive broadband adjustable THz metamaterial absorber is proposed and examined. The absorber is constructed of a periodic array of patterned graphene elements that is like the star as unit cell, placed on a $ SiO_{2} $ dielectric layer and it is terminated by a gold reflector. The simulation results display that the proposed absorber with single graphene layer has bandwidth of 1.96 THz for absorption above 90% with the peak absorption of 98.45% in 4.18 THz. This absorber with two graphene layers covers the frequency range of 2.99–6.16 THz for absorption > 90% with the highest absorption of 99.99% at 5.30 THz. The bandwidth for absorption above 99% is 0.72 THz. The absorption curves for TE and TM modes similar together. The electric fields and current surface of proposed absorber have been investigated on low and peak absorption frequency in TE and TM modes. This structure has features such as polarization independent for normal incident waves owing to its symmetric structure, good bearing angle of incident wave and adjustable by altering the Fermi level of graphene. Due to these properties, the broadband metamaterial perfect absorber is suitable for applications such as camouflage systems, imaging, detector, energy harvesting, and modulators. © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2022. corrected publication 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 article a polarization-insensitive broadband adjustable THz metamaterial absorber is proposed and examined. The absorber is constructed of a periodic array of patterned graphene elements that is like the star as unit cell, placed on a $ SiO_{2} $ dielectric layer and it is terminated by a gold reflector. The simulation results display that the proposed absorber with single graphene layer has bandwidth of 1.96 THz for absorption above 90% with the peak absorption of 98.45% in 4.18 THz. This absorber with two graphene layers covers the frequency range of 2.99–6.16 THz for absorption > 90% with the highest absorption of 99.99% at 5.30 THz. The bandwidth for absorption above 99% is 0.72 THz. The absorption curves for TE and TM modes similar together. The electric fields and current surface of proposed absorber have been investigated on low and peak absorption frequency in TE and TM modes. This structure has features such as polarization independent for normal incident waves owing to its symmetric structure, good bearing angle of incident wave and adjustable by altering the Fermi level of graphene. Due to these properties, the broadband metamaterial perfect absorber is suitable for applications such as camouflage systems, imaging, detector, energy harvesting, and modulators. © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2022. corrected publication 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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Wideband polarization-insensitive metamaterial perfect absorber based on bilayer graphene metasurface |
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Rezaei, Pejman Ghods, Vahid Babaeinik, Majid |
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| score |
7.3974237 |