Tunable ultra-wideband polarization insensitivity wide-angle perfect THz absorber based on metamaterials containing vanadium dioxide
Abstract In this paper, a dynamically tunable ultra-broadband metamaterial perfect absorber (MPA) containing vanadium dioxide (V$ O_{2} $) is proposed and verified. The simulation results show that the MPA designed by us can not only achieve more than 90% absorption in the ultra-wideband range of 4....
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Zhang, Pingsheng [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2023 |
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| Anmerkung: |
© The Author(s), under exclusive licence to Springer-Verlag GmbH, DE part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. |
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| Übergeordnetes Werk: |
Enthalten in: Applied physics - Berlin : Springer, 1973, 129(2023), 9 vom: 24. Aug. |
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| Übergeordnetes Werk: |
volume:129 ; year:2023 ; number:9 ; day:24 ; month:08 |
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| DOI / URN: |
10.1007/s00339-023-06918-1 |
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SPR05285535X |
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| 520 | |a Abstract In this paper, a dynamically tunable ultra-broadband metamaterial perfect absorber (MPA) containing vanadium dioxide (V$ O_{2} $) is proposed and verified. The simulation results show that the MPA designed by us can not only achieve more than 90% absorption in the ultra-wideband range of 4.5–10 THz, but also achieve more than 99% perfect absorption in the wideband range of 5.5–8.3 THz. And the high absorption rate is caused by electric dipole resonance, which can be demonstrated by the distribution of the electric field. By adjusting the conductivity of V$ O_{2} $ from 200 to 4 × $ 10^{4} $ S/m through changing the temperature to induce the phase transition of V$ O_{2} $, one can continuously adjust the absorption of the proposed MPA from 16 to 100%. Furthermore, the proposed structure can achieve perfect absorption in a wide range of angles with TE polarization within 60°and TM polarization within 50°, which can effectively promote the development of THz devices, such as optical switches and modulators. | ||
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| 700 | 1 | |a Qin, Kaipeng |4 aut | |
| 700 | 1 | |a Deng, Xin-Hua |0 (orcid)0000-0001-6707-5697 |4 aut | |
| 700 | 1 | |a Liu, Hongfei |4 aut | |
| 700 | 1 | |a Yuan, Jiren |4 aut | |
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10.1007/s00339-023-06918-1 doi (DE-627)SPR05285535X (SPR)s00339-023-06918-1-e DE-627 ger DE-627 rakwb eng Zhang, Pingsheng verfasserin aut Tunable ultra-wideband polarization insensitivity wide-angle perfect THz absorber based on metamaterials containing vanadium dioxide 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer-Verlag GmbH, DE part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract In this paper, a dynamically tunable ultra-broadband metamaterial perfect absorber (MPA) containing vanadium dioxide (V$ O_{2} $) is proposed and verified. The simulation results show that the MPA designed by us can not only achieve more than 90% absorption in the ultra-wideband range of 4.5–10 THz, but also achieve more than 99% perfect absorption in the wideband range of 5.5–8.3 THz. And the high absorption rate is caused by electric dipole resonance, which can be demonstrated by the distribution of the electric field. By adjusting the conductivity of V$ O_{2} $ from 200 to 4 × $ 10^{4} $ S/m through changing the temperature to induce the phase transition of V$ O_{2} $, one can continuously adjust the absorption of the proposed MPA from 16 to 100%. Furthermore, the proposed structure can achieve perfect absorption in a wide range of angles with TE polarization within 60°and TM polarization within 50°, which can effectively promote the development of THz devices, such as optical switches and modulators. Metamaterials (dpeaa)DE-He213 Ultra-wideband (dpeaa)DE-He213 Wide-angle perfect THz absorber (dpeaa)DE-He213 Qin, Kaipeng aut Deng, Xin-Hua (orcid)0000-0001-6707-5697 aut Liu, Hongfei aut Yuan, Jiren aut Enthalten in Applied physics Berlin : Springer, 1973 129(2023), 9 vom: 24. Aug. (DE-627)235503231 (DE-600)1398311-8 1432-0630 nnns volume:129 year:2023 number:9 day:24 month:08 https://dx.doi.org/10.1007/s00339-023-06918-1 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 129 2023 9 24 08 |
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10.1007/s00339-023-06918-1 doi (DE-627)SPR05285535X (SPR)s00339-023-06918-1-e DE-627 ger DE-627 rakwb eng Zhang, Pingsheng verfasserin aut Tunable ultra-wideband polarization insensitivity wide-angle perfect THz absorber based on metamaterials containing vanadium dioxide 2023 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 2023. 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 paper, a dynamically tunable ultra-broadband metamaterial perfect absorber (MPA) containing vanadium dioxide (V$ O_{2} $) is proposed and verified. The simulation results show that the MPA designed by us can not only achieve more than 90% absorption in the ultra-wideband range of 4.5–10 THz, but also achieve more than 99% perfect absorption in the wideband range of 5.5–8.3 THz. And the high absorption rate is caused by electric dipole resonance, which can be demonstrated by the distribution of the electric field. By adjusting the conductivity of V$ O_{2} $ from 200 to 4 × $ 10^{4} $ S/m through changing the temperature to induce the phase transition of V$ O_{2} $, one can continuously adjust the absorption of the proposed MPA from 16 to 100%. Furthermore, the proposed structure can achieve perfect absorption in a wide range of angles with TE polarization within 60°and TM polarization within 50°, which can effectively promote the development of THz devices, such as optical switches and modulators. Metamaterials (dpeaa)DE-He213 Ultra-wideband (dpeaa)DE-He213 Wide-angle perfect THz absorber (dpeaa)DE-He213 Qin, Kaipeng aut Deng, Xin-Hua (orcid)0000-0001-6707-5697 aut Liu, Hongfei aut Yuan, Jiren aut Enthalten in Applied physics Berlin : Springer, 1973 129(2023), 9 vom: 24. Aug. (DE-627)235503231 (DE-600)1398311-8 1432-0630 nnns volume:129 year:2023 number:9 day:24 month:08 https://dx.doi.org/10.1007/s00339-023-06918-1 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 129 2023 9 24 08 |
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10.1007/s00339-023-06918-1 doi (DE-627)SPR05285535X (SPR)s00339-023-06918-1-e DE-627 ger DE-627 rakwb eng Zhang, Pingsheng verfasserin aut Tunable ultra-wideband polarization insensitivity wide-angle perfect THz absorber based on metamaterials containing vanadium dioxide 2023 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 2023. 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 paper, a dynamically tunable ultra-broadband metamaterial perfect absorber (MPA) containing vanadium dioxide (V$ O_{2} $) is proposed and verified. The simulation results show that the MPA designed by us can not only achieve more than 90% absorption in the ultra-wideband range of 4.5–10 THz, but also achieve more than 99% perfect absorption in the wideband range of 5.5–8.3 THz. And the high absorption rate is caused by electric dipole resonance, which can be demonstrated by the distribution of the electric field. By adjusting the conductivity of V$ O_{2} $ from 200 to 4 × $ 10^{4} $ S/m through changing the temperature to induce the phase transition of V$ O_{2} $, one can continuously adjust the absorption of the proposed MPA from 16 to 100%. Furthermore, the proposed structure can achieve perfect absorption in a wide range of angles with TE polarization within 60°and TM polarization within 50°, which can effectively promote the development of THz devices, such as optical switches and modulators. Metamaterials (dpeaa)DE-He213 Ultra-wideband (dpeaa)DE-He213 Wide-angle perfect THz absorber (dpeaa)DE-He213 Qin, Kaipeng aut Deng, Xin-Hua (orcid)0000-0001-6707-5697 aut Liu, Hongfei aut Yuan, Jiren aut Enthalten in Applied physics Berlin : Springer, 1973 129(2023), 9 vom: 24. Aug. (DE-627)235503231 (DE-600)1398311-8 1432-0630 nnns volume:129 year:2023 number:9 day:24 month:08 https://dx.doi.org/10.1007/s00339-023-06918-1 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 129 2023 9 24 08 |
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10.1007/s00339-023-06918-1 doi (DE-627)SPR05285535X (SPR)s00339-023-06918-1-e DE-627 ger DE-627 rakwb eng Zhang, Pingsheng verfasserin aut Tunable ultra-wideband polarization insensitivity wide-angle perfect THz absorber based on metamaterials containing vanadium dioxide 2023 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 2023. 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 paper, a dynamically tunable ultra-broadband metamaterial perfect absorber (MPA) containing vanadium dioxide (V$ O_{2} $) is proposed and verified. The simulation results show that the MPA designed by us can not only achieve more than 90% absorption in the ultra-wideband range of 4.5–10 THz, but also achieve more than 99% perfect absorption in the wideband range of 5.5–8.3 THz. And the high absorption rate is caused by electric dipole resonance, which can be demonstrated by the distribution of the electric field. By adjusting the conductivity of V$ O_{2} $ from 200 to 4 × $ 10^{4} $ S/m through changing the temperature to induce the phase transition of V$ O_{2} $, one can continuously adjust the absorption of the proposed MPA from 16 to 100%. Furthermore, the proposed structure can achieve perfect absorption in a wide range of angles with TE polarization within 60°and TM polarization within 50°, which can effectively promote the development of THz devices, such as optical switches and modulators. Metamaterials (dpeaa)DE-He213 Ultra-wideband (dpeaa)DE-He213 Wide-angle perfect THz absorber (dpeaa)DE-He213 Qin, Kaipeng aut Deng, Xin-Hua (orcid)0000-0001-6707-5697 aut Liu, Hongfei aut Yuan, Jiren aut Enthalten in Applied physics Berlin : Springer, 1973 129(2023), 9 vom: 24. Aug. (DE-627)235503231 (DE-600)1398311-8 1432-0630 nnns volume:129 year:2023 number:9 day:24 month:08 https://dx.doi.org/10.1007/s00339-023-06918-1 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 129 2023 9 24 08 |
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10.1007/s00339-023-06918-1 doi (DE-627)SPR05285535X (SPR)s00339-023-06918-1-e DE-627 ger DE-627 rakwb eng Zhang, Pingsheng verfasserin aut Tunable ultra-wideband polarization insensitivity wide-angle perfect THz absorber based on metamaterials containing vanadium dioxide 2023 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 2023. 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 paper, a dynamically tunable ultra-broadband metamaterial perfect absorber (MPA) containing vanadium dioxide (V$ O_{2} $) is proposed and verified. The simulation results show that the MPA designed by us can not only achieve more than 90% absorption in the ultra-wideband range of 4.5–10 THz, but also achieve more than 99% perfect absorption in the wideband range of 5.5–8.3 THz. And the high absorption rate is caused by electric dipole resonance, which can be demonstrated by the distribution of the electric field. By adjusting the conductivity of V$ O_{2} $ from 200 to 4 × $ 10^{4} $ S/m through changing the temperature to induce the phase transition of V$ O_{2} $, one can continuously adjust the absorption of the proposed MPA from 16 to 100%. Furthermore, the proposed structure can achieve perfect absorption in a wide range of angles with TE polarization within 60°and TM polarization within 50°, which can effectively promote the development of THz devices, such as optical switches and modulators. Metamaterials (dpeaa)DE-He213 Ultra-wideband (dpeaa)DE-He213 Wide-angle perfect THz absorber (dpeaa)DE-He213 Qin, Kaipeng aut Deng, Xin-Hua (orcid)0000-0001-6707-5697 aut Liu, Hongfei aut Yuan, Jiren aut Enthalten in Applied physics Berlin : Springer, 1973 129(2023), 9 vom: 24. Aug. (DE-627)235503231 (DE-600)1398311-8 1432-0630 nnns volume:129 year:2023 number:9 day:24 month:08 https://dx.doi.org/10.1007/s00339-023-06918-1 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 129 2023 9 24 08 |
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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.</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract In this paper, a dynamically tunable ultra-broadband metamaterial perfect absorber (MPA) containing vanadium dioxide (V$ O_{2} $) is proposed and verified. The simulation results show that the MPA designed by us can not only achieve more than 90% absorption in the ultra-wideband range of 4.5–10 THz, but also achieve more than 99% perfect absorption in the wideband range of 5.5–8.3 THz. And the high absorption rate is caused by electric dipole resonance, which can be demonstrated by the distribution of the electric field. By adjusting the conductivity of V$ O_{2} $ from 200 to 4 × $ 10^{4} $ S/m through changing the temperature to induce the phase transition of V$ O_{2} $, one can continuously adjust the absorption of the proposed MPA from 16 to 100%. 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Zhang, Pingsheng |
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Tunable ultra-wideband polarization insensitivity wide-angle perfect THz absorber based on metamaterials containing vanadium dioxide Metamaterials (dpeaa)DE-He213 Ultra-wideband (dpeaa)DE-He213 Wide-angle perfect THz absorber (dpeaa)DE-He213 |
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tunable ultra-wideband polarization insensitivity wide-angle perfect thz absorber based on metamaterials containing vanadium dioxide |
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Tunable ultra-wideband polarization insensitivity wide-angle perfect THz absorber based on metamaterials containing vanadium dioxide |
| abstract |
Abstract In this paper, a dynamically tunable ultra-broadband metamaterial perfect absorber (MPA) containing vanadium dioxide (V$ O_{2} $) is proposed and verified. The simulation results show that the MPA designed by us can not only achieve more than 90% absorption in the ultra-wideband range of 4.5–10 THz, but also achieve more than 99% perfect absorption in the wideband range of 5.5–8.3 THz. And the high absorption rate is caused by electric dipole resonance, which can be demonstrated by the distribution of the electric field. By adjusting the conductivity of V$ O_{2} $ from 200 to 4 × $ 10^{4} $ S/m through changing the temperature to induce the phase transition of V$ O_{2} $, one can continuously adjust the absorption of the proposed MPA from 16 to 100%. Furthermore, the proposed structure can achieve perfect absorption in a wide range of angles with TE polarization within 60°and TM polarization within 50°, which can effectively promote the development of THz devices, such as optical switches and modulators. © The Author(s), under exclusive licence to Springer-Verlag GmbH, DE part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. |
| abstractGer |
Abstract In this paper, a dynamically tunable ultra-broadband metamaterial perfect absorber (MPA) containing vanadium dioxide (V$ O_{2} $) is proposed and verified. The simulation results show that the MPA designed by us can not only achieve more than 90% absorption in the ultra-wideband range of 4.5–10 THz, but also achieve more than 99% perfect absorption in the wideband range of 5.5–8.3 THz. And the high absorption rate is caused by electric dipole resonance, which can be demonstrated by the distribution of the electric field. By adjusting the conductivity of V$ O_{2} $ from 200 to 4 × $ 10^{4} $ S/m through changing the temperature to induce the phase transition of V$ O_{2} $, one can continuously adjust the absorption of the proposed MPA from 16 to 100%. Furthermore, the proposed structure can achieve perfect absorption in a wide range of angles with TE polarization within 60°and TM polarization within 50°, which can effectively promote the development of THz devices, such as optical switches and modulators. © The Author(s), under exclusive licence to Springer-Verlag GmbH, DE part of Springer Nature 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. |
| abstract_unstemmed |
Abstract In this paper, a dynamically tunable ultra-broadband metamaterial perfect absorber (MPA) containing vanadium dioxide (V$ O_{2} $) is proposed and verified. The simulation results show that the MPA designed by us can not only achieve more than 90% absorption in the ultra-wideband range of 4.5–10 THz, but also achieve more than 99% perfect absorption in the wideband range of 5.5–8.3 THz. And the high absorption rate is caused by electric dipole resonance, which can be demonstrated by the distribution of the electric field. By adjusting the conductivity of V$ O_{2} $ from 200 to 4 × $ 10^{4} $ S/m through changing the temperature to induce the phase transition of V$ O_{2} $, one can continuously adjust the absorption of the proposed MPA from 16 to 100%. Furthermore, the proposed structure can achieve perfect absorption in a wide range of angles with TE polarization within 60°and TM polarization within 50°, which can effectively promote the development of THz devices, such as optical switches and modulators. © The Author(s), under exclusive licence to Springer-Verlag GmbH, DE part of Springer Nature 2023. 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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Tunable ultra-wideband polarization insensitivity wide-angle perfect THz absorber based on metamaterials containing vanadium dioxide |
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https://dx.doi.org/10.1007/s00339-023-06918-1 |
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Qin, Kaipeng Deng, Xin-Hua Liu, Hongfei Yuan, Jiren |
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Qin, Kaipeng Deng, Xin-Hua Liu, Hongfei Yuan, Jiren |
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10.1007/s00339-023-06918-1 |
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2024-07-03T15:16:04.386Z |
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| score |
7.3997602 |