Laser-Excited Frequency-Switchable and Polarization-Controlled Amplitude-Tunable Terahertz Metamaterial Absorber
Abstract We achieve a frequency-switchable and amplitude-tunable terahertz metamaterial absorber (MMA) by means of introducing two different controlling degrees of freedom. Frequency-switchable function is controlled by external laser excitation, and amplitude-tunable function is controlled by the i...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Li, You [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2022 |
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| Schlagwörter: |
multifunctional frequency-switchable amplitude-tunable metamaterial absorber |
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| Anmerkung: |
© Springer Science+Business Media, LLC, part of Springer Nature 2022 |
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| Übergeordnetes Werk: |
Enthalten in: Journal of Russian laser research - New York, NY [u.a.] : Consultants Bureau, 1980, 43(2022), 3 vom: Mai, Seite 346-353 |
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| Übergeordnetes Werk: |
volume:43 ; year:2022 ; number:3 ; month:05 ; pages:346-353 |
| Links: |
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| DOI / URN: |
10.1007/s10946-022-10058-x |
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| Katalog-ID: |
SPR047345829 |
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| 520 | |a Abstract We achieve a frequency-switchable and amplitude-tunable terahertz metamaterial absorber (MMA) by means of introducing two different controlling degrees of freedom. Frequency-switchable function is controlled by external laser excitation, and amplitude-tunable function is controlled by the incident polarization angle. Two discrete resonance peaks can be detected, and the causes are investigated. With and without laser excitation, the absorption peak in the low-frequency band can dynamically switch between 1.285 and 1.295 THz and, in the high-frequency band, the one can dynamically switch between 2.845 and 2.42 THz. Meanwhile, the absorber is polarization sensitive for its symmetry structure. By rotating the device clockwise, an amplitude modulation depth of 13% can be obtained for the resonance absorption peak in the low-frequency band, and it is up to 100% for the one in the high-frequency band. Therefore, the amplitude dynamic modulation is realized at the same time as frequency switching, which provides a new approach for future terahertz devices possessing the characteristics of multifunction, portability, and intelligence. | ||
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| 650 | 4 | |a multifunctional frequency-switchable amplitude-tunable metamaterial absorber |7 (dpeaa)DE-He213 | |
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10.1007/s10946-022-10058-x doi (DE-627)SPR047345829 (SPR)s10946-022-10058-x-e DE-627 ger DE-627 rakwb eng Li, You verfasserin aut Laser-Excited Frequency-Switchable and Polarization-Controlled Amplitude-Tunable Terahertz Metamaterial Absorber 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer Science+Business Media, LLC, part of Springer Nature 2022 Abstract We achieve a frequency-switchable and amplitude-tunable terahertz metamaterial absorber (MMA) by means of introducing two different controlling degrees of freedom. Frequency-switchable function is controlled by external laser excitation, and amplitude-tunable function is controlled by the incident polarization angle. Two discrete resonance peaks can be detected, and the causes are investigated. With and without laser excitation, the absorption peak in the low-frequency band can dynamically switch between 1.285 and 1.295 THz and, in the high-frequency band, the one can dynamically switch between 2.845 and 2.42 THz. Meanwhile, the absorber is polarization sensitive for its symmetry structure. By rotating the device clockwise, an amplitude modulation depth of 13% can be obtained for the resonance absorption peak in the low-frequency band, and it is up to 100% for the one in the high-frequency band. Therefore, the amplitude dynamic modulation is realized at the same time as frequency switching, which provides a new approach for future terahertz devices possessing the characteristics of multifunction, portability, and intelligence. terahertz waves (dpeaa)DE-He213 multifunctional frequency-switchable amplitude-tunable metamaterial absorber (dpeaa)DE-He213 Wang, Xuan aut Enthalten in Journal of Russian laser research New York, NY [u.a.] : Consultants Bureau, 1980 43(2022), 3 vom: Mai, Seite 346-353 (DE-627)325573522 (DE-600)2037690-X 1573-8760 nnns volume:43 year:2022 number:3 month:05 pages:346-353 https://dx.doi.org/10.1007/s10946-022-10058-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_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_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_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 43 2022 3 05 346-353 |
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10.1007/s10946-022-10058-x doi (DE-627)SPR047345829 (SPR)s10946-022-10058-x-e DE-627 ger DE-627 rakwb eng Li, You verfasserin aut Laser-Excited Frequency-Switchable and Polarization-Controlled Amplitude-Tunable Terahertz Metamaterial Absorber 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer Science+Business Media, LLC, part of Springer Nature 2022 Abstract We achieve a frequency-switchable and amplitude-tunable terahertz metamaterial absorber (MMA) by means of introducing two different controlling degrees of freedom. Frequency-switchable function is controlled by external laser excitation, and amplitude-tunable function is controlled by the incident polarization angle. Two discrete resonance peaks can be detected, and the causes are investigated. With and without laser excitation, the absorption peak in the low-frequency band can dynamically switch between 1.285 and 1.295 THz and, in the high-frequency band, the one can dynamically switch between 2.845 and 2.42 THz. Meanwhile, the absorber is polarization sensitive for its symmetry structure. By rotating the device clockwise, an amplitude modulation depth of 13% can be obtained for the resonance absorption peak in the low-frequency band, and it is up to 100% for the one in the high-frequency band. Therefore, the amplitude dynamic modulation is realized at the same time as frequency switching, which provides a new approach for future terahertz devices possessing the characteristics of multifunction, portability, and intelligence. terahertz waves (dpeaa)DE-He213 multifunctional frequency-switchable amplitude-tunable metamaterial absorber (dpeaa)DE-He213 Wang, Xuan aut Enthalten in Journal of Russian laser research New York, NY [u.a.] : Consultants Bureau, 1980 43(2022), 3 vom: Mai, Seite 346-353 (DE-627)325573522 (DE-600)2037690-X 1573-8760 nnns volume:43 year:2022 number:3 month:05 pages:346-353 https://dx.doi.org/10.1007/s10946-022-10058-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_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_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_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 43 2022 3 05 346-353 |
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10.1007/s10946-022-10058-x doi (DE-627)SPR047345829 (SPR)s10946-022-10058-x-e DE-627 ger DE-627 rakwb eng Li, You verfasserin aut Laser-Excited Frequency-Switchable and Polarization-Controlled Amplitude-Tunable Terahertz Metamaterial Absorber 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer Science+Business Media, LLC, part of Springer Nature 2022 Abstract We achieve a frequency-switchable and amplitude-tunable terahertz metamaterial absorber (MMA) by means of introducing two different controlling degrees of freedom. Frequency-switchable function is controlled by external laser excitation, and amplitude-tunable function is controlled by the incident polarization angle. Two discrete resonance peaks can be detected, and the causes are investigated. With and without laser excitation, the absorption peak in the low-frequency band can dynamically switch between 1.285 and 1.295 THz and, in the high-frequency band, the one can dynamically switch between 2.845 and 2.42 THz. Meanwhile, the absorber is polarization sensitive for its symmetry structure. By rotating the device clockwise, an amplitude modulation depth of 13% can be obtained for the resonance absorption peak in the low-frequency band, and it is up to 100% for the one in the high-frequency band. Therefore, the amplitude dynamic modulation is realized at the same time as frequency switching, which provides a new approach for future terahertz devices possessing the characteristics of multifunction, portability, and intelligence. terahertz waves (dpeaa)DE-He213 multifunctional frequency-switchable amplitude-tunable metamaterial absorber (dpeaa)DE-He213 Wang, Xuan aut Enthalten in Journal of Russian laser research New York, NY [u.a.] : Consultants Bureau, 1980 43(2022), 3 vom: Mai, Seite 346-353 (DE-627)325573522 (DE-600)2037690-X 1573-8760 nnns volume:43 year:2022 number:3 month:05 pages:346-353 https://dx.doi.org/10.1007/s10946-022-10058-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_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_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_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 43 2022 3 05 346-353 |
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10.1007/s10946-022-10058-x doi (DE-627)SPR047345829 (SPR)s10946-022-10058-x-e DE-627 ger DE-627 rakwb eng Li, You verfasserin aut Laser-Excited Frequency-Switchable and Polarization-Controlled Amplitude-Tunable Terahertz Metamaterial Absorber 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer Science+Business Media, LLC, part of Springer Nature 2022 Abstract We achieve a frequency-switchable and amplitude-tunable terahertz metamaterial absorber (MMA) by means of introducing two different controlling degrees of freedom. Frequency-switchable function is controlled by external laser excitation, and amplitude-tunable function is controlled by the incident polarization angle. Two discrete resonance peaks can be detected, and the causes are investigated. With and without laser excitation, the absorption peak in the low-frequency band can dynamically switch between 1.285 and 1.295 THz and, in the high-frequency band, the one can dynamically switch between 2.845 and 2.42 THz. Meanwhile, the absorber is polarization sensitive for its symmetry structure. By rotating the device clockwise, an amplitude modulation depth of 13% can be obtained for the resonance absorption peak in the low-frequency band, and it is up to 100% for the one in the high-frequency band. Therefore, the amplitude dynamic modulation is realized at the same time as frequency switching, which provides a new approach for future terahertz devices possessing the characteristics of multifunction, portability, and intelligence. terahertz waves (dpeaa)DE-He213 multifunctional frequency-switchable amplitude-tunable metamaterial absorber (dpeaa)DE-He213 Wang, Xuan aut Enthalten in Journal of Russian laser research New York, NY [u.a.] : Consultants Bureau, 1980 43(2022), 3 vom: Mai, Seite 346-353 (DE-627)325573522 (DE-600)2037690-X 1573-8760 nnns volume:43 year:2022 number:3 month:05 pages:346-353 https://dx.doi.org/10.1007/s10946-022-10058-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_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_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_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 43 2022 3 05 346-353 |
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10.1007/s10946-022-10058-x doi (DE-627)SPR047345829 (SPR)s10946-022-10058-x-e DE-627 ger DE-627 rakwb eng Li, You verfasserin aut Laser-Excited Frequency-Switchable and Polarization-Controlled Amplitude-Tunable Terahertz Metamaterial Absorber 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer Science+Business Media, LLC, part of Springer Nature 2022 Abstract We achieve a frequency-switchable and amplitude-tunable terahertz metamaterial absorber (MMA) by means of introducing two different controlling degrees of freedom. Frequency-switchable function is controlled by external laser excitation, and amplitude-tunable function is controlled by the incident polarization angle. Two discrete resonance peaks can be detected, and the causes are investigated. With and without laser excitation, the absorption peak in the low-frequency band can dynamically switch between 1.285 and 1.295 THz and, in the high-frequency band, the one can dynamically switch between 2.845 and 2.42 THz. Meanwhile, the absorber is polarization sensitive for its symmetry structure. By rotating the device clockwise, an amplitude modulation depth of 13% can be obtained for the resonance absorption peak in the low-frequency band, and it is up to 100% for the one in the high-frequency band. Therefore, the amplitude dynamic modulation is realized at the same time as frequency switching, which provides a new approach for future terahertz devices possessing the characteristics of multifunction, portability, and intelligence. terahertz waves (dpeaa)DE-He213 multifunctional frequency-switchable amplitude-tunable metamaterial absorber (dpeaa)DE-He213 Wang, Xuan aut Enthalten in Journal of Russian laser research New York, NY [u.a.] : Consultants Bureau, 1980 43(2022), 3 vom: Mai, Seite 346-353 (DE-627)325573522 (DE-600)2037690-X 1573-8760 nnns volume:43 year:2022 number:3 month:05 pages:346-353 https://dx.doi.org/10.1007/s10946-022-10058-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_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_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_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 43 2022 3 05 346-353 |
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Li, You |
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Li, You misc terahertz waves misc multifunctional frequency-switchable amplitude-tunable metamaterial absorber Laser-Excited Frequency-Switchable and Polarization-Controlled Amplitude-Tunable Terahertz Metamaterial Absorber |
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Laser-Excited Frequency-Switchable and Polarization-Controlled Amplitude-Tunable Terahertz Metamaterial Absorber terahertz waves (dpeaa)DE-He213 multifunctional frequency-switchable amplitude-tunable metamaterial absorber (dpeaa)DE-He213 |
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laser-excited frequency-switchable and polarization-controlled amplitude-tunable terahertz metamaterial absorber |
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Laser-Excited Frequency-Switchable and Polarization-Controlled Amplitude-Tunable Terahertz Metamaterial Absorber |
| abstract |
Abstract We achieve a frequency-switchable and amplitude-tunable terahertz metamaterial absorber (MMA) by means of introducing two different controlling degrees of freedom. Frequency-switchable function is controlled by external laser excitation, and amplitude-tunable function is controlled by the incident polarization angle. Two discrete resonance peaks can be detected, and the causes are investigated. With and without laser excitation, the absorption peak in the low-frequency band can dynamically switch between 1.285 and 1.295 THz and, in the high-frequency band, the one can dynamically switch between 2.845 and 2.42 THz. Meanwhile, the absorber is polarization sensitive for its symmetry structure. By rotating the device clockwise, an amplitude modulation depth of 13% can be obtained for the resonance absorption peak in the low-frequency band, and it is up to 100% for the one in the high-frequency band. Therefore, the amplitude dynamic modulation is realized at the same time as frequency switching, which provides a new approach for future terahertz devices possessing the characteristics of multifunction, portability, and intelligence. © Springer Science+Business Media, LLC, part of Springer Nature 2022 |
| abstractGer |
Abstract We achieve a frequency-switchable and amplitude-tunable terahertz metamaterial absorber (MMA) by means of introducing two different controlling degrees of freedom. Frequency-switchable function is controlled by external laser excitation, and amplitude-tunable function is controlled by the incident polarization angle. Two discrete resonance peaks can be detected, and the causes are investigated. With and without laser excitation, the absorption peak in the low-frequency band can dynamically switch between 1.285 and 1.295 THz and, in the high-frequency band, the one can dynamically switch between 2.845 and 2.42 THz. Meanwhile, the absorber is polarization sensitive for its symmetry structure. By rotating the device clockwise, an amplitude modulation depth of 13% can be obtained for the resonance absorption peak in the low-frequency band, and it is up to 100% for the one in the high-frequency band. Therefore, the amplitude dynamic modulation is realized at the same time as frequency switching, which provides a new approach for future terahertz devices possessing the characteristics of multifunction, portability, and intelligence. © Springer Science+Business Media, LLC, part of Springer Nature 2022 |
| abstract_unstemmed |
Abstract We achieve a frequency-switchable and amplitude-tunable terahertz metamaterial absorber (MMA) by means of introducing two different controlling degrees of freedom. Frequency-switchable function is controlled by external laser excitation, and amplitude-tunable function is controlled by the incident polarization angle. Two discrete resonance peaks can be detected, and the causes are investigated. With and without laser excitation, the absorption peak in the low-frequency band can dynamically switch between 1.285 and 1.295 THz and, in the high-frequency band, the one can dynamically switch between 2.845 and 2.42 THz. Meanwhile, the absorber is polarization sensitive for its symmetry structure. By rotating the device clockwise, an amplitude modulation depth of 13% can be obtained for the resonance absorption peak in the low-frequency band, and it is up to 100% for the one in the high-frequency band. Therefore, the amplitude dynamic modulation is realized at the same time as frequency switching, which provides a new approach for future terahertz devices possessing the characteristics of multifunction, portability, and intelligence. © Springer Science+Business Media, LLC, part of Springer Nature 2022 |
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Laser-Excited Frequency-Switchable and Polarization-Controlled Amplitude-Tunable Terahertz Metamaterial Absorber |
| url |
https://dx.doi.org/10.1007/s10946-022-10058-x |
| remote_bool |
true |
| author2 |
Wang, Xuan |
| author2Str |
Wang, Xuan |
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| doi_str |
10.1007/s10946-022-10058-x |
| up_date |
2024-07-04T02:48:33.988Z |
| _version_ |
1803615012377329664 |
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Frequency-switchable function is controlled by external laser excitation, and amplitude-tunable function is controlled by the incident polarization angle. Two discrete resonance peaks can be detected, and the causes are investigated. With and without laser excitation, the absorption peak in the low-frequency band can dynamically switch between 1.285 and 1.295 THz and, in the high-frequency band, the one can dynamically switch between 2.845 and 2.42 THz. Meanwhile, the absorber is polarization sensitive for its symmetry structure. By rotating the device clockwise, an amplitude modulation depth of 13% can be obtained for the resonance absorption peak in the low-frequency band, and it is up to 100% for the one in the high-frequency band. 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