2020
DOI: 10.1016/j.carbon.2020.08.035
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Enhanced infrared photoresponse induced by symmetry breaking in a hybrid structure of graphene and plasmonic nanocavities

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Cited by 20 publications
(10 citation statements)
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“…To control the Seebeck coefficient, fabrication of a p – n junction through material doping or electrical gating can be employed to generate an asymmetric Seebeck coefficient, while such methods generally lead to complex device structures. The asymmetric metal contact with a large work function difference can also induce an asymmetric Seebeck coefficient, while inevitably introduce additional contact resistance to the system simultaneously. To generate a high temperature gradient, another widely used strategy is through localized illumination by focusing the light beam. , However, this strategy will be limited by the diffraction limit and is unpractical for an LWIR detector with sub-wavelength-scale dimensions. In addition, the temperature gradient can also be realized by nonuniform light absorption through localized optical absorption enhancement elements, such as plasmonic structures, antennas, nanocavities, and optical gratings. All strategies listed above need complex and/or sophisticated fabrication progresses, as well as high wavelength selectivity designs because of their specific optical resonances. These are undesirable for achieving a broadband photoresponse, which is one of the main advantages of PTE-based detectors.…”
mentioning
confidence: 99%
“…To control the Seebeck coefficient, fabrication of a p – n junction through material doping or electrical gating can be employed to generate an asymmetric Seebeck coefficient, while such methods generally lead to complex device structures. The asymmetric metal contact with a large work function difference can also induce an asymmetric Seebeck coefficient, while inevitably introduce additional contact resistance to the system simultaneously. To generate a high temperature gradient, another widely used strategy is through localized illumination by focusing the light beam. , However, this strategy will be limited by the diffraction limit and is unpractical for an LWIR detector with sub-wavelength-scale dimensions. In addition, the temperature gradient can also be realized by nonuniform light absorption through localized optical absorption enhancement elements, such as plasmonic structures, antennas, nanocavities, and optical gratings. All strategies listed above need complex and/or sophisticated fabrication progresses, as well as high wavelength selectivity designs because of their specific optical resonances. These are undesirable for achieving a broadband photoresponse, which is one of the main advantages of PTE-based detectors.…”
mentioning
confidence: 99%
“…Furthermore, as the Fermi level of graphene can be changed by applying a biased voltage, it provides an active and controllable method to tune the microwave absorption, absorption bandwidth, and modulation depth of the MGSS. [ 55–57 ] As shown in Figure S6, Supporting Information, the calculated peak absorption of the MGSS varied at different Fermi levels, and a bandwidth of over‐90% absorption can also be improved.…”
Section: Resultsmentioning
confidence: 99%
“…The photo-induced bond cleavage between the xanthene and phenyl group of a single rhodamine B isothiocyanate molecule is studied by combining Raman and fluorescence signals ( Figure 17 b). In addition, recently enhancements of the intensity of graphene Raman phonons and of graphene absorption have been reported when located in plasmonic nanocavities [ 136 , 137 ].…”
Section: Fluorescence Enhancement and Imagingmentioning
confidence: 99%