2017
DOI: 10.1063/1.4973898
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Enhanced universal absorption of graphene in a Salisbury screen

Abstract: As an emerging optoelectronic material, graphene's universal absorption of about 2.3% over a broad frequency range from infrared to visible, as determined by its interband transition, presents both a new opportunity and a limitation. Here we report on a multifold enhancement of the absorption using a simple strategy, often referred to as the Salisbury screen. It consists of a graphene sheet on top of a SiO2 dielectric layer backed with a copper metallic reflector. For a monolayer graphene, peak absorptions of … Show more

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Cited by 15 publications
(8 citation statements)
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“…The most effective frequency tuning is achieved with the mobility between µ m = 1000 cm 2 V −1 s −1 and µ m = 2000 cm 2 V −1 s −1 . This mobility range is also quite reasonable and can be obtained using CVD-grown graphene [21]- [23], [45].…”
Section: A Frequency-tunable Absorbersupporting
confidence: 65%
See 1 more Smart Citation
“…The most effective frequency tuning is achieved with the mobility between µ m = 1000 cm 2 V −1 s −1 and µ m = 2000 cm 2 V −1 s −1 . This mobility range is also quite reasonable and can be obtained using CVD-grown graphene [21]- [23], [45].…”
Section: A Frequency-tunable Absorbersupporting
confidence: 65%
“…In this case, perfect absorption may be possible even without the assistance of metallic patches. This explains the enhanced absorption of graphene Salisbury screen at TE grazing incidences reported in [44], [45].…”
Section: A Analytical Modelingmentioning
confidence: 73%
“…But, it is still a challenge, as pointed out in the very recent reports [ 44 46 ]. At present, different approaches have been proposed to broaden the bandwidth of graphene absorption in wide frequency range from THz [ 44 62 ] and infrared [ 63 65 ] to optical frequencies [ 19 , 23 , 29 , 31 , 34 36 , 38 40 , 43 ]. Especially, a multi-resonator approach was proven to be a very effective method to resolve the bandwidth limitation of graphene absorption in the THz and infrared regions [ 45 , 46 , 62 , 63 ].…”
Section: Introductionmentioning
confidence: 99%
“…Due to this sandwich structure, there exist two resonant cavities which are composed by the graphene and multi‐layer dielectrics, when the THz signal is being absorbed fully which results ‘0’ code (the THz wave reflection is 0.0425). When the gate voltage is unbiased, the graphene just works as a thin film (means above 2.3% of absorption from the previous study [20]), then a larger amplitude of signal can be detected and this could be translated into the digital signal ‘1’ code (the THz wave reflection reaches 0.9492) [21, 22]. The device can be characterised using a THz imaging and spectroscopy setup based on a Virginia Diode, Inc. multiplier source, capable of providing CW radiation in the 620–700 GHz frequency band and a broadband Schottky diode detector (as shown in Fig.…”
Section: Designmentioning
confidence: 99%