2016
DOI: 10.1038/ncomms10699
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Selectively enhanced photocurrent generation in twisted bilayer graphene with van Hove singularity

Abstract: Graphene with ultra-high carrier mobility and ultra-short photoresponse time has shown remarkable potential in ultrafast photodetection. However, the broad and weak optical absorption (∼2.3%) of monolayer graphene hinders its practical application in photodetectors with high responsivity and selectivity. Here we demonstrate that twisted bilayer graphene, a stack of two graphene monolayers with an interlayer twist angle, exhibits a strong light–matter interaction and selectively enhanced photocurrent generation… Show more

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Cited by 169 publications
(182 citation statements)
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“…However, the absence of a bandgap has impeded the applications of graphene in nanoelectroncis. To overcome the disadvantages caused by the gapless band in graphene, intensive efforts have been strived, such as chemical doping, topography control, etc 19, 20, 21. Unfortunately, only very limited success has been achieved 20, 22, 23, 24.…”
Section: Introductionmentioning
confidence: 99%
“…However, the absence of a bandgap has impeded the applications of graphene in nanoelectroncis. To overcome the disadvantages caused by the gapless band in graphene, intensive efforts have been strived, such as chemical doping, topography control, etc 19, 20, 21. Unfortunately, only very limited success has been achieved 20, 22, 23, 24.…”
Section: Introductionmentioning
confidence: 99%
“…Bilayer graphene (BLG) as a gapless semiconductor is similar to the monolayer and has widespread potential applications in various fields [24]. However, the BLG has drawn special attention mainly due to the controlled band gap and the magnetic properties from twisting, lattice vacancies and doping/inserting N, B and metal atoms [25][26][27][28][29][30]. BLG was expected to be a good candidate of anode material for LIB, and the Li ions in BLG were surrounded by two exterior graphene layers [31][32][33].…”
mentioning
confidence: 99%
“…For the latter, it introduces a stackingmisorientation structure, that is, twisted graphene, forming Moiré superlattices [142]. In both cases, the electronic properties of the graphene layers can be modified dramatically and depend sensitively on the stacking orders [46,[143][144][145]. In this section, we present the characteristic features of the stacking-dependent LL spectrum in graphene bilayers and trilayers.…”
Section: Stacking-dependent Ll Spectrum For Multilayer Graphenementioning
confidence: 99%