2016
DOI: 10.1126/sciadv.1501518
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Room temperature detection of individual molecular physisorption using suspended bilayer graphene

Abstract: Researchers detect individual CO2 physisorption with suspended bilayer graphene based on induced Coulomb impurity scattering.

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Cited by 131 publications
(81 citation statements)
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“…The potential slowly decays outwards towards 0 within a 9 -10 nm distance from the adsorbate. Similar behaviour of the potential was reported for CO 2 molecule on graphene whose simulated potential reached a constant value of the thermal energy at about 2.7 nm distance from the molecule [9]. For comparison, we selected a Coulomb potential of the form   0.02 / V r e r  and simulates the corresponding projected potential, shown in Fig.…”
Section: Discussionmentioning
confidence: 56%
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“…The potential slowly decays outwards towards 0 within a 9 -10 nm distance from the adsorbate. Similar behaviour of the potential was reported for CO 2 molecule on graphene whose simulated potential reached a constant value of the thermal energy at about 2.7 nm distance from the molecule [9]. For comparison, we selected a Coulomb potential of the form   0.02 / V r e r  and simulates the corresponding projected potential, shown in Fig.…”
Section: Discussionmentioning
confidence: 56%
“…The corresponding simulated projected potential exhibits a faster decay when compared to the experimentally obtained projected potential. Thus, the realistic potential distribution associated with a complex charge density redistribution between the adsorbate and graphene [9] can only roughly be approximated by a 1/ r dependency [23] that corresponds to a free charge and disregards any shielding due to an electronic rearrangement within the graphene. The simulated projected Coulomb potential does not reach zero as the experimentally measured projected potential does.…”
Section: Discussionmentioning
confidence: 99%
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“…The blue and yellow lobes represent charge depletion and charge accumulation, respectively. As shown in Figure g,h, The charge transfer from ammonia to ZGO is more prominent, which explains why pZGO with a defective structure are more likely to interact with ammonia gas molecule than sZGO . The presence of abundant defects in the pZGO results in stronger electron density depletion by ammonia gas molecules, and more of the transferred charge is spread around the adsorption site in the pZGO (Figure g).…”
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confidence: 93%
“…1 The full exposure of graphene surface to environment, together with easy doping 2 and low electrical noise of this material, 3 paves the way for the fabrication of sensitive chemical sensors. For example, the detection of NO2 gas on ppq-level 4 or even single adsorbed molecules 3,5 has been demonstrated in high vacuum or in inert (Ar) gas atmosphere.…”
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confidence: 99%