2017
DOI: 10.1016/j.matchemphys.2017.03.045
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Microwave assisted facile synthesis of reduced graphene oxide-silver (RGO-Ag) nanocomposite and their application as active SERS substrate

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Cited by 46 publications
(6 citation statements)
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“…This unique absorption pattern is attributed to the strong interaction between the irregular Ag NPs and incident light. [ 38 ] Besides, AFM image in Figure 5b indicates that the average topographic height of the prepared carbon nanostructure was 50 ± 0.5 nm, which is also confirmed by the cross‐section SEM image (Figure S2). And combining with the surface profile of SEM image (Figure 3b(ii)), it can be seen that Ag NPs (average size of 240 nm, Figure S3) were embedded within the nanopores, which is isolated by the carbon walls.…”
Section: Resultssupporting
confidence: 58%
“…This unique absorption pattern is attributed to the strong interaction between the irregular Ag NPs and incident light. [ 38 ] Besides, AFM image in Figure 5b indicates that the average topographic height of the prepared carbon nanostructure was 50 ± 0.5 nm, which is also confirmed by the cross‐section SEM image (Figure S2). And combining with the surface profile of SEM image (Figure 3b(ii)), it can be seen that Ag NPs (average size of 240 nm, Figure S3) were embedded within the nanopores, which is isolated by the carbon walls.…”
Section: Resultssupporting
confidence: 58%
“…Smaller peak was detected at 796-650 cm −1 , which belong to Ag-halide stretching, proving the formation of rGO@Ag x% nanoparticles [32]. These results may be due to the interaction between the functional groups which containing oxygen in rGO NPs with Ag NPs [39].…”
Section: Characterizationmentioning
confidence: 79%
“…Optical absorption performance of β‐Sn/RGO has been characterized along with two reference samples, inferring pure β‐Sn and pure RGO, and the results are shown in Figure . Clearly, for pure RGO, there is only one broad absorption peak at around 261 nm, which belongs to the π–π* transition of RGO . As for pure β‐Sn, an absorption peak at around 217 nm can be seen (to be clear, the position has been pointed out by an arrow in the inset of Figure ), which is due to the excitation of surface plasmons in the NPs, and the surface charge distribution of β‐Sn shown in Figure S2 (Supporting Information) indicates that the absorption can be assigned to the dipole resonance of β‐Sn.…”
Section: Resultsmentioning
confidence: 95%
“…On one hand, after contacting, hot electrons will transfer from β‐Sn NPs to RGO nanosheets because of the difference of work functions between β‐Sn (4.42 eV) and RGO (4.8 eV) . Such electron transition could promote charge transfer from R6G dye molecules to β‐Sn NPs, and eventually will intensify electron transfer to RGO, indicating the realization of chemical enhancement of SERS in β‐Sn/RGO . On the other hand, the existence of RGO could lead to stronger local electric field confinement, which will promote the enhancement of the Raman signals from R6G dye molecules as well…”
Section: Resultsmentioning
confidence: 99%