They could be attributed to the presence of epoxy, hydroxyl, and carbonyl groups, respectively [36]. From Figure 3b,c,d, with increasing the cycle number of microwave irradiation, the peak intensity of C1s which related to oxygenated functional groups (C-O-H and C-O-C) showed a significant decrease, confirming that most of the epoxide, hydroxyl, and carbonyl functional groups were removed and the degree of reduction

Bioactive Compound Library research buy of could be enhanced. It was noted that two new characteristic peaks of C-N and O-C = O were observed, and the intensity of C-N and O-C = O could be enhanced with increasing the cycle number of microwave irradiation. This could be reasonably attributed to the increase of arginine capped on the surface of Ag/rGO nanocomposites. Figure 3 The C 1s XPS spectra of (a) GO and SN-38 purchase Ag/rGO nanocomposites (b) 1C, (c) 4C, and (d) 8C. Figure 4 shows the XPS signature of the Ag 3d doublet (3d5/2 and 3d3/2) for the Ag EGFR inhibitor nanoparticles deposited on rGO. The Ag 3d5/2 and 3d3/2 peaks of Ag/rGO nanocomposites 1C appeared at 368 and 374 eV, respectively, which shifted to the lower binding energy compared with the characteristic peaks for

silver metal at 368.2 and 374.2 eV. In addition, the Ag 3d5/2 binding energies have values of 368.2, 367.4, and 367.8 eV for Ag, Ag2O, and AgO (with average oxidation states of 0, +1, and +2, respectively) [40]. As a result, slight oxidation on the surface of Ag nanoparticles might be the reason for the negative shift of Ag 3d3/2 and Ag 3d5/2 binding energy. Moreover, from Figure 4, the binding energy of 3d3/2 and Ag 3d5/2 increased with increasing the cycle

number of microwave Amine dehydrogenase irradiation. The results were due to the electron transfer from metallic Ag to the graphene sheets owing to the smaller work function of Ag (4.2 eV) than graphene (4.48 eV) and also proved that the content of Ag nanoparticles could be controlled via adjusting the cycle number of microwave irradiation. Figure 4 The Ag 3d XPS spectra of Ag/rGO nanocomposites (a) 1C, (b) 4C, and (c) 8C. Figure 5a shows the typical SERS spectra of 10−4 M 4-ATP acquired from rGO and Ag/rGO nanocomposites 1C, 4C, and 8C. For rGO, only two prominent peaks corresponding to the G and D bands were observed clearly and no evident Raman peaks of 4-ATP could be found. However, for Ag/rGO nanocomposites, the characteristic peaks of 4-ATP were observed clearly. This demonstrated that the Ag/rGO nanocomposites possessed significant SERS property. Their SERS intensities at 1,140 cm−1 were indicated in Figure 5b. It was obvious that the peak intensity increased significantly with increasing the cycle number of microwave irradiation. It is known that increasing the number density of Ag nanoparticles on the surface of graphene sheets as hot spots for strong localized EM fields produced by the gap between neighboring Ag nanoparticles [24].