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XPS spectra of N-doped graphene and schematic illustration of nitrogen functional groups. XPS spectra of N-doped graphene converted from GO with different oxygenic groups (a-e). Schematic illustration of nitrogen functional groups in the carbon lattice (f).

XPS spectra of N-doped graphene and schematic illustration of nitrogen functional groups. XPS spectra of N-doped graphene converted from GO with different oxygenic groups (a-e). Schematic illustration of nitrogen functional groups in the carbon lattice (f).

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Few-layer nitrogen doped graphene was synthesized originating from graphene oxide functionalized by selective oxygenic functional groups (hydroxyl, carbonyl, carboxyl etc.) under hydrothermal conditions, respectively. Transmission electron microscopy (TEM) and atomic force microscopy (AFM) observation evidenced few-layer feature of the graphene oxi...

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... However, controlling and analyzing the nitrogen doping process in GO, which involves the reduction of oxygen-bound and vacancy defect sites, poses more challenges due to its defective and poorly ordered structures [30,31]. Additionally, numerous experimental and theoretical studies have explored the bonding natures and evolution of nitrogen-doped sites on pure graphene [32][33][34][35]. Recent research has highlighted that defects in the conjugated graphene network significantly influence the N-doping mechanism and, consequently, the doping efficiency of the material [36][37][38][39]. ...
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Nitrogen-doped graphene has been increasingly utilized in a variety of energy-related applications, serving as a catalyst or support material for fuel cells, and as an anode material for lithium-ion batteries, among others. The thermal reduction of graphene oxide (GO) in nitrogenous sources to incorporate nitrogen, producing nitrogen-doped reduced graphene oxide (NRGO), is the most favored method. Controlling atomic configurations of nitrogen-doped sites is the key factor for tailoring the physico-chemical properties of NRGO, but major challenges remain in identifying detailed atomic arrangements at nitrogen binding sites on highly defective and chemically functionalized GO surfaces. In this paper, we present atomistic-scale modeling of the nitrogen doping process of GO with different types of vacancy defects. Molecular dynamics simulations using a reactive force field indicate that the edge carbon atoms on defect sites are the dominant initiation location for nitrogen doping. Further, first-principles calculations using density functional theory present energetically favorable chemical transition pathways for nitrogen doping. The significance of this work lies in providing important chemical insights for the effective control of the desired properties of NRGO by suggesting a detailed mechanism of the nitrogen doping process of GO.
... Fig. 2bshows the components with C 1 s binding energy: a main peak of C--C, of sp 2 graphitic domains, C-N/ C-O and C--N/C--O, of single and double bonds with heteroatoms, respectively, and O--C-O, of residual carboxyl groups[38,39]. The positions and proportions (at%) of each carbon chemical environment are presented in the table inserted inFig. ...
... Here it is shown that NGO consists of different C-N bond types, including pyridinic, pyrrolic-N and graphitic-N and these bond types have profound effects on the NGO properties and applications. The N level and N species could be controlled by tuning the experimental parameters such as mass ratio between dopant and GO source, reaction time and hydrothermal temperature [76,77]. In addition, the N content and N types with different amount can depend greatly on the amount and type of oxygen functionalities present on the GO surface. ...
... In addition, the N content and N types with different amount can depend greatly on the amount and type of oxygen functionalities present on the GO surface. For example, GO modified with more carboxyl groups (GO-OOH) had high N content compared to GO modified with −OH and −C=O functionalities under similar conditions due to the reduction in epoxy groups as the carboxyl groups introduced increases (Fig. 7) [76]. Therefore, an increase in the carboxyl groups enhances the surface activity of GO. ...
... This presumption was made due to the absence of N observed in the elemental analysis when GO was annealed with urea at 700 °C. Additionally, Mou et al. [77] and Chen et al. [76], stated that carboxyl Review groups which provide active sites on the GO are the main oxygen functionalities responsible for the reaction with N atoms. Chen et al. also added that at high-temperature and alkaline conditions the carbonyl groups are transformed into carboxyl groups, which reacted with NH 3 and favoured N-doping. ...
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... 42 The overlap may be due to the fact that there is sufficient carbonyl in FGO, which favors the electron attraction, resulting in a low number of charges on the C�C atom. 42,43 Overall, the FTIR data clearly show the successful preparation of FGO. Quantitative analysis of FGO3, FGO10, and FGO20 was carried out by XPS. ...
... This is because the amount of carboxylate moieties converted from the C6 primary hydroxyls of cellulose increases in accordance with the amount of TEMPO involved in the reaction. This observation complies with the characteristic absorption spectra obtained by Shao et al. [23]. ...
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... The oxidized functional group ratios of hydroxyl, carboxyl, and epoxy groups are 1.05:0.9:1.0 ∼ 1.0:1.2:0.96, which is comparable to the experimental value of 1.05:0.9:1.0 ∼ 1.0:1.2:0.96 [29,30]. The nanoscale and rectangle-shaped GQDs are studied in terms of current computation ability, as in previous simulation studies [6,7,14]. ...
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... Carbon materials with pyridinic N prepared without metal substrates have been reported [46,47], but the actual percentages of pyridinic N in the structures are uncertain due to the wide full width at half maximum (FWHM) of N1s X-ray photoelectron spectroscopy (XPS) spectra and the insufficient structural analysis (Fig. 1b). By top-down methods, carbon materials synthesized from N-containing hydrocarbon precursors other than ones with pyridinic N have also been reported, but the percentages of pyridinic N in these materials are as low as 73% [48], 70% [49], 60-70% [50], and 45% [51]. We have also attempted to introduce pyridinic N and other N-containing functional groups without using catalysts [52][53][54][55]. ...
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... 70,71 The O 1s peak ( Figure 4E,H,K) after deposition of copper featured two supplementary species, which were a cupric oxide (CuO) at 529.7 eV and a cuprous oxide (Cu 2 O) at 530.3 eV. Figure 4C shows the deconvolution of the N 1s peak into four nitrogencontaining species: a pyridinic (N-6) at 398.80 eV, a pyrrolic (N-5) at 399.8 eV, a quaternary/graphitic (N-Q) at 401.8 eV, and an oxidic (N-Ox) at 404.2 eV. 48,66,72,73 Figure 4F,I,L shows Cu 2p peaks, which were fit into the five species: a copper, a cuprous oxide, a cupric oxide, a copper hydroxide (CuOOH), and a copper sulfate (CuSO 4 ). 32,74,75 The contribution from copper sulfate after annealing was negligible and was therefore omitted in the further analysis. ...
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... In the N 1s XPS spectrum ( Figure S4b, Supporting Information), the three deconvoluted peaks located at 400.1, 403.4, and 406.9 eV can be assigned to pyridine N, pyrrolic N, and sorbed N. [33] It is also notable that the presence of pyridine type N atoms can increase the electron conduction, thus favoring the rate performance of the electrode. [34] From the above discussion, the enhanced-compressively strained interface in N-Pd/A-Co(II) was successfully constructed. ...
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The development of palladium‐based catalysts for alkaline hydrogen evolution reaction (HER) is highly desired for renewable hydrogen energy systems, yet still challenging due to the strong palladium–hydrogen bond. Herein, the bottleneck is largely overcome by constructing a nitridation‐induced compressively strained‐interface N‐doped palladium/amorphous cobalt (II) interface (N‐Pd/A‐Co(II)), which dramatically boosts HER performance in alkaline condition. The optimized catalyst with the compressive strain of 2.7% exhibits the higher activity with an overpotential of only 58 mV to achieve the current density of 10 mA cm⁻², much better than those of pure Pd (327 mV), and the state‐of‐art Pt/C (78 mV). Notably, it also shows excellent stability with negligible decline during a 30 h stability test. Detailed analyses reveal that the strong absorption of Hads on Pd can be efficiently reduced via the compressively strained N‐doped Pd. And the amorphous Co(II) component accelerates the water dissociation. Consequently, the cooperative effect between the compressed N‐doped Pd and amorphous Co(II) creates the impressive HER performance in alkaline condition, highlighting the importance of the functional interface to develop efficient electrocatalysts for HER and beyond.