2022
DOI: 10.1016/j.jmst.2021.05.035
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Binary doping of nitrogen and phosphorus into porous carbon: A novel di-functional material for enhancing CO2 capture and super-capacitance

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Cited by 75 publications
(35 citation statements)
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“…[56]. As shown in Figure 5c, the deconvoluted N 1s spectrum for unactivated GO(0.25)/MR results in two peaks at 399.5 and 401.5 eV, which can be attributed to amino/imino nitrogen and quaternary nitrogen, respectively [57,58]. After activation at 400−600 • C, the peak of amino/imino-N disappeared and three new peaks at 398.7, 400.1 and 403.2 eV appeared, attributable to pyridinic-N, pyrrolic-N and oxidized-N, respectively [59,60].…”
Section: Resultsmentioning
confidence: 90%
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“…[56]. As shown in Figure 5c, the deconvoluted N 1s spectrum for unactivated GO(0.25)/MR results in two peaks at 399.5 and 401.5 eV, which can be attributed to amino/imino nitrogen and quaternary nitrogen, respectively [57,58]. After activation at 400−600 • C, the peak of amino/imino-N disappeared and three new peaks at 398.7, 400.1 and 403.2 eV appeared, attributable to pyridinic-N, pyrrolic-N and oxidized-N, respectively [59,60].…”
Section: Resultsmentioning
confidence: 90%
“…The deconvolution of O 1s spectra for activated samples at 400-700 °C results five different peaks with BEs at 530.8, 532.1, 533.3, 534.3 and 536.1 eV, corresponding to C=O, O=C−N, C−O, O=C-O and adsorbed water, respectively [56]. As shown in Figure 5c, the deconvoluted N 1s spectrum for unactivated GO(0.25)/MR results in two peaks at 399.5 and 401.5 eV, which can be attributed to amino/imino nitrogen and quaternary nitrogen, respectively [57,58]. After activation at 400−600 °C, the peak of amino/imino-N disappeared and three new peaks at 398.7, 400.1 and 403.2 eV appeared, attributable to pyridinic-N, pyrrolic-N and oxidized-N, respectively [59,60].…”
Section: Resultsmentioning
confidence: 94%
“…It is evident and undeniable that each material has its own individual limitations hindering their large-scale deployment, i.e., (i) MOFs show outstanding features including easily tunable and tailored structures, well-defined pore properties, and high recyclability [20]; however, they are high-cost materials in terms of production, making them economically unviable, and also their stability is compromised in the presence of moisture [21]. (ii) Porous carbon materials, and in particular, their heteroatom-doped counterparts, have emerged as promising CO 2 uptake candidates [22,23]. The heteroatom improves the electronegativity of the material enhancing the CO 2 capture; however, there is an important discrepancy about the CO 2 binding mechanisms, as it is yet controversial whether the micropore distribution and not the heteroatom doping that determines the CO 2 capture and CO 2 /N 2 selectivity [24].…”
Section: Introductionmentioning
confidence: 99%
“…With an increase in hydrothermal reaction temperature ( Figure 2 a) and time ( Figure S1a ), some peaks within 1000–1500 cm −1 were more difficult to distinguish. The main characteristic FTIR bands were observed to include −OH, P=O, C−O, C−C, and C−N groups [ 9 , 25 , 26 ]. The stretching vibration of O−H in the hydroxyl groups and carboxyl groups leads to the appearance of peaks at 3454 cm −1 and 1641 cm −1 , respectively [ 27 ].…”
Section: Resultsmentioning
confidence: 99%