2021
DOI: 10.1016/j.ensm.2020.08.021
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Diamine molecules double lock-link structured graphene oxide sheets for high-performance sodium ions storage

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Cited by 51 publications
(27 citation statements)
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“…31 For example, 2D Mxene NSs show a facilitated directional ion transport; 32 graphene oxide sheets can achieve high-performance ions storage. 33 LTO NSs can be the perfect anode materials for being applied in high-power LIBs. 34 However, combining 2D NSs morphology with defect engineering of LTO has rarely been reported.…”
Section: Introductionmentioning
confidence: 99%
“…31 For example, 2D Mxene NSs show a facilitated directional ion transport; 32 graphene oxide sheets can achieve high-performance ions storage. 33 LTO NSs can be the perfect anode materials for being applied in high-power LIBs. 34 However, combining 2D NSs morphology with defect engineering of LTO has rarely been reported.…”
Section: Introductionmentioning
confidence: 99%
“…Fourier transform infrared (FTIR) spectra are exhibited in Figure b; the strong absorption peaks at 1441 and 3293 cm –1 corresponding to C–N and N–H bonds of Ti 3 C 2 -NH 2 and CC bonds at 1183 cm –1 are attributed to MA molecules. It is worth noting that the adsorption peak at 1625 cm –1 is CO in HN–CO bonds, , which further proves that MA molecules are linked with Ti 3 C 2 layers to form MA-Ti 3 C 2 . The X-ray photoelectron spectra (XPS) of MA-Ti 3 C 2 displays a new N 1s peak compared with pure Ti 3 C 2 , suggesting that N elements are introduced by chemical welding Ti 3 C 2 and MA molecules (Figure S1).…”
Section: Resultsmentioning
confidence: 99%
“…According to eq , the Li + diffusion coefficient ( D Li+ ) is inversely proportional to σ, in which the σ values of MA-Ti 3 C 2 and Ti 3 C 2 are 518.7 and 689.9, respectively (Figure b), illustrating that the approach of regulating interlayer spacing is significant to fast Li + diffusion. As shown in Figure c, the GITT test process can be divided into three stages: pulse, constant current, and relaxation, in which the diffusion coefficient ( D Li+ ) can be deduced directly from the following equation where L is the thickness of electrode sheets, τ is the relaxation time, and Δ E s and Δ E τ represent the total change of the voltage during current pulse and the change in steady-state voltage during the step at the plateau potentials, respectively. Specifically, the D Li+ values of MA-Ti 3 C 2 and Ti 3 C 2 are 1.4 × 10 –8 –5.8 × 10 –7 and 2.1 × 10 –9 –2.2 × 10 –7 cm 2 s –1 (Figure d), respectively, declaring that MA-Ti 3 C 2 with self-adaption layered structure can offer fast Li + transport pathways for facilitating Li + diffusion dynamics.…”
Section: Resultsmentioning
confidence: 99%
“…In addition, the Li + diffusion resistance of PPDA‐Nb 2 CT x and Nb 2 CT x can be quantificationally evaluated by Li + diffusion coefficients, which is achieved from GITT measurements (Figure 5e and S5). According to Equation S4, the Li + diffusion coefficients of PPDA‐Nb 2 CT x and Nb 2 CT x at different potentials can be obtained (the positive sign only represents charge process and negative sign represents discharge process) [44] . In Figure 5f, the Li + diffusion coefficient (1.5×10 −9 ∼4.6×10 −7 cm 2 s −1 ) of PPDA‐Nb 2 CT x is higher than that of Nb 2 CT x (1.2×10 −9 ∼2.6×10 −7 cm 2 s −1 ), indicating the intercalation of PPDA molecules can not only offer a large specific surface area to improve Li + storage performance, but also expand interlayer spacing to accelerate Li + diffusion rate.…”
Section: Resultsmentioning
confidence: 99%