2020
DOI: 10.1016/j.nanoen.2020.105360
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Oxygen vacancies-enriched sub-7 nm cross-linked Bi2.88Fe5O12- nanoparticles anchored MXene for electrochemical energy storage with high volumetric performances

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Cited by 29 publications
(13 citation statements)
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“…In addition, the CV curves of the MRC‐30 aerogel can still maintain the congruous shape with no distinct shape variation after 10 000, 50 000, and 100 000 cycles (inset of Figure 5J), also confirming the excellent cycling stability of the MRC‐30 aerogel. The cycling performance is greatly comparable with and even surpasses the previously announced MXene materials, such as Ti 3 C 2 film (20 000, 81.7%), [ 33 ] MXene (10 000, 90.0%), [ 42 ] MXene/BFO (10 000, 89.3%), [ 43 ] MXene hydrogel (10 000, 97.1%), [ 20 ] PPy/Ti 3 C 2 T x (25 000, 92.0%), [ 44 ] and MXene/BC‐5 (10 000, 96.5%). [ 45 ]…”
Section: Resultssupporting
confidence: 53%
“…In addition, the CV curves of the MRC‐30 aerogel can still maintain the congruous shape with no distinct shape variation after 10 000, 50 000, and 100 000 cycles (inset of Figure 5J), also confirming the excellent cycling stability of the MRC‐30 aerogel. The cycling performance is greatly comparable with and even surpasses the previously announced MXene materials, such as Ti 3 C 2 film (20 000, 81.7%), [ 33 ] MXene (10 000, 90.0%), [ 42 ] MXene/BFO (10 000, 89.3%), [ 43 ] MXene hydrogel (10 000, 97.1%), [ 20 ] PPy/Ti 3 C 2 T x (25 000, 92.0%), [ 44 ] and MXene/BC‐5 (10 000, 96.5%). [ 45 ]…”
Section: Resultssupporting
confidence: 53%
“…By increasing the current density from 0.1 to 4.0 A g −1 , no obvious plateaus are observed in these curves, indicating the excellent rate capability. The specific capacity is 627, 512, 433, 371, 309, and 244 mA h g −1 at current densities of 0.1, 0.2, 0.5, 1.0, 2.0, and 4.0 A g −1 , corresponding to volumetric specific capacity of 934, 763, 645, 553, 460, and 363 mA h cm −3 , respectively, superior to other results reported elsewhere (Table S1) [36][37][38][39][40][41][42][43][44][45]. Then, the rate performance of the VM POMs/MXenes is shown in Fig.…”
Section: Resultscontrasting
confidence: 50%
“…Ni 2p core-level XPS spectrum could be fitted with two pairs of Ni 2p 1/2 /2p 3/2 spin–orbit doublets at 875.9/858.0 and 872.7/854.9 eV, corresponding to the Ni 2p 1/2 /Ni 2p 3/2 of Ni 2+ and Ni 3+ (Figure C) . With regard to the Co 2p spectrum, it could also be deconvoluted into two spin–orbit doublets at 797.3/781.3 and 803.4/786.8 eV, attributed to the 2p 3/2 /2p 1/2 of Co 3+ and Co 2+ (Figure D). For the S 2p XPS spectrum (Figure E), it could be fitted with three peaks located at 161.2, 163.3, and 168.0 eV, which could be assigned to S 2p 3/2 , S 2p 1/2 , and SO due to sulfur oxidation in air. , High-resolution XPS spectrum of C 1s could be fitted by four peaks at 288.5, 286.0, 284.6, and 281.2 eV, , which belong to COO/C–F, C–O, C–C, and C–Ti bonds, respectively (Figure S10). High-resolution Ti 2p (Figure F) could be fitted with three spin–orbit doublets such as Ti–C (461.6 and 455.5 eV), Ti 2+ (463.8 and 457.7 eV), and TiO 2 (465.6 and 460.5 eV) .…”
Section: Results and Discussionmentioning
confidence: 98%
“…41−44 For the S 2p XPS spectrum (Figure 3E), it could be fitted with three peaks located at 161.2, 163.3, and 168.0 eV, 45 which could be assigned to S 2p 3/2 , S 2p 1/2 , and SO due to sulfur oxidation in air. 41,46 High-resolution XPS spectrum of C 1s could be fitted by four peaks at 288.5, 286.0, 284.6, and 281.2 eV, 47,48 which belong to COO/C−F, C−O, C−C, and C−Ti bonds, respectively (Figure S10). High-resolution Ti 2p (Figure 3F) could be fitted with three spin−orbit doublets such as Ti−C (461.6 and 455.5 eV), Ti 2+ (463.8 and 457.7 eV), and TiO 2 (465.6 and 460.5 eV).…”
Section: Resultsmentioning
confidence: 99%