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. 2019 Sep 25;11(1):81.
doi: 10.1007/s40820-019-0312-y.

Plate-to-Layer Bi2MoO6/MXene-Heterostructured Anode for Lithium-Ion Batteries

Affiliations

Plate-to-Layer Bi2MoO6/MXene-Heterostructured Anode for Lithium-Ion Batteries

Peng Zhang et al. Nanomicro Lett. .

Abstract

Bi2MoO6 is a potentially promising anode material for lithium-ion batteries (LIBs) on account of its high theoretical capacity coupled with low desertion potential. Due to low conductivity and large volume expansion/contraction during charge/discharge cycling of Bi2MoO6, effective modification is indispensable to address these issues. In this study, a plate-to-layer Bi2MoO6/Ti3C2Tx (MXene) heterostructure is proposed by electrostatic assembling positive-charged Bi2MoO6 nanoplates on negative-charged MXene nanosheets. MXene nanosheets in the heterostructure act as a highly conductive substrate to load and anchor the Bi2MoO6 nanoplates, so as to improve electronic conductivity and structural stability. When the mass ratio of MXene is optimized to 30%, the Bi2MoO6/MXene heterostructure exhibits high specific capacities of 692 mAh g-1 at 100 mA g-1 after 200 cycles and 545.1 mAh g-1 with 99.6% coulombic efficiency at 1 A g-1 after 1000 cycles. The results provide not only a high-performance lithium storage material, but also an effective strategy that could address the intrinsic issues of various transition metal oxides by anchoring them on MXene nanosheets to form heterostructures and use as anode materials for LIBs.

Keywords: Bi2MoO6; Electrostatic self-assembly; Heterostructure; Lithium-ion batteries; MXene.

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Figures

Fig. 1
Fig. 1
Schematic diagram for the simple electrostatic self-assembly of positive-charged Bi2MoO6 nanoplates on the negative-charged MXene nanosheets
Fig. 2
Fig. 2
SEM images of a MXene nanosheets, b Bi2MoO6 nanoplates, c, d Bi2MoO6/MXene-50%, e, f Bi2MoO6/MXene-30%, and g, h Bi2MoO6/MXene-10%
Fig. 3
Fig. 3
TEM images of a, b Bi2MoO6/MXene-50%, c, d Bi2MoO6/MXene-30%, and e, f Bi2MoO6/MXene-10%. g STEM and corresponding element (Bi, Mo, Ti, and C) mapping images of the Bi2MoO6/MXene-30%
Fig. 4
Fig. 4
Characterization of Bi2MoO6/MXene heterostructures: a, b XRD patterns, c Raman speatra of the Bi2MoO6/MXene heterostructures. High-resolution of d Bi 4f, e Mo 3d, f O 1s, and g Ti 2p XPS spectrum of Bi2MoO6/MXene-30%
Fig. 5
Fig. 5
Electrochemical performance of the Bi2MoO6/MXene electrodes: a CV curves of Bi2MoO6/MXene-30% for the first three cycles at 0.1 mV s−1. b Charge/discharge profiles of Bi2MoO6/MXene-30% at 100 mA g−1 at different cycles. c Cycling performance of Bi2MoO6/MXene-50%, Bi2MoO6/MXene-30%, Bi2MoO6/MXene-10%, and pristine Bi2MoO6 electrodes at 100 mA g−1 for 200 cycles. d Charge/discharge profiles of Bi2MoO6/MXene-30% at different current rates. e Comparison of rate capabilities of Bi2MoO6/MXene-30% at various current rates from 50 to 2000 mA g−1. f Long-term cycling performance of Bi2MoO6/MXene-30% in 1000 cycles at 1 A g−1
Fig. 6
Fig. 6
Electrochemical kinetic analysis of Li storage behavior of Bi2MoO6/MXene-30%. a GITT profiles (current pulse at 100 mA g−1 for 30 min followed by 1 h relaxation), b diffusion coefficients calculated from GITT profiles according to overpotential, c CV curves at various scan rates from 0.2 to 3 mV s−1 in the voltage range of 0.01–3 V (vs. Li+/Li), d log(i)–log(v) curves, e CV profile measured at 1 mV s−1 with shaded area displaying the pseudocapacitive contribution, and f normalized proportions of capacitive and diffusion-controlled contribution at various scan rates

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