jp8b11044_si_001.pdf (628.29 kB)
Download fileImproved Transport Properties and Novel Li Diffusion Dynamics in van der Waals C2N/Graphene Heterostructure as Anode Materials for Lithium-Ion Batteries: A First-Principles Investigation
journal contribution
posted on 2019-01-16, 00:00 authored by Yingchun Ding, Bing Xiao, Jiling Li, Qijiu Deng, Yunhua Xu, Haifeng Wang, Dewei RaoIn
this paper, we report a theoretical investigation of the electronic
structures, electron/phonon transport properties, and electrochemical
parameters of the C2N/graphene bilayer. The p-type C2N/graphene bilayer, with a direct band gap of 0.2 eV at Γ-point,
exhibits promising electric conductivity similar to that of the graphene
monolayer. In addition, it also shows excellent lattice thermal conductivity
of 1791.1 W/m·K, compared to 82.22 W/m·K of the C2N monolayer. The theoretical capacity of C2N/graphene
in Li-ion batteries is found to be 490.0 mA h/g. For Li diffusion,
the energy barriers for the energetically favorable diffusion pathways
are found to be in the range of 0.2–0.5 eV for both C2N monolayer and C2N/graphene bilayer. The planar diffusion
coefficients of the Li atom on C2N and C2N/graphene
materials are predicted to be 2.97 × 10–11 and
4.74 × 10–11 m2/s at 300 K, respectively,
comparable with that of the graphene monolayer. With the help of first-principles
molecular dynamics (FPMD) simulations at low temperature, it has been
revealed that the Li atoms either absorbed or intercalated in the
C2N/graphene heterostructure, which could migrate easily
in the vertical direction through the large hole of the C2N atomic layer, and these ascended Li atoms together with absorbed
Li atoms on the upper surface of the C2N monolayer are
able to hop further away from the substrate, giving the strongly absorbed
inner Li layer and weakly attached outer Li layer on the top of the
C2N atomic layer. The outer Li atoms are mainly responsible
for the ionic diffusion at room temperature. The hopping process between
the nearest adsorption sites, which is obtained from routine nudge
elastic band calculations, is only seen in FPMD simulations at high
temperatures (>800 K).