2022
DOI: 10.1039/d2cp00480a
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Improvement of the hydrogen storage performance of t-graphene-like two-dimensional boron nitride upon selected lithium decoration

Abstract: Lithium decoration enhances the hydrogen storage capacities, reversibility and diffusion kinetics of t-boron nitride monolayer.

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Cited by 23 publications
(17 citation statements)
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References 66 publications
(96 reference statements)
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“…Hydrogen molecules binding capability on the h-BN/Gr is tested first by calculating the binding energy of H 2 molecules using the following equation ,,, E normalB normalE = E normalT normalo normalt normala normall ( E h B N / G r + n E H 2 ) A single hydrogen molecule prefers a parallel orientation at the hexagonal site of the BN-ring with a binding energy of −1.37(−1.48) eV calculated by employing the DFT-D2(D3) Grimme’s dispersion method. Grimme’s semi-empirical D2 and D3 dispersion correction are proven to be better choice for weakly interacting hydrogen-bonded systems. , The single hydrogen molecule binding energy on h-BN/Gr is higher in comparison to many available results in the literature and also compared to its pristine counterparts. ,,,, We further tested the binding energy of a single hydrogen molecule on two more bilayer structures with AA type (where hexagon of graphene is symmetric with hexagon of boron nitride) and AB-Boron type (where boron atom is at the center of graphene hexagon) [refer to Figure S8 in Supporting Information] stacking orientation of h-BN/Gr.…”
Section: Resultsmentioning
confidence: 99%
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“…Hydrogen molecules binding capability on the h-BN/Gr is tested first by calculating the binding energy of H 2 molecules using the following equation ,,, E normalB normalE = E normalT normalo normalt normala normall ( E h B N / G r + n E H 2 ) A single hydrogen molecule prefers a parallel orientation at the hexagonal site of the BN-ring with a binding energy of −1.37(−1.48) eV calculated by employing the DFT-D2(D3) Grimme’s dispersion method. Grimme’s semi-empirical D2 and D3 dispersion correction are proven to be better choice for weakly interacting hydrogen-bonded systems. , The single hydrogen molecule binding energy on h-BN/Gr is higher in comparison to many available results in the literature and also compared to its pristine counterparts. ,,,, We further tested the binding energy of a single hydrogen molecule on two more bilayer structures with AA type (where hexagon of graphene is symmetric with hexagon of boron nitride) and AB-Boron type (where boron atom is at the center of graphene hexagon) [refer to Figure S8 in Supporting Information] stacking orientation of h-BN/Gr.…”
Section: Resultsmentioning
confidence: 99%
“…The average adsorption energy [ E ads (eV/H 2 )] are computed using the following equation: ,,, E normala normald normals = E normalT normalo normalt normala normall ( E h B N / G r + n E H 2 ) n where E Total is the total energy of the complex (h-BN/Gr+H2), E h–BN/Gr is the total energy of the h-BN/Gr heterostructure, n is the number of H 2 molecules, and E H 2 refer to the total energy of H 2 molecule. The hydrogen molecules are gradually increased on the hexagonal site of the cavity up to the maximum available adsorption sites, keeping in mind the average adsorption energy lying in the desirable range of −0.15 – −0.60 eV/H 2 . ,, In the case of 4H 2 molecules, adsorption energy per H 2 is −0.47 eV. Similarly, when the hydrogen molecules are increased to 8H 2 , the adsorption energy per H 2 reduces to 0.39 eV.…”
Section: Resultsmentioning
confidence: 99%
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