2011
DOI: 10.1021/jp203672u
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Native Defect Concentrations in NaAlH4 and Na3AlH6

Abstract: Titanium-doped sodium alanate has been shown to have potentially useful properties for storing hydrogen in fuel cell vehicles. To quantitatively explain the kinetic rates and activation energies for hydrogen release and absorption, it is necessary to calculate the rate of metal diffusion that is required for forming the dehydrogenation products, Na3AlH6 and Al. The bulk defects existing in large concentrations will likely play a dominant role in the transport of metal species. In the first of a series of paper… Show more

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Cited by 26 publications
(44 citation statements)
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“…The method proceeds as follows (Figure S10): (i) Identify all possible insertion sites in the original CuS structure using an in-house code. [56][57][58] CuS adopts a hexagonal covellite structure with unoccupied inlayer (A) and interlayer (B) as shown in Figure S10a. A supercell containing all symmetrically distinct configurations with Enum [59][60][61] for a series of compositions Li x ◻ 2-x CuS (0 < x < 2, ◻ denoting vacancy).…”
Section: Methodsmentioning
confidence: 99%
“…The method proceeds as follows (Figure S10): (i) Identify all possible insertion sites in the original CuS structure using an in-house code. [56][57][58] CuS adopts a hexagonal covellite structure with unoccupied inlayer (A) and interlayer (B) as shown in Figure S10a. A supercell containing all symmetrically distinct configurations with Enum [59][60][61] for a series of compositions Li x ◻ 2-x CuS (0 < x < 2, ◻ denoting vacancy).…”
Section: Methodsmentioning
confidence: 99%
“…Computational studies based on NEB methods have significantly added to understanding of the static energy landscape of ion migration pathways in electrode and SE materials. 16,[23][24][25][26][27][28] In addition, the diffusion pathway and energy barriers obtained from NEB calculations can be used as input for kinetic Monte Carlo calculations to obtain the overall diffusivity, conductivity, and activation energy in ion-conducting materials with non-dilute carrier concentrations. [29][30][31][32] However, for many SICs, such as LGPS and LLZO, with highly disordered Li-ion sublattices, NEB calculations require a priori guesses of ion-hopping sites and pathways and so are often more complicated and involved to perform.…”
Section: Ab Initio Molecular Dynamics Simulationmentioning
confidence: 99%
“…Na 3 AlH 6 has eleven inequivalent jumps attributed to the two symmetry‐inequivalent Na‐sites, Na1 (2 b ) and Na2 (4 e ), and the different orientation of [AlH 6 ] − unit . Michel and Ozolins revealed that the formation energy of the Na‐vacancy, V ′ Na , in Na1 site of Na 3 AlH 6 is lower than that in NaAlH 4 They also revealed that the Na‐vacancy diffusion coefficient in Na 3 AlH 6 is larger than that in NaAlH 4 in the temperature range from 250–400 K (The former and the latter have 1.19 × 10 −12 and 4.96 × 10 −11 m 2 s −1 , respectively, at 400 K, evaluated by the kinetic Monte Carlo simulations) . These might result in the higher Na‐ionic conductivity in Na 3 AlH 6 than in NaAlH 4 .…”
Section: Fast Na‐ionic Conductor Developmentmentioning
confidence: 99%