Crystal Structures, Phase
Stabilities, and Hydrogen
Storage Properties of Metal Amidoboranes
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Abstract
Metal amidoboranes, M(NH<sub>2</sub>BH<sub>3</sub>)<sub><i>n</i></sub> (M = alkali metal or alkaline-earth metal),
are
candidates for on-board hydrogen storage materials with high gravimetric
capacity, low H<sub>2</sub> release temperature, and the ability to
suppress toxic borazine emission. We have used a first-principles
density functional theory (DFT) combination with Monte Carlo method
to search for crystal structures for a wide array of metal amidoboranes
(M = Li, Na, K, Be, Mg, Ca, Sr, and Sc). In cases where the experimental
structures are known, the DFT energies of the theoretically predicted
LiNH<sub>2</sub>BH<sub>3</sub>, NaNH<sub>2</sub>BH<sub>3</sub>, KNH<sub>2</sub>BH<sub>3</sub>, and Ca(NH<sub>2</sub>BH<sub>3</sub>)<sub>2</sub> structures are degenerate with the DFT energies computed for the
experimental structures [to within 4 kJ/(mol f.u.)], confirming the
accuracy of our approach. On the basis of the decomposition reaction
pathway, M(NH<sub>2</sub>BH<sub>3</sub>)<sub><i>n</i></sub> → MH<sub><i>n</i></sub> + <i>n</i>BN
+ 2<i>n</i>H<sub>2</sub>, we compute the H<sub>2</sub> release
reaction enthalpies and show that the stability of metal amidoboranes
obeys the following trend: The metal amidoborane becomes more stable
(the decomposition reaction becomes less exothermic) as the metal
cation becomes more electropositive, that is, as the metal cation
goes down in the periodic table along a given column or as the metal
moves to the left along a given row. The only exception to this rule
is Mg(NH<sub>2</sub>BH<sub>3</sub>)<sub>2</sub>, which is more stable
than Ca(NH<sub>2</sub>BH<sub>3</sub>)<sub>2</sub>. Introducing vibrational
entropy effects does not change this exceptional behavior of Mg amidoborane:
the phonon contribution serves to shift all reaction enthalpies down
by a roughly constant amount, ∼22 kJ/(mol H<sub>2</sub>) at <i>T</i> = 300 K