6 research outputs found
Model for the Formation Energies of Alanates and Boranates
We develop a simple model for the formation energies (FEs) of alkali and alkaline earth alanates and boranates,
based upon ionic bonding between metal cations and AlH4- or BH4- anions. The FEs agree well with values
obtained from first principles calculations and with experimental FEs. The model shows that details of the
crystal structure are relatively unimportant. The small size of the BH4- anion causes a strong bonding in the
crystal, which makes boranates more stable than alanates. Smaller alkali or alkaline earth cations do not give
an increased FE. They involve a larger ionization potential that compensates for the increased crystal bonding
Core-Level Binding Energies from <i>GW</i>: An Efficient Full-Frequency Approach within a Localized Basis
The GW method is routinely used to predict charged
valence excitations in molecules and solids. However, the numerical
techniques employed in the most efficient GW algorithms
break down when computing core excitations as measured by X-ray photoelectron
spectroscopy (XPS). We present a full-frequency approach on the real
axis using a localized basis to enable the treatment of core levels
in GW. Our scheme is based on the contour deformation
technique and allows for a precise and efficient calculation of the
self-energy, which has a complicated pole structure for core states.
The accuracy of our method is validated by comparing to a fully analytic GW algorithm. Furthermore, we report the obtained core-level
binding energies and their deviations from experiment for a set of
small molecules and large polycyclic hydrocarbons. The core-level
excitations computed with our GW approach deviate
by less than 0.5 eV from the experimental reference. For comparison,
we also report core-level binding energies calculated by density functional
theory (DFT)-based approaches such as the popular delta self-consistent
field (ΔSCF) method. Our implementation is optimized for massively
parallel execution, enabling the computation of systems up to 100
atoms
A Density Functional Study of α-Mg(BH<sub>4</sub>)<sub>2</sub>
Boranates (tetrahydroborates) are studied intensively because of their potential use as hydrogen storage materials. In this Article, we present a first-principles study of α-Mg(BH4)2 at the level of density functional theory. We optimize the complex structure of α-Mg(BH4)2, starting from the experimental crystal structures with 30 formula units per unit cell. From total energy calculations, incorporating vibrational contributions at finite temperature, we show that the hydrogen desorption reaction α-Mg(BH4)2 → MgB2 + 4H2 has a reaction enthalpy of 38 kJ/mol H2 at room temperature. This makes Mg(BH4)2 an interesting candidate as a hydrogen storage material
Thermodynamic Stability of Boron: The Role of Defects and Zero Point Motion
Its low weight, high melting point, and large degree of hardness make elemental boron a
technologically interesting material. The large number of allotropes, mostly containing over a hundred atoms
in the unit cell, and their difficult characterization challenge both experimentalists and theoreticians. Even
the ground state of this element is still under discussion. For over 30 years, scientists have attempted to
determine the relative stability of α- and β-rhombohedral boron. We use density functional calculations in
the generalized gradient approximation to study a broad range of possible β-rhombohedral structures
containing interstitial atoms and partially occupied sites within a 105 atoms framework. The two most stable
structures are practically degenerate in energy and semiconducting. One contains the experimental 320
atoms in the hexagonal unit cell, and the other contains 106 atoms in the triclinic unit cell. When populated
with the experimental 320 electrons, the 106 atom structure exhibits a band gap of 1.4 eV and an in-gap
hole trap at 0.35 eV above the valence band, consistent with known experiments. The total energy of
these two structures is 23 meV/B lower than the original 105 atom framework, but it is still 1 meV/B above
the α phase. Adding zero point energies finally makes the β phase the ground state of elemental boron by
3 meV/B. At finite temperatures, the difference becomes even larger
High-Throughput Design of Non-oxide p‑Type Transparent Conducting Materials: Data Mining, Search Strategy, and Identification of Boron Phosphide
High-performance
p-type transparent conducting materials (TCMs)
are needed in a wide range of applications ranging from solar cells
to transparent electronics. p-type TCMs require a large band gap (for
transparency), low hole effective mass (for high mobility), and hole
dopability. It has been demonstrated that oxides have inherent limitations
in terms of hole effective masses making them difficult to use as
a high-performance p-type TCM. In this work, we use a high-throughput
computational approach to identify novel, non-oxide, p-type TCMs.
By data mining a large computational data set (more than 30,000 compounds),
we demonstrate that non-oxide materials can lead to much lower hole
effective masses but to the detriment of smaller gaps and lower transparencies.
We propose a strategy to overcome this fundamental correlation between
low effective mass and small band gap by exploiting the weak absorption
for indirect optical transitions. We apply this strategy to phosphides
and identify zinc blende boron phosphide (BP) as a very promising
candidate. Follow-up computational studies on defects formation indicate
that BP can also be doped p-type and potentially n-type as well. Our
work demonstrates how high-throughput computational design can lead
to identification of materials with exceptional properties, and we
propose a strategy to open the design of TCMs to non-oxide materials
LiBH<sub>4</sub>−Mg(BH<sub>4</sub>)<sub>2</sub>: A Physical Mixture of Metal Borohydrides as Hydrogen Storage Material
The LiBH4−Mg(BH4)2 system has been investigated as a possible hydrogen storage material. Several composites were synthesized by ball milling, namely, xLiBH4−(1−x)Mg(BH4)2 with x = 0, 0.10, 0.25, 0.33, 0.40, 0.50, 0.60, 0.66, 0.75, 0.80, 0.90, 1. The physical mixture was investigated by using X- ray powder diffraction and thermal analysis. Interestingly, already a small amount of LiBH4 makes the α to β transition of Mg(BH4)2 reversible, which has not been reported before. The eutectic composition was found to exist at 0.50 x x = 0.50 composite releases about 7.0 wt % of hydrogen
