3 research outputs found
Influences of Surface Substitutional Ti Atom on Hydrogen Adsorption, Dissociation, and Diffusion Behaviors on the α‑U(001) Surface
The hydrogen adsorption, dissociation,
and diffusion behaviors on both clean and Ti-doped α-U(001)
surfaces are systematically studied with density functional theory
method. Through detailed potential energy surface calculations, we
find that the dissociation at the bridge sites is energetically more
favorable, where the H<sub>2</sub> molecule dissociates without any
energy barrier and the dissociated hydrogen atoms move into two neighboring
3-fold sites. Once a substitutional Ti atom exists on the α-U(001)
surface, the hydrogen molecule similarly dissociates without any energy
barriers. However, the diffusion of the dissociated hydrogen atoms
is dramatically changed after introduction of a surface substitutional
Ti atom. The into-bulk penetration of a hydrogen atom through a defect-free
surface is endothermic and needs to overcome an energy barrier of
0.8–0.9 eV. In contrast, the penetration to the subsurface
sites near the doped Ti atom is exothermic, and the activation barrier
decreases by 0.3–0.4 eV. Our results indicate that surface
doped titanium atoms in the outermost layer may behave like hydrogen
trapping sites for α-U
New Insights into the Crystal Structures of Plutonium Hydrides from First-Principles Calculations
One of the important
research contents on hydrogen corrosion of
plutonium is the determination of the complex crystal structures of
plutonium hydrides and the bonding interactions between plutonium
and hydrogen. However, it is very difficult to carry out the structural
characterization of plutonium hydrides because of their high activity,
high toxicity, and radioactivity. In this work, the crystal structures,
lattice vibrations, and bonding properties of plutonium hydrides under
ambient pressure are investigated by means of the density functional
theory + <i>U</i> approach. Results show that PuH<sub>3</sub> exhibits many competition phase structures. After considering spin
polarization, strong correlation (<i>U</i>), and spin–orbit
coupling effects on the total energy and lattice dynamics stability,
it is found that PuH<sub>3</sub> at ambient pressure is more likely
to be hexagonal <i>P</i>6<sub>3</sub><i>cm</i> or trigonal <i>P</i>3<i>c</i>1 structure, instead
of the usual supposed structures of hexagonal <i>P</i>6<sub>3</sub>/<i>mmc</i> (LaF<sub>3</sub>-type) and face-centered
cubic (BiF<sub>3</sub>-type). The calculated electronic structures
clearly indicate that <i>P</i>6<sub>3</sub><i>cm</i> (<i>P</i>3<i>c</i>1) PuH<sub>3</sub> is a semiconductor
with a small band gap about 0.87 eV (0.85 eV). The Pu–H bonds
in Pu hydrides are dominated by the ionic interactions
Ammonia Activation by Ce Atom: Matrix-Isolation FTIR and Theoretical Studies
The
activation of ammonia by cerium atom has been investigated
in solid argon using infrared spectroscopy and density functional
theoretical calculations. The results reveal that the spontaneous
formation of CeNH<sub>3</sub> complex on annealing is the initial
step in the reactions of cerium atoms with ammonia. The CeNH<sub>3</sub> complexes rearrange to generate the inserted HCeNH<sub>2</sub> molecules
on irradiation. A “triplet–singlet” spin conversion
occurs along the reaction path in which HCeNH<sub>2</sub> (<sup>3</sup>A″) isomerizes into H<sub>2</sub>CeNH (<sup>1</sup>A′).
The H<sub>2</sub>CeNH molecules finally decompose to yield HCeN +
H<sub>2</sub> upon photolysis. The periodic trend and differences
for the M + NH<sub>3</sub> (M = Ti, Zr, Hf, Ce, Th) systems are discussed
on the basis of the present and previous works. DFT calculations predict
that the most stable ground state for HHfNH<sub>2</sub> and HThNH<sub>2</sub> is singlet due to the stronger relativistic effects in Hf
and Th atoms, while that for HTiNH<sub>2</sub>, HZrNH<sub>2</sub>,
and HCeNH<sub>2</sub> is triplet. Besides, the H<sub>2</sub>-elimination
process is different for Ce and M (Ti, Zr, Hf, Th) cases