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<title>First Principles Simulations Test</title>
<link>https://hdl.handle.net/11256/47</link>
<description/>
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<dc:date>2026-05-01T13:13:50Z</dc:date>
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<item rdf:about="https://hdl.handle.net/11256/997">
<title>Ws2-WTe2</title>
<link>https://hdl.handle.net/11256/997</link>
<description>Ws2-WTe2
Burton, Benjamin
First principles phase diagram calculations, that included&#13;
van der Waals interactions, were performed for the bulk&#13;
transition metal dichalcogenide&#13;
system (1-X)WS_2 - (X)WTe_2.&#13;
To obtain a converged phase diagram, a series of cluster expansion&#13;
calculations were performed with increasing numbers of structural energies,&#13;
(N_{str}) up to N_{str}=435, used to fit the cluster expansion Hamiltonian.&#13;
All calculated formation energies are positive and all ground-state&#13;
analyses predict that formation energies for supercells with 16 or&#13;
fewer anion sites are positive; but when 150 ~N_{str} &lt;~ 376,&#13;
false ordered ground-states are predicted. With N_{str} &gt;= 399, only a&#13;
miscibility gap is predicted, but one with dramatic asymmetry opposite to&#13;
what one expects from size-effect considerations; i.e. the calculations&#13;
predict more solubility on the small-ion S-rich side of the diagram and&#13;
less on the large-ion Te-rich side.&#13;
This occurs because S-rich low-energy metastable ordered configurations have&#13;
lower energies than their Te-rich counterparts which suggests that&#13;
elastic relaxation effects are not dominant for the shape of the miscibility gap.
</description>
<dc:date>2016-01-01T00:00:00Z</dc:date>
</item>
<item rdf:about="https://hdl.handle.net/11256/996">
<title>MoS2-MoTe2</title>
<link>https://hdl.handle.net/11256/996</link>
<description>MoS2-MoTe2
Singh, Arunima; Burton, Benjamin
A first principles phase diagram calculation, that included van der Waals interactions, was performed for the 3D bulk system (1−&#119883;)·&#119872;&#119900;&#119878;2−(&#119883;)·&#119872;&#119900;&#119879;&#119890;2. Surprisingly, the predicted phase diagram has at least two ordered phases, at &#119883;≈0.46, even though all calculated formation energies are positive; in a ground-state analysis that examined all configurations with 16 or fewer anion sites. The lower-temperature I-phase is predicted to transform to a higher-temperature &#119868;′-phase at &#119879;≈500K, and &#119868;′ disorders at &#119879;≈730K. Both these transitions are predicted to be first-order, and there are broad two-phase fields on both sides of the ordered regions. Both the I- and &#119868;′-phases are predicted to be incommensurate, i.e., aperiodic: I-phase in three dimensions; and &#119868;′-phase in two dimensions.
</description>
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