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        <identifier>oai:figshare.com:article/32414772</identifier>
        <datestamp>2026-09-30T20:26:13Z</datestamp>
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          <dc:title>Not all H atoms contribute to low activation barrier diffusion in Ba&lt;sub&gt;1.75&lt;/sub&gt;LiH&lt;sub&gt;2.7&lt;/sub&gt;O&lt;sub&gt;0.9&lt;/sub&gt;</dc:title>
          <dc:creator>Yoyo Hinuma (1270065)</dc:creator>
          <dc:subject>Biophysics</dc:subject>
          <dc:subject>Physical Sciences not elsewhere classified</dc:subject>
          <dc:subject>Medicine</dc:subject>
          <dc:subject>Chemical Sciences not elsewhere classified</dc:subject>
          <dc:subject>Information Systems not elsewhere classified</dc:subject>
          <dc:subject>Cancer</dc:subject>
          <dc:subject>Science Policy</dc:subject>
          <dc:subject>Computational  Biology</dc:subject>
          <dc:subject>Superionic conductivity</dc:subject>
          <dc:subject>tracer diffusion coefficient</dc:subject>
          <dc:subject>molecular dynamics</dc:subject>
          <dc:subject>neural network potential</dc:subject>
          <dc:subject>Ba1.75LiH2.7O0.9</dc:subject>
          <dc:description>&lt;p&gt;Superionic conductors have extremely high conductivity in some constituent ions even in the solid state, and many lose their superionicity below a critical temperature. The conductivity of K&lt;sub&gt;2&lt;/sub&gt;NiF&lt;sub&gt;4&lt;/sub&gt; structure-based Ba&lt;sub&gt;1.75&lt;/sub&gt;LiH&lt;sub&gt;2.7&lt;/sub&gt;O&lt;sub&gt;0.9&lt;/sub&gt; jumps over three orders of magnitude at ~ 573 K. This jump is not at a first-order structural phase transition temperature. Molecular dynamics (MD) simulations using a density functional theory (DFT) trained universal neural network potential (NNP) were conducted in this study. The Arrhenius plot of the tracer diffusion coefficient is a straight line between 455 and 741 K, inconsistent with the conductivity jump. The 3D activation barrier is ~0.3 eV, which is much lower than typical K&lt;sub&gt;2&lt;/sub&gt;NiF&lt;sub&gt;4&lt;/sub&gt; structure-based oxyhydrides. The features in the radial distribution function are almost temperature independent. However, statistical inspection of the tracer diffusion coefficient for each atom, which is very difficult with DFT-MD but is feasible with NNP-MD, revealed the existence of effectively immobile H atoms over the entire studied temperature range. Most H do not engage in concerted migration, according to a comparison with a universal curve for independent random walkers. These findings hold for all phases, which have different distributions of Li, O, and H atoms in the same structural framework. Incorporating many vacancies, especially in ‘K’ sites of the K&lt;sub&gt;2&lt;/sub&gt;NiF&lt;sub&gt;4&lt;/sub&gt; framework, could form a low activation barrier H diffusion network not available in conventional oxyhydrides with the same framework. Gaining access to such a percolating network above a certain temperature can explain the superionic transition at this temperature.&lt;/p&gt; &lt;p&gt;Neural network potential molecular dynamics show that the superionic transition in H&lt;sup&gt;−&lt;/sup&gt;-conductor Ba&lt;sub&gt;1.75&lt;/sub&gt;LiH&lt;sub&gt;2.7&lt;/sub&gt;O&lt;sub&gt;0.9&lt;/sub&gt; that does not accompany a structural transition is caused by changes in non-migrating H with temperature.&lt;/p&gt;</dc:description>
          <dc:date>2026-09-30T20:26:13Z</dc:date>
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          <dc:identifier>10.6084/m9.figshare.32414772.v2</dc:identifier>
          <dc:relation>https://figshare.com/articles/dataset/Not_all_H_atoms_contribute_to_low_activation_barrier_diffusion_in_Ba_sub_1_75_sub_LiH_sub_2_7_sub_O_sub_0_9_sub_/32414772</dc:relation>
          <dc:rights>CC BY</dc:rights>
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