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<title>Samuel J. Frost — University of Warwick</title>
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<h1>Samuel J. Frost</h1>
<code style="font-size: 1em">samuel<span class=sep> <dot> </span>frost<span class=sep> <at> </span>warwick<span class=sep> <dot> </span>ac<span class=sep> <dot> </span>uk</code>
<h3><a href="/">↩Home!</a></h3>
<h2>The 74<sup>th</sup> Diamond Research Conference</h2>
<p>
PDF of the poster is available <a href="/poster2024/poster.pdf">here</a>!
<!-- (<a href="https://github.com/Samuel-Frost/Poster">source code</a>) -->
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<h2>NnVH Defects</h2>
<h3>VH</h3>
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<h3>NVH</h3>
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<h3>N<sub>2</sub>VH</h3>
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<p>The typical structure of an N<sub>2</sub>VH defect, the hydrogen is rapdily quantum tunnelling between equivalent carbons, giving it an averaged C<sub>3v</sub> symmetry in EPR!</p>
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<h2>Vacancy Migration</h2>
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<h3>Bulk Vacancy Migration</h3>
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<p>The minimum energy path of a vacancy switching places with a carbon atom, calculated through DFT. The path is clearly crooked despite being in a periodic bulk cell.</p>
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<h3>Vacancy Migration to the Surface</h3>
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<strong>No. of Bonds</strong>
<ul>
<li>Yellow = 4</li>
<li>Blue = 3</li>
<li>Purple ≤ 2</li>
</ul>
<p>
The molecular dynamics simulation shows a vacancy moving from the bulk to the surface along the minimum energy path.
Since you cannot physically track a vacancy, as it does not exist, instead it's easiest to track atoms with fewer than 4 bonds.
<br>
The graph tracks the vacancy and shows its energy along the path to the surface.
There is a clear lowering of energy as the vacancy gets closer to the surface, implying there should be some form of diffusion gradient which could cause the destruction of the vacancy.
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