<p>The thermal conductivity of plasma-facing materials (PFM) exposed to intense radiation is a critical concern for the reliable usage of materials in fusion reactors. However, limited research has been performed regarding the thermal conductivity of structures that rapidly change in a short time during collision cascade processes under irradiation. In this study, we employed the tight-binding (TB) method to investigate the electronic thermal conductivity (<InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1653_Article_IEq1.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(\kappa _{\text {e}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>κ</mi> <mtext>e</mtext> </msub> </math></EquationSource> </InlineEquation>) of tungsten-based systems during various cascading processes. We found that <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1653_Article_IEq2.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(\kappa _{\text {e}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>κ</mi> <mtext>e</mtext> </msub> </math></EquationSource> </InlineEquation> values sharply decrease within the initial 0.3 picoseconds and then partially recover at a slow pace; this is closely linked to the evolution of defects and microstructural distortions. The increase in the initial kinetic energy of the primary knock-on atom and the presence of a high concentration of hydrogen atoms further decrease the <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1653_Article_IEq3.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(\kappa _{\text {e}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>κ</mi> <mtext>e</mtext> </msub> </math></EquationSource> </InlineEquation> values. Conversely, higher temperatures have a significant positive effect on <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1653_Article_IEq4.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(\kappa _{\text {e}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>κ</mi> <mtext>e</mtext> </msub> </math></EquationSource> </InlineEquation>. Furthermore, the presence of a grain boundary <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1653_Article_IEq5.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="105" /> </InlineMediaObject> <EquationSource Format="TEX">\(\sum 5\left[ 001 \right] \left( 130 \right)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>∑</mo> <mn>5</mn> <mfenced close="]" open="["> <mn>001</mn> </mfenced> <mfenced close=")" open="("> <mn>130</mn> </mfenced> </mrow> </math></EquationSource> </InlineEquation> substantially reduces <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1653_Article_IEq6.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(\kappa _{\text {e}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>κ</mi> <mtext>e</mtext> </msub> </math></EquationSource> </InlineEquation>, whereas the absorption effect of point defects by the grain boundary has little influence on <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41365_2025_1653_Article_IEq7.gif" Format="GIF" Height="12" Rendition="HTML" Resolution="72" Type="Linedraw" Width="17" /> </InlineMediaObject> <EquationSource Format="TEX">\(\kappa _{\text {e}}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>κ</mi> <mtext>e</mtext> </msub> </math></EquationSource> </InlineEquation> during cascades. Our findings provide a theoretical basis for evaluating changes in the thermal conductivity performance of PFMs during their usage in nuclear fusion reactors.</p>

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Electronic thermal conductivity of tungsten-based systems during collision cascade processes

  • Jiong-Rong Wang,
  • Bi-Cai Pan

摘要

The thermal conductivity of plasma-facing materials (PFM) exposed to intense radiation is a critical concern for the reliable usage of materials in fusion reactors. However, limited research has been performed regarding the thermal conductivity of structures that rapidly change in a short time during collision cascade processes under irradiation. In this study, we employed the tight-binding (TB) method to investigate the electronic thermal conductivity ( \(\kappa _{\text {e}}\) κ e ) of tungsten-based systems during various cascading processes. We found that \(\kappa _{\text {e}}\) κ e values sharply decrease within the initial 0.3 picoseconds and then partially recover at a slow pace; this is closely linked to the evolution of defects and microstructural distortions. The increase in the initial kinetic energy of the primary knock-on atom and the presence of a high concentration of hydrogen atoms further decrease the \(\kappa _{\text {e}}\) κ e values. Conversely, higher temperatures have a significant positive effect on \(\kappa _{\text {e}}\) κ e . Furthermore, the presence of a grain boundary \(\sum 5\left[ 001 \right] \left( 130 \right)\) 5 001 130 substantially reduces \(\kappa _{\text {e}}\) κ e , whereas the absorption effect of point defects by the grain boundary has little influence on \(\kappa _{\text {e}}\) κ e during cascades. Our findings provide a theoretical basis for evaluating changes in the thermal conductivity performance of PFMs during their usage in nuclear fusion reactors.