<p>The performance of Cu-exchanged chabazite (Cu-CHA) for the ammonia-assisted selective catalytic reduction of NO<sub><i>x</i></sub> (NH<sub>3</sub>-SCR) depends critically on the presence of paired <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41467_2025_55859_Article_IEq2.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="88" /> </InlineMediaObject> <EquationSource Format="TEX">\({[{{{\rm{Cu}}}}{({{{{\rm{NH}}}}}_{3})}_{2}]}^{+}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mrow> <mo>[</mo> <mrow> <mi mathvariant="normal">Cu</mi> <msub> <mrow> <mrow> <mo>(</mo> <mrow> <msub> <mrow> <mi mathvariant="normal">NH</mi> </mrow> <mrow> <mn>3</mn> </mrow> </msub> </mrow> <mo>)</mo> </mrow> </mrow> <mrow> <mn>2</mn> </mrow> </msub> </mrow> <mo>]</mo> </mrow> </mrow> <mrow> <mo>+</mo> </mrow> </msup> </math></EquationSource> </InlineEquation> complexes. Here, a machine-learning force field augmented with long-range Coulomb interactions is developed to investigate the effect of Al-distribution and Cu-loading on the mobility and pairing of <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41467_2025_55859_Article_IEq3.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="88" /> </InlineMediaObject> <EquationSource Format="TEX">\({[{{{\rm{Cu}}}}{({{{{\rm{NH}}}}}_{3})}_{2}]}^{+}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mrow> <mo>[</mo> <mrow> <mi mathvariant="normal">Cu</mi> <msub> <mrow> <mrow> <mo>(</mo> <mrow> <msub> <mrow> <mi mathvariant="normal">NH</mi> </mrow> <mrow> <mn>3</mn> </mrow> </msub> </mrow> <mo>)</mo> </mrow> </mrow> <mrow> <mn>2</mn> </mrow> </msub> </mrow> <mo>]</mo> </mrow> </mrow> <mrow> <mo>+</mo> </mrow> </msup> </math></EquationSource> </InlineEquation> complexes. Performing unbiased and constrained molecular dynamics simulations, we obtain unique information inaccessible to first-principle calculations and experiments. The free energy barrier for <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41467_2025_55859_Article_IEq4.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="88" /> </InlineMediaObject> <EquationSource Format="TEX">\({[{{{\rm{Cu}}}}{({{{{\rm{NH}}}}}_{3})}_{2}]}^{+}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mrow> <mo>[</mo> <mrow> <mi mathvariant="normal">Cu</mi> <msub> <mrow> <mrow> <mo>(</mo> <mrow> <msub> <mrow> <mi mathvariant="normal">NH</mi> </mrow> <mrow> <mn>3</mn> </mrow> </msub> </mrow> <mo>)</mo> </mrow> </mrow> <mrow> <mn>2</mn> </mrow> </msub> </mrow> <mo>]</mo> </mrow> </mrow> <mrow> <mo>+</mo> </mrow> </msup> </math></EquationSource> </InlineEquation> diffusion between CHA-cages depends sensitively on both the local and distant Al-distribution. Importantly, certain Al-distributions and arrangements of neighboring <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41467_2025_55859_Article_IEq5.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="88" /> </InlineMediaObject> <EquationSource Format="TEX">\({[{{{\rm{Cu}}}}{({{{{\rm{NH}}}}}_{3})}_{2}]}^{+}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mrow> <mo>[</mo> <mrow> <mi mathvariant="normal">Cu</mi> <msub> <mrow> <mrow> <mo>(</mo> <mrow> <msub> <mrow> <mi mathvariant="normal">NH</mi> </mrow> <mrow> <mn>3</mn> </mrow> </msub> </mrow> <mo>)</mo> </mrow> </mrow> <mrow> <mn>2</mn> </mrow> </msub> </mrow> <mo>]</mo> </mrow> </mrow> <mrow> <mo>+</mo> </mrow> </msup> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41467_2025_55859_Article_IEq6.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="41" /> </InlineMediaObject> <EquationSource Format="TEX">\({{{{{\rm{NH}}}}}_{4}}^{+}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <msub> <mrow> <mi mathvariant="normal">NH</mi> </mrow> <mrow> <mn>4</mn> </mrow> </msub> </mrow> <mrow> <mo>+</mo> </mrow> </msup> </math></EquationSource> </InlineEquation> cations make paired <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41467_2025_55859_Article_IEq7.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="88" /> </InlineMediaObject> <EquationSource Format="TEX">\({[{{{\rm{Cu}}}}{({{{{\rm{NH}}}}}_{3})}_{2}]}^{+}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mrow> <mo>[</mo> <mrow> <mi mathvariant="normal">Cu</mi> <msub> <mrow> <mrow> <mo>(</mo> <mrow> <msub> <mrow> <mi mathvariant="normal">NH</mi> </mrow> <mrow> <mn>3</mn> </mrow> </msub> </mrow> <mo>)</mo> </mrow> </mrow> <mrow> <mn>2</mn> </mrow> </msub> </mrow> <mo>]</mo> </mrow> </mrow> <mrow> <mo>+</mo> </mrow> </msup> </math></EquationSource> </InlineEquation> complexes exothermic with respect to separated configurations. Our results suggest that the NH<sub>3</sub>-SCR activity can be enhanced by increasing the Cu-loading and Al-content. The dynamic interplay between <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41467_2025_55859_Article_IEq8.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="88" /> </InlineMediaObject> <EquationSource Format="TEX">\({[{{{\rm{Cu}}}}{({{{{\rm{NH}}}}}_{3})}_{2}]}^{+}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mrow> <mo>[</mo> <mrow> <mi mathvariant="normal">Cu</mi> <msub> <mrow> <mrow> <mo>(</mo> <mrow> <msub> <mrow> <mi mathvariant="normal">NH</mi> </mrow> <mrow> <mn>3</mn> </mrow> </msub> </mrow> <mo>)</mo> </mrow> </mrow> <mrow> <mn>2</mn> </mrow> </msub> </mrow> <mo>]</mo> </mrow> </mrow> <mrow> <mo>+</mo> </mrow> </msup> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41467_2025_55859_Article_IEq9.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="41" /> </InlineMediaObject> <EquationSource Format="TEX">\({{{{{\rm{NH}}}}}_{4}}^{+}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <msub> <mrow> <mi mathvariant="normal">NH</mi> </mrow> <mrow> <mn>4</mn> </mrow> </msub> </mrow> <mrow> <mo>+</mo> </mrow> </msup> </math></EquationSource> </InlineEquation> diffusion is crucial for the <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="41467_2025_55859_Article_IEq10.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="88" /> </InlineMediaObject> <EquationSource Format="TEX">\({[{{{\rm{Cu}}}}{({{{{\rm{NH}}}}}_{3})}_{2}]}^{+}\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mrow> <mo>[</mo> <mrow> <mi mathvariant="normal">Cu</mi> <msub> <mrow> <mrow> <mo>(</mo> <mrow> <msub> <mrow> <mi mathvariant="normal">NH</mi> </mrow> <mrow> <mn>3</mn> </mrow> </msub> </mrow> <mo>)</mo> </mrow> </mrow> <mrow> <mn>2</mn> </mrow> </msub> </mrow> <mo>]</mo> </mrow> </mrow> <mrow> <mo>+</mo> </mrow> </msup> </math></EquationSource> </InlineEquation> mobility and stresses the need to explore large systems including long-range Coulomb interactions when studying diffusion of charged species in zeolites.</p>

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Influence of aluminium distribution on the diffusion mechanisms and pairing of [Cu(NH3)2]+ complexes in Cu-CHA

  • Joachim D. Bjerregaard,
  • Martin Votsmeier,
  • Henrik Grönbeck

摘要

The performance of Cu-exchanged chabazite (Cu-CHA) for the ammonia-assisted selective catalytic reduction of NOx (NH3-SCR) depends critically on the presence of paired \({[{{{\rm{Cu}}}}{({{{{\rm{NH}}}}}_{3})}_{2}]}^{+}\) [ Cu ( NH 3 ) 2 ] + complexes. Here, a machine-learning force field augmented with long-range Coulomb interactions is developed to investigate the effect of Al-distribution and Cu-loading on the mobility and pairing of \({[{{{\rm{Cu}}}}{({{{{\rm{NH}}}}}_{3})}_{2}]}^{+}\) [ Cu ( NH 3 ) 2 ] + complexes. Performing unbiased and constrained molecular dynamics simulations, we obtain unique information inaccessible to first-principle calculations and experiments. The free energy barrier for \({[{{{\rm{Cu}}}}{({{{{\rm{NH}}}}}_{3})}_{2}]}^{+}\) [ Cu ( NH 3 ) 2 ] + diffusion between CHA-cages depends sensitively on both the local and distant Al-distribution. Importantly, certain Al-distributions and arrangements of neighboring \({[{{{\rm{Cu}}}}{({{{{\rm{NH}}}}}_{3})}_{2}]}^{+}\) [ Cu ( NH 3 ) 2 ] + and \({{{{{\rm{NH}}}}}_{4}}^{+}\) NH 4 + cations make paired \({[{{{\rm{Cu}}}}{({{{{\rm{NH}}}}}_{3})}_{2}]}^{+}\) [ Cu ( NH 3 ) 2 ] + complexes exothermic with respect to separated configurations. Our results suggest that the NH3-SCR activity can be enhanced by increasing the Cu-loading and Al-content. The dynamic interplay between \({[{{{\rm{Cu}}}}{({{{{\rm{NH}}}}}_{3})}_{2}]}^{+}\) [ Cu ( NH 3 ) 2 ] + and \({{{{{\rm{NH}}}}}_{4}}^{+}\) NH 4 + diffusion is crucial for the \({[{{{\rm{Cu}}}}{({{{{\rm{NH}}}}}_{3})}_{2}]}^{+}\) [ Cu ( NH 3 ) 2 ] + mobility and stresses the need to explore large systems including long-range Coulomb interactions when studying diffusion of charged species in zeolites.