<p>Hydrogen incorporation at MoS<InlineEquation ID="IEq7"> <EquationSource Format="TEX">\({}_2\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>2</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>/SiO<InlineEquation ID="IEq8"> <EquationSource Format="TEX">\({}_2\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>2</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation> interfaces governs charge doping, yet the atomistic transfer pathways and kinetic barriers depend strongly on the SiO<InlineEquation ID="IEq9"> <EquationSource Format="TEX">\({}_2\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>2</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation> surface&#xa0;termination. Using first-principles simulations, we quantify hydrogen transfer barriers as a function of SiO<InlineEquation ID="IEq10"> <EquationSource Format="TEX">\({}_2\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>2</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation> surface reconstruction and out-of-plane boundary conditions. We compare two reconstructed oxide terminations interfaced with monolayer MoS<InlineEquation ID="IEq11"> <EquationSource Format="TEX">\({}_2\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>2</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>. At interfaces with dangling bonds, H transfers barrier-free from MoS<InlineEquation ID="IEq12"> <EquationSource Format="TEX">\({}_2\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>2</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation> to SiO<InlineEquation ID="IEq13"> <EquationSource Format="TEX">\({}_2\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>2</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>, while reverse transfer into defect-free MoS<InlineEquation ID="IEq14"> <EquationSource Format="TEX">\({}_2\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>2</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation> remains kinetically blocked even in the presence of a sulfur vacancy (barrier &gt;3 eV). At saturated interfaces, H transfers barrier-free from SiO<InlineEquation ID="IEq15"> <EquationSource Format="TEX">\({}_2\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>2</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation> to MoS<InlineEquation ID="IEq16"> <EquationSource Format="TEX">\({}_2\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>2</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>, while subsurface-to-surface transfer has a barrier of <InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(\sim\)</EquationSource> <EquationSource Format="MATHML"><math> <mo>∼</mo> </math></EquationSource> </InlineEquation>0.4 eV. On MoS<InlineEquation ID="IEq18"> <EquationSource Format="TEX">\({}_2\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>2</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>, H transfers laterally with <InlineEquation ID="IEq19"> <EquationSource Format="TEX">\(\sim\)</EquationSource> <EquationSource Format="MATHML"><math> <mo>∼</mo> </math></EquationSource> </InlineEquation>0.3 eV barriers, whereas incorporation into the monolayer requires <InlineEquation ID="IEq20"> <EquationSource Format="TEX">\(\sim\)</EquationSource> <EquationSource Format="MATHML"><math> <mo>∼</mo> </math></EquationSource> </InlineEquation>0.7 eV. These results show that reconstruction-driven passivation reverses the preferred direction of interfacial H transfer and determines the preferred incorporation side.</p> Graphical abstract <p></p>

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Hydrogen transfer at MoS2/SiO2 heterostructures and across their interfaces

  • Vasileios Fotopoulos,
  • Longlong Xu,
  • Mantao Huang,
  • Matthäus Siebenhofer,
  • Bilge Yildiz

摘要

Hydrogen incorporation at MoS \({}_2\) 2 /SiO \({}_2\) 2 interfaces governs charge doping, yet the atomistic transfer pathways and kinetic barriers depend strongly on the SiO \({}_2\) 2 surface termination. Using first-principles simulations, we quantify hydrogen transfer barriers as a function of SiO \({}_2\) 2 surface reconstruction and out-of-plane boundary conditions. We compare two reconstructed oxide terminations interfaced with monolayer MoS \({}_2\) 2 . At interfaces with dangling bonds, H transfers barrier-free from MoS \({}_2\) 2 to SiO \({}_2\) 2 , while reverse transfer into defect-free MoS \({}_2\) 2 remains kinetically blocked even in the presence of a sulfur vacancy (barrier >3 eV). At saturated interfaces, H transfers barrier-free from SiO \({}_2\) 2 to MoS \({}_2\) 2 , while subsurface-to-surface transfer has a barrier of \(\sim\) 0.4 eV. On MoS \({}_2\) 2 , H transfers laterally with \(\sim\) 0.3 eV barriers, whereas incorporation into the monolayer requires \(\sim\) 0.7 eV. These results show that reconstruction-driven passivation reverses the preferred direction of interfacial H transfer and determines the preferred incorporation side.

Graphical abstract