<p>We present a first-principles study of Fe(NO<InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(_3\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>3</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>)<InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(_3\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>3</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>-functionalized monolayer germanene, focusing on its structural stability, electronic structure, magnetism, and spin-dependent thermoelectric transport. Fe(NO<InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(_3\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>3</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>)<InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(_3\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>3</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation> is weakly adsorbed on germanene and preserves the buckled honeycomb lattice, indicating a physisorption-dominated interaction. Nevertheless, interfacial charge transfer produces moderate <i>p</i>-type doping and induces a total magnetic moment of 4.3&#xa0;<InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\mu _B\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>μ</mi> <mi>B</mi> </msub> </math></EquationSource> </InlineEquation>, mainly localized on the Fe atom. Bader charge analysis confirms a net electron transfer of about 0.71&#xa0;<i>e</i> from germanene to Fe(NO<InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(_3\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>3</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>)<InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(_3\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>3</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>, with stronger charge depletion in the upper Ge sublayer near the adsorption interface. Band-unfolding and projected density of states analyses show that the Dirac cone of germanene is largely retained, while Fe-derived spin-polarized 3<i>d</i> states emerge near the Fermi level. These electronic changes lead to spin-dependent transport coefficients, a modified Seebeck response, and enhanced <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(PF/\tau \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>P</mi> <mi>F</mi> <mo stretchy="false">/</mo> <mi>τ</mi> </mrow> </math></EquationSource> </InlineEquation> and electronic figure of merit <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(ZT_e\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>Z</mi> <msub> <mi>T</mi> <mi>e</mi> </msub> </mrow> </math></EquationSource> </InlineEquation>. The results highlight superhalogen adsorption as a noncovalent strategy for introducing coupled charge-transfer, magnetic, and spin-dependent thermoelectric functionalities into germanene.</p>

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Electronic, magnetic, and spin-dependent thermoelectric transport properties of Fe(NO\(_3\))\(_3\)-adsorbed monolayer germanene

  • Nguyen Thi Han,
  • Vo Khuong Dien

摘要

We present a first-principles study of Fe(NO \(_3\) 3 ) \(_3\) 3 -functionalized monolayer germanene, focusing on its structural stability, electronic structure, magnetism, and spin-dependent thermoelectric transport. Fe(NO \(_3\) 3 ) \(_3\) 3 is weakly adsorbed on germanene and preserves the buckled honeycomb lattice, indicating a physisorption-dominated interaction. Nevertheless, interfacial charge transfer produces moderate p-type doping and induces a total magnetic moment of 4.3  \(\mu _B\) μ B , mainly localized on the Fe atom. Bader charge analysis confirms a net electron transfer of about 0.71 e from germanene to Fe(NO \(_3\) 3 ) \(_3\) 3 , with stronger charge depletion in the upper Ge sublayer near the adsorption interface. Band-unfolding and projected density of states analyses show that the Dirac cone of germanene is largely retained, while Fe-derived spin-polarized 3d states emerge near the Fermi level. These electronic changes lead to spin-dependent transport coefficients, a modified Seebeck response, and enhanced \(PF/\tau \) P F / τ and electronic figure of merit \(ZT_e\) Z T e . The results highlight superhalogen adsorption as a noncovalent strategy for introducing coupled charge-transfer, magnetic, and spin-dependent thermoelectric functionalities into germanene.