Why Mg<sub>2</sub>IrH<sub>6</sub> Is Predicted to Be a High‐Temperature Superconductor, But Ca<sub>2</sub>IrH<sub>6</sub> Is Not

The X<sub>2</sub>MH<sub>6</sub> family, consisting of an electropositive cation X<sup>n+</sup> and a main group metal M octahedrally coordinated by hydrogen, have been identified as promising templates for high-temperature conventional superconductivity. Herein, we analyze the electronic structure of two members of this family, Mg<sub>2</sub>IrH<sub>6</sub> and Ca<sub>2</sub>IrH<sub>6</sub>, showing why the former may possess superconducting properties rivaling those of the cuprates, whereas the latter does not. Within Mg<sub>2</sub>IrH<sub>6</sub> the vibrations of the anions IrH<sub>6</sub> <sup>4-</sup> anions are key for the superconducting mechanism, and they induce coupling in the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:semantics><mml:msubsup><mml:mi>e</mml:mi> <mml:mi>g</mml:mi> <mml:mo>*</mml:mo></mml:msubsup> <mml:annotation>${e_g^{\ast} }$</mml:annotation> </mml:semantics> </mml:math> set of orbitals, which are antibonding between the H 1s and the Ir <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:semantics><mml:msub><mml:mi>d</mml:mi> <mml:mrow><mml:msup><mml:mi>x</mml:mi> <mml:mn>2</mml:mn></mml:msup> <mml:mo>-</mml:mo> <mml:msup><mml:mi>y</mml:mi> <mml:mn>2</mml:mn></mml:msup> </mml:mrow> </mml:msub> <mml:annotation>${d_{x^2 - y^2 } }$</mml:annotation> </mml:semantics> </mml:math> or <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:semantics><mml:msub><mml:mi>d</mml:mi> <mml:msup><mml:mi>z</mml:mi> <mml:mn>2</mml:mn></mml:msup> </mml:msub> <mml:annotation>${d_{z^2 } }$</mml:annotation> </mml:semantics> </mml:math> orbitals. Because calcium possesses low-lying d-orbitals, <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:semantics><mml:msubsup><mml:mi>e</mml:mi> <mml:mi>g</mml:mi> <mml:mo>*</mml:mo></mml:msubsup> <mml:annotation>${e_g^{\ast} }$</mml:annotation> </mml:semantics> </mml:math> →Ca d back-donation is preferred, quenching the superconductivity. Our analysis explains why high critical temperatures were only predicted for second or third row X metal atoms, and may provide rules for identifying likely high-temperature superconductors in other systems where the antibonding anionic states are filled.

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Publication Details

Journal
Angewandte Chemie International Edition
Published
2024-10-11
DOI
https://doi.org/10.1002/anie.202412687
Citations
10
Primary Topic
Hydrogen Storage and Materials
Type
article
Field-Weighted Citation Impact
1.17

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article

Why Mg2IrH6 Is Predicted to Be a High‐Temperature Superconductor, But Ca2IrH6 Is Not

Eva Zurek, Rohit P. Prasankumar, Warren E. Pickett, Michael Hutcheon et al.
10 citations
Angewandte Chemie International Edition
Hydrogen Storage and Materials
1.17
article

Why Mg2IrH6 Is Predicted to Be a High‐Temperature Superconductor, But Ca2IrH6 Is Not

Eva Zurek, Rohit P. Prasankumar, Warren E. Pickett, Michael Hutcheon, Xiaoyu Wang
article en
10 citations

Abstract

The X<sub>2</sub>MH<sub>6</sub> family, consisting of an electropositive cation X<sup>n+</sup> and a main group metal M octahedrally coordinated by hydrogen, have been identified as promising templates for high-temperature conventional superconductivity. Herein, we analyze the electronic structure of two members of this family, Mg<sub>2</sub>IrH<sub>6</sub> and Ca<sub>2</sub>IrH<sub>6</sub>, showing why the former may possess superconducting properties rivaling those of the cuprates, whereas the latter does not. Within Mg<sub>2</sub>IrH<sub>6</sub> the vibrations of the anions IrH<sub>6</sub> <sup>4-</sup> anions are key for the superconducting mechanism, and they induce coupling in the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:semantics><mml:msubsup><mml:mi>e</mml:mi> <mml:mi>g</mml:mi> <mml:mo>*</mml:mo></mml:msubsup> <mml:annotation>${e_g^{\ast} }$</mml:annotation> </mml:semantics> </mml:math> set of orbitals, which are antibonding between the H 1s and the Ir <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:semantics><mml:msub><mml:mi>d</mml:mi> <mml:mrow><mml:msup><mml:mi>x</mml:mi> <mml:mn>2</mml:mn></mml:msup> <mml:mo>-</mml:mo> <mml:msup><mml:mi>y</mml:mi> <mml:mn>2</mml:mn></mml:msup> </mml:mrow> </mml:msub> <mml:annotation>${d_{x^2 - y^2 } }$</mml:annotation> </mml:semantics> </mml:math> or <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:semantics><mml:msub><mml:mi>d</mml:mi> <mml:msup><mml:mi>z</mml:mi> <mml:mn>2</mml:mn></mml:msup> </mml:msub> <mml:annotation>${d_{z^2 } }$</mml:annotation> </mml:semantics> </mml:math> orbitals. Because calcium possesses low-lying d-orbitals, <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:semantics><mml:msubsup><mml:mi>e</mml:mi> <mml:mi>g</mml:mi> <mml:mo>*</mml:mo></mml:msubsup> <mml:annotation>${e_g^{\ast} }$</mml:annotation> </mml:semantics> </mml:math> →Ca d back-donation is preferred, quenching the superconductivity. Our analysis explains why high critical temperatures were only predicted for second or third row X metal atoms, and may provide rules for identifying likely high-temperature superconductors in other systems where the antibonding anionic states are filled.

Angewandte Chemie International EditionVol. 63(52)
Intellectual Ventures (United States) (US), University at Buffalo, State University of New York (US), University of California, Davis (US)
Division of Materials Research
Openalex Percentile: Top 18%
Hydrogen Storage and Materials
1.17
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