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.
Authors
- Eva Zurek (ORCID: https://orcid.org/0000-0003-0738-867X)
- Rohit P. Prasankumar (ORCID: https://orcid.org/0000-0003-0902-2831)
- Warren E. Pickett (ORCID: https://orcid.org/0000-0003-4591-7691)
- Michael Hutcheon (ORCID: https://orcid.org/0000-0002-5562-6049)
- Xiaoyu Wang (ORCID: https://orcid.org/0000-0001-7549-6010)
Institutions
- Intellectual Ventures (United States) (US)
- University at Buffalo, State University of New York (US)
- University of California, Davis (US)
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
Funders
- Division of Materials Research