Unconventional Superconductivity in ScIr<sub>2</sub> Chiral Crystal With a Kagome Lattice.
basic_science · Level V
Where this comes from
- Record sourced from PubMed, PMID 42557834.
- Also identified by DOI 10.1002/adma.74399.
- No licence information is recorded for this record.
- Because redistribution is not established, this page shows the abstract only. Follow the links below for the full text.
Abstract
Materials with a kagome lattice host exotic quantum phenomena driven by the interplay between band topology, spin-orbit coupling, magnetism, and electronic correlations. While the magnetism of kagome materials has been widely investigated, their unconventional superconductivity (SC) remains largely unexplored due to the limited availability of suitable materials. Here, we report evidence of unconventional SC in the <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow><msub><mi>ScIr</mi> <mrow><mn>2</mn> <mo>-</mo> <mi>x</mi></mrow> </msub> <msub><mi>Si</mi> <mi>x</mi></msub> </mrow> </math> family by combining muon-spin spectroscopy measurements with band-structure calculations. The parent <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>ScIr</mi> <mn>2</mn></msub> </math> undergoes a structural phase transition from a high- <math xmlns="http://www.w3.org/1998/Math/MathML"><mi>T</mi></math> cubic- to a low- <math xmlns="http://www.w3.org/1998/Math/MathML"><mi>T</mi></math> rhombohedral phase, while the Ir kagome layer remains, albeit slightly, distorted. Although the structural transition is suppressed by Si substitution, the superconducting pairing of <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow><msub><mi>ScIr</mi> <mrow><mn>2</mn> <mo>-</mo> <mi>x</mi></mrow> </msub> <msub><mi>Si</mi> <mi>x</mi></msub> </mrow> </math> remains well described by a two-gap model. Since at least one of the gaps exhibits nodes, this indicates an unconventional SC. Its unconventional nature can be explained by the distinct flat bands occurring near the Fermi level, leading to strong electronic correlations in the <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow><msub><mi>ScIr</mi> <mrow><mn>2</mn> <mo>-</mo> <mi>x</mi></mrow> </msub> <msub><mi>Si</mi> <mi>x</mi></msub> </mrow> </math> family. Moreover, the low- <math xmlns="http://www.w3.org/1998/Math/MathML"><mi>T</mi></math> phase of <math xmlns="http://www.w3.org/1998/Math/MathML"><msub><mi>ScIr</mi> <mn>2</mn></msub> </math> exhibits an Ir chiral chain; therefore, it can be classified as a topological chiral crystal. Overall, the unusual properties of the <math xmlns="http://www.w3.org/1998/Math/MathML"> <mrow><msub><mi>ScIr</mi> <mrow><mn>2</mn> <mo>-</mo> <mi>x</mi></mrow> </msub> <msub><mi>Si</mi> <mi>x</mi></msub> </mrow> </math> family make it an interesting, albeit rare, system for studying the interplay between unconventional SC, flat bands, and chirality.