From weak- to strong-coupling superconductivity in the AlB<sub>2</sub>-type solid solution SrGa<sub>1−x</sub>Al<sub>x</sub>Ge with honeycomb layers

We report on the structure and the superconducting properties of 9-electron 111 compounds with honeycomb layers, namely SrGaGe, SrAlGe, and the SrGa1-xAl<sub><i>x</i></sub>Ge solid solution. By means of single-crystal x-ray diffraction we show that, on one hand, SrGaGe crystallizes into the centrosymmetric<i>P</i>6/<i>mmm</i>space group (<i>a</i>= 4.2555(2) Å,<i>c</i>= 4.7288(2) Å) with statistical disorder in the [GaGe]62-honeycomb layers. On the other hand, we confirm that SrAlGe crystallizes in a non-centrosymmetric space group, namely<i>P</i>6¯<i>m2</i>(<i>a</i>= 4.2942(1) Å,<i>c</i>= 4.7200(2) Å) with fully ordered [AlGe]62-honeycomb layers. By using magnetization and specific heat measurements, we show that the superconducting properties of SrGaGe and SrAlGe differ significantly from each other. SrGaGe is a superconductor with a critical temperature ofTc= 2.6 K falling into the weak coupling limit, while SrAlGe has aTc= 6.7 K and can be classified in the strong coupling limit. By realizing the SrGa1-xAl<sub><i>x</i></sub>Ge solid solution, we were able to investigate the transition between the different crystal structures as well as the evolution of the electronic properties. We show that the transition from the weak-to strong-coupling superconductivity in this system is likely associated with the disorder-to-order transition of the honeycomb layer, along with the loss of the inversion center in the crystal structure.

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Journal
Journal of Physics Condensed Matter
Published
2024-10-28
DOI
https://doi.org/10.1088/1361-648x/ad8c0b
Citations
2
Primary Topic
Superconductivity in MgB2 and Alloys
Type
article
Field-Weighted Citation Impact
0.62

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article

From weak- to strong-coupling superconductivity in the AlB2-type solid solution SrGa1−xAlxGe with honeycomb layers

Olivier Blacque, Fabian O. von Rohr, Tomasz Klimczuk, Dorota I. Walicka
2 citations
Journal of Physics Condensed Matter
Superconductivity in MgB2 and Alloys
0.62
article

From weak- to strong-coupling superconductivity in the AlB2-type solid solution SrGa1−xAlxGe with honeycomb layers

Olivier Blacque, Fabian O. von Rohr, Tomasz Klimczuk, Dorota I. Walicka
article en
2 citations

Abstract

We report on the structure and the superconducting properties of 9-electron 111 compounds with honeycomb layers, namely SrGaGe, SrAlGe, and the SrGa1-xAl<sub><i>x</i></sub>Ge solid solution. By means of single-crystal x-ray diffraction we show that, on one hand, SrGaGe crystallizes into the centrosymmetric<i>P</i>6/<i>mmm</i>space group (<i>a</i>= 4.2555(2) Å,<i>c</i>= 4.7288(2) Å) with statistical disorder in the [GaGe]62-honeycomb layers. On the other hand, we confirm that SrAlGe crystallizes in a non-centrosymmetric space group, namely<i>P</i>6¯<i>m2</i>(<i>a</i>= 4.2942(1) Å,<i>c</i>= 4.7200(2) Å) with fully ordered [AlGe]62-honeycomb layers. By using magnetization and specific heat measurements, we show that the superconducting properties of SrGaGe and SrAlGe differ significantly from each other. SrGaGe is a superconductor with a critical temperature ofTc= 2.6 K falling into the weak coupling limit, while SrAlGe has aTc= 6.7 K and can be classified in the strong coupling limit. By realizing the SrGa1-xAl<sub><i>x</i></sub>Ge solid solution, we were able to investigate the transition between the different crystal structures as well as the evolution of the electronic properties. We show that the transition from the weak-to strong-coupling superconductivity in this system is likely associated with the disorder-to-order transition of the honeycomb layer, along with the loss of the inversion center in the crystal structure.

Journal of Physics Condensed MatterVol. 37(4)
University of Geneva (CH), Gdańsk University of Technology (PL), University of Zurich (CH), Paul Scherrer Institute (CH)
Schweizerischer Nationalfonds zur Förderung der Wissenschaftlichen Forschung
Openalex Percentile: Top 32%
Superconductivity in MgB2 and Alloys
0.62
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