Strong enhancement of s-wave superconductivity near a quantum critical point of Ca3Ir4Sn13
P. K. Biswas, Z. Guguchia, R. Khasanov, M. Chinotti, L. Li, Kefeng Wang, C. Petrovic, E. Morenzoni
DOI 10.1103/PhysRevB.92.195122 · Physical Review B
Active bibliographic source — not scientific approval
Bibliographic access preserves source history; it does not approve extracted materials or validate reported claims. Review warnings on each occurrence separately.
Abstract
We report microscopic studies by muon spin rotation/relaxation as a function of pressure of the Ca3Ir4Sn13 and Sr3Ir4Sn13 cubic compounds, which are members of the (Ca1−xSrx)3Ir4Sn13 system displaying superconductivity and a structural phase transition associated with the formation of a charge density wave (CDW). We find a strong enhancement of the superfluid density and a dramatic increase of the pairing strength above a pressure of ≈1.6 GPa, giving direct evidence of the presence of a quantum critical point separating a superconducting phase coexisting with CDW from a pure superconducting phase. The superconducting order parameter in both phases has the same s-wave symmetry. In spite of the conventional phonon-mediated BCS character of the weakly correlated (Ca1−xSrx)3Ir4Sn13 system, the dependence of the effective superfluid density on the critical temperature puts this compound in the “Uemura” plot close to unconventional superconductors. This system exemplifies that conventional BCS superconductors in the presence of competing orders or multiband structure can also display characteristics of unconventional superconductors.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| Ca3Ir4Sn13 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 7 | Pressure not reported | unknown |
| Sr3Ir4Sn13 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 5 | Pressure not reported | unknown |
| Ca3Ir4Sn13 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 8.9 | 4 GPa | unknown |
| Ca3Ir4Sn13 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 6.79 | Pressure unresolved | unknown |
Similar papers
Microscopic studies of the normal and superconducting state of Ca3Ir4Sn13
similarity 0.96S. Gerber et al.
Source status unknown — claims are unverified
Electronic structure and phonon instabilities in the vicinity of the quantum phase transition and superconductivity of (Sr,Ca)3Ir4Sn13
similarity 0.96D. A. Tompsett
Source status unknown — claims are unverified
Superconducting and magnetic properties of Sr3Ir4Sn13
similarity 0.96P. K. Biswas et al.
Source status unknown — claims are unverified
Strong-coupling phonon-mediated scenario of superconductivity in Ca3Ir4Sn13 and Ca3(Ir0.91Co0.09)4Sn13
similarity 0.95Jianqiang Hou et al.
Source status unknown — claims are unverified
Pressure- and Composition-Induced Structural Quantum Phase Transition in the Cubic Superconductor (Sr,Ca)3Ir4Sn13
similarity 0.95Lina E. Klintberg et al.
Source status unknown — claims are unverified
Unconventional charge-density wave in Sr3Ir4Sn13 cubic superconductor revealed by optical spectroscopy study
similarity 0.95A. F. Fang et al.
Source status unknown — claims are unverified