Abstract

Polycrystalline LiGa2Ir has been prepared by a solid state reaction method. A Rietveld refinement of powder x-ray diffraction data confirms a previously reported Heusler-type crystal structure (space group Fm-3m, No. 225) with lattice parameter a = 6.0322(1) Å. The normal and superconducting state properties were studied by magnetic susceptibility, heat capacity, and electrical resistivity techniques. A bulk superconductivity with Tc = 2.94 K was confirmed by detailed heat capacity studies. The measurements indicate that LiGa2Ir is a weak-coupling type-II superconductor ({uplambda }e–p = 0.57, {Delta }C/{upgamma }Tc = 1.4). Electronic structure, lattice dynamics, and the electron–phonon interaction are studied from first principles calculations. Ir and two Ga atoms equally contribute to the Fermi surface with a minor contribution from Li. The phonon spectrum contains separated high frequency Li modes, which are seen clearly as an Einstein-like contribution in the specific heat. The calculated electron–phonon coupling constant {uplambda }e–p = 0.68 confirms the electron–phonon mechanism for the superconductivity. LiGa2Ir and recently reported isoelectronic LiGa2Rh are the only two known representatives of the Heusler superconductors with the valence electron count VEC = 16.

Highlights

  • The Powder x-ray diffraction (pXRD) analysis indicates an excellent quality of the examined sample and the refinement confirms that the compound crystallizes in the cubic L21 crystal structure

  • The refined lattice parameter a = 6.0322(1) Å is in a good agreement with the previously reported for ­LiGa2Ir36,37 and slightly larger than refined for ­LiGa2Rh (a = 5.9997(8) Å)[26]

  • L­ iGa2Ir forms in a fullHeusler crystal structure type with a refined lattice parameter a = 6.0322(1) Å, in agreement with that reported by Czybulka, et al in ref. 36,37

Read more

Summary

Introduction

Phonon spectrum (n = 4 Since the Einstein term in in our case gives no contribution to the specific heat at low temperatures, adopting to the combined model (i.e. changing to n = 3) we get ΘD = 252 K, very close to the value obtained from the fit for the broad temperature range.

Results
Conclusion
Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call