Crystal structure and phonon softening in Ca3Ir4Sn13
D. G. Mazzone, S. Gerber, J. L. Gavilano, R. Sibille, M. Medarde, B., Delley, M. Ramakrishnan, M. Neugebauer, L. P. Regnault, D. Chernyshov, A., Piovano, T. M. Fernandez-Diaz, L. Keller, A. Cervellino, E. Pomjakushina, K., Conder, M. Kenzelmann

TL;DR
This study reveals a second-order structural transition in Ca3Ir4Sn13 at T* ~ 38 K, driven by phonon softening of a breathing mode of Sn12 icosahedra, combining experimental and theoretical insights.
Contribution
It provides a detailed analysis of the crystal structure change and phonon softening mechanism in Ca3Ir4Sn13 using neutron, x-ray scattering, and density functional theory.
Findings
Structural transition at T* is second-order and well described by mean-field theory.
Phonon softening of a low-energy mode causes the structural change.
The soft mode is identified as a breathing mode of Sn12 icosahedra.
Abstract
We investigated the crystal structure and lattice excitations of the ternary intermetallic stannide Ca3Ir4Sn13 using neutron and x-ray scattering techniques. For T > T* ~ 38 K the x-ray diffraction data can be satisfactorily refined using the space group Pm-3n. Below T* the crystal structure is modulated with a propagation vector of q = (1/2, 1/2, 0). This may arise from a merohedral twinning in which three tetragonal domains overlap to mimic a higher symmetry, or from a doubling of the cubic unit cell. Neutron diffraction and neutron spectroscopy results show that the structural transition at T* is of a second-order, and that it is well described by mean-field theory. Inelastic neutron scattering data point towards a displacive structural transition at T* arising from the softening of a low-energy phonon mode with an energy gap of Delta(120 K) = 1.05 meV. Using density functional…
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