At ambient conditions
SrAl4 adopts the
BaAl4 structure type with space group
I4/mmm. It undergoes a charge-density-wave (CDW) transition at
TCDW=243 K, followed by a structural transition at
TS=87 K. Temperature-dependent single-crystal x-ray diffraction (SXRD) leads to the observation of incommensurate superlattice reflections at
q=σc* with
σ=0.1116 at 200 K. The CDW has orthorhombic symmetry with the noncentrosymmetric superspace group
F222(00σ)00s, where
F222 is a subgroup of
Fmmm as well as of
I4/mmm. Atomic displacements mainly represent a transverse wave, with displacements that are 90 deg out of phase between the two diagonal directions of the
I-centered unit cell, resulting in a helical wave. Small longitudinal displacements are provided by the second harmonic modulation. The orthorhombic phase realized in
SrAl4 is similar to that found in
EuAl4, except that no second harmonic could be determined for the latter compound. Electronic structure calculations and phonon calculations by density functional theory (DFT) have failed to reveal the mechanism of CDW formation. No clear Fermi surface nesting, electron-phonon coupling, or involvement of Dirac points could be established. However, DFT reveals that Al atoms dominate the density of states near the Fermi level, thus corroborating the SXRD measurements.
SrAl4 remains incommensurately modulated at the structural transition, where the symmetry lowers from orthorhombic to
b-unique monoclinic. The present work draws a comparison on the modulated structures of nonmagnetic
SrAl4 and magnetic
EuAl4 elucidating their similarities and differences, and firmly establishing that although substitution of Eu to Sr plays little to no role in the structure, the transition temperatures are affected by the atomic sizes. We have identified a simple criterion that correlates the presence of a phase transition with the interatomic distances. Only those compounds
XAl4−xGax (X=Ba, Eu, Sr, Ca; 0<x<4) undergo phase transitions, for which the ratio
c/a falls within the narrow range
2.51<c/a<2.54. Published by the American Physical Society 2024