Soft phonon and the central peak at the structural phase transition in SrTiO<sub>3</sub>

ORAL

Abstract

The continuous displacive phase transition in SrTiO3 near Tc ≈ 105 K is characterized by a central elastic peak observed in neutron-scattering experiments above Tc, i.e., before the associated soft phonon mode becomes overdamped upon cooling. The origin of this central peak remains unresolved. Here we present inelastic x-ray scattering results on the cubic-to-tetragonal phase transition in SrTiO3. We quantitatively compare the soft phonon mode and central peak in two differently grown SrTiO3 samples with well-characterized defect concentrations and discuss the results in relation to thermodynamic and transport probes such as specific heat and thermal conductivity. Our results show that the soft mode evolves similarly in both samples, although the central peak intensity differs by a factor of four, suggesting that the local crystal properties that are insensitive to the collective lattice excitations are likely responsible for the central elastic line in SrTiO3. High momentum and milli-electronvolt energy resolution of our inelastic x-ray sacattering measurements allow us to separate the elastic intensity of the central peak from low-energy quasielastic phonon scattering, revealing anisotropic correlation lengths on cooling toward Tc.

Publication: A. Maity, K. Habicht, M. Merz, A. H. Said, C. Guguschev, D. Kojda, B. Ryll, J.-E. Hoffmann, A. Dittmar, T. Keller, and F. Weber, Soft phonon and the central peak at the cubic-to-tetragonal phase transition in SrTiO3, Phys. Rev. B 111, 134108 (2025).

Presenters

  • Avishek Maity

    • Oak Ridge National Laboratory

Authors

  • Avishek Maity

    • Oak Ridge National Laboratory
  • Klaus Habicht

    • Department Dynamics and Transport in Quantum Materials, Helmholtz-Zentrum Berlin für Materialien und Energie, Hahn-Meitner-Platz 1, D-14109 Berlin, Germany
  • Michael Merz

    • Institute for Quantum Materials and Technologies, Karlsruhe Institute of Technology, Kaiserstr. 12, D-76131 Karlsruhe, Germany
  • Ayman H Said

    • Advanced Photon Source, Argonne National Laboratory, Lemont, Illinois 60439, USA
  • Christo Guguschev

    • Leibniz-Institut für Kristallzüchtung, Max-Born-Straße 2, D-12489 Berlin, Germany
  • Danny Kojda

    • Department Dynamics and Transport in Quantum Materials, Helmholtz-Zentrum Berlin für Materialien und Energie, Hahn-Meitner-Platz 1, D-14109 Berlin, Germany
  • Britta Ryll

    • Department Dynamics and Transport in Quantum Materials, Helmholtz-Zentrum Berlin für Materialien und Energie, Hahn-Meitner-Platz 1, D-14109 Berlin, Germany
  • Jan-Ekkehard Hoffmann

    • Department Dynamics and Transport in Quantum Materials, Helmholtz-Zentrum Berlin für Materialien und Energie, Hahn-Meitner-Platz 1, D-14109 Berlin, Germany
  • Andrea Dittmar

    • Leibniz-Institut für Kristallzüchtung, Max-Born-Straße 2, D-12489 Berlin, Germany
  • Thomas Keller

    • Max Planck Society Outstation at the Heinz Maier-Leibnitz Zentrum (MLZ), D-85748 Garching, Germany
  • Frank A Weber

    • Institute for Quantum Materials and Technologies, Karlsruhe Institute of Technology, Kaiserstr. 12, D-76131 Karlsruhe, Germany