Magnetodielectric coupling and phonon properties of compressively strained EuTiO3 thin films deposited on LSAT

Abstract

Compressively strained epitaxial (001) EuTiO3 thin films of tetragonal symmetry have been deposited on (001) (LaAlO3)_0.29-(SrAl_{1/2}Ta_{1/2}O3)_0.71 (LSAT) substrates by reactive molecular-beam epitaxy. Enhancement of the Neel temperature by 1 K with 0.9% compressive strain was revealed. The polar phonons ofthe films have been investigated as a function of temperature and magnetic field by means of infrared reflectance spectroscopy. All three infrared active phonons show strongly stiffened frequencies compared to bulk EuTiO3 in accordance with first principles calculations. The phonon frequencies exhibit gradual softening on cooling leading to an increase in static permittivity. A new polar phonon with frequency near the TO1 soft mode was detected below 150 K. The new mode coupled with the TO1 mode was assigned as the optical phonon from the Brillouin zone edge, which is activated in infrared spectra due to an antiferrodistortive phase transition and due to simultaneous presence of polar and/or magnetic nanoclusters. In the antiferromagnetic phase we have observed a remarkable softening of the lowest-frequency polar phonon under an applied magnetic field, which qualitatively agrees with first principles calculations. This demonstrates the strong spin-phonon coupling in EuTiO3, which is responsible for the pronounced dependence of its static permittivity on magnetic field in the antiferromagnetic phase.

Submitted to Phys. Rev. B

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Cited by in corpus (6)

• Antiferrodistortive phase transition in EuTiO3
• Origin of giant spin-lattice coupling and the suppression of ferroelectricity in EuTiO3 from first principles
• Phonon Softening and Dispersion in EuTiO3
• Far infrared and terahertz spectroscopy of ferroelectric soft modes in thin films: A review
• Spin-phonon interaction increased by compressive strain in antiferromagnetic MnO thin films
• Magnetic resonance study of bulk and thin film EuTiO3