J Phys Condens Matter
May 2018
The Tb (4f ) crystal-field (CF) excitations and the infrared phonons in TbMnO are studied as a function of temperature and under an applied magnetic field. The phonon energy shifts reflect local displacement of the oxygen ions that contribute to the CF energy level shifts below 120 K and under magnetic field. The CF polarized transmission spectra provide interesting information about the debated nature of the excitations at 41, 65, 130 cm.
View Article and Find Full Text PDFIn this paper, we present a detailed Raman study of the non-multiferroic compounds PrMnO and NdMnO and the multiferroic compounds TbMnO and DyMnO as a function of temperature and magnetic field. All studied systems show anomalous phonon shifts close to the Néel transition T . In PrMnO and NdMnO , the frequency softenings are partly attributed to an orbital-spin-phonon coupling whereas in TbMnO and DyMnO , the relatively weak frequency shifts are rather attributed to an expansion of the Mn-O bond lengths.
View Article and Find Full Text PDFJ Phys Condens Matter
November 2016
First-order Raman scattering and multiphonons are studied in RVO3 (R = Ho and Y) as a function of temperature in the orthorhombic and monoclinic phases. Raman spectra of HoVO3 and YVO3 unveil similar features since both compounds have nearly identical R-radii. However, the most important difference lies in the transition temperature involving the V(3+) orbitals, the V(3+) magnetic moments as well as the crystallographic structure.
View Article and Find Full Text PDFWe have studied the Raman and infrared spectral response of TbMn2O5 under an applied magnetic field parallel to the easy magnetic a-axis at 4.2 K. Strong spin-lattice coupling in TbMn2O5 is evidenced by a frequency shift of Raman and infrared phonons as a function of magnetic field compared to the phonon response of BiMn2O5 that remains unaffected.
View Article and Find Full Text PDFJ Phys Condens Matter
November 2013
In hexagonal DyMnO3, Dy(3+) crystal-field excitations are studied as a function of temperature and applied magnetic field. They are complemented with the measurements of infrared active phonon frequency shifts under applied magnetic field at T = 4.2 K.
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