TY - JOUR
T1 - Lattice dynamics and magnetic exchange interactions in
T2 - A spinel with pyrochlore lattice
AU - Pramanik, Prativa
AU - Singh, Sobhit
AU - Chowdhury, Mouli Roy
AU - Ghosh, Sayandeep
AU - Sathe, Vasant
AU - Rabe, Karin M.
AU - Vanderbilt, David
AU - Seehra, Mohindar S.
AU - Thota, Subhash
N1 - Funding Information:
Office of Naval Research Department of Science and Technology, Ministry of Science and Technology
Funding Information:
S.S., K.M.R., and D.V. acknowledge the support from Office of Naval Research (ONR) Grants No. N00014-16-1-2951 and No. N00014-19-1-2073. P.P. and S.G. acknowledge the FIST program of the Department of Science and Technology, India for partial support of this work (References No. SR/FST/PSII-020/2009 and No. SR/FST/PSII-037/2016).
Publisher Copyright:
© 2021 American Physical Society
PY - 2021/7/1
Y1 - 2021/7/1
N2 - is a unique system in the family of cobalt spinels (= Sn, Ti, Ru, Mn, Al, Zn, Fe, etc.) in which magnetic Co ions stabilize on the pyrochlore lattice exhibiting a large degree of orbital frustration. Due to the complexity of the low-temperature antiferromagnetic (AFM) ordering and long-range magnetic exchange interactions, the lattice dynamics and magnetic structure of a spinel have remained puzzling. To address this issue, here we present theoretical and experimental investigations of the highly frustrated magnetic structure, and the infrared (IR) and Raman-active phonon modes in the spinel , which exhibits an AFM ordering below the Néel temperature K and an associated cubic () to tetragonal () structural phase transition whose location at vs at a lower K is controversial. Our density functional theory () calculations reveal that one needs to consider magnetic-exchange interactions up to the third-nearest neighbors to get an accurate description of the low-temperature AFM order in . At room temperature, three distinct IR-active modes () are observed at frequencies 680, 413, and 325 along with four Raman-active modes (1), (2), and at frequencies 760, 647, 550, and 308 , respectively, which match reasonably well with our calculated values. All the IR-active and Raman-active phonon modes exhibit signatures of moderate spin-phonon coupling. The temperature dependence of various parameters, such as the shift, width, and intensity, of the Raman-active modes is also discussed. Noticeable changes around K and K are observed in the Raman line parameters of the and (1) modes, which are associated with the modulation of the Co-O bonds in octahedra during the excitations of these modes.
AB - is a unique system in the family of cobalt spinels (= Sn, Ti, Ru, Mn, Al, Zn, Fe, etc.) in which magnetic Co ions stabilize on the pyrochlore lattice exhibiting a large degree of orbital frustration. Due to the complexity of the low-temperature antiferromagnetic (AFM) ordering and long-range magnetic exchange interactions, the lattice dynamics and magnetic structure of a spinel have remained puzzling. To address this issue, here we present theoretical and experimental investigations of the highly frustrated magnetic structure, and the infrared (IR) and Raman-active phonon modes in the spinel , which exhibits an AFM ordering below the Néel temperature K and an associated cubic () to tetragonal () structural phase transition whose location at vs at a lower K is controversial. Our density functional theory () calculations reveal that one needs to consider magnetic-exchange interactions up to the third-nearest neighbors to get an accurate description of the low-temperature AFM order in . At room temperature, three distinct IR-active modes () are observed at frequencies 680, 413, and 325 along with four Raman-active modes (1), (2), and at frequencies 760, 647, 550, and 308 , respectively, which match reasonably well with our calculated values. All the IR-active and Raman-active phonon modes exhibit signatures of moderate spin-phonon coupling. The temperature dependence of various parameters, such as the shift, width, and intensity, of the Raman-active modes is also discussed. Noticeable changes around K and K are observed in the Raman line parameters of the and (1) modes, which are associated with the modulation of the Co-O bonds in octahedra during the excitations of these modes.
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U2 - 10.1103/PhysRevB.104.014433
DO - 10.1103/PhysRevB.104.014433
M3 - Article
AN - SCOPUS:85111685661
SN - 0163-1829
VL - 104
JO - Physical Review B-Condensed Matter
JF - Physical Review B-Condensed Matter
IS - 1
M1 - 014433
ER -