Magnetic complexity, magnetodielectric effect and DFT calculations on correlation driven Gd2CoMnO6 insulator

dc.contributor.authorPrashanth, C.H.
dc.contributor.authorReddy, I.
dc.contributor.authorTarafder, K.
dc.contributor.authorChandrasekhar Kakarla, D.
dc.contributor.authorYang, H.D.
dc.contributor.authorAdyam, V.
dc.contributor.authorJyothinagaram, K.
dc.date.accessioned2026-02-04T12:27:24Z
dc.date.issued2022
dc.description.abstractIn the family of Re<inf>2</inf>CoMnO<inf>6</inf> manganite double perovskites, in contrast to parent La<inf>2</inf>CoMnO<inf>6</inf> compound, Gd<inf>2</inf>CoMnO<inf>6</inf> exhibits multiple magnetic transitions; ferromagnetic (FM) ordering, T<inf>C</inf> ∼ 112 K followed by AFM transition, T<inf>N</inf> ∼ 47 K, Gd spins ordering for T < 10 K and large isothermal entropy changes. A study of DC field-superimposed AC magnetic susceptibility measurements revealed the field-induced magnetic glassy behavior below T<inf>C</inf> and enhancement of FM correlations above T<inf>C</inf>. From the analysis of Almeida-Thouless behavior and dynamical power-law fit to frequency dependent AC susceptibility, Gd<inf>2</inf>CoMnO<inf>6</inf> exhibits a volume spin glass-like nature below the freezing temperature, T<inf>f</inf> ∼ 117.5 K. The isothermal field-dependent magnetic and dielectric permittivity data and temperature dependent Raman measurements (reported in ref. R. X. Silva et al., J, Appl. Phys. 114 194,102 (2013)) confirms the spin-phonon coupling induced magnetodielectric effect. Further, the ground-state electronic structure and magnetic properties of Gd<inf>2</inf>CoMnO<inf>6</inf> are investigated using DFT + U formalism with Vienna Ab-initio Simulation Package (VASP) code and predicted the material to be a correlation-driven insulator. The correlation value of the Hubbard U parameter at the 4f-Gd elements changes the stability of the magnetic state from Ferri to FM spin alignment for U<inf>eff</inf> ≥ 3 eV and is correlated to the experimentally observed field-induced transformation of the short-range-order FiM/spin-glass-like phase into the long-range ordered FM phase. © 2022
dc.identifier.citationJournal of Magnetism and Magnetic Materials, 2022, 563, , pp. -
dc.identifier.issn3048853
dc.identifier.urihttps://doi.org/10.1016/j.jmmm.2022.169880
dc.identifier.urihttps://idr.nitk.ac.in/handle/123456789/22281
dc.publisherElsevier B.V.
dc.subjectCalculations
dc.subjectCobalt compounds
dc.subjectDensity functional theory
dc.subjectElectronic structure
dc.subjectFrequency modulation
dc.subjectGadolinium compounds
dc.subjectGlass
dc.subjectGlass transition
dc.subjectGround state
dc.subjectIsotherms
dc.subjectLanthanum compounds
dc.subjectMagnetic susceptibility
dc.subjectManganites
dc.subjectPermittivity
dc.subjectPerovskite
dc.subjectSpin glass
dc.subjectStrontium compounds
dc.subjectAFM
dc.subjectDFT calculation
dc.subjectDouble perovskites
dc.subjectFerromagnetic orderings
dc.subjectField-induced
dc.subjectMagnetic transitions
dc.subjectMagnetodielectric effect
dc.subjectMagnetodielectric effect and DFT calculation
dc.subjectSpin order
dc.subjectSpin-glass
dc.subjectFerromagnetism
dc.titleMagnetic complexity, magnetodielectric effect and DFT calculations on correlation driven Gd2CoMnO6 insulator

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