Abstract

The temperature dependence of electrical resistivity, ρ, of ceramic La0.7Ca0.3−x K x MnO3 (x = 0.05, 0.1) is investigated in metallic and semi-conducting phase. The metallic resistivity is attributed to be caused by electron–phonon, electron–electron and electron–magnon scattering. Substitutions affect average mass and ionic radii of A–site resulting in an increase in Debye temperature θ D attributed to hardening of lattice with K doping. The optical phonon modes shift gradually to lower mode frequencies leading to phonon softening. Estimated resistivity compared with reported metallic resistivity, accordingly ρ diff. = [ρ exp. − {ρ 0 + ρ e−ph (=ρ ac + ρ op)}], infers electron–electron and electron–magnon dependence over most of the temperature range. Semi-conducting nature is discussed with variable range hopping and small polaron conduction model. The decrease in activation energies and increase in density of states at the Fermi level with enhanced Ca doping is consistently explained by cationic disorder and Mn valence.

Highlights

  • IntroductionThe unique properties of mixed-valence manganites as La1-xAxMnO3 (A = Na, K, Rb) depend mainly on the relative amount of Mn3?

  • The unique properties of mixed-valence manganites as La1-xAxMnO3 (A = Na, K, Rb) depend mainly on the relative amount of Mn3? and Mn4? ions

  • We first retrace the experimental data with q0 as the free parameter, and contribution from acoustic and optical phonons together with the residual resistivity is compared to the reported data and the difference is analysed in the light of electron–electron and electron–magnon scattering mechanisms

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Summary

Introduction

The unique properties of mixed-valence manganites as La1-xAxMnO3 (A = Na, K, Rb) depend mainly on the relative amount of Mn3? Raman, infrared spectroscopy and neutron inelastic scattering measurements had obtained the most convincing evidence for the phonons and structural properties related to phase transition. Raman spectroscopy measurement of La0.7Ca0.3-xKxMnO3 (x = 0.05, 0.1) confirmed the structural lattice disorder with orthorhombic to rhombohedral structure and identified three peaks. The La0.7Ca0.3-xKxMnO3 manganites show an orthorhombic structure with space group Pnma for (x = 0.05) and rhombohedral structure with space group R 3"C for (x = 0.1) and illustrate a metallic behaviour below a temperature referred as metal–insulator transition temperature (TMI) and behave like a semiconductor above that temperarture. For La0.7Ca0.3-xKxMnO3, TMI enhances with the increased K doping concentration and is 269 (275) K for x = 0.05 (0.1) [5]

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