Crystal structure and electronic properties of Ca4Mn2TiO9.93, an n=3 Ruddlesden-Popper compound

J MATER CHEM 11:1 (2001) 160-167

Authors:

PD Battle, SJ Blundell, AI Coldea, EJ Cussen, MJ Rosseinsky, J Singleton, LE Spring, JF Vente

Abstract:

Traditional solid state synthetic methods were used to prepare a polycrystalline sample of the n = 3 Ruddlesden-Popper phase Ca4Mn2TiO9.93. The crystal structure (space group Pbca, a = 5.31411(5), b = 5.31148(5), c = 26.9138(2)Angstrom) was determined by the simultaneous analysis of neutron and X-ray diffraction data, with near-edge anomalous scattering being used to provide contrast between Mn and Ti cations. The latter show a small preference for the octahedral sites at the centre of the three-layer perovskite blocks within the structure. Neutron diffraction data collected at 5 K show no evidence for long-range magnetic ordering, although an enhanced magnetisation with a weak remanence is observed at low temperature; this is ascribed to the presence of antisymmetric exchange interactions. Ca4Mn2TiO9.93 is a semiconductor with a temperature-dependent activation energy of similar to 100 meV. Only weak (rho (B)/rho (0) > 0.9 in 14 T at 75 K) magnetoresistance was observed.

Enhancement of the magnetoresistance at the curie temperature of the ferromagnetic insulator La1.5Sr0.5MnRhO6

Physical Review B - Condensed Matter and Materials Physics 62:10 (2000) R6077-R6080

Authors:

AI Coldea, IM Marshall, SJ Blundell, J Singleton, LD Noailles, PD Battle, MJ Rosseinsky

Abstract:

We report a study of the magnetic and electrical properties of the ferromagnetic insulator La1.5Sr0.5MnRhO6. A significant magnetoresistance is found in this system which is largest at the Curie temperature (Tc) even though there is no metal-insulator transition. The electrical transport is found to be activated above Tc and described by a variable range hopping law below Tc. Above Tc the carriers are magnetic polarons with a size which increases as the temperature approaches the magnetic transition. Rh substitution preserves ferromagnetic ordering, in contrast with the effect of other dopants on the B sites, but modifies the electrostatic potential leading to carrier localization. We attribute the peak in the magnetoresistance at Tc to the field-induced suppression of critical spin fluctuations which modulate the energetic barriers seen by the carriers.

Rapid synthesis of colossal magnetoresistance manganites by microwave dielectric heating

Chemical Communications Royal Society of Chemistry (RSC) 0:2 (2000) 159-160

Authors:

Kay E Gibbons, Martin O Jones, Stephen J Blundell, Amalia I Mihut, Ian Gameson, Peter P Edwards, Yuzuru Miyazaki, Neil C Hyatt, Adrian Porch

Magnetotransport studies on the Ruddlesden Popper phases Sr2RMn2O7 (R = Nd, Pr, Ho, Y) and Sr2-xNd1+xMn2O7 (x = 0, 0.1, 0.2, 0.5)

Journal of Physics Condensed Matter IOP Publishing 11:46 (1999) 9053

Authors:

AI Coldea, LE Spring, SJ Blundell, J Singleton, W Hayes

Structural Chemistry and Electronic Properties of the n = 3 Ruddlesden−Popper Phases Ca4Mn2FeO9.75 and Sr4Mn2FeO9.80

Chemistry of Materials American Chemical Society (ACS) 11:3 (1999) 674-683

Authors:

PD Battle, WR Branford, A Mihut, MJ Rosseinsky, J Singleton, J Sloan, LE Spring, JF Vente