Changes of the spin dynamics in perovskite and bilayer manganite
PHYSICA B 326:1-4 (2003) 500-504
Abstract:
We report a series of muSR measurements performed on single crystals of La1-x,SrxMnO3, (0 less than or equal to x less than or equal to 0.125) and on a polycrystalline bilayer manganite La2-2x Sr1+2xMn2O7 (v = 0.52). We find that the temperature dependence of the spinlattice relaxation rate is strongl, dependent on the hole doping and the associated changes in the magnetic structure. Y The systems have competing, anisotropic interactions, leading to a complex interplay of charge, spin and orbital order. This has a significant influence on the spin dynamics, both for perovskite and layered manganites. (C) 2002 Elsevier Science B.V. All rights reserved.Spin freezing and magnetic inhomogeneities in bilayer manganites
(2003)
Synthesis and Characterization of Ru‐Doped n = 1 and n = 2 Ruddlesden—Popper Manganates.
ChemInform Wiley 33:48 (2002) 7-7
Synthesis and characterization of Ru-doped n = 1 and n = 2 Ruddlesden-Popper manganates
Chemistry of Materials 14:9 (2002) 3976-3983
Abstract:
Polycrystalline samples of Sr3MnRuO7 and Sr2Mn0.5Ru0.5O4 have been synthesized and characterized by neutron diffraction, dc magnetometry, and magnetotransport measurements. They are, respectively, n = 2 and n = 1 members of the Ruddlesden-Popper (RP) An+1BnO3n+1 family; both have tetragonal (I4/mmm) symmetry and a disordered distribution of Ru and Mn over the six-coordinate sites within the perovskite layers of the RP structure. Neither compound shows long-range magnetic order at 2 K, but a spin-glass transition is observed at 16 K (n = 1) or 25 K (n = 2). In the case of the n = 2 compound only, the magnetic transition is accompanied by a reduction in the zero-field electrical conductivity. A maximum magnetoresistance of ∼8% in 14 T is found in both compounds.ChemInform Abstract: Spin, Charge, and Orbital Ordering in the B‐Site Diluted Manganates La2‐xSrxGaMnO6.
ChemInform Wiley 33:14 (2002) no-no