Structure and superconductivity of YSr2Cu3O7-d

PHYSICA C 341 (2000) 605-606

Authors:

E Gilioli, PG Radaelli, A Gauzzi, F Licci, M Marezio

ChemInform Abstract: Phase Segregation in Manganese Perovskites

ChemInform Wiley 30:41 (1999) no-no

Authors:

PG Radaelli, DN Argyriou, DE Cox, L Capogna, H Casalta, K Andersen, S‐W Cheong, JF Mitchell, M Marezio

Spatial cross-over of polarons across the CMR transition in La0.75Ca0.25MnO3 system.

J Synchrotron Radiat 6:Pt 3 (1999) 776-778

Authors:

A Lanzara, F Natoli, NL Saini, A Bianconi, PG Radaelli

Transition from itinerant to polaronic conduction in La1-xSrxCoO3 perovskites

Europhysics Letters 45:3 (1999) 399-405

Authors:

R Caciuffo, J Mira, J Rivas, MA Señarís-Rodríguez, PG Radaelli, F Carsughi, D Fiorani, JB Goodenough

Abstract:

Neutron diffraction and small-angle scattering on La1-xSrxCoO3 (0 < x ≤ 0.30) show that for x = 0.3 the system is near a two-phase percolation threshold and undergoes a transition from itinerant to polaronic conduction at the Curie temperature TC-The stabilization of superparamagnetic clusters on warming through TC is revealed by an anomalous thermal expansion of the volume and a deviation of the paramagnetic susceptibility from the Curie-Weiss law. The development of a temperature-dependent small-angle-scattering signal confirms that regions of short-range ferromagnetic order are present above TC.

Lattice effects and magnetic structure in the layered colossal magnetoresistance manganite La2-2xSr1+2xMn2O7, x = 0.3

Physical Review B - Condensed Matter and Materials Physics 59:13 (1999) 8695-8702

Authors:

DN Argyriou, JF Mitchell, PG Radaelli, HN Bordallo, DE Cox, M Medarde, JD Jorgensen

Abstract:

We report on the temperature dependence of the crystal and magnetic structure of the layered colossal magnetoresistive manganite, La2-2xSr1+2xMn2O7, x = 0.3. Neutron-diffraction measurements show that the insulator-metal (IM) transition (TIM) at 100 K is accompanied by a ferromagnetic (FM) ordering of spins within MnO6 bilayers (intrabilayer coupling), but with an antiferromagnetic coupling between neighboring bilayers (interbilayer coupling). Below TIM, the Mn spins rotate from 45° inclination to the c axis until they are almost parallel to the c axis at 5 K. Coincident with this spin reorientation, a FM c axis component develops below 75 K. Evidence from both neutron and synchrotron x-ray-diffraction experiments suggest that the FM c-axis magnetic moment results from a second layered manganite phase with composition 0.3≲x≲0.32. This observation emphasizes the need for thorough examination of the homogeneity when measuring bulk properties (e.g., magnetization, transport) of nominally x=0.3 samples. Associated with the electronic and magnetic transitions, a pronounced lattice response along the c axis (observed in both phases) signals a transfer of charge into dx2-y2 orbitals in the low-temperature phase. That the lattice effects here are opposite in sign to those observed in the x=0.4 layered manganite points to the sensitivity of the spin-lattice-charge coupling to dopant concentration in these reduced-dimensionality manganites. © 1999 ThAmerican Physical Society.