Electric field switching of antiferromagnetic domains in YMn2O5: a probe of the multiferroic mechanism

(2008)

Authors:

PG Radaelli, LC Chapon, A Daoud-Aladine, C Vecchini, PJ Brown, T Chatterji, S Park, S-W Cheong

The commensurate phase of multiferroic HoMn2O5 studied by X-ray magnetic scattering

(2008)

Authors:

G Beutier, A Bombardi, C Vecchini, PG Radaelli, S Park, S-W Cheong, LC Chapon

The commensurate phase of multiferroic HoMn2O5 studied by X-ray magnetic scattering

ArXiv 0803.3779 (2008)

Authors:

G Beutier, A Bombardi, C Vecchini, PG Radaelli, S Park, S-W Cheong, LC Chapon

Abstract:

The commensurate phase of multiferroic HoMn2O5 was studied by X-ray magnetic scattering, both off resonance and in resonant conditions at the Ho-L3 edge. Below 40 K, magnetic ordering at the Ho sites is induced by the main Mn magnetic order parameter, and its temperature dependence is well accounted for by a simple Curie-Weiss susceptibility model. A lattice distortion of periodicity twice that of the magnetic order is also evidenced. Azimuthal scans confirm the model of the magnetic structure recently refined from neutron diffraction data for both Mn and Ho sites, indicating that the two sublattices interact via magnetic superexchange.

Crystal and magnetic structure of (La0.70Ca0.30)(CryMn1-y)O3: a neutron powder diffraction study

(2008)

Authors:

L Capogna, A Martinelli, MG Francesconi, PG Radaelli, J Rodriguez Carvajal, O Cabeza, M Ferretti, C Castellano, T Corridoni, N Pompeo

Crystal and magnetic structure of (La0.70Ca0.30)(CryMn1-y)O3: a neutron powder diffraction study

ArXiv 0801.4683 (2008)

Authors:

L Capogna, A Martinelli, MG Francesconi, PG Radaelli, J Rodriguez Carvajal, O Cabeza, M Ferretti, C Castellano, T Corridoni, N Pompeo

Abstract:

The crystal and magnetic structure of (La0.70Ca0.30)(CryMn1-y)O3 for y = 0.70, 0.50 and 0.15 has been investigated using neutron powder diffraction. The three samples crystallize in the Pnma space group at both 290 K and 5 K and exhibit different magnetic structures at low temperature. In (La0.70Ca0.30)(Cr0.70Mn0.30)O3, antiferromagnetic order with a propagation vector k = 0 sets in. The magnetic structure is Gx, i.e. of the G-type with spins parallel to the a-axis. On the basis of our Rietveld refinement and the available magnetisation data, we speculate that only Cr3+ spins order, whereas Mn4+ act as a random magnetic impurity. In (La0.70Ca0.30)(Cr0.50Mn0.50)O3 the spin order is still of type Gx, although the net magnetic moment is smaller. No evidence for magnetic order of the Mn ions is observed. Finally, in (La0.70Ca0.30)(Cr0.15Mn0.85)O3 a ferromagnetic ordering of the Mn spins takes place, whereas the Cr3+ ions act as random magnetic impurities with randomly oriented spins.