2,041 research outputs found

    Direct evidence for the magnetic ordering of Nd ions in NdMn2_2Si2_2 and NdMn2_2Ge2_2 by high resolution inelastic neutron scattering

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    We have investigated the low energy nuclear spin excitations in NdMn2_2Si2_2 and NdMn2_2Ge2_2 by high resolution inelastic neutron scattering. Previous neutron diffraction investigations gave ambiguous results about Nd magnetic ordering at low temperatures. The present element-specific technique gave direct evidence for the magnetic ordering of Nd ions. We found considerable difference in the process of the Nd magnetic ordering at low temperature in NdMn2_2Si2_2 and NdMn2_2Ge2_2. Our results are consistent with those of magnetization and recent neutron diffraction measurements

    Polarisation dependence of magnetic Bragg scattering in YMn2_2O5_5

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    The polarisation dependence of the intensity of elastic magnetic scattering from \ymno\ single crystals has been measured at 25 K in magnetic fields between 1 and 9 T. A significant polarisation dependence was observed in the intensities of magnetic satellite reflections, propagation vector \pv=0.5,0,0.25 measured with both the [100] and [010] axes parallel to the common polarisation and applied field direction. The intensity asymmetries AA observed in sets of orthorhombicly equivalent reflections show systematic relationships which allow the phase relationship between different components of their magnetic interaction vectors to be determined. They fix the orientation relationships between the small yy and zz moments on the \mnfp\ and \mntp\ sub-lattices and lend support to the structure reported by Kim et al. It was found that that A(hkl)≠A(hˉkˉlˉ)A(hkl)\ne A(\bar h\bar k\bar l) which suggests that there is a small modulation of the nuclear structure which has the same wave-vector as the magnetic modulation leading to a small nuclear structure factor for the satellite reflections. The differences A(hkl)−A(hˉkˉlˉ)A(hkl)- A(\bar h\bar k\bar l) observed indicate shifts in the atomic positions of order 0.005 \AA
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