2004
DOI: 10.1016/s0925-8388(03)00591-7
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Neutron diffraction study of the magnetic structure of α-Mn2O3

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Cited by 92 publications
(50 citation statements)
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“…Regarding magnetic ordering of the a-Mn 2 O 3 bulk phase, a neutron study has shown [13] that majority of the magnetic peaks disappear above T N~8 0 K (a similar transition temperature T N~7 9 -80 K was reported also from heat capacity measurements [14] and magnetic susceptibility and Mö ssbauer effect [15] on Mn 2-x Fe x O 3 ). According to the neutron results [13], magnetic order in the bulk a-Mn 2 O 3 can be described by a set of six collinear AFM spin arrangements on a cubic lattice. The peak at 80 K in the M(T) of the investigated b-MnO 2 nanorods can be thus associated with the magnetic ordering within the a-Mn 2 O 3 surface layer.…”
Section: Discussionsupporting
confidence: 56%
“…Regarding magnetic ordering of the a-Mn 2 O 3 bulk phase, a neutron study has shown [13] that majority of the magnetic peaks disappear above T N~8 0 K (a similar transition temperature T N~7 9 -80 K was reported also from heat capacity measurements [14] and magnetic susceptibility and Mö ssbauer effect [15] on Mn 2-x Fe x O 3 ). According to the neutron results [13], magnetic order in the bulk a-Mn 2 O 3 can be described by a set of six collinear AFM spin arrangements on a cubic lattice. The peak at 80 K in the M(T) of the investigated b-MnO 2 nanorods can be thus associated with the magnetic ordering within the a-Mn 2 O 3 surface layer.…”
Section: Discussionsupporting
confidence: 56%
“…The relative energies agree with experiment, where the orthorhombic structure is considered stable at low temperature [46,50]. The structure was only simulated in its ferromagnetic (FM) form as there is no consensus yet on its low temperature magnetic structure from experiment [56,57].…”
Section: Ii/iii) and Mno(ii) For The Manganese Oxides Insupporting
confidence: 58%
“…For their magnetic orders of cubic d-Pu and PuO 2 , our DFT + U calculations and other similar calculations by other researchers show that the collinear 1 À k antiferromagnetic (AFM) states along (1 0 0) lattice direction are energetically more favorable than nonmagnetic (NM) and ferromagnetic (FM) states. For Pu 2 O 3 , we compare the total energy of the so-called 1 À k AFM configuration (AFM-1) mentioned above and the magnetic configuration (AFM-2) proposed by Regulski et al [36]; in the latter configuration, its spin arrangements have four sublattices I, II, III and IV, as shown in Fig. 1 Total energy calculations are performed with VASP code, the projector augmented wave (PAW) method, and relativistic effective core potentials (ECPs) [37][38][39].…”
Section: Computational Detailsmentioning
confidence: 99%