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The classical example of magnetic structure determination by neutrons for MnO2, which has the NaCl structure. It explains the extra neutron reflections present at 80 K but not at 293 K and how they may be classified in terms of a cubic unit cell of lattice constant 8.85 Å. The document concludes that the chemical unit cell has the 4.43 Å lattice parameter, but that at 80 K the electronic magnetic moments of the Mn+2 ions are ordered in some nonferromagnetic arrangement. The document also lists experimental values of θ /T N for antiferromagnetic crystals.
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A classical example of magnetic structure determination by neutrons is shown in figure (1) for MnO 2 which has the NaCl structure. At 80 K there are extra neutron reflections not present at 293 K. The reflections at 80 K may be classified in terms of a cubic unit cell of lattice constant 8.85 Å. At 293 K the reflections correspond to an fcc unit cell of lattice constant 4.43 Å. But the lattice constant determined by x-ray reflection is 4.43 Å at both temperatures, 80 K and 293 K. We conclude that the chemical unit cell has the 4.43 Å lattice parameter, but that at 80 K the electronic magnetic moments of the Mn
ions are ordered in some nonferromagnetic arrangement. If the ordering were ferromagnetic the chemical and magnetic cells would give the same reflections. The spin arrangement shown in figure (2) is consistent with the neutron diffraction results and with magnetic measurements. The spins in a single [111] planes are parallel, but spins in adjacent [111] planes are antiparallel.
Thus, MnO is an antiferromagnetic, as shown in figure 3. In an antiferromagnet the spins are ordered in an antiparallel arrangement with zero net moment at temperatures below ordering or Neel temperature. Figure 1. Neutron diffraction patterns for MnO below and above the spin ordering temperature of 120 K, after C.G. Shull, W.A. Strauser, and E.O. Wollan. The reflection indices are based on an 8.85 Å cell at 293 K.
Figure 3. Spin ordering in ferromagnets (J>0) and antiferromagnets (J<0). The susceptibility of an antiferromagnet is not infinite at T=TN but has a weak cusp, as shown in figure (4). An antiferromagnetic is a special case of a ferrimagnet for which both sublattices A and B have equal saturation magnetizations. Thus CA = CB in the equation of susceptibility and the Neel temperature in the mean field approximation is given by Where C refers to a single sublattice. The susceptibility in the paramagnetic region T >
TN is obtained from the equation of susceptibility. χ = 2 CT − 2 μ C 2 T 2 −( μC ) 2 =^ 2 C T + μC = 2 C T + T (^) N ( 1 ) The experimental results at T > TN are of the form ( CGS ) χ = 2 C T + θ ( 2 ) Substan ce Paramagne tic Ion lattice Transition Temperatu re TN, in K Curie
Weis s θ , in K θ T (^) N χ ( 0 ) χ ( T (^) N ) MnO fcc 116 610 5.3 2/ MnS fcc 160 528 3.3 0. MnTe hex. layer 307 690 2. 5 MnF 2 bc tetr. 67 82 1. 4
FeF 2 bc tetr. 79 117 1. 8
FeCl 2 hex. Layer 24 48 2.0 <0. FeO fcc 198 570 2.9 0. CoCl 2 hex. Layer 25 38.1 1. 3 CoO fcc 291 330 1. 4