Spin canting

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Some antiferromagnetic materials exhibit a non-zero magnetic moment at a temperature of absolute zero. This effect is ascribed to spin canting, a phenomenon through which spins are tilted by a small angle about their axis rather than being exactly co-parallel.

Antisymmetric exchange would align spins perpendicular to each other

Spin canting is due to two factors contrasting each other: isotropic exchange would align the spins exactly antiparallel, while antisymmetric exchange arising from relativistic effects (spin-orbit coupling) would align the spins at 90° to each other. The net result is a small perturbation, the extent of which depends on the relative strength of these effects.[1]

This effect is observable in many clusters such as hematite.[2]

References

  1. ↑ Richard Winpenny (2011). Molecular Cluster Magnets. World Scientific. p. 119. ISBN 9789814322942. 
  2. ↑ "Ferromagnetism". University of California, San Diego. Retrieved 2 January 2013. 
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