Answers are grounded in this paper and cite their sources.
Using a single crystal from which nonstoichiometries have been removed, the principal susceptibilities, χ_∥ and χ_⊥, of CoO have been determined in the temperature range of 4.2 to 350 K, bracketing TN289 K. A stress {} 210 bars along [001] was applied during measurements and in cooling through TN (to remove T domains), and the initial χ was measured for →H∥[001] and →H⊥[001] at →H=250 Oe. These measured χ's are then related to χ_∥ and χ_⊥ using the known magnetic structure of CoO, from which χ_∥ and χ_⊥ at various temperatures are determined. Then, using the relation χₚ=(χ_∥+2χ_⊥)3, the calculated χₚ (powder) is found to agree well with the measured χₚ at all temperatures, thus providing a consistency check on the procedures used in this work. For T→0 K, the experimental χ_∥(0)39.5×10^-6 cm³/g. This value is about 50% higher than the only available theoretical estimate by Tachiki [although his estimates of χ_⊥ (0) and χ(TN) are in good agreement with our measured values]. Various sources for this discrepancy are examined, and it is suggested that further theoretical work is needed to explain this discrepancy as well as the observed temperature dependence of χ_∥ and χ_⊥. A comparison with the recent results of a similar study in MnO is also made.
No takes yet. Share an insight, caveat, or question.
Silinsky et al. (1981) studied this question.
Synapse has enriched 10 related papers. Consider them for comparative context: