1986
DOI: 10.1103/physrevb.33.4706
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Magnetization ofHg1xMnet al.

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Cited by 31 publications
(23 citation statements)
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“…From our obtained results, we have noted that these features are similar to those observed for CdMnTe alloys, where the occupied Mn d states couple with the neighboring unoccupied Mn d ones and, thus, lowering the total energy . Moreover, these remarks are in agreement with the experimental results for the magnetization of these alloys …”
Section: Results and Discusssionssupporting
confidence: 89%
See 1 more Smart Citation
“…From our obtained results, we have noted that these features are similar to those observed for CdMnTe alloys, where the occupied Mn d states couple with the neighboring unoccupied Mn d ones and, thus, lowering the total energy . Moreover, these remarks are in agreement with the experimental results for the magnetization of these alloys …”
Section: Results and Discusssionssupporting
confidence: 89%
“…[19,21] Moreover, these remarks are in agreement with the experimental results for the magnetization of these alloys. [22,23] From our preliminary results, we can deduce that the HgMnTe alloys in the lower total spin configuration are energetically more favorable. However, calculations with clusters larger than the 8-atom supercell, together with a careful analysis of both the total spin configurations and the Mn-Mn interactions in these alloys, are necessary to have a precise feature of their electronic and magnetic properties.…”
Section: Results and Discusssionsmentioning
confidence: 74%
“…Anderson et al [19] proposed that the low temperature susceptibility follows a power law in temperature as T α where -1 T α 0. α is considered to be a measurement of the random nature of the spin interactions. The smaller the α is, the stronger the interaction will be.…”
Section: Resultsmentioning
confidence: 99%
“…The high-temperature expansion is valid as long as T | |, where the Curie-Weiss temperature = x 0 . In a wider temperature range, χ (T ) of random antiferromagnets is well described by 56,57 χ (T ) = aT −α , where a is a temperatureindependent constant and α < 1. Figure 9 presents room temperature dependence of (volume) magnetization M(H ) on the applied field H for selected (Zn,Co)O layers grown at 160…”
Section: Theoretical Modelingmentioning
confidence: 99%