2000
DOI: 10.1002/1521-396x(200009)181:1<185::aid-pssa185>3.0.co;2-g
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Transport Properties of ?-Fe1-xMnxSi2 Alloys

Abstract: The results of transport measurements on b-Fe 1Àx Mn x Si 2 alloys in the temperature range of 80 to 300 K are presented and explained assuming the existence of an impurity band. The values of the activation energies of the shallow and deep acceptors, their concentrations, the concentration of the compensating donors as well as the impurity band width were calculated.

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Cited by 3 publications
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“…22) and Mn (Ref. 25), yielding, however, less confident data (Table I). The values of ε 2 , N d , and N A2 were obtained for the β-FeSi 2 crystals grown from Zn solvent (see Table I).…”
Section: Impurity (Defect) Band Conductionmentioning
confidence: 99%
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“…22) and Mn (Ref. 25), yielding, however, less confident data (Table I). The values of ε 2 , N d , and N A2 were obtained for the β-FeSi 2 crystals grown from Zn solvent (see Table I).…”
Section: Impurity (Defect) Band Conductionmentioning
confidence: 99%
“…1(a)] and films, 22) the single crystals, both Aldoped 23) and grown from Zn solvent [Fig. 1(b)], 24) as well as the β-Fe 1−x Mn x Si 2 alloys 25) show an exponential increase of the Hall coefficient R(T) with decreasing temperature T down to ∼50-170 K. In addition, it should be mentioned a wellpronounced maximum of R(T), which implies importance of the conductivity over a band formed by shallow impurity (or defect) levels. When the concentration of shallow impurities is increased, the magnitude of the Hall coefficient maximum 22) The numbers of the curves correspond to the sample numbers (Table I).…”
Section: Impurity (Defect) Band Conductionmentioning
confidence: 99%
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