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Suppression of ferromagnetism due to hole doping in grown by molecular-beam epitaxy
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10.1063/1.2130387
/content/aip/journal/apl/87/19/10.1063/1.2130387
http://aip.metastore.ingenta.com/content/aip/journal/apl/87/19/10.1063/1.2130387
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

(Color online) Nitrogen concentration (circle), hole concentration (triangle) (vertical axis on the left) and activation ratio of holes (square) (vertical axis on the right) are plotted as a function of Cr composition for a series of the samples which were grown under different Cr flux and the same nitrogen doping condition. was estimated from the lattice parameter assuming Vegard’s law and was deduced from Hall measurement at room temperature.

Image of FIG. 2.
FIG. 2.

(Color online) The temperature dependence of the electric resistivity of with various . These samples are of the same series as in Fig. 1.

Image of FIG. 3.
FIG. 3.

(Color online) curves of undoped (No. 0) and -doped (Nos. 1–3) . (Sample No. 3 is the same as the one plotted in Figs. 1 and 2.) The measurements were performed at 2 K with magnetic fields applied perpendicular to the film plane.

Image of FIG. 4.
FIG. 4.

(Color online) (a)–(c) curves in undoped and -doped with (a) , (b) , and (c) . (-doped samples are the same as those plotted in Figs. 1 and 2.) (d) The magnetic-field dependence of the MCD signal intensity at around 2.3 eV of the same samples as in (c). All these measurements were performed at 2 K with magnetic fields applied perpendicular to the film plane.

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/content/aip/journal/apl/87/19/10.1063/1.2130387
2005-11-04
2014-04-19
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Suppression of ferromagnetism due to hole doping in Zn1−xCrxTe grown by molecular-beam epitaxy
http://aip.metastore.ingenta.com/content/aip/journal/apl/87/19/10.1063/1.2130387
10.1063/1.2130387
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