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Ferromagnetic and antiferromagnetic ordering in the wurtzite-type diluted magnetic semiconductors

机译:纤锌矿型稀磁半导体中的铁磁和反铁磁有序

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摘要

We determined the magnetic symmetry groups (Shubnikov groups) of the wurtzite-type crystals doped with magnetic atoms periodically distributed at cation sites. The magnetic groups of doped crystals with ferro- or antiferromagnetic properties arise from the P6 _3mc (C _(6v) ~4), P3m1 (C _(3v) ~1), C _s ~3 (Cm) or C _1 ~1 (P1) ordinary space groups. Those arising from the P6 _3mc or P3m1 group can present macroscopic ferromagnetic polarization only along the wurtzite symmetry axis whereas those arising from the C _s ~3 (Cm) group can present ferromagnetic polarization only in the symmetry plane and those arising from the C _1 ~1 (P1) group can present polarization along any direction. Actual structures do not keep in general long-range order for magnetic atom distribution but the samples with macroscopic polarization should present local symmetries close to those listed above. Therefore, orientation of easy magnetization can provide information about the most frequent local symmetry.
机译:我们确定了周期性地分布在阳离子部位的掺杂了磁原子的纤锌矿型晶体的磁对称基团(Shubnikov基团)。具有铁磁性或反铁磁性的掺杂晶体的磁性基团来自P6 _3mc(C _(6v)〜4),P3m1(C _(3v)〜1),C ss〜3(Cm)或C _1〜1 (P1)普通空间群。由P6 _3mc或P3m1组产生的那些只能沿纤锌矿对称轴呈现宏观铁磁极化,而由C _s〜3(Cm)组产生的那些只能在对称平面呈现铁磁极化,而由C _1〜产生的铁磁极化。 1(P1)组可以沿任何方向出现极化。实际的结构不会保持原子原子分布的一般长距离顺序,但是具有宏观极化的样本应具有接近于上面列出的局部对称性。因此,容易磁化的方向可以提供有关最频繁的局部对称性的信息。

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