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首页> 外文期刊>Journal of Applied Physics >Magnetic properties of bulk Zn_(1-x)Mn_xO and Zn_(1-x)Co_xO single crystals
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Magnetic properties of bulk Zn_(1-x)Mn_xO and Zn_(1-x)Co_xO single crystals

机译:块状Zn_(1-x)Mn_xO和Zn_(1-x)Co_xO单晶的磁性

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Manganese and cobalt-doped ZnO have been produced using a modified melt-growth technique. X-ray diffraction measurements indicate that the samples are high-quality single crystals with ω -2θ full width at half maximum values of 78 arc sec for the undoped ZnO and 252 arc sec for Zn_(1-x)Mn_xO (x=0.05). The lattice parameter of the Zn_(1-x)Mn_xO was observed to increase with Mn concentration. Transmission measurements showed systematic variations dominated by absorption from interatomic Mn~(2+) and Co~(2+) transitions. No evidence of diluted magnetic semiconductor mean-field ferromagnetic behavior was observed in any of these nominally noncarrier-doped samples. The magnetic properties instead showed paramagnetic behavior for Zn_(1-x)Mn_xO dominated by an antiferromagnetic Mn-Mn exchange interaction at low temperatures. Zn_(1-x)Co_xO showed hysteresis that was attributed to superparamagnetic Co clusters embedded in a diamagnetic ZnO matrix. It has been shown that in the bulk single-crystal form, intrinsic and noncarrier-doped Zn_(1-x)Mn_xO is not ferromagnetic; thus creative processing and doping techniques are necessary to achieve practical ferromagnetism in these materials.
机译:锰和钴掺杂的ZnO使用改进的熔体生长技术生产。 X射线衍射测量表明,样品是高质量的单晶,具有ω-2θ的全宽度,未掺杂的ZnO的一半最大值为78弧秒,而Zn_(1-x)Mn_xO的最大值为252弧秒(x = 0.05) 。观察到Zn_(1-x)Mn_xO的晶格参数随着Mn浓度的增加而增加。透射测量结果表明,系统变化主要由原子间Mn〜(2+)和Co〜(2+)跃迁的吸收引起。在任何这些标称非载流子掺杂的样品中均未观察到稀释的磁性半导体平均场铁磁行为的证据。磁性表现为在低温下以反铁磁Mn-Mn交换相互作用为主的Zn_(1-x)Mn_xO的顺磁行为。 Zn_(1-x)Co_xO显示出滞后现象,这归因于嵌入在反磁性ZnO基质中的超顺磁性Co团簇。已经表明,在块状单晶形式中,本征和非载流子掺杂的Zn_(1-x)Mn_xO不是铁磁性的。因此,创新的加工和掺杂技术对于在这些材料中实现实用的铁磁性是必不可少的。

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