$_{1 - {rm x}} {hbox {Co}}_{rm x}$O and Zn $_{1 - {rm x}}$Co<'/> Magnetic Properties of Zn<formula formulatype='inline'><tex Notation='TeX'>$_{1 - {rm x}} {hbox {Co}}_{rm x}$</tex></formula>O Thin Films Grown by RF Magnetron Co-Sputtering in Ar and N<formula formulatype='inline'><tex Notation='TeX'>$_{2}$</tex></formula>O Atmosphere
首页> 外文期刊>Magnetics, IEEE Transactions on >Magnetic Properties of Zn$_{1 - {rm x}} {hbox {Co}}_{rm x}$O Thin Films Grown by RF Magnetron Co-Sputtering in Ar and N$_{2}$O Atmosphere
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Magnetic Properties of Zn$_{1 - {rm x}} {hbox {Co}}_{rm x}$O Thin Films Grown by RF Magnetron Co-Sputtering in Ar and N$_{2}$O Atmosphere

机译:Zn的磁性能<公式> inline“> $ _ {1-{rm x}} {hbox {Co}} _ {rm x} $ 在Ar和N中通过RF磁控管共溅射生长的O薄膜 $ _ {2} $ O气氛

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摘要

The Zn$_{1 - {rm x}} {hbox {Co}}_{rm x}$O and Zn $_{1 - {rm x}}$Co $_{rm x}$N $_{rm y}$O $_{1 -{rm y}}$ thin films were grown by RF magnetron co-sputtering, but in different sputtering gases (Ar and N$_{2}$O, respectively). X-ray diffraction analysis indicated that all the samples had $c$-axis preferred orientation, without any segregated secondary phase. UV–visible spectroscopy and X-ray photoelectron spectroscopy showed that Co$^{2 +}$ ions substituted tetrahedrally coordinated Zn$^{2 +}$ ions site for the films. The electrical and magnetic properties were investigated by the Hall effect and superconducting quantum interference device (SQUID) measurements, respectively. The Zn$_{1 - {rm x}} {hbox {Co}}_{rm x}$O had $n$-type conduction with electron concentration of 10$^{19}$ cm$^{- 3}$, and exhibited paramagnetism. Due to the charge compensation by N doping, the Zn$_{1 - {rm x}}$Co$_{rm x}$N$_{rm y}$O$_{1 -{rm y}}$ possessed large resistivity, and also presented paramagnetism, besides the film Zn$_{1 - {rm x}}$Co$_{rm x}$N$_{rm y}$O$_{1 -{rm y}}$ $({rm x} = 0.0162, {rm y} = 0.0004)$ , which possessed room temperature ferromagnetism (RTFM).
机译:Zn $ _ {1-{rm x}} {hbox {Co}} _ {rm x} $ $ _ {1-{rm x}} $ Co $ _ {rm x} $ N $ _ {rm y} $ O $ _ {1-{rm y}} $ 薄膜是通过RF磁控共溅射生长的,但薄膜的生长方式不同溅射气体(分别为Ar和N <公式> =“ inline”> $ _ {2} $ $ c $ 轴优先取向,且没有任何分离的次生相。紫外可见光谱和X射线光电子能谱显示Co $ ^ {2 +} $ 离子取代了四面体配位的Zn <薄膜的Formula Formulatype =“ inline”> $ ^ {2 +} $ 离子位点。分别通过霍尔效应和超导量子干涉仪(SQUID)测量研究了电学和磁学性质。 Zn $ _ {1-{rm x}} {hbox {Co}} _ {rm x} $ $ n $ 型传导 $ ^ {19} $ cm $ ^ {-3} $ ,并展示顺磁性。由于通过N掺杂进行电荷补偿,因此Zn <配方公式type =“ inline”> $ _ {1-{rm x}} $ $ _ {rm x} $ N <公式Formulatype =“ inline”> $ _ {rm y } $ O $ _ {1-{rm y}} $ 除了薄膜Zn $ _ {1-{rm x}} $ Co <公式Formulatype =“ inline”> $ _ {rm x} $ N <公式Formulatype =“ inline”> $ _ { rm y} $ O $ _ {1-{rm y}} $ <公式具有室温铁磁性(RTFM)的Formulatype =“ inline”> $({rm x} = 0.0162,{rm y} = 0.0004)$

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