$D$ and the Curie temperature $T_{rm C}$ Spin Wave-Stiffness Constants of Half-Metallic Ferromagnets <formula formulatype='inline'><tex Notation='TeX'>${rm Co}_{2}YZ$</tex></formula> (<formula formulatype='inline'><tex Notation='TeX'>$Y={rm Cr}$</tex></formula>, Mn, and Fe, <formula formulatype='inline'><tex Notation='TeX'>$Z={rm Ga}$</tex></formula>, Al, and Si) Heusler Alloys
首页> 外文期刊>Magnetics, IEEE Transactions on >Spin Wave-Stiffness Constants of Half-Metallic Ferromagnets ${rm Co}_{2}YZ$ ($Y={rm Cr}$, Mn, and Fe, $Z={rm Ga}$, Al, and Si) Heusler Alloys
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Spin Wave-Stiffness Constants of Half-Metallic Ferromagnets ${rm Co}_{2}YZ$ ($Y={rm Cr}$, Mn, and Fe, $Z={rm Ga}$, Al, and Si) Heusler Alloys

机译:半金属铁磁体的自旋波刚度常数 $ {rm Co} _ {2} YZ $ $ Y = {rm Cr} $ ,Mn和Fe, $ Z = {rm Ga} $

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The spin-wave stiffness constant $D$ and the Curie temperature $T_{rm C}$ for series of $L2_{1}$ phase in ${rm Co}_{2}{rm CrGa}$, ${rm Co}_{2}{rm MnGa}$, ${rm Co}_{2}{rm Mn}({rm Al}_{1-x}{rm Si}_{x})$ , ${rm Co}_{2}{rm Fe}({rm Al}_{1-x}{rm Si}_{x})$, and ${rm Co}_{2}{rm Fe}({rm Ga}_{1-x}{rm Si}_{x})$ Heusler alloys were evaluated from the thermomagnetization measurements. For the ${rm Co}_{2}{rm CrGa}$, ${rm Co}_{2}{rm MnGa}$, and ${rm Co}_{2}{rm Mn}({rm Al}_{1-x}{rm Si}_{x})$ alloys, there was a linear relation between $D$ and $T_{rm C}$ . The tendency between $D$ and $T_{rm C}$ was different from that for ${rm Co}_{2}{rm Fe}({rm Al}_{1-x}{rm Si}_{x})$ and ${rm Co}_{2}{rm Fe}({rm Ga}_{1-x}{rm Si}_{x})$ alloys, that is, $T_{rm C}$ was in the temperature r-n-negion from 1040 to 1100 K indicating weak concentration dependence, whereas $D$ was sensitive to the composition. For example, $D$ changed from 2.28 ${rm meV} cdot {rm nm}^{2}$ for $x=1$ $({rm Co}_{2}{rm FeSi})$ to 5.24 $ {rm meV} cdot {rm nm}^{2}$ for $x=0$ $({rm Co}_{2}{rm FeGa})$ in the case of ${rm Co}_{2}{rm Fe}({rm Ga}_{1-x}{rm Si}_{x})$ alloys. It was suggested that magnetic stability against the temperature of the Co-based Heusler alloys containing Fe element was governed not only by the spin-wave excitation but also by the other kinds of excitation.
机译:自旋波刚度常数 $ D $ 和居里温度 $ T_ {rm C} $ 公式> =” tex> =“ tex =” =“ TeX”> $ L2_ {1} $ 中的阶段 $ {rm Co} _ {2} {rm CrGa} $ $ {rm Co} _ {2} {rm MnGa} $ $ {rm Co} _ {2} {rm Mn}({rm Al} _ {1-x} {rm Si} _ {x})$ ,<公式Formulatype =“ inline”> $ {rm Co} _ {2} {rm Fe}({rm Al} _ {1-x} {rm Si} _ {x})$ ,和 $ {rm Co} _ {2} {rm Fe}({rm Ga} _ {1-x} {rm Si} _ {x})$ 通过热磁化测量对Heusler合金进行了评估。对于 $ {rm Co} _ {2} {rm CrGa} $ < tex Notation =“ TeX”> $ {rm Co} _ {2} {rm MnGa} $ $ {rm Co} _ {2} {rm Mn}({rm Al} _ {1-x} {rm Si} _ {x})$ 合金之间,<分子式类型之间存在线性关系=“ inline”> $ D $ $ T_ {rm C} $ $ D $ $ T_ {之间的趋势rm C} $ $ {rm Co} _ {2} {rm Fe}({rm Al } _ {1-x} {rm Si} _ {x})$ $ {rm Co} _ {2 } {rm Fe}({rm Ga} _ {1-x} {rm Si} _ {x})$ 合金,即 $ T_ {rm C} $ 的温度为rn负,从1040到1100 K,表明浓度依赖性较弱,而 $ D $ 对组成敏感。例如, $ D $ 从2.28 $ {rm meV} cdot {rm nm} ^ {2} $ 用于<公式Formulatype =“ inline”> $ x = 1 $ $({rm Co} _ {2} {rm FeSi})$ 到5.24 $ {rm meV} cdot {rm nm} ^ {2} $ 表示 $ x = 0 $ $({rm Co} _ {2} {rm FeGa})$ < / formula>(对于 $ {rm Co} _ {2} {rm Fe}({rm Ga} _ {1-x} {rm Si } _ {x})$ 合金。有人提出,含Fe元素的Co基霍斯勒合金对温度的磁稳定性不仅受自旋波激发的影响,还受其他种类激发的影响。

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