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首页> 外文期刊>Bulletin of the Russian Academy of Sciences. Physics >Studying the effect of biaxial anisotropy on nonlinear magnetization oscillations accompanying the 90° pulsed magnetization process in ferrite–garnet films with easy-plane anisotropy
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Studying the effect of biaxial anisotropy on nonlinear magnetization oscillations accompanying the 90° pulsed magnetization process in ferrite–garnet films with easy-plane anisotropy

机译:在具有易于平面各向异性的铁氧体 - 石榴膜中伴随90°脉冲磁化过程的双轴各向异性对非线性磁化振荡的影响

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摘要

AbstractTime dependences of the azimuthal component of the torqueTΦ(t) acting on magnetization are calculated to understand the nature of the delayed magnetization acceleration effect observed during the 90° pulsed magnetization of real ferrite–garnet films, in which biaxial anisotropy exists alongside with in-plane anisotropy. A calculation technique based on analyzing an operating point trajectory is used. Calculations show that if the effective anisotropy fieldHK2is comparable to the magnetizing pulse amplitudeHma, abruptly ascending regions at characteristic timest* in curvesTΦ(t) arise, in the limit of which nonlinear magnetization oscillations formed. The shape of these regions depends weakly on the magnetizing pulse front duration τf. This explains the reason of the weak dependence of the nonlinear magnetization oscillations on duration of the magnetizing pulse front. Calculations also show that the main features of the delayed acceleration effect are less clear upon an increase of the pulse amplitude: the behavior of curvesTΦ(t) becomes smoother near timest*, and an increase in the pulse front duration is accompanied by a stronger drop in the intensity of magnetization oscillations.]]>
机译:<![CDATA [<标题>抽象 <帕拉>转矩<重点类型=“斜体”> T <下标>φ(<重点类型)的方位角分量的时间依赖性计算作用于磁化的“斜体”> T 以了解在真正的铁氧体 - 石榴石膜的90°脉冲磁化期间观察到的延迟磁化加速度效应的性质,其中双轴各向异性与在线旁边存在各向异性。使用基于分析操作点轨迹的计算技术。计算表明,如果有效的各向异性字段<重点类型=“斜体”> H <下标> K2 则与磁化脉冲幅度<重点类型=“斜体”> H <下标> ma ,突然上升的区域在特征时代<重点类型=“斜体”> t *在曲线<重点类型=“斜体”> t <下标>φ(<强调类型=“斜体”> t ),在形成的非线性磁化振荡的极限中。这些区域的形状在磁化脉冲前持续时间τ<下标> f 上弱而取决于弱。这说明了非线性磁化振荡效果弱依赖性在磁化脉冲前沿的持续时间的原因。计算还表明,在脉冲幅度的增加时,延迟加速度效果的主要特征不太清楚:曲线的行为<重点类型=“斜体”> t <下标>φ(<重点类型=“斜体”> T )在近时更平滑<强调类型=“斜体”> T *,脉冲前持续时间的增加伴随着强度的更强下降磁化振荡。]]>

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