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However, the exchange bias field is influenced by the magnitude andthe direction of the stress, the magnitude of biquadratic coupling field, and the angleof the ferromagnetic and antiferromagnetic easy axes.

结果表明交换偏置场依赖于外磁场的方向,而与其大小无关;此外应力场的大小和方向,双二次耦合场的大小以及铁磁和反铁磁易轴间夹角均对系统的交换偏置场有影响。

In order to clearly understand the nature of exchange bias of the FM/AFMbilayers, we first discuss the influence of the biquadratic coupling field on both thehysteresis loops and the dependence of exchange bias field on the applied magneticfield angle.

为了更加清楚地认识铁磁/反铁磁双层膜中交换偏置的本质,我们首先研究了双层膜界面中双二次耦合对磁滞回线和交换偏置场随外磁场角度变化曲线的影响。

The result shows: the maximum of the exchange bias field moves towardsthe easy axis with increasing the biquadratic coupling field or bilinear coupling field;additionally, the oscillations of the curves for the angular dependence of exchangebias field become weak and gradually resembles the sine function with increasing thebiquadratic coupling field.

结果发现:双线性耦合或双二次耦合的增加都可使交换偏置场的最大值位置向易轴方向靠近,并且双二次耦合的增加使交换偏置场随外磁场的角度变化曲线的振荡也随之减弱,变为类似于正弦函数的图象。

The apparatus use Lm336 as constant voltage source, and it been converted to constant - current source by amplification, which provide current for the Hall probe. The non-idiostatic offset circuit use the bridge method to offset the circuit. So while the magnetic density is null, the output voltage of Hall probe is null too.

仪器采用恒压源经过放大器转换为恒流源,为霍尔探头提供工作电流;不等位电势补偿电路采用桥式补偿网络,补偿电压通过调节可变电阻获得,实现霍尔电势的幅值补偿,使外磁场为零时,霍尔探头输出电势为零;磁通电路主要提供对样品的磁特性测量,它由测量线圈和积分器组成。

In rectangular microwave resonator, under the action of high frequency electro-magnetic field and inhomogeneous static magnetic field, the electron cyclotron resonance motion of the plasma electrons have been studied.

对矩形微波谐振腔中的等离子体,在高频电磁场和非均匀稳恒外磁场作用下的电子回旋共振运动进行了讨论。

The relationship between diffraction and external static magnetic field strength is non-monotonic.

其静态衍射与外磁场强度呈非单调的关系;其动态衍射的特征时间与外磁场的强度成反比,与磁性液体的浓度成正比。

Additionally disclosed is a method of fabricating a magnetic element (10) by providing a plurality of thin film layers wherein the bit end magneto-static demagnetizing fields of the thin film layers cancel the total positive coupling of the structure to obtain dual magnetic states in a zero external field.

另外还公开了一种通过提供多个薄膜层来构成一种磁性元件(10)的方法,其中单元端部静磁退磁场将抵消这种结构的全部正耦合以在零外磁场下获得双磁态。

The experiment of the auxiliary heated arc plasma generator shows that thekey arc root has contraction under the condition of having magnetic field when thekey arc root is at the edge of the cathode surface.

在辅助加热电弧等离子体发生器的实验中看到:在有外磁场的情况下,主弧弧根在阴极边缘时,弧根有收缩的迹象,而当主弧弧根在阴极中心附近时,观察不到明显的弧根收缩迹象,并拍摄到有双弧柱的图片;当关掉磁场和弧电流〓时,主弧在阴极和阳极之间稳定的燃烧,主弧弧根稳定在阴极中心附近的一点上,而且弧根没有收缩的迹象,主弧弧根亮区的直径约为6.8毫米,与弧柱段的亮区直径相差无几;因而从实验结果分析可以看出,阴极表面温度的升高,能使主弧弧根直径增大:另一方面,由于主弧弧根直径的增大(即也意味着主弧弧根截面积的增大),因而使电弧通过主弧弧根传入阴极表面的有效比热流降低,从而减少了阴极烧损。

The load carrying capacity of the ferrofluid lubricating films can be controlled directly by means of the applied magnetic field, since the viscosity of the ferrofluid increases in the case of magnetic field.

利用外加磁场可以直接调节铁磁流体润滑膜的承载能力,因为在外磁场中铁磁流体的粘度增大。

The results indicate that CEPNPs are core-shell nanostructure, the particles size is 75 nm on an average; CEPNPs magnetic fluid looks black and viscous and stable, and the viscosity of CEPNPs magnetic fluid decreases with increasing shear rate without magnetic field and increases with the applied magnetic field.

结果表明:制备的CEPNPs具有壳/内核包覆结构,平均粒径在75nm左右;以其制备的磁流体外观呈黑色粘稠状,稳定性好,在无磁场条件下磁流体粘度随转子转速的增大而减小,有外磁场时,磁流体粘度随磁场强度增大而增大。

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