系列脉冲偏磁场作用下硬磁泡的形成

实验研究了系列脉冲偏场作用下外延石榴石薄膜的硬磁泡(包括哑铃畴)的形成规律。发现系列脉冲对畴段的作用不是单次脉冲作用(软畴段硬化的物理过程)的简单迭加,而有其特有的规律性,存在着硬畴段进一步硬化及硬畴段软化的另两个物理过程。运用上述三个物理过程对实验结果作了解释。 关键词：     

面内磁场对硬磁泡形成的影响

实验研究了面内磁场对一次脉冲偏磁场作用下外延石榴石薄膜中硬磁泡形成的影响,发现存在一个使硬磁泡不再形成的临界面内磁场H_in⁰,它与材料参量有关,通过实验,运用面内磁场对条状畴的作用和枝状畴的形成,定性解释了软硬磁泡形成的分界场H_[b]随面内磁场增大、快降以及缓降这三个物理过程。 关键词：     

脉冲偏磁场作用下硬磁泡形成与温度的关系

用一次脉冲偏场法研究了外延石榴石磁泡薄膜条状畴畴壁中VBL群体形成与温度的关系。发现了与材料参量有关的临界温度T₀₂,当T>T₀₂时,硬磁泡不再形成。还发现了当T02时,VBL群体形成有两个明显不同的阶段,它们的分界温度为T₀₁。定性解释了第一个阶段的实验曲线并用双重曝光照相法揭示了两个阶段中导致软畴段硬化的运动形式的差别。 关键词：     

脉冲偏场作用下硬磁泡的形成

对低频脉冲偏场产生磁泡的过程中硬磁泡的形成条件进行了实验研究。发现硬磁泡的百分比p随着脉冲偏场强度的增加而迅速减小,同时发现存在一临界脉冲偏场强度H_po,当H_p≥H_po时,所产生的磁泡都是软磁泡。 关键词：     

脉冲偏场作用下石榴石磁泡薄膜中布洛赫线的形成

实验研究了石榴石磁泡薄膜中不同脉冲宽度下产生的硬磁畴的动态特性.结果表明：由零偏场下产生的枝状畴收缩而成的哑铃畴均逆时针转动,与产生枝状畴时所用的脉冲偏场的脉冲宽度无关.而固定直流偏场下由软畴段硬化而成的哑铃畴的转动状态,则与所用的硬化脉冲偏场的脉冲宽度有关.低脉冲宽度下硬化成的哑铃畴均逆时针转动,随硬化脉冲宽度的升高,出现混合转动向顺时针转动的过渡.由此揭示了直流偏场和脉冲偏场在石榴石磁泡薄膜中形成正、负垂直布洛赫线的作用. 关键词： 磁畴 磁泡 垂直布洛赫线     

垂直布洛赫线在畴段畴壁中的形成和消失

在不同的直流偏场下,对脉冲偏场作用后的磁泡膜中的磁畴观测结果表明:磁泡膨胀时的分枝生长往往伴随有大量垂直布洛赫线(以下称VBL)产生;它的正负与反向畴膨胀时所施加的直流偏场大小有确定关系;在幅度不太高的系列脉冲作用下畴端运动可使畴壁中形成大量VBL;足够强的脉冲偏场可使VBL消失。 关键词：     

石榴石磁泡膜中3类硬磁畴的形成方法

研究石榴石磁泡膜中硬磁畴畴壁中垂直布洛赫线的稳定性可为研制布洛赫线存储器提供有益的帮助 .3类硬磁畴的形成是研究硬磁畴稳定性的前提 .本文综述了在石榴石磁泡膜上形成硬磁畴的 2类方法———“脉冲偏场法”和“低直流偏场法” .结合文献中的典型样品 ,对用“脉冲偏场法”和“低直流偏场法”形成 3类硬磁畴的过程进行了简单介绍 .     

温度对普通硬磁泡的影响

实验研究了温度对外延石榴石磁泡薄膜中硬磁泡及其相应硬条畴的影响。发现了一个与材料参量有关的临界温度T₀当试验温度T0时,硬条畴畴壁中的VBL链在升降温后不变;而当T>T₀时,VBL链消失,所有硬磁泡都软化为正常磁泡。当畴壁中的VBL处于压缩态时,较硬的硬磁泡在较低的温度下软化。软化时,VBL消失的方式是整个VBL链的解体。 关键词：     

面内磁场中垂直布洛赫线的消失

当面内磁场大于某一阈值H_in′时,硬磁泡和硬畴段将变为正常泡和段。我们测量了不同磁泡材料的H_in′。随垂直于膜面直流偏磁场的增大,H_in′减小。观察到这种转变是一种弛豫过程,在适当条件下可以持续数秒或数十秒。采用Slonczewski和Malozemoff提出的面内场布洛赫点形核的概念对得到的实验结果做了定性的解释。 关键词：     

磁泡的动态测量

前 言 磁泡材料的畴壁迁移率和磁泡状态的测定是磁泡动态测量的两个重要内容.早先的阶梯函数响应法[1]和磁泡破灭法[2]虽然都能测量畴壁迁移率μω,但用作常规测试都不理想,并且都不能用来确定磁泡的状态. 本文所介绍的脉冲梯度场磁泡传输法[3],直接测量孤立磁泡在脉冲梯度场中的运动速度,从而测得迁移率.同时又从磁泡的运动方向确定磁泡的状态,方法简便,原理直观,所以这个方法被广泛地应用于常规测试和基础研究. 一、测量原理 1.用脉冲梯度场磁泡传输法测迁移率μω。 在梯度为　H的不均匀偏场中,磁泡将受力而沿-　H的方向运动.磁泡速度V…     

Morphological and microstructural study of L10-ordered FePt and L10-FePt/Fe ultrathin films grown by UHV e-beam evaporation technique

Ultrathin films of L1₀-ordered FePt alloy with different thickness were grown by UHV e-beam evaporation technique. In this ultrathin regime, the increase of the thickness induces a strong improvement of the magnetic properties followed by a decrease of the grain size. Starting from these hard layers, FePt/Fe/FePt trilayers with different thickness of the outermost layer have been grown. The samples show a single-phase magnetic behaviour and a strong perpendicular anisotropy thanks to the exchange-coupling that established at the soft/hard interfaces. By increasing the thickness of the outer layer, a strong reduction of the switching field distribution has been obtained with the appearance of a predominant exchange-type interaction among the magnetic grains. The morphology is characterized by well separated and elongated islands, while the magnetic pattern shows finely dispersed bubble domains.     

枝状畴的形成及分形维数计算

对于石榴石磁泡薄膜,提出了产生单个枝状畴（MBD)的“低静态偏磁场法”.MBD的形成是与其畴壁内垂直布洛赫线（VBL）的形核相联系的.随着静态偏磁场H_b从“枝状膨胀的临界偏磁场”H[d]的降低,相应的MBD的畴形变得越来越复杂,伴随有几类硬磁泡的相继形成.对MBD进行了分形研究,把线结构维数的计算应用于MBD极其弯曲的畴壁结构,定量地描述了它们的弯曲和分枝程度,并与其畴壁内VBL的形核联系起来. 关键词：     

The interaction of shockwaves with a vapour bubble in boiling histotripsy: The shock scattering effect

Boiling histotripsy is a High Intensity Focused Ultrasound (HIFU) technique which uses a number of short pulses with high acoustic pressures at the HIFU focus to induce mechanical tissue fractionation. In boiling histotripsy, two different types of acoustic cavitation contribute towards mechanical tissue destruction: a boiling vapour bubble and cavitation clouds. An understanding of the mechanisms underpinning these phenomena and their dynamics is therefore paramount to predicting and controlling the overall size of a lesion produced for a given boiling histotripsy exposure condition. A number of studies have shown the effects of shockwave heating in generating a boiling bubble at the HIFU focus and have studied its dynamics under boiling histotripsy insonation. However, not much is known about the subsequent production of cavitation clouds that form between the HIFU transducer and the boiling bubble. The main objective of the present study is to examine what causes this bubble cluster formation after the generation of a boiling vapour bubble. A numerical simulation of 2D nonlinear wave propagation with the presence of a bubble at the focus of a HIFU field was performed using the k-Wave MATLAB toolbox for time domain ultrasound simulations, which numerically solves the generalised Westervelt equation. The numerical results clearly demonstrate the appearance of the constructive interference of a backscattered shockwave by a bubble with incoming incident shockwaves. This interaction (i.e., the reflected and inverted peak positive phase from the bubble with the incoming incident rarefactional phase) can eventually induce a greater peak negative pressure field compared to that without the bubble at the HIFU focus. In addition, the backscattered peak negative pressure magnitude gradually increased from 17.4 MPa to 31.6 MPa when increasing the bubble size from 0.2 mm to 1.5 mm. The latter value is above the intrinsic cavitation threshold of –28 MPa in soft tissue. Our results suggest that the formation of a cavitation cloud in boiling histotripsy is a threshold effect which primarily depends (a) the size and location of a boiling bubble, and (b) the sum of the incident field and that scattered by a bubble.     

The size of active bubbles for the production of hydrogen in sonochemical reaction field

The sonication of aqueous solution generates microscopic cavitation bubbles that may growth and violently collapse to produce highly reactive species (i.e. OH, HO₂ and H₂O₂), hydrogen and emit light, sonoluminescence. The bubble size is a key parameter that influences the chemical activity of the system. This wok aims to study theoretically the size of active bubbles for the production of hydrogen in ultrasonic cavitation field in water using a single bubble sonochemistry model. The effect of several parameters such as frequency of ultrasound, acoustic intensity and liquid temperature on the range of sonochemically active bubbles for the production of hydrogen was clarified. The numerical simulation results showed that the size of active bubbles is an interval which includes an optimum value at which the production rate of H₂ is maximal. It was shown that the range of ambient radius for an active bubble as well as the optimum bubble radius for the production of hydrogen increased with increasing acoustic intensity and decreased with increasing ultrasound frequency and bulk liquid temperature. It was found that the range of ambient bubble radius dependence of the operational conditions followed the same trend as those reported experimentally for sonoluminescing bubbles. Comparison with literature data showed a good agreement between the theoretical determined optimum bubble sizes for the production of hydrogen and the experimental reported sizes for sonoluminescing bubbles.