共查询到19条相似文献,搜索用时 203 毫秒
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用Langevin分子动力学方法模拟磁通运动的纵向电压噪声谱随磁场和电流的变化.计算结果表明,外加磁场增大到磁通运动动力学相变场FP,电压噪声 谱中低频宽带噪声减小而出现洛伦兹形高频窄带噪声.外加磁场增大到熔化场Fm附近,高频窄带噪声 峰值增高 ,峰值对应频率增大.在外加电流增强到磁通弹性运动区域,高频窄带噪声频谱呈现搓衣板 形式.搓衣板高频窄带噪声产生于磁通平移速度的周期性调制,它表明层状超导体中运动的 磁通格子存在有平移序的BG相.
关键词:
第Ⅱ类超导体
电压噪声
动力学模拟 相似文献
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对c轴择优取向的熔融织构样品(Nd0.33Eu0.33Gd0.33) Ba2Cu3O7-δ(含Gd(211)相)的磁通跳跃现象进行 了系统研究.结果表明,在外加磁 场平行于样品c轴条件下,在2到3K的温度范围内明显观测到了部分磁通跳跃现象,而 在5K及以上温区并未出现.在磁场垂直于样品的c轴情况,在2K到Tc的整个温 区都没有观察到磁通跳跃现象.这种各向异性磁通跳跃现象可归因于各向异性钉扎力和几何 退磁因子的结果.随着温度的增加,磁通跳跃数目减少,且M(H)曲线的第三象限是磁通 跳跃的最不稳定过程.最后,研究了磁通跳跃对磁场扫描速率的依赖关系,并讨论了磁通蠕 动对磁通跳跃的影响.
关键词:
0.33Eu0.33Gd0.33)Ba2Cu3O7-δ超导体')" href="#">(Nd0.33Eu0.33Gd0.33)Ba2Cu3O7-δ超导体
OCMG方法
磁通跳跃 相似文献
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利用半导体霍尔探头测量法在液氮温度下研究了低场下圆柱状熔融织构YBa2Cu3O7-δ样品的局域磁通蠕动行为.对瞬时加减场样品端面局域磁场的磁弛豫,磁滞回线以及不同扫场速率下局域磁场的变化进行了测量,观察到了对数时间磁弛豫的行为,发现由加场和去场数据所得的激活能U0有明显的不同.磁滞回线测量中,局域点的磁场随外场几乎同步变化,不同扫场速率下局域磁场随外场变化的差别不大.实验结果表明,外场除对样品侧面外,对端面也有明显的穿
关键词:
局域磁通蠕动
激活能
磁弛豫 相似文献
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超导磁悬浮列车在加速启动的过程中,载有恒定大电流的超导线圈处在变化的磁场中,这会导致超导线圈发生磁通跳跃,从而降低线圈的载流能力.并且磁通跳跃会产生大量热量而使超导线圈温度急剧升高,严重时会导致超导线圈失超,所以对磁通跳跃的研究具有非常重要的科学意义.Nb3Sn超导线是由多根微米级的超导芯丝、铜和环氧树脂形成的复合结构.本文通过约束每根芯丝的静电流为零的二维模型来分析三维绞扭效应,研究了超导线在交变磁场和恒定电流下的磁热不稳定性行为.通过分析交变磁场的幅值和频率对Nb3Sn超导线磁通跳跃的影响,发现当磁场幅值不变时,初次发生磁通跳跃的磁场阈值Bth随频率非单调变化.而当频率一定时,初次发生磁通跳跃的磁场阈值Bth随交变磁场幅值单调变化.此外,随着幅值的减小,发生磁通跳跃的频率区间先变大后变小,直到某个临界频率后超导线不再发生磁通跳跃.本文的研究结果能够为调控超导线的磁热不稳定性行为提供理论依据. 相似文献
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借助2 MeV直线感应加速器注入器平台,利用四极质谱仪研究了碳纳米管阴极的强流脉冲发射放气质谱特性. 研究结果表明:在脉冲高压电场下,碳纳米管阴极材料释放出较多的吸附气体,解吸气体又以CO2,N2(CO),H2三种气体居多,这些解吸气体在阴极等离子体形成过程中起着重要的作用. 通过分析解吸气体成分的含量,证明碳纳米管阴极强流脉冲电子发射过程为场致等离子体发射,而不是场致爆炸发射.
关键词:
碳纳米管阴极
强流脉冲发射
质谱分析
场致等离子体发射 相似文献
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高温超导块材在零场冷条件下感应产生的涡流可以有效地屏蔽外加磁场, 从而改变空间磁场分布. 通过合理的设计, 该效应可以被用来约束、 聚集磁通, 从而增大局域磁通密度, 对于需要高磁通密度和磁场梯度的应用具有重要意义. 本论文利用基于 H 方程的二维有限元数值模拟, 结合 GdBa2Cu3 O7 -δ 材料实测的Jc (B ,T ) 关系,研究了 GdBa2Cu3 O7 -δ 超导块材的磁通汇聚效果, 分析了超导块材的空间位置、 工作温度及不同外加磁场对其磁通密度放大效果的影响. 结果显示在30 K 的温度下, 外加11 T 的外加磁场时, 可以在间距为2 mm 的两块超导块体间隙获得17.2 T 的磁场, 磁场放大效率达到56 % . 相似文献
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Wentao Liu Federico Casanova Bernhard Blümich Donglin Zu 《Applied magnetic resonance》2012,42(1):101-112
The main magnetic fields of mobile nuclear magnetic resonance (NMR) magnets differ from those of conventional NMR and magnetic
resonance imaging (MRI) magnets. In the Halbach magnet, the main field B
0 is perpendicular to the longitudinal axis, the symmetry of the current distribution with respect to the symmetry of the magnetic
field differs from that in conventional target-field applications, and the current distribution on the coil surface cannot
be expressed in terms of periodic basis functions. To obtain the winding pattern of the coil, an efficacious target-field
approach. The surface of a coil is divided into small discrete elements, where each element is represented by a magnetic dipole.
From the stream function of the elements, the resultant magnetic field is calculated. The optimization strategy follows an
objective function defined by the power dissipation or efficiency of the coil. This leads to the optimum stream function on
the coil surface, whose contour lines define the winding patterns of the coil. This paper shows winding patterns designed
of shim coils for Halbach magnet and illustrates the craft of a shim coil using flexible printed circuit board. The performance
of the coils is verified by simulating the fields they produce over the sensitive volume. 相似文献
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Y. Koyama T. Takao Y. Yanagisawa H. Nakagome M. Hamada T. Kiyoshi M. Takahashi H. Maeda 《Physica C: Superconductivity and its Applications》2009,469(13):694-701
The screening current-induced magnetic field in the (Bi,Pb)2Sr2Ca2Cu3Ox (Bi-2223) insert coil proposed for a beyond 1 GHz nuclear magnetic resonance (NMR) spectrometer may generate a long-term field drift, resulting in a loss of field-frequency lock operation and an inability to make high resolution NMR measurements. The measured screening current-induced magnetic field of a Bi-2223 double-pancake coil exhibits a hysteresis effect at 4.2 K that is reproduced by a numerical simulation based on a finite thickness rectangular superconductor bar model. The screening current-induced field at the coil center is of opposite polarity to that generated by the coil current, and thus the apparent field intensity shows a positive drift with time. On the contrary, the field at a coil end is of the same polarity as the coil field, and the apparent field intensity decreases with time. If we wait for ∼1000 h after coil excitation, the field drift rate approaches the field decay rate of the persistent current of 10−8 h−1, suitable for a long-term NMR measurement in a beyond 1 GHz NMR spectrometer. 相似文献
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R. M. Arutyunyan V. L. Ginzburg G. F. Zharkov 《Journal of Experimental and Theoretical Physics》1997,84(6):1186-1196
The question of a surface barrier which determines the behavior of a vortex in a hollow superconducting cylinder of finite
thickness in an external magnetic field is discussed, taking into account magnetic flux quantization in the cavity. The behavior
of magnetic vortices in a hollow superconductor in the presence of a thermoelectric current is also considered. Pairs of magnetic
vortices with opposite magnetic field orientations (vortex-antivortex pairs) are generated by this current near T
c. The thermoelectric current drives the antivortex (the vortex with oppositely directed field) out of the cylinder, whereas
the vortex is ejected into the cavity and remains on the inside cylinder surface as a current. The number of magnetic flux
quanta trapped inside the cylinder increases by one. The relation of this mechanism to the “giant” thermoelectric effect in
hollow superconductors is discussed.
Zh. éksp. Teor. Fiz. 111, 2175–2193 (June 1997) 相似文献
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偏转磁场的场参数H0,H2,H4常用来表示偏转系统的电子光学性质。本文从毕奥-沙伐定律出发,先得出单匝喇叭状鞍形线圈场参数的解析表达式,接着运用傅里叶谐波分析法求出当线匝具有某种分布时的场参数的解析表达式,从而建立谐波分量与场参数的直接关系,并得出一些有用的结果。可用于显象管、摄象管、雷达显示管、扫描电子显微镜、电子束曝光机等的偏转线圈设计。
关键词: 相似文献
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本文报道了当外磁场He较低时(He<4Hrm,其中Hrm是超导管的最大捕获磁场),超导管的内磁场Hi与时间及外磁场的关系可表示为H0+B0(lnt+1-exp(-t/τ)),式中B0Int与磁通蠕动有关,Bc(1-exp(-t/τ))与外磁场引起的磁通扰动有关。扰动随时间很快衰减.H0,B0及1/τ随外磁场增加,在He>Hrm时,这几个量增加较大。当直流外磁场He<1/2Hrm时,超导管可将其完全屏蔽,对交流场不能完全屏蔽,但其屏蔽效果仍优于最好的金属屏蔽筒。
关键词: 相似文献
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本文分析了放置于高Q谐振腔中的Josephson结、双结SQUID和单结超导环,当其Josephson频率ω=2eV0/h和腔的本征频率相等时,Josephson电流在一个磁通量子内可以产生多次阶梯或振荡的物理本质。指出对于Josephson结或双结SQUID,当ω=ωr时,被激发起的腔的本征振荡将反馈辐照结或SQUID,反馈场的频率作用使Josephson电流产生一般地感应台阶;而反馈场的振幅是受到外磁场调制的,当这种调制作用使反馈场振幅的空间部分与辐射场的空间部分匹配时,则引起电流在一个磁通量子内产生一系列的新的阶跃。对单结超导环,当nω=ωr时,被激发起的腔的振荡反馈辐照作用将迫使其超流电流产生周期小于φ0的振荡。
关键词: 相似文献