磁性d波超导体,ferromagnetic d-wave superconductor,音标,读音,翻译,英文例句,英语词典

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1) ferromagnetic d-wave superconductor 点击朗读

磁性d波超导体

2) FdS/FdS junction 点击朗读

双层磁性d波超导结

It is found that the Josephson critical currents in FdS/FdS junction depend to a great extent on the relative orientation of the effective exchange field of the two S electrodes,and the crystal orientation of the FdS.

通过计算双层磁性d波超导结界面势垒散射效应,研究了双层磁性d波超导结中Josephson临界电流随温度、磁交换能以及势垒强度的变化关系。

更多例句>>

3) d-wave superconductor 点击朗读

d波超导体

Using the square barrier to describe the insulating layer,tunneling conductance in normal metal/insulator/d-wave superconductor c-axis tunneling junction is studied theoretically as a function of the bias voltage,insulating layer barrier strength and insulating layer thickness.

以方势垒描述绝缘层,对N/I/d波超导体c轴隧道结的微分电导进行了研究。

A number of experimental studies revealed that the order parameter in high-Tc cuprates is of d-wave symmetry, and thus the properties of d-wave superconductors have been investigated theoretically for many years.

因而许多理论工作者对d波超导体的性质进行了多年研究。

更多例句>>

4) ferromagnetic s-wave superconductor 点击朗读

磁性s波超导体

5) d-wave superconductor 点击朗读

d波超导

Zeeman Effects on the differential conductance in normal-metal/d-wave superconductor tunnel junctions;

塞曼效应对正常金属/d波超导结中微分电导的影响

We solve self-consistent equation for the d-wave superconducting gap and the Zeeman energy in the mean-field approximation under a Zeeman magnetic on the d-wave superconductor,study the Zeeman effects on the d-wave superconducting gap and the thermodynamic potential,and discuss the condition of coexistence for ferromagnetism and superconductivity.

通过外加Zeeman磁场在d波超导中,在平均场近似下,自洽求解d波超导能隙和Zeeman能量的方程,研究了Zeeman效应对d波超导序参数和热力学势的影响,阐述了磁性与超导共存条件。

Taking into account the scattering effect of the insulator in normal metal-insulator-d-wave superconductor junctions, and using the Bogoliubov-de Gennes equation and the Blonder-Tinkham-Klapwijk model, we calculate the differential conductance and shot noise.

在正常金属绝缘层 d波超导隧道结中 ,考虑到绝缘层的势垒散射效应 ,运用Bogoliubov deGennes方程和Blonder Tinkham Klapwijk理论模型 ,计算系统的微分电导和散粒噪声随偏压的变化关系。

更多例句>>

6) magnetic superconductor 点击朗读

磁性超导体

The single phase magnetic superconductors RESr 2RuCu 2O 8 (RE=Gd and Eu) were successfully synthesized and the investigations on their physical properties were carried out.

报道了磁性超导体RESr2 RuCu2 O8(RE =Gd和Eu)单相样品的合成以及对其结构和物性的研究。

补充资料：磁性材料2．薄膜磁性材料

磁性材料2．薄膜磁性材料
Magnetie Materials 2.Thin Film

在一定外加磁场作用下，其反磁化畴(磁矩取向与外磁场方向相反的畴)变为圆柱形磁畴。从膜面上看，这些柱形畴好像浮着的一群圆泡，故称磁泡或叫泡踌(另见磁性材料2.昨晶态磁性材料)。在特定的电路图形、电流方向和一定磁场情况下，可做到控制材料中磁泡的产生、传翰和消失，实现信息的储存和逻辑运算的功能。磁泡的直径在微米量级(0 .5~5协m)，每个磁泡的迁移率在1 .26~12.6em八s·A/m)〔 102一i03cm八s·oe)〕，因而可制成存储密度为兆位/cmZ(Mbit/cmZ)和数据处理速率为兆位/s(M肠t/s)的运算器件。磁泡器件经过近20年研究和开发，已取得广泛的实际应用。对磁泡材料的主要要求是:(l)各向异性常数凡>粤斌，磁化强度从>外磁场强度H;(2)杂质缺陷小，2一~”~’.J泌~-一‘产’~~一~一’、~尹一~~~’J”均匀性好。目前研究得比较清楚的有铁氧体单晶薄膜和稀土一过渡金属薄膜。从制备工艺和性能稳定、器件开发等情况看，以铁氧体磁泡材料比较成熟，早期是用钙钦石型铁氧体单晶片来作磁泡材料，后为YIG单晶薄膜所取代。它是用液相外延法在Gd3Ga5OI:(简称GGO)基片上生成的单晶薄膜，其厚为微米量级。表4为稀土石榴石R3FesolZ的磁性;表5为一些磁泡材料的基本特性数值。农4稀土石抽石R.Fe‘ol，的磁性┌───────────┬────┬────┬────┬────┬────┬────┬────┬────┬─────┬────┬────┐│R │Y │Sm │EU │Gd │Tb │Dy │、Ho │Er │T】11 │Yb │Lu │├───────────┼────┼────┼────┼────┼────┼────┼────┼────┼─────┼────┼────┤│补偿温度，~p，K │ 560 │ 560 │ 570 │ 290 │ 246 │ 220 │ 136 │ 84│41000 ││ │ (ZMHz) │ (20MHz) │└────────┴──────┴────────┘·3.磁光材料呻〕当前所用的磁光材料是利用磁光效应制作的磁性材料。

说明：补充资料仅用于学习参考，请勿用于其它任何用途。

参考词条

磁超导体 Bi2223/Ag超导磁体稳定性超导电磁体超导永磁体超导主磁体 NbTi超导磁体 BESIII超导磁体

N/I/d波超导体结 N-I-d波超导体结 d波超导序超导磁体

说明：双击或选中下面任意单词，将显示该词的音标、读音、翻译等；选中中文或多个词，将显示翻译。
	您的位置：首页 -> 词典 -> 磁性d波超导体 1) ferromagnetic d-wave superconductor 磁性d波超导体 2) FdS/FdS junction 双层磁性d波超导结 1. It is found that the Josephson critical currents in FdS/FdS junction depend to a great extent on the relative orientation of the effective exchange field of the two S electrodes,and the crystal orientation of the FdS. 通过计算双层磁性d波超导结界面势垒散射效应,研究了双层磁性d波超导结中Josephson临界电流随温度、磁交换能以及势垒强度的变化关系。更多例句>> 3) d-wave superconductor d波超导体 1. Using the square barrier to describe the insulating layer,tunneling conductance in normal metal/insulator/d-wave superconductor c-axis tunneling junction is studied theoretically as a function of the bias voltage,insulating layer barrier strength and insulating layer thickness. 以方势垒描述绝缘层,对N/I/d波超导体c轴隧道结的微分电导进行了研究。 2. A number of experimental studies revealed that the order parameter in high-Tc cuprates is of d-wave symmetry, and thus the properties of d-wave superconductors have been investigated theoretically for many years. 因而许多理论工作者对d波超导体的性质进行了多年研究。更多例句>> 4) ferromagnetic s-wave superconductor 磁性s波超导体 5) d-wave superconductor d波超导 1. Zeeman Effects on the differential conductance in normal-metal/d-wave superconductor tunnel junctions; 塞曼效应对正常金属/d波超导结中微分电导的影响 2. We solve self-consistent equation for the d-wave superconducting gap and the Zeeman energy in the mean-field approximation under a Zeeman magnetic on the d-wave superconductor,study the Zeeman effects on the d-wave superconducting gap and the thermodynamic potential,and discuss the condition of coexistence for ferromagnetism and superconductivity. 通过外加Zeeman磁场在d波超导中,在平均场近似下,自洽求解d波超导能隙和Zeeman能量的方程,研究了Zeeman效应对d波超导序参数和热力学势的影响,阐述了磁性与超导共存条件。 3. Taking into account the scattering effect of the insulator in normal metal-insulator-d-wave superconductor junctions, and using the Bogoliubov-de Gennes equation and the Blonder-Tinkham-Klapwijk model, we calculate the differential conductance and shot noise. 在正常金属绝缘层 d波超导隧道结中 ,考虑到绝缘层的势垒散射效应 ,运用Bogoliubov deGennes方程和Blonder Tinkham Klapwijk理论模型 ,计算系统的微分电导和散粒噪声随偏压的变化关系。更多例句>> 6) magnetic superconductor 磁性超导体 1. The single phase magnetic superconductors RESr 2RuCu 2O 8 (RE=Gd and Eu) were successfully synthesized and the investigations on their physical properties were carried out. 报道了磁性超导体RESr2 RuCu2 O8(RE =Gd和Eu)单相样品的合成以及对其结构和物性的研究。补充资料：磁性材料2．薄膜磁性材料磁性材料2．薄膜磁性材料 Magnetie Materials 2.Thin Film 在一定外加磁场作用下，其反磁化畴(磁矩取向与外磁场方向相反的畴)变为圆柱形磁畴。从膜面上看，这些柱形畴好像浮着的一群圆泡，故称磁泡或叫泡踌(另见磁性材料2.昨晶态磁性材料)。在特定的电路图形、电流方向和一定磁场情况下，可做到控制材料中磁泡的产生、传翰和消失，实现信息的储存和逻辑运算的功能。磁泡的直径在微米量级(0 .5~5协m)，每个磁泡的迁移率在1 .26~12.6em八s·A/m)〔 102一i03cm八s·oe)〕，因而可制成存储密度为兆位/cmZ(Mbit/cmZ)和数据处理速率为兆位/s(M肠t/s)的运算器件。磁泡器件经过近20年研究和开发，已取得广泛的实际应用。对磁泡材料的主要要求是:(l)各向异性常数凡>粤斌，磁化强度从>外磁场强度H;(2)杂质缺陷小，2一~”~’.J泌~-一‘产’~~一~一’、~尹一~~~’J”均匀性好。目前研究得比较清楚的有铁氧体单晶薄膜和稀土一过渡金属薄膜。从制备工艺和性能稳定、器件开发等情况看，以铁氧体磁泡材料比较成熟，早期是用钙钦石型铁氧体单晶片来作磁泡材料，后为YIG单晶薄膜所取代。它是用液相外延法在Gd3Ga5OI:(简称GGO)基片上生成的单晶薄膜，其厚为微米量级。表4为稀土石榴石R3FesolZ的磁性;表5为一些磁泡材料的基本特性数值。农4稀土石抽石R.Fe‘ol，的磁性┌───────────┬────┬────┬────┬────┬────┬────┬────┬────┬─────┬────┬────┐│R │Y │Sm │EU │Gd │Tb │Dy │、Ho │Er │T】11 │Yb │Lu │├───────────┼────┼────┼────┼────┼────┼────┼────┼────┼─────┼────┼────┤│补偿温度，~p，K │ 560 │ 560 │ 570 │ 290 │ 246 │ 220 │ 136 │ 84│41000 ││ │ (ZMHz) │ (20MHz) │└────────┴──────┴────────┘·3.磁光材料呻〕当前所用的磁光材料是利用磁光效应制作的磁性材料。说明：补充资料仅用于学习参考，请勿用于其它任何用途。参考词条磁超导体 Bi2223/Ag超导磁体稳定性超导电磁体超导永磁体超导主磁体 NbTi超导磁体 BESIII超导磁体

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