1) 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。
2) ferromagnetic d-wave superconductor
磁性d波超导体
3) 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 。
4) N/I/d-wave superconductor junctions
N/I/d波超导体结
1.
Under the condition of superconducting phase factor φ±=0,using the square barrier to describe the influence of the insulating layer on the quasi-particle transport in N/I/d-wave superconductor junctions,we calculate the tunnel spectra utilizing the Bogoliubov-de Gennes(BdG) equation and Blonder-Tinkham-Klapwijk(BTK) theory.
以方势垒描述N/I/d波超导体结中绝缘层对准粒子输运的影响,在超导相位因子φ±=0的情况下,利用Bogoliubov-de Gennes(BdG)方程和Blonder-Tinkham-Klapwijk(BTK)理论,计算了N/I/d波超导体结的隧道谱。
2.
Taking into account the inelastic scattering of the quasi-particles and the impurities scattering in the normal metal region,using the square barrier to describe the influence of the insulating layer on the quasi-particles transport in N/I/d-wave superconductor junctions,we calculate the tunnel spectra utilizing the Bogoliubov-de Gennes(BdG) equation and Blonder-Tinkham-Klapwijk(BTK) theory.
考虑准粒子的非弹性散射和正常金属区域的杂质散射,以方势垒描述N/I/d波超导体结中绝缘层对准粒子输运的影响,运用Bogoliubov-de Gennes(BdG)方程和Blonder-Tinkham-Klapwijk(BTK)理论,计算了N/I/d波超导体结的隧道谱。
5) N-I-d-wave superconductor junctions
N-I-d波超导体结
1.
Using the square barrier to describe the influence of the insulating layer on the quasi-particle transport in N-I-d-wave superconductor junctions, we calculate the tunnel spectra utilizing the Bogoliubov-de Gennes(BdG) equation and Blonder-Tinkham-Klapwijk (BTK) theory.
以方势垒描述N-I-d波超导体结中绝缘层对准粒子输运的影响,通过求解Bogoliubov-de Gennes(BdG)方程,利用Blonder-Tinkham-Klapwijk(BTK)理论,计算了N-I-d波超导体结的隧道谱。
6) ferromagnetic s-wave superconductor
磁性s波超导体
补充资料：双[1-(4-二甲氨基)苯基2-苯基1,2-二硫代乙烯合镍]
分子式：
CAS号：
性质：紫黑色单斜晶体。熔点277～278℃。溶于苯、甲苯、三氯甲烷等大多数有机溶剂。红外频率υ(C＝S)1190、1165、1140cm-1,红外频率υ(S-C-C-S)880cm-1。由对二甲氨基安息香、五硫化二磷在二噁烷(二氧六环)中反应后,加入镍(Ⅱ)盐溶液制得。用作光学非线性材料。
CAS号：
性质：紫黑色单斜晶体。熔点277～278℃。溶于苯、甲苯、三氯甲烷等大多数有机溶剂。红外频率υ(C＝S)1190、1165、1140cm-1,红外频率υ(S-C-C-S)880cm-1。由对二甲氨基安息香、五硫化二磷在二噁烷(二氧六环)中反应后,加入镍(Ⅱ)盐溶液制得。用作光学非线性材料。
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