1) s/I/d junctions
s/I/d超导结
2) 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。
3) 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。
4) FS/I/S junction
FS/I/S超导隧道结
5) s/I/s junction
s/I/s结
1.
It is found that dc Josephson currents are suppressed by rough interface scattering and the Josephson effect depends on strongly the symmetry of s/I/s junction.
在不对称s波超导体/绝缘层/s波超导体Josephson结(s/I/s)中,考虑结界面粗糙散射情况下,运用Bogoliubov deGennes(BdG)方程和Furusaki Tsukada(FT)的电流公式计算准粒子的输运系数及s/I/s结的直流Josephson电流。
6) S/FI/S junction
S/FI/S超导结
补充资料：正常（超导）—超导（正常）转变
正常（超导）—超导（正常）转变
transitionfromnormal(superconducting)statetosuperconducting(normal)state
一般指在常压下改变温度到Tc时，物质的电阻从R＞0（R=0）的正常态（超导态）到R=0（R＞0）的超导态（正常态）的转变。无磁场时这种转变属二级相变。
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