Zero phase difference supercurrent in ferromagnetic Josephson junctions

2010 ◽  
Vol 22 (44) ◽  
pp. 445701 ◽  
Author(s):  
I Margaris ◽  
V Paltoglou ◽  
N Flytzanis
2015 ◽  
Vol 62 (4) ◽  
pp. 938-947 ◽  
Author(s):  
Shunta Iguchi ◽  
Pyungwoo Yeon ◽  
Hiroshi Fuketa ◽  
Koichi Ishida ◽  
Takayasu Sakurai ◽  
...  

2007 ◽  
Vol 460-462 ◽  
pp. 1305-1306 ◽  
Author(s):  
Tomio Koyama ◽  
Masahiko Machida ◽  
Masaru Kato ◽  
Takekazu Ishida

Author(s):  
Yueshi Guan ◽  
Zhenyu Shi ◽  
Chang Liu ◽  
Yijie Wang ◽  
Dian Guo Xu

2021 ◽  
Vol 11 (1) ◽  
Author(s):  
N. Satchell ◽  
T. Mitchell ◽  
P. M. Shepley ◽  
E. Darwin ◽  
B. J. Hickey ◽  
...  

AbstractWe report on the electrical transport properties of Nb based Josephson junctions with Pt/Co$$_{68}$$ 68 B$$_{32}$$ 32 /Pt ferromagnetic barriers. The barriers exhibit perpendicular magnetic anisotropy, which has the main advantage for potential applications over magnetisation in-plane systems of not affecting the Fraunhofer response of the junction. In addition, we report that there is no magnetic dead layer at the Pt/Co$$_{68}$$ 68 B$$_{32}$$ 32 interfaces, allowing us to study barriers with ultra-thin Co$$_{68}$$ 68 B$$_{32}$$ 32 . In the junctions, we observe that the magnitude of the critical current oscillates with increasing thickness of the Co$$_{68}$$ 68 B$$_{32}$$ 32 strong ferromagnetic alloy layer. The oscillations are attributed to the ground state phase difference across the junctions being modified from zero to $$\pi $$ π . The multiple oscillations in the thickness range $$0.2~\leqslant ~d_\text {CoB}~\leqslant ~1.4$$ 0.2 ⩽ d CoB ⩽ 1.4  nm suggests that we have access to the first zero-$$\pi $$ π and $$\pi $$ π -zero phase transitions. Our results fuel the development of low-temperature memory devices based on ferromagnetic Josephson junctions.


2020 ◽  
Vol 11 (1) ◽  
Author(s):  
William Mayer ◽  
Matthieu C. Dartiailh ◽  
Joseph Yuan ◽  
Kaushini S. Wickramasinghe ◽  
Enrico Rossi ◽  
...  

AbstractIn a standard Josephson junction the current is zero when the phase difference between superconducting leads is zero. This condition is protected by parity and time-reversal symmetries. However, the combined presence of spin–orbit coupling and magnetic field breaks these symmetries and can lead to a finite supercurrent even when the phase difference is zero. This is the so called anomalous Josephson effect—the hallmark effect of superconducting spintronics—which can be characterized by the corresponding anomalous phase shift. Here we report the observation of a tunable anomalous Josephson effect in InAs/Al Josephson junctions measured via a superconducting quantum interference device. By gate controlling the density of InAs, we are able to tune the spin–orbit coupling in the Josephson junction. This gives us the ability to tune the anomalous phase, and opens new opportunities for superconducting spintronics, and new possibilities for realizing and characterizing topological superconductivity.


Energies ◽  
2017 ◽  
Vol 10 (7) ◽  
pp. 949 ◽  
Author(s):  
Bo Zhang ◽  
J.F. Pan ◽  
Jianping Yuan ◽  
Wufeng Rao ◽  
Li Qiu ◽  
...  

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