Critical current of a Josephson junction with spatial fluctuations of the order parameter

1992 ◽  
Vol 46 (21) ◽  
pp. 13951-13955 ◽  
Author(s):  
V. V. Dorin ◽  
M. V. Fistul’
1978 ◽  
Vol 39 (C6) ◽  
pp. C6-550-C6-551
Author(s):  
H. Suhl ◽  
J. Hurell ◽  
A. H. Silver ◽  
Y. Song

2002 ◽  
Vol 16 (03) ◽  
pp. 453-461 ◽  
Author(s):  
GRZEGORZ LITAK

The effect of nonmagnetic disorder on the pairing amplitude is studied by means of a perturbation method. Using an extended one band Hubbard model with an intersite attraction we analyze various solutions of p-wave pairing symmetry and discuss their instability calculating fluctuations of order parameter. The model is applied to describe the effect of disorder in Sr2RuO4. The results shows that the real solution with line nodes can be favoured by disorder.


2020 ◽  
Vol 101 (6) ◽  
Author(s):  
Diego A. Manjarrés ◽  
Shirley Gómez Páez ◽  
William J. Herrera

2011 ◽  
Vol 23 (2) ◽  
pp. 201-244 ◽  
Author(s):  
GIANNE DERKS ◽  
ARJEN DOELMAN ◽  
CHRISTOPHER J. K. KNIGHT ◽  
HADI SUSANTO

We consider a Josephson junction system installed with a finite length inhomogeneity, either of micro-resistor or micro-resonator type. The system can be modelled by a sine-Gordon equation with a piecewise-constant function to represent the varying Josephson tunneling critical current. The existence of pinned fluxons depends on the length of the inhomogeneity, the variation in the Josephson tunneling critical current and the applied bias current. We establish that a system may either not be able to sustain a pinned fluxon, or – for instance by varying the length of the inhomogeneity – may exhibit various different types of pinned fluxons. Our stability analysis shows that changes of stability can only occur at critical points of the length of the inhomogeneity as a function of the (Hamiltonian) energy density inside the inhomogeneity – a relation we determine explicitly. In combination with continuation arguments and Sturm–Liouville theory, we determine the stability of all constructed pinned fluxons. It follows that if a given system is able to sustain at least one pinned fluxon, a microresistor has exactly one pinned fluxon, i.e. the system selects one unique pinned stable pinned configuration, and a microresonator has at least one stable pinned configuration. Moreover, it is shown that both for micro-resistors and micro-resonators this stable pinned configuration may be non-monotonic – something which is not possible in the homogeneous case. Finally, it is shown that results in the literature on localised inhomogeneities can be recovered as limits of our results on micro-resonators.


Nano Letters ◽  
2015 ◽  
Vol 15 (3) ◽  
pp. 1803-1808 ◽  
Author(s):  
J. Paajaste ◽  
M. Amado ◽  
S. Roddaro ◽  
F. S. Bergeret ◽  
D. Ercolani ◽  
...  

1988 ◽  
Vol 01 (11n12) ◽  
pp. 431-435 ◽  
Author(s):  
CHANGXIN FAN ◽  
LIANGKAI YU

The V-I characteristics of Y-Ba-Cu-O device is different from that of conventional low Tc Josephson junction. This enables us to use the small critical current device as an electromagnetic radiation detector. Experiment shows that the smaller the critical current is, the greater the dynamic resistance and the higher the voltage responsibility to radiation power. When the critical current is adjusted down to zero but the V-I curve is still obviously nonlinear, the device will have highest responsibility.


2009 ◽  
Vol 80 (9) ◽  
Author(s):  
Rogério de Sousa ◽  
K. Birgitta Whaley ◽  
Theresa Hecht ◽  
Jan von Delft ◽  
Frank K. Wilhelm

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