2007
DOI: 10.1103/physrevb.75.020502
|View full text |Cite
|
Sign up to set email alerts
|

Angular dependence of Josephson currents in unconventional superconducting junctions

Abstract: Josephson effect in junctions between unconventional superconductors is studied theoretically within the model describing the effects of interface roughness. The particularly important issue of applicability of the frequently used Sigrist-Rice ͑SR͒ formula for Josephson current in d-wave superconductor/insulator/d-wave superconductor junctions is addressed. We show that although the SR formula is not applicable in the ballistic case, it works well for rough interfaces when the diffusive normal metal regions ex… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
4
1

Citation Types

5
116
0

Year Published

2007
2007
2021
2021

Publication Types

Select...
9

Relationship

1
8

Authors

Journals

citations
Cited by 77 publications
(121 citation statements)
references
References 35 publications
5
116
0
Order By: Relevance
“…Until both better theoretical models and more varied experimental observations are made available, one cannot conclusively say that there is indeed an induced triplet state in these systems, but at this point the facts fit this explanation and no better one has been proposed. 17 Many theoretical studies agree that it is possible to induce this exotic state in certain SF systems 17,18,19,20,21,22,23,24,25,26,27,28,29 (perhaps even in the nonmagnetic 30 case) with ordinary singlet pairing in S. Some studies use an SFF ′ S arrangement in which the F and F ′ layers have different magnetization orientations. Others assume that a domain structure in a single F layer is responsible for the symmetry breaking.…”
Section: Introductionmentioning
confidence: 99%
“…Until both better theoretical models and more varied experimental observations are made available, one cannot conclusively say that there is indeed an induced triplet state in these systems, but at this point the facts fit this explanation and no better one has been proposed. 17 Many theoretical studies agree that it is possible to induce this exotic state in certain SF systems 17,18,19,20,21,22,23,24,25,26,27,28,29 (perhaps even in the nonmagnetic 30 case) with ordinary singlet pairing in S. Some studies use an SFF ′ S arrangement in which the F and F ′ layers have different magnetization orientations. Others assume that a domain structure in a single F layer is responsible for the symmetry breaking.…”
Section: Introductionmentioning
confidence: 99%
“…[8][9][10] In particular, it was predicted that the local density of states ͑LDOS͒ in the ferromagnet is enhanced in the presence of the odd-frequency pairing. 11 Recently, it was shown that an odd-frequency pairing state is possible even without magnetic ordering. Tanaka and Golubov predicted that the odd-frequency pair amplitude can be induced in a diffusive normal metal attached to a spin-triplet superconductor.…”
Section: Introductionmentioning
confidence: 99%
“…Therefore, the x component of the magnetization in the N is always zero, as discussed below. (23) in the N of the S1/F1/N/F2/S2 junction. Where ω n is the Fermion Matsubara frequency andp F = cos χ. χ is the angle between the Fermi momentum and the x axis.…”
Section: Anomalous Green's Function In Normal Metalmentioning
confidence: 99%
“…When the magnetization in the F is uniform in a S/F junction, the STC composed of opposite spin electrons (i.e., total spin projection on z axis being S z = 0) and SSCs penetrates into the F due to the proximity effect. 22,23) The penetration length of STC with S z = 0 and SSC as described above into the F is very short and the amplitude of STC exhibits a damped oscillatory behavior inside the F with increasing the thickness of F.…”
Section: Introductionmentioning
confidence: 99%