2012
DOI: 10.1103/physrevb.85.184526
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Josephson junctions incorporating a conical magnetic holmium interlayer

Abstract: Josephson junctions incorporating a conical magnetic spacer layer of Ho were measured as a function of spacer layer thickness and an applied magnetic field. The characteristic voltage decreased as a function of layer thickness without the obvious presence of any π phase shifts, although the decay was somewhat fragmented. The decay is exponential with a decay coherence length of ξ f ≈ 4.34 nm and the Ho mean-free path is calculated to be l Ho = 0.28-0.87 nm, which suggests the system is in the dirty limit. The … Show more

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Cited by 38 publications
(38 citation statements)
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“…9). Even if we assume that exchange coupling with Ho introduces additional domain walls into the Py, given the high saturation field of Ho thin films (B4 T) 19,31 the domain configuration would hardly change in the field range investigated and so we would expect to see a monotonic increase in resistance with field rather than a sharp switching as observed in our data. Moreover, the asymmetry in the resistance peaks in R-H for the spin valve without Ho clearly shows that R-H reflects the exchange bias observed in the M-H loop, and thus the magnetic state of the spin valve is the underlying factor responsible for the observed resistance peaks.…”
Section: Discussionmentioning
confidence: 39%
See 1 more Smart Citation
“…9). Even if we assume that exchange coupling with Ho introduces additional domain walls into the Py, given the high saturation field of Ho thin films (B4 T) 19,31 the domain configuration would hardly change in the field range investigated and so we would expect to see a monotonic increase in resistance with field rather than a sharp switching as observed in our data. Moreover, the asymmetry in the resistance peaks in R-H for the spin valve without Ho clearly shows that R-H reflects the exchange bias observed in the M-H loop, and thus the magnetic state of the spin valve is the underlying factor responsible for the observed resistance peaks.…”
Section: Discussionmentioning
confidence: 39%
“…More direct evidence for the generation of triplet pairing was obtained from S-F-S Josephson junctions in which, if interfacial spin-mixer layers were present, supercurrents could be measured through F-layer thicknesses much larger than the singlet coherence length [15][16][17][18][19][20][21][22][23] . As spin-one triplet pairs, unlike singlet pairs, can carry spin, these results mean that combining superconducting and spin electronics (superconducting spintronics) opens up real potential for practical lowtemperature applications 24 .…”
mentioning
confidence: 99%
“…We have used the definitions of the Dyakonov-Perel spin relaxation tensor Γ ab and the diffusive spin precession tensor C ab k presented in Eqs. (7) and (8). In the most general SO coupling, one can show, that the structure of Eqs.…”
Section: The Singlet-triplet Conversion In Diffusive S/f Structumentioning
confidence: 94%
“…For example, consider a S-F -F-F -S Josephson junction [7]: If the F and F layer magnetizations are collinearly aligned, spin-zero triplet pairs form which, like singlet pairs, are short ranged [8] with a coherence length in F metals of only a few nanometers (Ni [9][10][11][12], NiFe [13,14], Co [11,15,16], and Fe [17,18]). However, if F and F layer magnetizations are noncollinearly aligned spin-one triplet pairs form and the coherence length is greatly extended [19][20][21][22][23][24][25][26][27]. See also spectroscopic works on triplet S-F structures in Refs.…”
mentioning
confidence: 99%