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Transport and spectroscopic properties of superconductor - ferromagnet - superconductor junctions of
L
a
1.9
S
r
0.1
C
u
O
4
La_{1.9}Sr_{0.1}CuO_4
L
a
1.9
S
r
0.1
C
u
O
4
-
L
a
0.67
C
a
0.33
M
n
O
3
La_{0.67}Ca_{0.33}MnO_3
L
a
0.67
C
a
0.33
M
n
O
3
-
L
a
1.9
S
r
0.1
C
u
O
4
La_{1.9}Sr_{0.1}CuO_4
L
a
1.9
S
r
0.1
C
u
O
4
Authors
A. F. Andreev
A. F. Andreev
G. Koren
T. Kirzhner
Publication date
5 July 2011
Publisher
'American Physical Society (APS)'
Doi
View
on
arXiv
Abstract
Transport and Conductance spectra measurements of ramp-type junctions made of cuprate superconducting
L
a
1.9
S
r
0.1
C
u
O
4
La_{1.9}Sr_{0.1}CuO_4
L
a
1.9
S
r
0.1
C
u
O
4
electrodes and a manganite ferromagnetic
L
a
0.67
C
a
0.33
M
n
O
3
La_{0.67}Ca_{0.33}MnO_3
L
a
0.67
C
a
0.33
M
n
O
3
barrier are reported. At low temperatures below
T
c
T_c
T
c
, the conductance spectra show Andreev-like broad peaks superposed on a tunneling-like background, and sometimes also sub-gap Andreev resonances. The energy gap values
Δ
\Delta
Δ
found from fits of the data ranged mostly between 7-10 mV. As usual, the gap features were suppressed under magnetic fields but revealed the tunneling-like conductance background. After field cycling to 5 or 6 T and back to 0 T, the conductance spectra were always higher than under zero field cooling, reflecting the negative magnetoresistance of the manganite barrier. A signature of superparamagnetism was found in the conductance spectra of junctions with a 12 nm thick LCMO barrier. Observed critical currents with barrier thickness of 12 nm or more, were shown to be an artifact due to incomplete milling of one of the superconducting electrodes.Comment: 10 figure
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info:doi/10.1103%2Fphysrevb.84...
Last time updated on 03/01/2020