banner image
No data available.
Please log in to see this content.
You have no subscription access to this content.
No metrics data to plot.
The attempt to load metrics for this article has failed.
The attempt to plot a graph for these metrics has failed.
Superconducting and transport properties of bilayers
Rent this article for
View: Figures


Image of FIG. 1.
FIG. 1.

Magnetization vs temperature for a single LSMO film with under a field of 500 Oe (note: the open circles are the data with a field-cool mode, while the closed ones are with a zero-field-cool mode). The magnetization is not leveled off to zero at 300 K, suggesting that the ferromagnetic transition temperature is above 300 K.

Image of FIG. 2.
FIG. 2.

Resistivity vs for single LSMO films with (solid circles) and (open circles).

Image of FIG. 3.
FIG. 3.

Resistivity vs for YBCO(150 nm/LSMO bilayers with , 20, 30, 40, and 50 nm from bottom to top.

Image of FIG. 4.
FIG. 4.

Resistivity vs for the YBCO(150 nm) /LSMO(150 nm) bilayer. It indicates a transition from the metallic to the insulating phase near 150 K.

Image of FIG. 5.
FIG. 5.

Thermoelectric power vs for YBCO (150 nm)/ LSMO bilayers with (solid circles), 10 (open circles), 30 (solid triangles), and 50 nm (solid rhombuses).

Image of FIG. 6.
FIG. 6.

vs for YBCO (150 nm)/LSMO (50) bilayers with the magnetic field changing from zero (solid circles) to 1 T (open circles) to 3 T (down triangles).

Image of FIG. 7.
FIG. 7.

Magnetoresistance vs magnetic field for the YBCO (150 nm)/LSMO (50 nm) bilayer at room temperature.


Article metrics loading...


Full text loading...

This is a required field
Please enter a valid email address
752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Superconducting and transport properties of YBa2Cu3O7∕La0.7Sr0.3MnO3 bilayers