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Flux pinning properties and microstructure of thin films with systematically controlled nanorods
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10.1063/1.3498812
/content/aip/journal/jap/108/9/10.1063/1.3498812
http://aip.metastore.ingenta.com/content/aip/journal/jap/108/9/10.1063/1.3498812

Figures

Image of FIG. 1.
FIG. 1.

Cross-sectional TEM images of BZO-doped SmBCO films fabricated by LTG technique (LTG- film) on MgO (100) substrate. LTG- films were grown at upper layer substrate temperature, , of (a) 920, (b) 860, and (c) .

Image of FIG. 2.
FIG. 2.

Irreversibility field lines as a function of reduced temperature for LTG- films grown at (a) for and (b) for . Arrows in Fig. 2(b) indicate respective starting point and ending point of the upturn shift in LTG- films grown at and .

Image of FIG. 3.
FIG. 3.

Magnetic field dependence of at 77 K for LTG- films grown at . Applied magnetic field is parallel to the -axis. Arrows indicate ending points of the plateau regions.

Image of FIG. 4.
FIG. 4.

Field angular dependence of at 77 K for LTG- films grown at of (a) and (b) under 0.5 to 3 T.

Tables

Generic image for table
Table I.

Superconducting transition temperatures and self-field critical current densities for LTG- films grown at .

Generic image for table
Table II.

Magnetic fields at two kinks obtained from irreversibility field line (we defined the magnetic fields at the starting point and the ending point of upturn as and , respectively), , mean diameter, and mean spacing between BZO nanorods calculated from TEM images.

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/content/aip/journal/jap/108/9/10.1063/1.3498812
2010-11-02
2014-04-25
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Flux pinning properties and microstructure of SmBa2Cu3Oy thin films with systematically controlled BaZrO3 nanorods
http://aip.metastore.ingenta.com/content/aip/journal/jap/108/9/10.1063/1.3498812
10.1063/1.3498812
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