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Large rotating field entropy change in ErFeO3 single crystal with angular distribution contribution
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10.1063/1.4825274
/content/aip/journal/apl/103/16/10.1063/1.4825274
http://aip.metastore.ingenta.com/content/aip/journal/apl/103/16/10.1063/1.4825274
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

Temperature dependence of the magnetization curves under the ZFC process for (a) magnetic field applied along the axis and (b) magnetic field applied along the axis of the ErFeO single crystal.

Image of FIG. 2.
FIG. 2.

Isothermal magnetization curves were measured from 3 K to 40 K under decreasing magnetic field for the ErFeO single crystal along the , , and axes.

Image of FIG. 3.
FIG. 3.

Temperature dependence of the magnetic entropy change of the ErFeO single crystal for (a) the axis, (b) the axis, and (c) the axis.

Image of FIG. 4.
FIG. 4.

RC versus magnetic field curves for axis (black triangle line) and c axis (red square line) of the ErFeO single crystal.

Image of FIG. 5.
FIG. 5.

The difference in Δ between the and axes of the ErFeO single crystal under different temperature and magnetic field.

Image of FIG. 6.
FIG. 6.

Angle dependent magnetization curves measured by rotating the ErFeO single crystal from the to axis under different magnetic fields at 6 K.

Image of FIG. 7.
FIG. 7.

(a) Isothermal magnetization curve for the axis of the ErFeO single crystal at 6 K with experimental result (black squares) and fitted curve (red line). (b) The results of rotating field entropy change from to axis in a field of 3.6 T at 6 K were calculated from thermodynamic Maxwell relations (blue diamond) and Fermi-Dirac angle distribution (red circle), respectively.

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/content/aip/journal/apl/103/16/10.1063/1.4825274
2013-10-17
2014-04-16
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Large rotating field entropy change in ErFeO3 single crystal with angular distribution contribution
http://aip.metastore.ingenta.com/content/aip/journal/apl/103/16/10.1063/1.4825274
10.1063/1.4825274
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