2021
DOI: 10.1016/j.jnoncrysol.2021.120885
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Outstanding glass formability and magneto-caloric effect of a Fe85Co3Zr5B4Nb3 metallic glass

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Cited by 17 publications
(18 citation statements)
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“…Each set of point plots is linearly fitted well, and the slope (expressed by n ) of the linear fitting is 0.756 for x = 5, 0.759 for x = 6, and 0.750 for x = 7, respectively. The values of n are consistent with that of other MGs [ 16 , 17 , 18 , 23 , 24 , 25 , 26 , 29 , 30 ] but slightly larger than the predicted value of the mean field model [ 35 ]. This deviation is mainly caused by local inhomogeneity in MGs because the presence of short-range ordered clusters in MGs leads to a magnetic transformation in a wide temperature range [ 17 ].…”
Section: Resultssupporting
confidence: 87%
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“…Each set of point plots is linearly fitted well, and the slope (expressed by n ) of the linear fitting is 0.756 for x = 5, 0.759 for x = 6, and 0.750 for x = 7, respectively. The values of n are consistent with that of other MGs [ 16 , 17 , 18 , 23 , 24 , 25 , 26 , 29 , 30 ] but slightly larger than the predicted value of the mean field model [ 35 ]. This deviation is mainly caused by local inhomogeneity in MGs because the presence of short-range ordered clusters in MGs leads to a magnetic transformation in a wide temperature range [ 17 ].…”
Section: Resultssupporting
confidence: 87%
“…Figure 5 a displays the −Δ S m peak under 5 T of the Fe 87 Ce 13−x B x (x = 5, 6, 7) amorphous ribbons and some Fe-Zr-B-based MGs [ 15 , 16 , 17 , 18 , 23 , 24 , 25 , 26 , 36 ]. A positive correlation between −Δ S m peak and T c was observed in the Fe-Zr-B-based MGs, implying that the higher −Δ S m peak can only be achieved at higher temperatures for the Fe-Zr-B-based MGs, which is very unfriendly for the application of magnetic refrigeration at room temperature.…”
Section: Resultsmentioning
confidence: 99%
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