For simplicity, the magnetic moment was then directly measured from 300 to 5 K to get the FC curve. Figure 6 shows the ZFC/FC curves of three typical samples, i.e., the as-synthesized sample, the sample annealed for 4 h, and the sample annealed for 6 h. For the as-synthesized sample in Figure 6, the irreversibility exists in the whole selleck products temperature range. The ZFC magnetization increases rapidly from 5 to 65 K and then decreases slightly with increasing T, exhibiting a broad peak (T max approximately 65 K). The FC magnetization decreases continuously as temperature increases
from 5 to 300 K. These behaviors of ZFC/FC curves are related to a superparamagnetic behavior of the crystal grains whose blocking temperatures are widely distributed. The distribution Pifithrin-�� in vivo of the blocking temperature indicates that the energy barriers,
which are contributed by the anisotropy energy and the dipolar interactions, have wide distributions. This distribution may be caused by the distribution of the crystal grain sizes as TEM images show in Figure 2. Similar to the as-synthesized sample, the 4-h annealed sample also exhibits Eltanexor the superparamagnetic behavior. The bifurcations are also higher than 300 K. The most important feature is that the ZFC magnetization shows a maximum around 170 K, which is higher than 65 K of the as-synthesized sample. The fact that the block peak shifted to the higher temperature implies that the strength of the energy barriers is increased to overcome the thermal fluctuations. For the 6-h annealed sample, the peak temperature is further improved, indicating that the strength of the energy barriers is further increased. Figure 6 ZFC/FC magnetization curves measured under an applied magnetic field of 200 Oe. Conclusions In conclusion, the Fe@α-Fe2O3 nanowires have been synthesized using the chemical method. Some novel fluffy-like α-Fe2O3 grows on the surface of the nanowires Ergoloid through the post-annealing in air. The coercivity of the as-synthesized nanowires is above 684 Oe
in the temperature range of 5 to 300 K, which is significantly higher than that of the bulk Fe. Through the annealing process in air, the coercivity and the exchange field are evidently improved. Both the coercivity and the exchange field increase with increasing T A and reach their maximum values of 1,042 and 78 Oe, respectively, at T A = 4 h. The magnetic measurements show that the effective anisotropy is increased with increasing the thickness of the α-Fe2O3 by annealing. The large values of coercivity and exchange field, as well as the high surface area to volume ratio, may make the fluffy Fe@α-Fe2O3 core-shell nanowire a promising candidate for the applications of the magnetic drug delivery, electrochemical energy storage, gas sensors, photocatalysis, and so forth. Acknowledgements This work was supported by the National Natural Science Foundation of China (nos.
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