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The strength of internal stresses is determined by the thickness of glass coating and metallic nucleus diameter.
〈z1〉 for the 4-μm nucleus diameter was about two to four times higher than for the 6-μm and 8-μm follicle cell nucleus diameters, respectively.
Within each composition of metallic nucleus, we also produced microwires with different ratios of metallic nucleus diameter and total diameter, D, i.e., with different ratios ρ = d/D.
The nucleus diameter measurement was performed in two directions and the value was expressed as the mean value and standard deviation.
Shells implanted with the optimum nucleus diameter and number of pearls produced the highest layer thickness of 17 μm after 9 months cultivation.
Assuming a nucleus diameter of (3 - 5) nm housing the radioactive payload in the nanoparticle, the diameter of a gold-encapsulated α-particle nanogenerator should not exceed approximately 75 nm before surface functionalization.
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Hysteresis loops of a few studied microwires (Fe70B15Si10C5 and Fe72.75Co2.25B15Si10) with different metallic nucleus diameters and similar Fe-rich composition are shown in Figure1.
Our results for 〈z〉 and 〈z1〉 for follicle cell nucleus diameters of 4, 6 and 8 μm show good agreement (only 2.8%to3.7%7% higher values) compared with the published data.
Previously, similar increasing of coercivity with decreasing the metallic nucleus diameters has been attributed to enhanced magnetoelastic energy arising from enhanced internal stresses when ρ ratio is small[5, 8, 14].
We studied the effect of magnetoelastic anisotropy on domain wall (DW) dynamics and remagnetization process of magnetically bistable Fe-Co-rich microwires with metallic nucleus diameters (from 1.4 to 22 μm).
Testicular histopathology revealed a significant reduction in the means of seminiferous tubules and Sertoli cell nucleus diameters as well as germinal epithelium height on day 10 in both heated groups.
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