Figures & data
Figure 1. (a) TEM image [Citation1] of Co80Ni20 nanoparticles with 50 nm average diameter and (b) SEM image [Citation13] of the Co80Ni20 nanoparticles prepared by polyol process.
![Figure 1. (a) TEM image [Citation1] of Co80Ni20 nanoparticles with 50 nm average diameter and (b) SEM image [Citation13] of the Co80Ni20 nanoparticles prepared by polyol process.](/cms/asset/9c611259-18fc-4a87-85ae-7b13c2b0c0f0/tsnm_a_672343_o_f0001g.gif)
Figure 2. (a) Hysteresis loops of the Co80Ni20 nanocomposite at selected temperatures from 5 K to 300 K after correction for the diamagnetic PVC matrix. Main panel: highlight of the hysteresis loops over field range –0.5 to 0.5 Tesla. Inset: hysteresis loops over the field range –5 to 5 Tesla. (b) Highlight of hysteresis loops in (a) over the field range –0.2 to 0.0 Tesla. The arrow illustrates the shift of decreasing coercivity H c (increasing –H c) as the temperature increases from 5 K to 300 K.
![Figure 2. (a) Hysteresis loops of the Co80Ni20 nanocomposite at selected temperatures from 5 K to 300 K after correction for the diamagnetic PVC matrix. Main panel: highlight of the hysteresis loops over field range –0.5 to 0.5 Tesla. Inset: hysteresis loops over the field range –5 to 5 Tesla. (b) Highlight of hysteresis loops in (a) over the field range –0.2 to 0.0 Tesla. The arrow illustrates the shift of decreasing coercivity H c (increasing –H c) as the temperature increases from 5 K to 300 K.](/cms/asset/c17a93b0-2a27-42c7-ba95-2c9221c8da17/tsnm_a_672343_o_f0002g.jpg)
Figure 3. Applied field dependence of irrversible susceptibility for the Co80Ni20 nanocomposite at selected temperatures from 5 K to 300 K. The maximum irreversible susceptibility χ irr,max of each curve (peak value) is represented by black dot. The arrow illustrates the shift of increasing χ irr,max as the temperature increases from 5 K to 300 K.
![Figure 3. Applied field dependence of irrversible susceptibility for the Co80Ni20 nanocomposite at selected temperatures from 5 K to 300 K. The maximum irreversible susceptibility χ irr,max of each curve (peak value) is represented by black dot. The arrow illustrates the shift of increasing χ irr,max as the temperature increases from 5 K to 300 K.](/cms/asset/1d6c6072-6a66-4f79-84e1-da910183ba73/tsnm_a_672343_o_f0003g.jpg)
Figure 4. Applied field and temperature dependence of irreversible susceptibility for the Co80Ni20 nanocomposite. The color varies from light green for small values of χ irr to purple for χ irr,max.
![Figure 4. Applied field and temperature dependence of irreversible susceptibility for the Co80Ni20 nanocomposite. The color varies from light green for small values of χ irr to purple for χ irr,max.](/cms/asset/626b42cb-1e60-4088-9568-26f84e9becca/tsnm_a_672343_o_f0004g.jpg)
Figure 6. Holding field dependence of decay coefficient, S, for the Co80Ni20 nanocomposite at selected temperatures from 10 K to 300 K. As temperature increases from 10 K to 300 K, S max increases first from 10 K to 50 K, reaches peak value at 50 K and then decreases from 50 K to 300 K.
![Figure 6. Holding field dependence of decay coefficient, S, for the Co80Ni20 nanocomposite at selected temperatures from 10 K to 300 K. As temperature increases from 10 K to 300 K, S max increases first from 10 K to 50 K, reaches peak value at 50 K and then decreases from 50 K to 300 K.](/cms/asset/6141ecfa-c458-44c3-8946-781b902486f7/tsnm_a_672343_o_f0006g.jpg)
Figure 7. Temperature dependence of the maximum decay coefficient for the Co80Ni20 nanocomposite. MPA model evaluated S max at selected temperatures are represented by red dots. The non-Arrhenius behavior is illustrated by the black fitting curve.
![Figure 7. Temperature dependence of the maximum decay coefficient for the Co80Ni20 nanocomposite. MPA model evaluated S max at selected temperatures are represented by red dots. The non-Arrhenius behavior is illustrated by the black fitting curve.](/cms/asset/39861d92-898d-431e-a6ce-23d672ebaeb9/tsnm_a_672343_o_f0007g.jpg)
Figure 8. Temperature and field dependence of the maximum decay coefficient for the Co80Ni20 nanocomposite. The maximum decay coefficient varies from light green for small values of S max to dark blue for peak value of S max.
![Figure 8. Temperature and field dependence of the maximum decay coefficient for the Co80Ni20 nanocomposite. The maximum decay coefficient varies from light green for small values of S max to dark blue for peak value of S max.](/cms/asset/cd1d0e6a-5672-48ff-9b28-4e466a12736b/tsnm_a_672343_o_f0008g.jpg)
Figure 9. Temperature and applied field dependence of the fluctuation field for the Co80Ni20 nanocomposite. hf were rigorously determined from macroscopic measurements of S and χ irr .
![Figure 9. Temperature and applied field dependence of the fluctuation field for the Co80Ni20 nanocomposite. hf were rigorously determined from macroscopic measurements of S and χ irr .](/cms/asset/3c128aae-a81f-4266-a492-658b783faed3/tsnm_a_672343_o_f0009g.jpg)
Figure 10. Temperature dependence of fluctuation field at a representative applied field of –0.1 Tesla.
![Figure 10. Temperature dependence of fluctuation field at a representative applied field of –0.1 Tesla.](/cms/asset/53ab401c-16e8-4563-8714-a118d2eb619c/tsnm_a_672343_o_f0010g.jpg)
Figure 11. Temperature and applied field dependence of the fluctuation field for the Co80Ni20 nanocomposite. hf
were evaluted using EquationEquation (7)(7).
![Figure 11. Temperature and applied field dependence of the fluctuation field for the Co80Ni20 nanocomposite. hf were evaluted using EquationEquation (7)(7).](/cms/asset/9c016aa3-3e25-406b-9840-b59c6282fda0/tsnm_a_672343_o_f0011g.jpg)