| نویسندگان | امیرحسن منتظر-عبد العلی رمضانی-محمد الماسی کاشی-ج زاواسنیک |
| تاریخ انتشار | 2016-10-01 |
| نمایه نشریه | ISI ,SCOPUS |
چکیده مقاله
Experimental realization of analytically predicted behavior at nanoscale magnetic systems can pave the way for promoting
the synergistic research and has significant importance for applications and thorough understanding in nanomagnetism.
Here, we report on the magnetism of a nearly ideal nanowire (NW) system, vertically aligned hcp-Co(001) single-crystal
NWs electrochemically deposited inside the aluminum oxide template, as a function of the angle (0° ≤ θ ≤ 90°) between
the magnetic field and NW axis. Using high resolution transmission electron microscopy, detailed structural investigations
on the few micrometers long and approximately 45 nm diameter NWs exhibit crystalline inhomogeneities at NW ends,
evidencing magnetic localization in the single crystalline NWs. Using a vibrating sample magnetometer enabled us to
extract different magnetic parameters, thereby evaluating angular dependence of magnetism in NW arrays and individual
NWs. While the conventional hysteresis and first-order reversal curve (FORC) diagram methods show monotonic
decreasing and increasing behavior for the coercivity as a function of θ, respectively, the average coercivity obtained from
the irreversible distribution indicates a non-monotonic behavior, involving a complex magnetization reversal triggered by
the propagation of vortex domain walls (DWs) and single vortex states for high field angles. Additionally, the hysteresis
curve coercivity is phenomenologically parameterized at each θ based on the angular FORC (AFORC) measurements.
Comparing the AFORC coercivities (varying between 5 kOe at θ= 0° and 9.3 kOe at θ= 90°) with absolute values of the
angular dependence of vortex nucleation field confirms an almost complete concurrence between experimental findings
and analytical calculations on individual NWs. Consequently, our results show first analytically supported evidences on
capturing the nucleation fields and the occurrence of vortex DW propagation at each θ for weakly interacting Co NW
arrays with large magnetocrystalline anisotropy along the length.