Teresis loops for an Fe NW array (three inin length) plus the Fe/Cu NWs with hysteresis loops for an Fe NW array (three length) plus the Fe/Cu NWs with 1, magnetic hysteresis loops for an Fe NW array (three in length) as well as the Fe/Cu NWs with five, and 20 biD-Tyrosine Biological Activity layers are presented in Figure 3. In all Fmoc-Gly-Gly-OH MedChemExpress instances, an increase inside the 1, five, and 20 bilayers are presented in Figure three. Inall circumstances, an increase within the coercivity and 1, 5, and 20 bilayers are presented in Figure 3. In all circumstances, a rise in the coercivity and remanence values is observed when the magnetic field is applied parallel towards the wire’s axis, values is observed when the magnetic field is applied parallel for the wire’s remanence values is observed when the magnetic field is applied parallel for the wire’s confirming the the anisotropic behavior from the structures. A equivalent magnetic behavior axis, confirminganisotropic behavior of your structures. A equivalent magnetic behavior has axis, confirming the anisotropic behavior in the structures. A related magnetic behavior been observed for for all samples, being independent from the quantity of bilayers. has been observed all samples, becoming independent with the quantity of bilayers. has been observed for all samples, becoming independent of the quantity of bilayers.Figure three. Magnetic hysteresis loops of (a) Fe NW arrays with nm in in diameter and 3000 nm in length and (b) Fe/Cu Figure three. Magnetic hysteresis loops of (a) Fe NW arrays with 45 nm in diameter and 3000 in length and and (b) Fe/Cu Figure 3. Magnetic hysteresis loops of (a) Fe NW arrays with 4545 nm diameter and 3000 nm nm in length (b) Fe/Cu NW NW arrays with 45 nm in diameter, Fe lengths of 300 nm, Cu segment lengths of 120 nm, and (b) 1, (c) 5, and (d) 20 arrays with with 45 nm in diameter, Fe lengths ofnm, Cu segment lengthslengths of 120 nm, and (b) and (d) 20 bilayers, NW arrays 45 nm in diameter, Fe lengths of 300 300 nm, Cu segment of 120 nm, and (b) 1, (c) 5, 1, (c) five, and (d) 20 measured along the parallel (black) and perpendicular (red) directions. Insets show the respective 3D simulated magnetic configurations at the switching field state, when applying the magnetic field parallel to the wire axis.Nanomaterials 2021, 11, x FOR PEER REVIEW6 ofbilayers, measured along the parallel (black) and perpendicular (red) directions. Insets show the respective 3D simulatedNanomaterials 2021, 11, 2729 magnetic configurations at the switching field state, when applying the magnetic field parallel towards the wire axis. six ofTo analyze the magnetization reversal modes in Fe/Cu NWs as a function of your number of bilayers, 3-D micromagnetic simulations using the MuMax3 software program (Version To analyze the magnetization reversal modes in Fe/Cu NWs as a function with the quantity 3.9.1) [42] were performed. Following the experimental benefits and our prior function of bilayers, 3-D micromagnetic simulations employing the MuMax3 software program (Version three.9.1) [42] [19], multi-segmented individual NWs 40 nm in diameter, with ferromagnetic Fe layers were performed. Following the experimental results and our previous perform [19], multi300 nm in length and non-magnetic Cu spacers 120 nm in length, have been simulated. The segmented person NWs 40 nm in diameter, with ferromagnetic Fe layers 300 nm in number of bilayers was varied from 1 to 15. A person extended Fe NW (3 in length) length and non-magnetic Cu spacers 120 nm in length, were simulated. The number of was also simulated for comparison (inset in Figure 3a). bilayers was varied from.
