Teresis loops for an Fe NW array (three inin length) as well as the Fe/Cu NWs with hysteresis loops for an Fe NW array (3 length) along with the Fe/Cu NWs with 1, magnetic hysteresis loops for an Fe NW array (3 in length) and also the Fe/Cu NWs with five, and 20 bilayers are presented in Figure 3. In all circumstances, an increase within the 1, five, and 20 bilayers are presented in Figure three. Inall circumstances, a rise inside the coercivity and 1, five, and 20 bilayers are presented in Figure 3. In all circumstances, an increase in the coercivity and remanence values is observed when the magnetic field is applied parallel to the wire’s axis, values is observed when the magnetic field is applied parallel towards the wire’s remanence values is observed when the magnetic field is applied parallel towards the wire’s confirming the the anisotropic behavior with the structures. A similar magnetic behavior axis, confirminganisotropic behavior from the structures. A comparable magnetic behavior has axis, confirming the anisotropic behavior on the structures. A comparable magnetic behavior been observed for for all samples, being independent from the quantity of bilayers. has been observed all samples, being independent in the number of bilayers. has been observed for all samples, being independent with the quantity of bilayers.Figure three. Magnetic hysteresis loops of (a) Fe NW arrays with nm in in diameter and 3000 nm in 8-Bromo-cGMP site 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 three. 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) five, 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) five, 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 towards 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 in the switching field state, when applying the magnetic field parallel for the wire axis. six ofTo analyze the magnetization reversal modes in Fe/Cu NWs as a function of your quantity of bilayers, 3-D micromagnetic simulations utilizing the MuMax3 computer software (Version To analyze the magnetization reversal modes in Fe/Cu NWs as a function in the number three.9.1) [42] have been performed. Following the experimental results and our earlier operate of bilayers, 3-D micromagnetic simulations using the MuMax3 software program (Version three.9.1) [42] [19], multi-segmented person NWs 40 nm in diameter, with Imeglimin Inhibitor ferromagnetic Fe layers have been performed. Following the experimental outcomes and our preceding function [19], multi300 nm in length and non-magnetic Cu spacers 120 nm in length, had been simulated. The segmented person NWs 40 nm in diameter, with ferromagnetic Fe layers 300 nm in quantity of bilayers was varied from 1 to 15. A person lengthy Fe NW (three in length) length and non-magnetic Cu spacers 120 nm in length, were simulated. The amount of was also simulated for comparison (inset in Figure 3a). bilayers was varied from.