2001
DOI: 10.1016/s0304-8853(00)00711-3
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Low-temperature study of the magnetization reversal and magnetic anisotropy of Fe, Ni, and Co nanowires

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Cited by 275 publications
(180 citation statements)
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References 26 publications
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“…Furthermore, thermal effects ͑reduction of the coercive field and remanence͒ are greatly suppressed by the large volume ͑and the related activation energies͒ of the particles. 10 We show that our arrays of magnetic wires behave exactly as predicted by Preisach-type models, in which the StonerWohlfarth response ͑square hysteresis loop͒ is modified by interactions. This simplifies considerably the interpretation and enables us to draw conclusions with a minimum modeling of the data.…”
Section: Introductionsupporting
confidence: 65%
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“…Furthermore, thermal effects ͑reduction of the coercive field and remanence͒ are greatly suppressed by the large volume ͑and the related activation energies͒ of the particles. 10 We show that our arrays of magnetic wires behave exactly as predicted by Preisach-type models, in which the StonerWohlfarth response ͑square hysteresis loop͒ is modified by interactions. This simplifies considerably the interpretation and enables us to draw conclusions with a minimum modeling of the data.…”
Section: Introductionsupporting
confidence: 65%
“…10 Pore diameters D p varied from 50 nm down to 6 nm, i.e., of the same order and even lower than the values of the domain-wall width w ϭ2(A J /K s ) 1/2 , where A J and K s are, respectively, the exchange constant and the shape anisotropy. For the Fe and Ni nanowires, one has w Ӎ6 -8 nm and 22-28 nm, respectively.…”
Section: Introductionmentioning
confidence: 92%
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“…In Ivanov Importantly, the simulations showed the differences between the angular dependence of the nucleation and the coercivity fields Hn and Hc. For large applied field angles, Hc is not equal to Hn in agreement with the experimental data reported by numerous authors (Escrig, 2008;Yang, 2000;Paulus, 2001). Their angular dependence is the same in the range of the applied field angles 0 0 ≤α≤60 0 .…”
Section: Reversal Modes In Cylindrical Nanowiressupporting
confidence: 89%
“…In general the experimental value of the coercivity of the arrays is less than the coercivity of the single NW (Vega, 2012). The experimental loop of the arrays of the NWs with dominated shape anisotropy is inclined [Nielsch, 2001;Paulus, 2001;Pan, 2005;Liu, 2008;Escrig, 2008;Vivas, 2012a;Salem, 2012] and does not show the one step magnetization reversal process as for single NW in the case of the magnetic field applied parallel to the NW axis. Such behavior is also reproduced in micromagnetic simulations.…”
Section: Simulation Of Hysteresis In Individual Nanowires and Nanowirmentioning
confidence: 83%