2002
DOI: 10.1016/s0921-4526(02)01188-2
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The electronic properties of FeCo, Ni3Mn and Ni3Fe at the order–disorder transition

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Cited by 26 publications
(16 citation statements)
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“…3, the calculated density of states of pure BCC Fe is shown, the occupancy of both majority and minority d-states of Fe sites can explain its enhanced ferromagnetic moment compared to pure Fe that has partially filled majority-spin d-bands. The calculated local magnetic moment for the Fe atom in the BCC Fe 0:94 Ni 0:06 ''alloy'' is in good agreement with that calculated by means of the KKR coherent potential approximation combined with the localdensity functional method by Kulkova et al [15]. Our results are in good agreement with experimental values [33][34][35], and with theoretical results obtained by differents methods.…”
Section: Effect Of Co Impurities On Electronic Structure and Magnetissupporting
confidence: 88%
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“…3, the calculated density of states of pure BCC Fe is shown, the occupancy of both majority and minority d-states of Fe sites can explain its enhanced ferromagnetic moment compared to pure Fe that has partially filled majority-spin d-bands. The calculated local magnetic moment for the Fe atom in the BCC Fe 0:94 Ni 0:06 ''alloy'' is in good agreement with that calculated by means of the KKR coherent potential approximation combined with the localdensity functional method by Kulkova et al [15]. Our results are in good agreement with experimental values [33][34][35], and with theoretical results obtained by differents methods.…”
Section: Effect Of Co Impurities On Electronic Structure and Magnetissupporting
confidence: 88%
“…Since several decades, numerous investigations on magnetism in Fe-based ordered and disordered alloys, both theoretically and experimentally, have been made [6][7][8]. The experimental investigations have provided a variety of information about the magnetic properties of these systems, e.g., variation of magnetization with band filling [9], moment distribution in dilute Fe alloys at low as well as at finite temperatures [10], local environments effects on magnetic properties [11], spatial distribution and thermal variation of hyperfine fields [12], concentration dependence of high field susceptibility [13], low-temperature specific heat [14], order-disorder phase transition and magnetic phase stability [15,16], leading eventually to magnetic phase diagrams.…”
Section: Introductionmentioning
confidence: 99%
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“…In other words, the precise values of the measurement temperatures of the HMF's between 0 K and RT do not need to be considered to get the estimates given below. At 0 K, the mean magnetic moments hl Fe i are 3.02 and 2.92 l B in disordered A2 FeCo and in ordered B2 FeCo respectively while the moments hl Co i are respectively 1.81 and 1.62 l B [64][65][66]. The previous model yields then hB S (Co)i = -23.6 T and hB S (Fe)i = ?2.5 T. Table 1 compares mean 119 Sn HMF's measured at RT in various Fe x Co y Sn 100-x-y alloys.…”
Section: Discussionmentioning
confidence: 99%
“…Several synthetic methods have been applied to synthesize magnetic FeCo alloy nanoparticles [18], such as self-assembly techniques [19], sonoelectrochemical [20], co-precipitation [21], modified mechanochemical procedure [22] and high-energy ballmilling [23]. Precipitation from solution is a simple method to prepare magnetic nanoparticles with a rigorous control over their size and shape [24][25][26][27][28][29].…”
Section: Introductionmentioning
confidence: 99%