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  • 1990-1994  (4)
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  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 75 (1994), S. 6574-6576 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Using molecular beam epitaxy and ion implantation, Japanese workers have formed Fe16N2 in thin Fe films. They report a large magnetic induction for this nitride, ≥2.8 T. In the present study, Fe16N2 has been prepared in bulk form by treating Fe powder with NH3/H2 gas mixtures at temperatures in the range 660–670 °C. The γ phase alloy, which forms under these conditions, was quenched to room temperature to form the α'-Fe-N phase and then heat treated at 120–150 °C to form the α‘-Fe-N phase. The α' phase has been prepared in 80% purity, the other phase being nonmagnetic γ-Fe-N. The α‘ phase has been prepared in 50% purity, the impurity phases being α-Fe and γ-Fe-N. Magnetic measurements give saturation magnetizations at room temperature of 250±10 emu/g (2.6μB/Fe) for the α' phase, 285±10 emu/g (2.9μB/Fe) for the α‘ phase, and essentially zero for the γ phase. Mössbauer measurements confirm that nitrogen austenite is nonmagnetic. The anisotropy of Fe16N2 is small but detectable.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 69 (1991), S. 6070-6070 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: In order to improve the understanding of Co site preference and 59Co hyperfine fields in Nd2Fe14B, a NMR study has been carried out on Nd2(Fe1−xCox)14B for low Co contents, 0.0015≤x≤0.15. Using a high sensitivity NMR spectrometer, good quality 59Co spectra for frequencies from 100 to 300 MHz have been recorded at 4.2 K, even for very low Co concentration −0.15%. The identical spectrum shapes for the concentrations 0.0015 and 0.015 show that these spectra are free from the satellite lines due to local environment effects and are representative of the isolated Co atoms in the Nd2Fe14B lattice. A high frequency triplet structure in these spectra, with the maxima of intensity at 249, 260, and 273 MHz, has been identified as arising from a single crystallographic position. With increasing Co content the triplet progressively evolves towards a doublet and shifts rapidly to lower frequencies: 235, 247 MHz for x=0.15. This doublet has been traced through the whole Co concentration range down to pure Nd2Co14B,1 and has been assigned to 16k2 sites based on an NMR spin reorientation study.2 Independent evidence for single site origin of the triplet structure is based on NMR line shape simulation in the special case of an NMR signal, with strong hyperfine field anisotropy, originating from conical domain walls in the canted magnetic structure of Nd2(FeCo)14B. The 16k2 structure, for the lowest Co concentration, contains 60% of the overall spectrum intensity and slowly decreases to around 50% for x=0.15. the rest of the spectral intensity is divided amongst four other lines located at the frequencies 156, 190, 202, and 213 MHz. The ratio of the respective intensities of these lines is close to 1:4:2:1, indicating that they originate from the 4e, 16k1, 8j, and 4c sites, respectively. The results obtained confirm that Co enters preferentially the 16k2 sites and avoids one of 8j sites in Nd2Fe14B structure.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 69 (1991), S. 6043-6045 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: 59Co NMR has been studied at 4.2 K and as a function of temperature in the mixed (Nd1−xYx)2Co14B compounds throughout the full substitution range. It was found that the anisotropy of the Nd sublattice determines the canted magnetic structure of the system at 4.2 K up to the threshold Y content of 92%. Above 92% Y, the system switches rapidly to a planar structure which is enforced by the 3d sublattices. Below the threshold Y content, the system undergoes two spin reorientations with increasing temperature: a second-order phase transition from canted to uniaxial state and a first-order phase transition from uniaxial to planar structure.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    s.l. ; Stafa-Zurich, Switzerland
    Materials science forum Vol. 30 (Jan. 1991), p. 177-186 
    ISSN: 1662-9752
    Source: Scientific.Net: Materials Science & Technology / Trans Tech Publications Archiv 1984-2008
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics
    Type of Medium: Electronic Resource
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