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  • 1
    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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  • 2
    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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  • 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.] : 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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  • 5
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 64 (1988), S. 5586-5586 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The 10B, 11B, and 57Fe spin-echo nuclear magnetic resonance (NMR) and magnetization experiments have been performed for naturally abundant and 10B-enriched Nd2Fe14B at 1.3 and 4.2 K for frequencies from 10 to 80 MHz. It was found from a comparison of NMR spectra in zero field and in an external field of 6.0 kOe that the hyperfine fields at the domain edges and at the domain-wall centers are nearly the same. This implies that the Fe hyperfine field anisotropy is small in this system. The presence of spin canting was verified by the result that the 11B NMR frequency shift due to the applied external magnetic field does not exactly follow γ(11B)ΔH. The NMR technique proves to be sensitive in detecting the trace of Fe precipitate in the Nd-Fe-B permanent magnets.
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 63 (1988), S. 3710-3712 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: R2Fe14−xGaxB (R=Pr and Nd) and PrCo5−xGax alloys were synthesized and examined by powder x-ray diffraction at room temperature and by magnetometry in the temperature range 4.2–1100 K. Lattice parameters, Curie temperature, spin-reorientation temperatures, anisotropy fields, and saturation magnetizations were determined. Phase analysis revealed that single-phase materials exist only for x≤1 in the case of 2:14:1 alloys and for x≤2 for 1:5 alloys. An increase in lattice parameters is observed upon Ga substitution in all cases. About 20 K increase in the Curie temperature is observed for 2:14:1 alloys, whereas there is a dramatic decrease in 1:5 alloys. Saturation magnetization values decrease upon Ga substitution. The anisotropy field is slightly enhanced by Ga addition in the Nd2Fe14−xGaxB system. Spin-reorientation phenomena in Nd2Fe14−xGaxB and PrCo5−xGax are strongly affected by Ga addition. The observed behavior is discussed in terms of preferential substitution of Ga atoms into the Nd2Fe14B-type crystal structure and random substitution into the CaCu5-type crystal structure.
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 63 (1988), S. 3719-3721 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: 10B, 11B, 57Fe, and 59Co spin-echo NMR experiments have been performed for naturally abundant and 10B-enriched Nd2Fe14B and Nd2Fe14−xCox B (x≤0.7) at 1.3 and 4.2 K for frequencies from 10 to 300 MHz. The Fe hyperfine field (HF) values in the Nd2Fe14B compound and their assignment to the six iron sites are the following: 302(e) 320(c) 325(k1), 334( j1), 352(k2), and 378( j2) kOe. The substitution of Co for Fe decreases the HF at the Fe nuclei at j2, k2, j1, k1, and c sites while no obvious change in the HF at the e site nor at the B nuclei has been found. The spin-echo amplitude corresponding to the Fe(k2) site line decreases with increasing Co content. A complex 59Co spectrum is found in the frequencies between 150 and 260 MHz with a strong peak around 250 MHz. These results confirm that Co atoms have a strong preference to enter the k2 site.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 61 (1987), S. 3439-3441 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The R2Co14−xSixB systems (R=Y, Pr, and Nd) have been synthesized for x ranging from 0.0 to 3.0 and found to have the tetragonal crystal structure for x≤2 in Pr- and Nd-based systems and for x≤1.6 in Y-based systems. Bulk magnetization measurements have been carried out in the temperature range 4.2–1100 K to determine the saturation magnetizations, anisotropy fields, Curie temperatures, TC, and spin-reorientation temperatures for different Si contents. A decrease of the TC and the saturation magnetization was observed with increasing Si content. The anisotropy field in Pr- and Nd-based systems was found to increase at 77 K and decrease at 295 K. The high-temperature spin reorientations for Nd- and Pr-based systems disappear for x≥1.3 and 1.0, respectively. The low-temperature spin reorientation observed in Nd2Co14B also vanishes for x〉0.3. The observed features are discussed in terms of weakening the 3d sublattice magnetization and its anisotropy due to Si dilution.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 61 (1987), S. 3471-3471 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The easy direction of magnetization (DOM) is an extremely important property of a magnetic material, in regards to both permanent magnet and recording applications. In many magnetic materials, most notably Nd2Fe14B, the DOM is temperature dependent. When utilizing methods which permit the orientation of either a single crystal or pseudo-single crystal to be rigidly constrained (e.g., VSM and extraction), it is possible to determine the temperature dependence of the DOM directly. However, the determination of spin reorientation temperatures with powder samples is not always straightforward. In some cases, a peak is observed in the magnetization versus temperature curve, while in others either a drop or an increase is observed. Using a two-dimensional, two-crystallite grain as a model and assumed temperature dependencies of the anisotropy constants, K1 and K2, it is shown that these peaks and other features can be explained by polycrystalline particles (or, equivalently, imperfect alignment of the powder). It is further shown that spin reorientation temperatures are invariably characterized by the inflection points in the low-field magnetization versus temperature curve. Examples of such curves obtained from a Faraday balance for Nd2Fe12Si2B and Pr2Co14B are given.
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    Springer
    Hyperfine interactions 50 (1989), S. 701-705 
    ISSN: 1572-9540
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract The results of57Fe Mössbauer effect measurements and magnetic studies performed on Dy2Fe14C and Er2Fe14C compounds are reported. The magnetic contributions of different iron sites are estimated and compared with those of corresponding boron compounds. The magnetic behaviour of the studied compounds is analysed in the molecular field approximation considering a two sublattices ferrimagnet.
    Type of Medium: Electronic Resource
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