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  • 1
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Results of a pulsed NMR study of the soft ferromagnetic amorphous alloy Co74.26Fe4.74Si2.1B18.9 in the as-cast and the heat treated (at 410 °C for 12 minutes) states re reported. The measurements were performed at 4.2 K. Very intense resonances lines are observed in the frequency region 10–110 MHz (range of the present study), for both as-cast and heat treated samples. The NMR signal intensity depends on the rf power level; this suggests the existence of several magnetic regions with different local anisotropies. We identify NMR lines in two frequency ranges: (a) 10–50 MHz, which probably come from 57Fe, 11B, and 29Si nuclei in Fe–Si-like regions and 57Fe in Co(Fe) solid solutions; and (b) for frequencies above 50 MHz, lines from 59Co (and probably 11B) in Co-rich crystalline-like environments with short-range order as in Co2B, in the range 70–110 MHz. In the higher frequency region, the NMR spectra suggest that the environments are similar to Co3B and to Co(B) solid solutions. For the heat treated sample, lines above 95 MHz disappear for lower rf power levels; also, this sample shows lines around 75 MHz narrower than those for the amorphous alloy. These results give evidence of the concentration inhomogeneity of the samples, both in the as-cast and heat-treated forms. © 1996 American Institute of Physics.
    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 70 (1991), S. 7632-7634 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: 89Y pulsed nuclear magnetic resonance measurements have been performed at low temperatures in (RxY1−x)Fe2 compounds, where R is a heavy rare-earth (Gd, Tb, Dy, Ho, Er, and Tm) in the range 0≤x≤0.05. The spectra were measured at 4.2 K, except for Dy (77.4 K). The spectra were analyzed in terms of direct and indirect (through common Fe neighbors) transferred hf interactions. The direct transferred hf field amounts to a few kOe per rare earth 1st neighbor; the indirect contributions of the first two shells are smaller by a factor of 10. We have found that a model that restricts the transferred hyperfine interactions to the indirect hf field or considers the first three neighbor shells in the same way is not satisfactory to explain the changes in the hyperfine field at Y nuclei.
    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 67 (1990), S. 5867-5869 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: In a previous work, 89Y measurements at 4.2 K in (RxY1−x)Fe2 compounds, with R=Tb and Ho and 0.05≤x≤0.20, have shown broad nuclear-magnetic-resonance (NMR) spectra, due to transferred hyperfine interactions. 89Y NMR signals could not be observed with R=Dy in the same composition range. In the present work, compounds were prepared with Dy in the concentration range 0.005≤x≤0.02 to investigate the origin of this anomaly. Compared to the pure YFe2 compound, the observed NMR spectra are broadened and show a shift towards higher frequencies. With increasing Dy concentration, the NMR signals fall very rapidly. Magnetization measurements at 4.2 K were performed in samples with Tb, Ho, and Dy; the results indicate that the behavior of the Dy compounds is qualitatively different in the low-magnetic-field region of the curves, requiring a minimum applied field to start increasing the magnetization. The NMR data and the magnetization results of the Dy compounds can both be explained as arising from a much lower mobility of the domain walls.
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  • 4
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 69 (1991), S. 5467-5467 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The magnetic behavior at T=0 K of a system consisting of conduction electrons coupled to localized electrons is studied in the molecular-field approximation with a simple exchange parameter distribution. The localized electrons are also submitted to an axial crystal field. We define an average ionic magnetic moment and obtain a condition for the spontaneous magnetic order involving the crystal field, the width, and the center of the exchange distribution. We also study the magnetic behavior in the para- and ferromagnetic regions of the phase diagram. In a previous study1 the same model was applied to a system containing a crystal-field distribution.
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  • 5
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 61 (1987), S. 3985-3986 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The intermetallic compound HoCo2 is magnetically ordered and changes its directon of magnetization around 15 K, as the temperature is increased, from [110] to [100]. We report a 59Co pulsed NMR study of HoCo2 in the temperature range 4–65 K. The NMR spectra show two peaks at low temperature and one peak at high temperatures, as expected from a model whereby the magnetic equivalence of the cobalt sites is determined by the direction of magnetization. This change in the spectra can be simulated from lattice sums of the magnetic dipolar fields acting on the cobalt sites. The present results are consistent with a change of direction of magnetization from [110] to [100] through intermediate directions contained in the plane z=0.
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  • 6
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 67 (1990), S. 4582-4584 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The magnetic behavior at T=0 K of a system consisting of conduction electrons coupled to localized electrons (e.g., 4f electrons), the latter submitted to an inhomogeneous crystal-field distribution, is studied. We consider a simple crystal-field distribution and define an average ionic magnetic moment using the results of the homogeneous case. We obtain a condition for the onset of spontaneous magnetic order and study the magnetic behavior in the paramagnetic and ferromagnetic regions of the phase diagram. The study implies that the inhomogeneity of the crystal field attenuates the quenching effects. The model is interesting to the study of disordered rare-earth intermetallic compounds.
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