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  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 74 (1993), S. 6847-6850 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Carbon was introduced by arc melting to RTiFe11, where R=Sm, Gd, Th, Dy, Ho, Er, and Y, and its effects on the crystallographic and magnetic properties of these compounds have been investigated by x-ray and magnetic measurements. The experimental results show that the carbon atoms occupy 8i sites in ThMn12 structure. It is found that the substitution does not have an effect on the Curie temperature, but instead increases both saturation magnetization and magnetocrystalline anisotropy. The intrinsic magnetic properties of SmTiFe11 are improved with the addition of the carbon atoms, indicating that SmTiFe11−xCx is a better candidate for permanent magnetic applications than SmTiFe11.
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 72 (1992), S. 2989-2992 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The crystallographic and magnetic properties of the series of R2Fe17CNx, where R=Y, Sm, Gd, Tb, Dy, and Er have been investigated in comparison with those of R2Fe17C and R2Fe17N3−δ. The results indicate that Sm2Fe17CNx, which possesses a higher Curie temperature, a larger saturation magnetization, and a stronger anisotropy field than Sm2Fe17C or Sm2Fe17Nx, seems to be a more favorable candidate for permanent magnet applications.
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  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 67 (1990), S. 4765-4767 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The crystallographic structure and magnetic behavior of R2(Fe1−xMnx)14B have been studied, where R represents Nd, Pr, and Y. A large coercive force of up to 20 kOe has been observed at 1.5 K in as-cast bulk samples of the pseudoternary compounds. The coercivity does not depend on treatment such as milling, sintering, and annealing. It is intrinsic. The intrinsic coercive iHc shows a composition dependence. The form of the virgin magnetization curves is characterized by a propagation field Hp, indicating that the coercive force is created by domain wall pinning. Based on the magnetic measurements, the domain wall thickness of these compounds was calculated. The magnetic behavior of R2(Fe1−xMnx)14B can be understood in terms of narrow domain walls.
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  • 4
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We succeed in inserting a number of nitrogen atoms into the RTiFe11 intermetallics. The nitrides retain the ThMn12-type structure, but with an increase in the unit cell volume. The crystallographic sites located by nitrogen atoms are determined by using neutron diffraction techniques. The nitrogen atoms are found to have an effect of increasing Curie temperature and saturation magnetization. Moreover, an essential change in magnetocrystalline anisotropy is observed upon nitrogenation. By all of these effects, the NdTiFe11N1−δ compounds have excellent intrinsic magnetic properties favorable for permanent magnet applications.
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  • 5
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We have carried out neutron diffraction measurements on powder samples of Nd2Fe17Nx and Y2Fe17Nx at room temperature. The refinements of the neutron data indicate that the nitrogen atoms occupy the 9e interstices in the nitride Nd2Fe17Nx (Th2Zn17 type, R3¯m) or the 6h interstices in the nitride Y2Fe17Nx (Th2Ni17 type, P63/mmc), respectively. At room temperature, both Nd2Fe17Nx and Y2Fe17Nx adopt a magnetic structure in which the easy magnetization direction is perpendicular to the c axis. Using the above results, we have briefly discussed the effect of a nitrogenation on the magnetocrystalline anisotropy of the Sm sublattice of Sm2Fe17Nx.
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  • 6
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 89 (2001), S. 2852-2856 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A systematic investigation of crystallographic and intrinsic magnetic properties of the compounds RFe9Si2Cx (R=Ce, Pr, Nd, Sm; x=0.5, 1.0, 1.5) has been carried out. The lattice parameters a, c and the unit cell volumes increase with increasing C contents, resulting in the increases of Curie temperatures by about 100–150 K between x=0.5 and x=1.5. The saturation magnetization of RFe9Si2Cx (R=Pr, Nd, Sm) at 1.5 K passes through a maximum at x=1.0, and then decreases slightly. Meanwhile, the average iron moment μFe at 1.5 K is 1.57μB for x=1.0 and 1.63μB for x=1.5 in CeFe9Si2Cx compounds. SmFe9Si2Cx compounds have uniaxial anisotropy with the anisotropy fields HA estimated around 132 kOe at 1.5 K and 50 kOe at 300 K (x=1.5), respectively. First-order magnetization processes are observed in the NdFe9Si2Cx compounds and the first-order magnetization processes critical field Hcr is found to increase with x. In addition, the critical temperature for the onset of the first-order magnetization processes transition is around 90 K in the case of x=1.0. © 2001 American Institute of Physics.
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  • 7
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Review of Scientific Instruments 65 (1994), S. 1479-1479 
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: The major purpose of this paper is to describe that organic impurities cause harm to the arc discharge in the multiampere DuoPIGatron ion source and attempt to analyze the mechanism. Though we knew before that the existence of oil in the source is always harmful, for financial reasons, we had to use the available oil pump to pump gas. But we did not think that the oil pollution in the discharge chamber of the source could cause arc discharge failure so seriously that the source cannot operate normally. After encountering and solving the problem, we have recognized the severe action of oil pollution, and seen the damage mechanism. The up-stream oil vapor from big pumps entered the chamber of the plasma generator. Should the parts of plasma chamber, especially, the target cathode be polluted by oil vapor, it resulted in destroying the reflected discharge in the chamber so that the stable condition of plasma, that is Iig(very-much-greater-than)Iil could not be maintained. Here Iig and Iil represent generated and lost ion current, respectively. The arc discharge died. After protecting the target cathode from oil pollution by various ways, our 15-cm duoPIGatron can keep high performance operation for more than one year without recleaning. During this period, the arc current was larger than 300 A and the saturated ion current was above 234 mA/cm2.
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  • 8
    Electronic Resource
    Electronic Resource
    Westerville, Ohio : American Ceramics Society
    Journal of the American Ceramic Society 81 (1998), S. 0 
    ISSN: 1551-2916
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics , Physics
    Notes: Conventional transmission electron microscopy (TEM), coupled with energy-dispersive X-ray (EDX) analysis, has been used to examine the intermediate phases produced during the transformation of Ba-Al-alpha-Al2O3-SiO2 (cristobalite) precursors into celsian, BaAl2Si2O8. Analyses were conducted on samples that had been exposed to pure, flowing oxygen at peak temperatures of 300°C for 24 h, 650°C for 72 h, or 900°C for 24 h. Particles of Al2O3 retained after the 300-900°C heat treatments were coated with a layer of BaAl2O4. An amorphous, alumina-poor Ba-Al-Si-O (G1) phase was observed in contact with residual SiO2 particles after the 650°C heat treatment. Although not a starting component of the precursor, elemental silicon was also detected after the 300-900°C heat treatments. Silicon particles produced during the 300°C heat treatment were surrounded by an amorphous Ba-Al-Si-O (G2) phase that contained more alumina than the G1 phase. Fine-grained barium orthosilicate (Ba2SiO4) and sanbornite (BaSi2O5) were observed after the 650°C treatment, along with thin, plate-shaped grains of BaAl2Si2O8. The latter two phases were surrounded by an amorphous Ba-Al-Si-O (G3) phase that possessed less alumina than the G2 phase. Smaller platelets of BaAl2Si2O8 were also detected after the 300°C treatment. After annealing at a peak temperature of 1650°C, BaAl2Si2O8 was the only silicate compound detected by TEM. Novel reaction paths to BaAl2Si2O8, which are consistent with the present TEM observations and prior XRD and SEM/EDX analyses (Part I), are discussed.
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  • 9
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 75 (1994), S. 5441-5443 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: A study of the permanent magnetic properties of Pr(Mo, Fe)12Nx powders has been carried out by using a mechanical alloying technique. The variations of coercive force and remanence as a function of composition and crystallizing temperature have been investigated. A coercive force of up to 6.0 kOe was obtained. The temperature dependence of the coercive force is presented in comparison with that of Nd2Fe14B-type magnets.
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  • 10
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The permanent magnetic properties of isotropic and anisotropic powders of R(Fe,Mo)12Nx compounds, where R=Pr and Nd, were investigated by using mechanical alloying and a conventional milling process. For the isotropic magnetic powders, a coercive force of up to 9 kOe and a maximum energy product of 6.6 MGOe were obtained in Nd compounds, while with the anisotropic powders a maximum energy product of 12 MGOe was achieved. In the isotropic Pr(Fe,Mo)12Nx compounds the best result were 4.5 MGOe for (BH)max and 6.0 kOe for iHc. The temperature dependence of coercive force has been investigated in a temperature range between 300 and 500 K, and the results are reported in a comparison with that of Nd-Fe-B magnets.
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