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  • 1
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The dilute insulating ferromagnet Fe1−xAsx[S2CN(C2H5)2]2Cl is examined in single crystal form for several compositions spanning the range x=0.014 to x=0.040. For x=0.0143 and x=0.0162 crystals, the inverse molar susceptibility along the [101] ferromagnetic easy axis is quite linear in temperature for T greater than a few times Tc. In the case of x=0.0313 and x=0.0402 crystals, in contrast, significant curvature appears in χ−1vs T throughout the 20–80 K temperature range. The initial (low-field) susceptibility along [101] for each crystal is measured in the critical region and analyzed via a standard power law form χ0=Γt−γ, where t=(T−Tc)/Tc. Tc decreases with increasing x, but somewhat slowly. The critical exponent γ increases with increasing x, from 1.19±0.01 near x=0.014 to 1.22±0.01 near x=0.040. The prefactor Γ is significantly smaller for the two higher As crystals, probably due to increased disorder. The variation in γ is not entirely unexpected, since the pure material, which is a candidate Z2xS1 system, has an unusual set of critical exponents, including a large positive α. Thus new critical behavior on dilution can occur by the Harris criterion. © 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 75 (1994), S. 5940-5942 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The fully deuterated form of previously studied Fe[S2CN(C2H5)2]2Cl, needed for neutron diffraction and scattering measurements, has been prepared for the first time and its magnetic behavior in single crystal form studied at low temperatures. Susceptibility and magnetization data show that Fe[S2CN(C2D5)2]2Cl has extremely similar magnetic anisotropy to the normal material: the monoclinic [101] direction is the only easy axis of ferromagnetism, with the orthogonal [010] and (1¯01)⊥ axes even showing antiferromagnetic-like maxima in their χ(T) near Tc. Only along [101] does M approach saturation at low fields. Analysis of χ(T) in the paramagnetic regime, assuming axial and rhombic crystal field distortions described by H= D[Sˆ32z−S(S+1)/3]+E[Sˆ32x −Sˆ32y] and including exchange interactions in a mean field approximation, leads to D/k=−3.03(5) K, E/k=−0.49(4) K, and zJ/k=0.99(3) K along with gx=2.058(20), gy=2.060(20), and gz=2.080(20). These parameters are rather similar to those of the normal material, though zJ/k is significantly larger. The ordering temperature, obtained from a critical law fit to [101] data in a small field, i.e., χ0=Γt−γ, is Tc=2.486(2) K, with γ=1.16(1) and Γ=1.07(5) emu/mol. The critical exponent γ is the same as in the normal material and corresponds to the theoretical value in Kawamura's Z2×S1 model. An ∼1.2% enhancement in Tc over that of the normal material occurs, which may be due to slightly closer molecular packing. 75.30.Kz, 75.30.Cr, 75.30.Gw, 75.40.Cx
    Type of Medium: Electronic Resource
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