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  • 1995-1999  (4)
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  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 79 (1996), S. 4718-4720 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The trihydrate of nickelous bromide, NiBr2⋅3H2O, is examined magnetically for the first time. A Curie–Weiss fit, χM=C/(T−θ), to the susceptibility between 70 and 300 K yields g=2.31±0.01 (S=1) and θ=6.6±0.5 K. Systematic curvature in χ−1 vs T is evident below 70 K. Despite the positive θ, NiBr2⋅3H2O appears to order antiferromagnetically at Tc=3.82±0.05 K, somewhat below a maximum in χ(T) at T(χmax)=6.17±0.10 K, with χmax=0.0900±0.0005 emu/mol. The ratio Tc/T(χmax)=0.62±0.01 suggests lower magnetic dimensionality. Between 4 and 12 K an acceptable fit with a two-dimensional Heisenberg model can be made, with g=2.58±0.01, J/k=−1.36±0.02 K (assuming Hˆex=−2J∑i(approximately-greater-than)jSˆi⋅Sˆj), and a correction for interlayer exchange z′J′/k=−0.99±0.02 K. Well above Tc the susceptibility is analyzed assuming axial and rhombic crystal field distortions, i.e., D[Sˆ2z−S(S+1)/3] and E[Sˆ2x−Sˆ2y] spin Hamiltonian terms, with exchange included in a mean field approximation: g=2.33±0.02, D/k=57.3±5.0 K, E/k=−24.9±3.0 K, and zJ/k=5.28±0.20 K. The parameters are provisional lacking single-crystal data, but the zero-field splitting is clearly quite large. Magnetization versus field isotherms depart only slightly from linearity for fields above 10 kG, and show a small hysteresis, even for temperatures above Tc. It is likely that ferromagnetically coupled NiBr2NiBr2Ni... chains are present, and that there are antiferromagnetic interactions between chains, such that strongly coupled layers occur, with weaker interactions between layers. © 1996 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 2
    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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  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4527-4529 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Reported here are field-cooled (FC) and zero-field-cooled (ZFC) magnetizations (MFC and MZFC, respectively) in smaller and larger fields than used in previous work, and thermoremanent magnetization data (TRM) for various temperatures and wait times. For fields of 12.8 and 0.1 G a separation between MFC and MZFC develops near 9 K, well below the 16.1 K magnetization maximum or the ∼14 K antiferromagnetic transition; thus, reentrant behavior occurs as for the higher fields used previously. Maxima in MZFC(T) are observed at 7.2 and 8.0 K for 12.8 and 0.1 G, respectively. Similar measurements in fields of from 3.0 to 15.5 kG show an evolution in the form of MFC(T) and MZFC(T); the separation between these develops at somewhat higher temperatures than 9 K and no maximum appears in MZFC. The field dependence of (MIRR/H)MAX, where MIRR=MFC−MZFC, is determined and shows a change in regime between 2 and 3 kG. The TRM as a function of time is measured for temperatures of 1.6, 4.3, and 5.8 K, with wait times ranging from 10 to 500 min. The relaxation rate is quite small, consistent with glassy dynamics with a wide distribution of relaxation times, and increases with increasing temperature. Remarkably, however, aging effects are absent even at 5.8 K, although this is 69% of the splitting temperature between MFC and MZFC. An explanation may reside in randomized antiferromagnetic couplings between chemical chains which are individually ordered ferromagnetically, and in the formation of a structure of almost independent clusters. © 1999 American Institute of Physics.
    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 81 (1997), S. 4403-4405 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The latest member of the new series of transition metal dichloride monohydrates to exhibit novel magnetic behavior is FeCl2⋅H2O. Reported here are field cooled and zero-field cooled magnetizations (MFC and MZFC, respectively) for different fields as a function of temperature, and time-dependent thermoremanent magnetizations (TRM) for different temperatures and wait times. Near 20.4 K a peak appears in both MFC and MZFC using H=106 G, as seen previously. In the smaller fields of 26.5 and 0.1 G, MFC is more nearly constant for temperatures below the 20.4 K peak in MZFC which still appears. The irreversible magnetization, MFC−MZFC, is more pronounced for lower measuring field. Unusual behavior is seen in the temperature and wait-time (tw) dependence of TRM(t). Data at 4.4 K (0.22Tc) show no wait time, or aging, effects, using a cooling field of 9.95 G. At 15.1 K (0.74Tc), for the same cooling field, differences occur among TRM(t) data for tw=10, 100, and 500 min. The data become essentially coincident, however, if the measuring time is scaled by the wait time. Although the general behavior is similar at 18.0 K (0.88Tc), there is a noticeable shift of the tw=500 min data in this case. The results suggest that below the critical temperature the system must equilibrate among a huge number of metastable states. It takes an almost infinite time to probe all these states below 0.88Tc, which explains the t/tw scaling. At 0.22Tc, the system remains stuck in one specific state and the aging disappears. Two different time scales appear to control the relaxation. The observed properties are not altogether typical of spin glasses, and the system may better be viewed as a weakly and randomly coupled array of ferromagnetic chains, in which dynamic domains readily form and evolve, and in which the aging effects are associated with domain wall growth. © 1997 American Institute of Physics.
    Type of Medium: Electronic Resource
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