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  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 67 (1990), S. 5863-5863 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Among systems of the type Mn(SCN)2(ROH)2, where R=CH3, C2H5, i-C3H7, or n-C3H7, only the title compound with R=i-C3H7 fails to exhibit a magnetic ordering transition in the vicinity of 10 K. As with the other members of this series, superexchange interactions between manganese ions are mediated by bridging thiocyanate ions, but for the isopropanol compound a distinctly different type of bridging network is revealed by a crystal structure determination.1 The structure, presented and described in detail, is monoclinic, P21/n, Z=2 with a=11.584(2) A(ring), b=5.781(1) A(ring), c=11.163(2) A(ring), and β=111.86(1)°. Only along the b axis do efficient thiocyanate superexchange bridges occur, so that magnetically one-dimensional behavior can be anticipated. This is evident in susceptibility measurements, which reveal a broad maximum near 16 K and which can be fit reasonably well assuming one-dimensional antiferromagnetic Heisenberg model behavior. A magnetic anisotropy of a few percent is also evident in the single-crystal susceptibility. No magnetic ordering appears to occur down to a temperature of about 1.65 K.
    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 67 (1990), S. 5857-5859 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The magnetic properties of MnCl2⋅H2O, a heretofore unexamined hydrate of manganese dichloride, have been studied. The behavior is clearly distinguishable from that of the anhydrous material or either the dihydrate or the tetrahydrate. At high temperatures the susceptibility is Curie–Weiss-like, with a Weiss constant θ=−4.9±0.3 K in χM=C/(T−θ); this may be compared with the values θ=−3.3 K for the anhydrous material, −14.5±0.3 K for the dihydrate (as determined in this work), and −1.8 K for the tetrahydrate. Departures from linearity occur below 20 K, and a broad maximum in the powder susceptibility appears at T(χmax)=3.60±0.10 K with χmax=0.304±0.003 emu/mol. The susceptibility drops sharply below 2.23 K, and ∂χ/∂T is a maximum at 2.16±0.01 K, which is identified with the Néel temperature Tc. Certain features of the data suggest two-dimensional Heisenberg model behavior, for example the ratios Tc/||θ||=0.44 and Tc/T(χmax)=0.60. However, fits to χ(T) using a high-temperature series expansion for the S=5/2 two-dimensional square planar Heisenberg model are unconvincing, as are similar attempts based on a three-dimensional model. In contrast, the model of a classical Heisenberg antiferromagnetic spin chain scaled to S=5/2 permits an excellent fit, with J/k=−0.49±0.04 K the intrachain exchange (in Hˆex=−2J∑i〉 jSˆi⋅Sˆ j). An interchain exchange of ||J'/k||=0.015±0.004 K, probably antiferromagnetic, can also be inferred, from the antiferromagnetic transition at Tc =2.16 K. The intrachain exchange is very similar to that in MnCl2⋅2H2O, while the interchain exchange is much weaker.
    Type of Medium: Electronic Resource
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