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  • 11
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 69 (1991), S. 5807-5809 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Recent magnetic susceptibility measurements on polycrystalline MnCl2⋅H2O indicate that it behaves like a quasi-one-dimensional antiferromagnet. The heat capacity of this compound has now been measured between ∼0.5 and 80 K in a liquid-3He-cooled vacuum calorimeter. Cp exhibits a large, sharp λ-type peak at TN = 2.18 ± 0.01 K marking the onset of long-range spin order. The critical entropy S(TN) is found to be ∼0.40R ln 6, confirming the short-range, low-dimensional nature of most of the spin ordering. An anisotropic elastic continuum model has been used to calculate the contribution of lattice vibrations to Cp. The data above ∼3 K are well represented by this model (with suitable choice of three parameters) plus the theoretical heat capacity of the 1D Heisenberg antiferromagnet with S =5/2 and exchange constant J/k=−0.45 K. Below ∼ 0.7TN, the magnetic part of Cp is well described by an anisotropic 3D spin-wave model with Jz/k = J/k = −0.45 K, Jx/k = Jy/k = −0.015 K, and an anisotropy field HA ≈ 3.3 kOe. The intra- and interchain exchange constants agree well with those inferred from χM. 〈lz〉
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  • 12
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 87 (2000), S. 6052-6054 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The magnetic behavior of NiCl2⋅H2O has been studied for the first time. A Curie–Weiss fit, χM=C/(T−θ), to the susceptibility between 90 and 300 K yields g=2.23±0.01(S=1) and θ=30.4±0.05 K. Systematic curvature in χ−1(T) is evident below 90 K. Despite the very positive θ, NiCl2⋅H2O appears to order antiferromagnetically at Tc=5.65±0.1 K, somewhat below a maximum in χ(T) at T(χmax)=8.4±0.1 K, with χmax=0.1297±0.0005 emu/mol. The ratios Tc/T(χmax)=0.67±0.01 and Tc/θ=0.186±0.005 suggest lower magnetic dimensionality, most likely one-dimensional character. Plausible looking fits to the low temperature susceptibility based on a one-dimensional antiferromagnetic Heisenberg model can be obtained. However, these presuppose antiferromagnetic intrachain exchange, and in NiCl2⋅H2O such exchange is almost certainly ferromagnetic, with weaker antiferromagnetic interchain interactions. Well above Tc the susceptibility can be accounted for assuming axial and rhombic crystal-field distortions, i.e., D[S(circumflex)z2−S(S+1)/3] and E[S(circumflex)x2−S(circumflex)y2] spin Hamiltonian terms, with exchange included in a mean field approximation. In the absence of single crystal data the parameters are only provisional, but clearly |D| and |E| are very large; the associated mean exchange interaction zJ/k=25.1 K is consistent with the observed θ value. Magnetization versus field isotherms exhibit an unusual evolution in shape with varying temperature; significant hysteresis is present even for temperatures somewhat above Tc. © 2000 American Institute of Physics.
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  • 13
    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.
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  • 14
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 87 (2000), S. 6540-6542 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The title system is the first mixed insulating magnet to be examined composed of three separate magnetic components. Each of the three possible binary mixtures based on the same isostructural MCl2⋅2H2O components has been examined. The Co/Fe mixture has competing orthogonal spin anisotropies, the Co/Mn mixture competing ferromagnetic and antiferromagnetic exchange interactions, and the Fe/Mn mixture both competing anisotropies and competing exchange interactions. Hence various pairwise competitions will occur in a ternary mixture of these components. Four different compositions are examined, with (x,y)=(0.830,0.681), (0.623,0.464), (0.539,0.377), and (0.366,0.272). These provide representative coverage of several interesting regions in the three binary T−x phase diagrams, specifically in terms of a relative binary composition (rbc) which can be defined for a ternary mixture in pairwise fashion. High temperature susceptibilities follow a Curie–Weiss form χM=C/(T−θ) rather well. Curie constants are approximately as expected based on fractions of different metal ions present, and both C and θ are closest to values characterizing the Co/Mn binary mixture. Low temperature susceptibilities exhibit features suggesting phase transitions. The temperatures at which these occur are often close to what might be anticipated from the binary T−x phase diagrams for the appropriate rbc. In certain cases, however, transitions anticipated on such a basis do not seem to be present. The ternary mixtures also exhibit behavior suggestive of spin glass properties. © 2000 American Institute of Physics.
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  • 15
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 63 (1988), S. 3569-3571 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Three new members of the title series, where R=CH3, C2H5, i-C3H7 or n-C3H7, have been studied in addition to the previously examined ethanol homologue. A crystal structure for the methanol compound reveals a two-dimensional network of manganese ions bridged by thiocyanate groups with methanols separating they layers. The situation is somewhat similar to that occurring for the ethanol compound, in which magnetic quasi-two-dimensionality was apparent. On the other hand, for the isopropanol compound a crystal structure suggests more nearly one-dimensional magnetic character. Weiss constants in Curie–Weiss fits to high-temperature data are −22.4, −20.9, −20.5, and −37.2 K for the methanol, ethanol, n-propanol, and isopropanol systems, respectively. The susceptibilities exhibit broad maxima at about 12.7 K for the methanol and n-propanol systems and about 16.0 K for the isopropanol system. All but the isopropanol exhibit a phase transition at about 10 K. For the methanol and ethanol systems weak ferromagnetism occurs below the ordering temperature; this appears not to occur for the n-propanol system. Susceptibility data are analyzed on the basis of two-dimensional (methanol, n-propanol) or one-dimensional (isopropanol) S=5/2 antiferromagnetic Heisenberg models. The exchange interaction is substantially stronger in the isopropanol than in the other members of the series.
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  • 16
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 61 (1987), S. 3298-3300 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Single-crystal susceptibility and magnetization data have been obtained for this unusual Cu(II) metamagnet. The structure has also been determined and is monoclinic, P21/c, with two magnetic ions per unit cell. Structural details strongly suggest an effective lattice dimensionality of two. This is confirmed by the failure of the high-temperature susceptibility to conform to a Curie–Weiss law, and by an excellent fit to the susceptibility data using a high-temperature series expansion for the square-planar, S=1/2, Heisenberg model, with g=2.144 and J/k=20.1 K. The single-crystal susceptibility is markedly anisotropic below the approximately 9.55-K Néel temperature, and is also somewhat anisotropic above it. Metamagnetic transitions are clearly observed along the b easy axis, the transition field being quite small (Hc≈31 G near 0 K) and decreasing with increasing temperature. The interlayer antiferromagnetic exchange is estimated to be only about 0.0094 K.
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  • 17
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 57 (1985), S. 3460-3460 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Magnetization and susceptibility measurements have been made on the title system in order to determine the phase diagram (T vs x plane) and to investigate hysteretic and time-dependent effects. The pure constituents are rather isotropic (Mn) and rather anisotropic (Co) isomorphous antiferromagnets which order at 6.7 and 17.2 K, respectively. The ordered spin arrangements are of different periodicity, and competing ferromagnetic and antiferromagnetic interactions can be anticipated in mixtures. Anomalies in susceptibility versus temperature reveal the presence of paramagnetic- (antiferromagnetic) phase boundaries. The transition temperatures lie on curves Tc(x) which descend fairly sharply from the two sides of the phase diagram; i.e., the pure component ordering temperatures are not connected by a continuous phase boundary. In all mixtures lower transitions are observed as well. Below these transitions more significant hysteresis in magnetization versus field is observed than above them, and in certain mixtures pronounced time dependences also. The thermoremanent magnetization and the isothermal remanent magnetization as a function of field in a 54%-Co/46%-Mn sample exhibit maxima, and have a general appearance typical of spin glasses. The time dependence, followed long enough, appears to be neither logarithmic nor algebraic in form, but rather more nearly that of a "stretched'' exponential.
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  • 18
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The magnetic properties of Fe[S2CNC4H8]2I have been studied, the first pentacoordinate Fe(III) system of this type with a cyclic terminal group, rather than an alkyl group, to be examined in detail. The susceptibility of a polycrystalline sample is of Curie–Weiss form above 30 K, with g¯=2.16 ±0.02 and S=3/2 and with θ=−0.75±1.0 K. Thus the unusual intermediate spin state occurs here as in earlier examples. The susceptibility can be fit quite well down to about 6 K assuming that axial and rhombic crystal field distortions occur, represented by D[Sˆ2z − S(S + 1)/3] and E[Sˆ2x − Sˆ2y] terms in the spin Hamiltonian, and incorporating exchange interactions in a mean-field approximation. Fitted parameters are D/k=9.3± 0.5 K, E/k=−0.6±0.2 K, gx=2.23± 0.05, gy= 2.19 ± 0.05, gz=2.04 ± 0.05, and zJ/k=−0.235 ±0.02 K. At low temperatures the susceptibility exhibits a broad maximum with T(χmax)=3.23± 0.04 K and χmax =0.376±0.004 emu/mol. An antiferromagnetic transition at Tc=2.21±0.01 K is inferred from the position of a maximum in (∂χ/∂T), an ordering temperature in reasonable agreement with earlier Mössbauer results. The ratio Tc/T(χmax) =0.68±0.01 is suggestive of quasi-two-dimensionality. In the region of the maximum an acceptable fit according to a 2D- XY model with plausible parameter values can be achieved, but only with a ferromagnetic interlayer exchange interaction about 28% as strong as the leading antiferromagnetic intralayer interaction. Isotherms of M vs H show somewhat unusual curvature, the explanation of which is unclear.
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  • 19
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 69 (1991), S. 6004-6006 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The magnetic properties of Ni(SCN)2(C2H5OH)2 have been studied, the first Ni(II) system in the general family of compounds M(SCN)2(ROH)2 (where M=divalent Mn, Fe, Co, or Ni and R=CH3, C2H5, i- or n-C3H7) to be examined at low temperatures. In contrast to previously studied Mn(II) and Co(II) members of this family, which exhibit predominant antiferromagnetism, the present compound is ferromagnetic. The susceptibility of a polycrystalline sample is of Curie–Weiss form only above 75 K, with g¯ = 2.175 ± 0.01 and S=1 and with θ=24.1±1.0 K. The initial susceptibility is well accounted for by an asymptotic critical law, χ0 = Γ[T/Tc − 1]−γ, in the reduced temperature range 0.147–0.013, with Tc = 13.081 ± 0.01 K, γ=1.354±0.02, and Γ=0.0925±0.003 emu/mol. The γ value is between 3D-XY and 3D-Heisenberg model predictions. The susceptibility in the paramagnetic regime well above Tc is analyzed including the effects of axial and rhombic crystal field distortions, represented by D[Sˆ2z − S(S + 1)/3] and E[Sˆ2x − Sˆ2y] terms in the spin Hamiltonian, and incorporating exchange interactions in a mean-field approximation. An excellent fit is obtained with g=2.175, D/k=−64.3±5 K, E/k=23.1±4 K, and zJ/k=19.4±1 K. The magnitude of D is the largest we know of in a Ni(II) compound. The three spin states of the 3A crystal field ground term are strongly split, probably contributing to the relatively low value of Tc compared to zJ/k. Some two-dimensional character in the exchange, as has been found for other members of this family of compounds, may also contribute.
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  • 20
    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.
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