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  • 1
    ISSN: 1520-5126
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology
    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 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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  • 3
    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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  • 4
    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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  • 5
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 75 (1994), S. 5529-5531 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Recent magnetic studies of polycrystalline CoCl2⋅H2O showed an antiferromagnetic ordering transition at TN∼14 K and an apparent spin glass transition at ∼7 K. We now have extended the magnetic susceptibility measurements up to 300 K. The results above TN can be well described if the lowest electronic states of Co2+ in this salt are two Kramers doublets separated by ΔE/k=230 K, and if a predominantly ferromagnetic mean field interaction is introduced. The heat capacity of CoCl2⋅H2O over the range 0.6–80 K has also been measured. Below ∼10 K, Cp≈aT−2+bT3. The first term is the hyperfine contribution of the 59Co2+ nuclei. The second is the sum of lattice vibrational and electronic spin parts. Cp exhibits a λ-type peak at TN1=15.0±0.05 K, and a second λ anomaly of comparable size at TN2=13.9±0.05 K, which appears to be associated with a spin reorientation transition. Correcting the observed Cp data for the nuclear spin contribution, one may calculate the sum of lattice vibration and electron spin entropies, and thus obtain at TN1 an upper limit to the critical magnetic entropy. This amounts to 0.38 R ln 2, suggesting that a substantial part of the spin ordering in this system is of short-range and lower dimensionality. Cp also exhibits an inflection point near 4.5 K, where an unusual feature in the temperature dependence of the spin glass thermoremanent magnetization was found.
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 73 (1993), S. 5503-5503 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Previous magnetization and susceptibility measurements on the mixed magnet Co1−xMnxCl2⋅2H2O disclosed a spin glass transition near 2.45 K over a wide composition range.1 Recent heat capacity and NMR measurements have confirmed and extended this finding.2 The time dependence of the thermoremanent magnetization (TRM) below Tg for an x=0.452 mixture was studied in some detail1 and was found to conform approximately to a decay of stretched exponential type, or perhaps slightly more accurately to the product of a stretched exponential and a power law. Small systematic deviations of data from fitted curves were apparent however. Recently a percolation model for relaxation in random systems was proposed,3 and yielded significantly improved fits to the TRM decay in an Au:Fe spin glass. The model assumes dispersive excitations within fixed finite domains, and includes as parameters the fastest and slowest relaxation rates characterizing the spectrum of domains. We find that this model also permits much better fits to be obtained for the TRM decay in Co1−xMnxCl2⋅2H2O, x=0.452. Systematic deviations that were present when using more traditional decay functions are virtually eliminated. The variation of fitted parameters with cooling field and temperature is also explored.
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 73 (1993), S. 5386-5388 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The magnetic behavior of Ni(SCN)2 has been studied at low temperatures for the first time. A Curie–Weiss fit, χM=C/(T−θ), to the susceptibility between 100 and 300 K yields g=2.13±0.01 (S=1) and θ=39.8±1.4 K. Systematic curvature in χ−1 vs T is evident, however. Despite the large positive θ Ni(SCN)2 appears to order antiferromagnetically at Tc=52±1 K, slightly below a maximum in χ(T) at T(χmax)=57.2±0.5 K, with χmax=0.0331±0.0003 emu/mol. The ratio Tc/T(χmax)=0.91±0.02 does not suggest lower magnetic dimensionality. Magnetization isotherms are linear to 16 kG; some features suggesting lower temperature transitions occur. Well above Tc the susceptibility is analyzed assuming axial and rhombic crystal field distortions, i.e., D[Sˆz2−S(S+1)/3] and E[Sˆx2−Sˆy2] spin Hamiltonian terms, with exchange incorporated in a mean field approximation. An extraordinarily large ||D/k||≈119 K seems to emerge, a result which is very provisional lacking single crystal data. A mean field analysis of Tc and θ yields ferromagnetic intrachain exchange J1/k=8.6±0.5 K and antiferromagnetic interchain exchange J2/k=−0.76±0.4 K. It seems more likely that D is negative, but even if it is positive the exchange interaction is large enough to induce magnetic order at finite Tc in light of theories relating Tc, J, and D.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 73 (1993), S. 5654-5656 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Recent studies of the magnetic susceptibility of powdered Fe[S2CNC4H8]2I confirm that Fe(III) in this salt is in the unusual spin state S=3/2 and that the system behaves as a quasi-2D antiferromagnet. Analysis of the data indicates that the ||±1/2(approximately-greater-than) ground doublet is separated by Δ/k=18.7 K from an excited ||±3/2(approximately-greater-than) doublet. We have now measured the heat capacity of polycrystalline Fe[S2CNC4H8]2I between 0.5 and 80 K in a liquid 3He-cooled calorimeter. CP exhibits a λ-type peak at TN=2.18±0.01 K. The critical entropy, S(TN)=0.25R ln2, indicates that most of the spin order is of a short-range, low-dimensional nature. The contribution of lattice vibrations to CP was estimated using the method of Sorai and Seki [J. Phys. Soc. Jpn. 32, 382 (1972)], which assumes a Schottky contribution from two doublets whose separation Δ was determined from the magnetic data. At the same time, the cooperative peak was reasonably represented by the results for the 2D S=1/2 XY model with Jxy/k=−2.18 K. In order to obtain a self-consistent fit of the lattice heat capacity, however, it was necessary to use a larger splitting (Δ/k=32 K) than that found from susceptibility data. This discrepancy between the doublet-doublet separations indicated by χ and CP measurements may suggest a possible temperature dependence of Δ.
    Type of Medium: Electronic Resource
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  • 9
    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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  • 10
    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.
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