GLORIA

GEOMAR Library Ocean Research Information Access

feed icon rss

Ihre E-Mail wurde erfolgreich gesendet. Bitte prüfen Sie Ihren Maileingang.

Leider ist ein Fehler beim E-Mail-Versand aufgetreten. Bitte versuchen Sie es erneut.

Vorgang fortführen?

Exportieren
Filter
Publikationsart
Erscheinungszeitraum
  • 1
    ISSN: 1089-7550
    Quelle: AIP Digital Archive
    Thema: Physik
    Notizen: 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.
    Materialart: Digitale Medien
    Standort Signatur Einschränkungen Verfügbarkeit
    BibTip Andere fanden auch interessant ...
  • 2
    Digitale Medien
    Digitale Medien
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 79 (1996), S. 4718-4720 
    ISSN: 1089-7550
    Quelle: AIP Digital Archive
    Thema: Physik
    Notizen: 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.
    Materialart: Digitale Medien
    Standort Signatur Einschränkungen Verfügbarkeit
    BibTip Andere fanden auch interessant ...
  • 3
    Digitale Medien
    Digitale Medien
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 75 (1994), S. 5529-5531 
    ISSN: 1089-7550
    Quelle: AIP Digital Archive
    Thema: Physik
    Notizen: 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.
    Materialart: Digitale Medien
    Standort Signatur Einschränkungen Verfügbarkeit
    BibTip Andere fanden auch interessant ...
  • 4
    Digitale Medien
    Digitale Medien
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 81 (1997), S. 4403-4405 
    ISSN: 1089-7550
    Quelle: AIP Digital Archive
    Thema: Physik
    Notizen: 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.
    Materialart: Digitale Medien
    Standort Signatur Einschränkungen Verfügbarkeit
    BibTip Andere fanden auch interessant ...
  • 5
    Digitale Medien
    Digitale Medien
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 75 (1994), S. 5940-5942 
    ISSN: 1089-7550
    Quelle: AIP Digital Archive
    Thema: Physik
    Notizen: 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
    Materialart: Digitale Medien
    Standort Signatur Einschränkungen Verfügbarkeit
    BibTip Andere fanden auch interessant ...
  • 6
    Digitale Medien
    Digitale Medien
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 87 (2000), S. 6052-6054 
    ISSN: 1089-7550
    Quelle: AIP Digital Archive
    Thema: Physik
    Notizen: 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.
    Materialart: Digitale Medien
    Standort Signatur Einschränkungen Verfügbarkeit
    BibTip Andere fanden auch interessant ...
  • 7
    Digitale Medien
    Digitale Medien
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 63 (1988), S. 3569-3571 
    ISSN: 1089-7550
    Quelle: AIP Digital Archive
    Thema: Physik
    Notizen: 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.
    Materialart: Digitale Medien
    Standort Signatur Einschränkungen Verfügbarkeit
    BibTip Andere fanden auch interessant ...
  • 8
    Digitale Medien
    Digitale Medien
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 85 (1999), S. 4527-4529 
    ISSN: 1089-7550
    Quelle: AIP Digital Archive
    Thema: Physik
    Notizen: 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.
    Materialart: Digitale Medien
    Standort Signatur Einschränkungen Verfügbarkeit
    BibTip Andere fanden auch interessant ...
  • 9
    Digitale Medien
    Digitale Medien
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 87 (2000), S. 6540-6542 
    ISSN: 1089-7550
    Quelle: AIP Digital Archive
    Thema: Physik
    Notizen: 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.
    Materialart: Digitale Medien
    Standort Signatur Einschränkungen Verfügbarkeit
    BibTip Andere fanden auch interessant ...
  • 10
    Digitale Medien
    Digitale Medien
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 73 (1993), S. 5386-5388 
    ISSN: 1089-7550
    Quelle: AIP Digital Archive
    Thema: Physik
    Notizen: 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.
    Materialart: Digitale Medien
    Standort Signatur Einschränkungen Verfügbarkeit
    BibTip Andere fanden auch interessant ...
Schließen ⊗
Diese Webseite nutzt Cookies und das Analyse-Tool Matomo. Weitere Informationen finden Sie hier...