68,522 research outputs found

    Finite-Temperature Scaling of Magnetic Susceptibility and Geometric Phase in the XY Spin Chain

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    We study the magnetic susceptibility of 1D quantum XY model, and show that when the temperature approaches zero, the magnetic susceptibility exhibits the finite-temperature scaling behavior. This scaling behavior of the magnetic susceptibility in 1D quantum XY model, due to the quantum-classical mapping, can be easily experimentally tested. Furthermore, the universality in the critical properties of the magnetic susceptibility in quantum XY model is verified. Our study also reveals the close relation between the magnetic susceptibility and the geometric phase in some spin systems, where the quantum phase transitions are driven by an external magnetic field.Comment: 6 pages, 4 figures, get accepted for publication by J. Phys. A: Math. Theo

    Quantitative Susceptibility Mapping: Contrast Mechanisms and Clinical Applications.

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    Quantitative susceptibility mapping (QSM) is a recently developed MRI technique for quantifying the spatial distribution of magnetic susceptibility within biological tissues. It first uses the frequency shift in the MRI signal to map the magnetic field profile within the tissue. The resulting field map is then used to determine the spatial distribution of the underlying magnetic susceptibility by solving an inverse problem. The solution is achieved by deconvolving the field map with a dipole field, under the assumption that the magnetic field is a result of the superposition of the dipole fields generated by all voxels and that each voxel has its unique magnetic susceptibility. QSM provides improved contrast to noise ratio for certain tissues and structures compared to its magnitude counterpart. More importantly, magnetic susceptibility is a direct reflection of the molecular composition and cellular architecture of the tissue. Consequently, by quantifying magnetic susceptibility, QSM is becoming a quantitative imaging approach for characterizing normal and pathological tissue properties. This article reviews the mechanism generating susceptibility contrast within tissues and some associated applications

    Novel Magnetic and Thermodynamic Properties of Thiospinel Compound CuCrZrS4_{4}

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    We have carried out dc magnetic susceptibility, magnetization and specific heat measurements on thiospinel CuCrZrS4_{4}. Below TC∗=T_{\rm C}^{*} = 58 K, dc magnetic susceptibility and magnetization data show ferromagnetic behavior with a small spontaneous magnetization 0.27 μB/\mu_{\rm B}/f. u.. In dc magnetic susceptibility, large and weak irreversibilities are observed below Tf=T_{\rm f} = 6 K and in the range Tf<T<TC∗T_{\rm f}< T < T_{\rm C}^{*} respectively. We found that there is no anomaly as a peak or step in the specific heat at TC∗T_{\rm C}^{*}.Comment: 11 pages, 4 figure

    Magnetic Susceptibility for CaV4O9CaV_4O_9

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    We examine experimental magnetic susceptibility χtot(T)\chi^{tot}(T) for CaV4_4O9_9 by fitting with fitting function αχmag(T)+c\alpha \chi^{mag}(T) + c. The function χmag(T)\chi^{mag}(T) is a power series of 1/T and the lowest order term is fixed as C/TC/T, where CC is the Curie constant as determined by the experimental gg-value (g=1.96). Fitting parameters are α\alpha, cc and expansion coefficients except for the first one in χmag(T)\chi^{mag}(T). We determine α\alpha and cc as α≃\alpha \simeq 0.73 and c≃c\simeq 0 for an experimental sample. We interpret α\alpha as the volume fraction of CaV4_4O9_9 in the sample and χmag(T)\chi^{mag}(T) as the susceptibility for the pure CaV4_4O9_9. The result of α≠1\alpha \ne 1 means that the sample includes nonmagnetic components. This interpretation consists with the result of a perturbation theory and a neutron scattering experiment.Comment: 4pages, 4figure

    Phenomenological theory of a scalar electronic order: application to skutterudite PrFe4P12

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    By phenomenological Landau analysis, it is shown that a scalar order parameter with the point-group symmetry Γ1g\Gamma_{1g} explains most properties associated with the phase transition in PrFe4_4P12_{12} at 6.5 K. The scalar-order model reproduces magnetic and elastic properties in PrFe4_4P12_{12} consistently such as (i) the anomaly of the magnetic susceptibility and elastic constant at the transition temperature, (ii) anisotropy of the magnetic susceptibility in the presence of uniaxial pressure, and (iii) the anomaly in the elastic constant in magnetic field. An Ehrenfest relation is derived which relates the anomaly of the magnetic susceptibility to that of the elastic constant at the transition.Comment: 16 pages, 9 figure
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