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Neutron-diffraction study of the staggered magnetization of Cu Cl 2 ·2 D 2 O

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TLDR
In this paper, the authors used the neutron-scattering technique to measure the staggered magnetization of the antiferromagnet Cu${\mathrm{Cl}}_{2}$\ifmmode\cdot\else\textperiodcentered\fi{}2$
Abstract
The neutron-scattering technique has been used to measure the staggered magnetization of the $S=\frac{1}{2}$, $d=3$ antiferromagnet Cu${\mathrm{Cl}}_{2}$\ifmmode\cdot\else\textperiodcentered\fi{}2${\mathrm{D}}_{2}$O as a function of temperature and magnetic field. The critical exponents ${\ensuremath{\beta}}_{\ensuremath{\perp}}$, ${\ensuremath{\beta}}_{\ensuremath{\parallel}}$ describing the temperature variation of the order parameter in the regions well above and well below the bicritical point, respectively, were found to be ${\ensuremath{\beta}}_{\ensuremath{\perp}}=0.321\ifmmode\pm\else\textpm\fi{}0.01$ and ${\ensuremath{\beta}}_{\ensuremath{\parallel}}=0.324\ifmmode\pm\else\textpm\fi{}0.013$. These values are within experimental error of the theoretically expected value of 0.325 for the $d=3$ Ising model. At the spin-flop transition the staggered magnetization changed 8% in magnitude, the reduction being due to the anisotropy of the $g$ factor. The magnetic form factor in the spin-flop region was found to be the same as that previously determined in zero field. In addition, with the applied field tilted in the $a\ensuremath{-}b$ plane away from the $\stackrel{\ensuremath{\rightarrow}}{\mathrm{a}}$ axis, the direction of the staggered magnetization was found to rotate continuously from the $\stackrel{\ensuremath{\rightarrow}}{\mathrm{a}}$ to the $\stackrel{\ensuremath{\rightarrow}}{\mathrm{b}}$ direction as is expected theoretically. The observed range in field over which the rotation takes place, however, is narrower than the predictions of mean-field theory.

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Magnetic structures and reorientation transitions in noncentrosymmetric uniaxial antiferromagnets

TL;DR: In this paper, a phenomenological theory of magnetic states in non-centrosymmetric tetragonal antiferromagnets is developed, which has to include homogeneous and inhomogeneous terms (Lifshitz invariants) derived from Dzyaloshinskii-Moriya couplings.
Journal ArticleDOI

Crystal structures, phase relationships, and magnetic phase transitions of R5M4 compounds (R = rare earths, M = Si, Ge)

TL;DR: In this article, the crystal structures, phase relationships, and magnetic properties of several 5:4 compounds, including Nd5Si4−xGex, Pr5Si2Ge2 and Pr5Ge4 investigated by neutron powder diffraction and small-angle neutron scattering are presented.
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Possible ground states and parallel magnetic-field-driven phase transitions of collinear antiferromagnets

TL;DR: Li et al. as mentioned in this paper provided an integrated theoretical model for the magnetic states of collinear antiferromagnets with two interpenetrating sublattices and offered a practical approach as an alternative to the estimation of magnetic exchange parameters (J, γ and D).
Journal ArticleDOI

Mössbauer studies of iron-rich metallic glasses

TL;DR: In this paper, the application of 57Fe Mossbauer spectroscopy to magnetic studies on metallic glasses mainly based on the iron-boron alloy system, and some of the significant results obtained which are characteristic of the glassy/amorphous state.
Journal ArticleDOI

A second-order spin-flop transition in collinear two-sublattice antiferromagnets

TL;DR: In this article, a mean-field theoretical calculation endowed with AFM exchange interaction (J), easy axis anisotropy ($gamma$), uniaxial single-ion exchange anisotropic (D), and Zeeman coupling to a magnetic field parallel to the easy axis unambiguously reveals that a spin-flop (SFO) transition indeed exists by virtue of its relatively lower free energy.
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