By (auth.), H.P.J. Wijn (eds.)
The magnetic homes of halides were compiled in subvolume 27J. The 3rd half, 27J3, comprises information on structural and magnetic homes of halide perovskite-type layer constructions of the kinds A2MX4 (monolayer compounds), A3M2X7 (double-layer) and A4M3X10 (triple-layer) the place X=F-, Cl-, etc.; M=Mg2+, Cr2+, Mn2+, Zn2+, Cd2+, etc.; and A=K+, Rb+, Cs+, and so on. furthermore, for X=Cl- and Br- info are offered on compounds the place the alkali ions are changed through n-alkylammonium chains, and in addition for diammonium compounds the place alkali ions are changed by way of divalent alkylene-diammonium ions. a quick comic strip of the idea of section transitions and of the correct types (2D Ising version, second XY-model, second Ising spin glass) is additionally given in addition to a finished choice of info on severe homes close to the part transitions.
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153 (Sect. e. its angle of orientation with the a-axis δ i = δ (ri) orientation angle δ of the spin at ri δ, κ factors for the terms with space derivatives in the Landau-type free energy, cf. Eq. 37 (Sect. g. q0 = δ ⋅ a* + σ ⋅ b* ε = ε' + iε" dielectric constant, real and imaginary part ε tensor of the dielectric constant with components εxx εyy and εzz, assuming orthorhombic lattice symmetry ζ, ζx0, ζx, ζz reduced wavevector (ζx0 = qx0 /a*, ζx = qx /a*, ζz = qz /c* ) ζ1, ζ2 values of ζx0 indicating the crossover 3D XY ↔ 2D XY and 2D XY ↔ 2D Heisenberg, cf.
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