By R. Troc, D. Kaczorowski (auth.), H.P.J. Wijn (eds.)
In subvolume III/27C2 magnetic and similar homes of binary actinide oxides were compiled. This subvolume covers information acquired considering the fact that 1980 and will consequently be considered as complement to quantity III/12c. half 27C1 bargains with binary oxides of the lanthanide components. Magnetic houses of the binary oxides of 3d transition parts are given in subvolume 27 G.
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Additional info for Binary Actinide Oxides
C. Magnetic susceptibility χm vs. c. c. 80DFFR 81BFHL 83BCFM 87CLSF La n d o l t - B ö r n s t e i n New Series III/27C2 Ref. p. , Tables Ref. c. 3 K Heat capacity at 10…305 K and magnetic entropy vs. 3 Survey of binary actinide oxides (CaF2-type structure) State Crystal structure, magnetic and related properties [Ref. p. , Tables Ref. 75 Inverse magnetic susceptibility: χ g−1 vs. 180 K Electrical conductivity vs. T and oxygen partial pressure Neutron diffraction - magnetic form factor Square root of magnetic intensity vs.
Of electronic contribution to heat capacity Calculated Cp on the basis of enthalpy data Heat capacity at 300…1100 K Heat capacity at 300…1000 K Heat capacity at 500…1500 K Heat capacity at 300…8000 K Heat capacity at 300…1500 K Heat capacity at high temperatures 15 268 124 53OW 52JGL, 62WG 71HW 269 125, 215, 271 126 127 68FOW 71HW, 53OW, 68FOW 65DCW 67DGV 16 128 129 192 Theory on transition into a superionic state; explanation of the nature of the anomalies observed in heat capacity and diffusion coeff.
ThO2, UO2 and PuO2. Some quantities related to the elastic and infrared dielectric properties ([66AP] and [70MB]). See caption of Fig. 20 for classical dispersion formula. RM–0: effective short range force constant between M-O nearest neighbors. 9 (continued) La n d o l t - B ö r n s t e i n New Series III/27C2 Ref. p. 17 Table 3. ThO2 . Calculated wavenumbers of Raman active combination differences and overtones at Γ, M and L points in the Brillouin zone and selection rules for Raman process [76IK].