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Crystal LaMnO

The calculations [754] are performed for the high-temperature cubic phase of LaMnOs (LMO)-based crystals doped with Sr, substituting for La atoms in different fractions. This substitution results in a charge-compensating hole formation. The formation of other defects like oxygen or metal vacancies is neglected. [Pg.453]

In Table 11.3 are given in brackets the atomic planes charges for (001) surface in SrTiOs and LaMnOs crystals calculated for the bufk crystals with the use of Wannier-type atomic functions in the population analysis, see Chap. 9 and reference [736], As the Ti-0 bond in SrTiOs presents a non-negligible part of covalent character the actual charges of atomic planes SrO and Ti02 are nonzero. This means that SrTiOs (001) should be considered as a polar (type-3) surface. [Pg.470]

Figure 10 shows the Curie-Weiss paramagnetic susceptibility x(T) and its inverse for the same single crystal of LaMnOs as measured under... [Pg.35]

See other pages where Crystal LaMnO is mentioned: [Pg.268]    [Pg.264]    [Pg.268]    [Pg.264]    [Pg.564]    [Pg.43]    [Pg.43]    [Pg.44]    [Pg.48]    [Pg.51]    [Pg.52]    [Pg.54]    [Pg.57]    [Pg.58]    [Pg.59]    [Pg.60]    [Pg.61]    [Pg.63]    [Pg.66]    [Pg.68]    [Pg.70]    [Pg.72]    [Pg.73]    [Pg.75]    [Pg.80]    [Pg.266]    [Pg.3445]    [Pg.6037]    [Pg.705]    [Pg.3444]    [Pg.6036]    [Pg.309]    [Pg.309]    [Pg.212]    [Pg.1]    [Pg.45]    [Pg.353]    [Pg.383]    [Pg.384]    [Pg.385]    [Pg.387]    [Pg.390]    [Pg.75]    [Pg.594]    [Pg.34]    [Pg.128]    [Pg.129]    [Pg.246]    [Pg.550]    [Pg.43]   
See also in sourсe #XX -- [ Pg.38 ]



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