EXPERIMENTAL-EVIDENCE FOR THE EXISTENCE OF NONNUCLEAR MAXIMA IN THE ELECTRON-DENSITY DISTRIBUTION OF METALLIC BERYLLIUM - A COMPARATIVE-STUDY OF THE MAXIMUM-ENTROPY METHOD AND THE MULTIPOLE REFINEMENT METHOD
Bb. Iversen et al., EXPERIMENTAL-EVIDENCE FOR THE EXISTENCE OF NONNUCLEAR MAXIMA IN THE ELECTRON-DENSITY DISTRIBUTION OF METALLIC BERYLLIUM - A COMPARATIVE-STUDY OF THE MAXIMUM-ENTROPY METHOD AND THE MULTIPOLE REFINEMENT METHOD, Acta crystallographica. Section B, Structural science, 51, 1995, pp. 580-591
The electron-density distribution (EDD) of metallic beryllium has been
derived from the structure factors of Larsen and Hansen [(1984), Acta
Cryst. B40, 169-179] using the maximum entropy method (MEM). Subseque
nt topological analysis reveals non-nuclear maxima (NNM) in the EDD. P
lots of the gradient field of the electron density illustrates this fi
nding. A possible critical-point network for the hexagonal close-packe
d (h.c.p.) structure of beryllium is suggested. It is thus demonstrate
d that it is possible to obtain detailed topological information about
the electron density in metallic beryllium without the use of a struc
tural model. In order to test the findings of the MEM, the same set of
structure factors were analysed using the multipole refinement method
(MRM). Use of the MRM also reveals NNM. The results of the two differ
ent approaches to electron-density analysis are contrasted and discuss
ed. Expressed within the framework of the theory of atoms in molecules
, our results suggest that the h.c.p. structure of beryllium has no Be
atoms directly bonded to other Be atoms. The structure is held togeth
er through a three-dimensional network of bonds between the NNM and Be
atoms as well as between different NNM. The topological analysis thus
reveals that the beryllium structure has important interactions conne
cting Be atoms of different basal plane layers. The breaking of these
interactions when forming a surface may explain the abnormally large e
xpansion of the inter-layer distance in the beryllium surface structur
e.