Abstract
To build up a theory of metallic phase stability the conventional arguments for the discussion of crystal structures have to be completed by the concept of spatial correlation of electrons. The parameters of the spatial correlations may be analyzed from the ample empirical material of determined crystal structures by means of several evident rules. The surprising result is that for many crystal structures two correlations are essential for understanding the special features of the crystal structures. This two-correlations model makes possible an easy survey of metallic structures. Two examples of crystal structure-type families are considered, the Cu-family and the W-family. In the Cu-family substitutional variants, simple shear variants, multiple shear variants, and displacive variants may be distinguished. In the W-family cubic substitutional variants, deformed substitutional variants, vacancy variants with weak deformations, variants with stronger deformations, and variants with row shear may be distinguished. The essential feature of the present exposition is that the structural types are not only organized in a geometrical manner but that the arrangement of the structural types is put on an energetic base. This energetic base gives an answer to the fundamental question why certain phases are formed in certain mixtures.
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Abbreviations
- AC:
-
atomic spatial correlation
- CEC:
-
core electron spatial correlation
- Ds=1/L:
-
shear density=1/shear length
- N /AC :
-
number of core electrons per atom
- N /AP′ :
-
number of valence electron places per atom
- N /AP″ :
-
number of core electron places per atom
- N /AV :
-
number of valence electrons per atom
- N /CV :
-
number of valence electrons per cell
- VEC:
-
valence electron spatial correlation
- VEP:
-
valence electron places
- A0:
-
cubic primitive translation lattice
- A1:
-
cubic face-centered lattice
- A2:
-
cubic body-centered lattice
- AH:
-
hexagonal primitive lattice with equal distances
- C11:
-
tetragonal body-centered lattice with hexagonal (110) plane
- a ia0.H :
-
hexagonal three-fold primitive cell of A0 lattice described in coordinates i; the i is mostly dropped.
- a iA1.I :
-
innercentered cell of A1 (two-fold primitive)
- aA1.F :
-
an A1 cell which is filled to A0 or A2 in certain regions of the crystal cell.
- C:
-
cubic primitive
- B:
-
cubic body-centered
- F:
-
cubic face-centered
- T:
-
tetragonal primitive
- U:
-
tegragonal body-centered
- H:
-
hexagonal primitive
- R:
-
hexagonal rombohedral
- O:
-
orthorhombic primitive
- P:
-
orthorhombic body-centered
- Q:
-
orthohomic one-face centered
- S:
-
orthorhombic all-face centered
- M:
-
monoclinic primitive
- N:
-
monoclinic C-face centered
- Z:
-
triclinic
- A1 :
-
alcali
- A2 :
-
earth alcali
- T3…T10 :
-
homologous classes of transition elements
- B1…B7 :
-
classes of Cu … Br
- B8 :
-
noble gases
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Schubert, K. (1977). The two-correlations model, a valence model for metallic phases. In: New Concepts. Structure and Bonding, vol 33. Springer, Berlin, Heidelberg. https://doi.org/10.1007/BFb0117580
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DOI: https://doi.org/10.1007/BFb0117580
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