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Next: II. Coordination of the atoms Up: Nomenclature of Inorganic Structure Types Previous: Introduction

I. Terms that define different degrees of similarity between inorganic structures

The following hierarchy of terms is considered based on the degree of structural similarity: isopointal, isoconfigurational, crystal-chemically isotypic, and homeotypic structures. Other relationships of interest are also listed.


I.1. Two structures are defined as isopointal if :

(i) they have the same space-group type (as defined in IT , $\S$8.2.1) [*] or belong to a pair of enantiomorphic space-group types; and

(ii) the atomic positions, occupied either fully or partially at random, are the same in both structures, i.e . the complete sequence of the occupied Wyckoff positions (including the number of times each Wyckoff position is occupied) is the same for both structures when the structural data have been standardized.


As there are no limitations on the values of the adjustable parameters of the Wyckoff positions (as used in IT ) or on the cell parameters, isopointal structures may have different geometric arrangements and atomic coordinations.

Two structures may be shown to be isopointal if they can be described in such a way that corresponding occupied Wyckoff positions have the same Wyckoff letters; to achieve this, it may be necessary to shift the origin and/or rotate/permute the coordinate system. This can be done by application of the affine normalizer (IT $\S\S$ 8.3.2 and 14.1) or by standardization procedures (Parthé & Gelato, 1984; Gelato & Parthé, 1987).


I.2. Two structures are defined as isoconfigurational (configurationally isotypic ) if:

(i) they are isopointal; and

(ii) for all corresponding Wyckoff positions, both the crystallographic point configurations (crystallographic orbits[*]) and their geometrical interrelationships are similar.


These conditions require the entire configurations of the two structures to be similar. Consequently, all geometrical properties, such as axial ratios, angles between crystallographic axes, values of corresponding adjustable positional parameters (x, y, z), and coordinations of corresponding atoms are similar. The term `similar' used in this definition is discussed below.

Standardization procedures may be necessary to test whether two structures are isoconfigurational.


I.3. Two structures are defined as crystal-chemically isotypic if:

(i) they are isoconfigurational; and

(ii) the corresponding atoms and corresponding bonds (interactions) have similar physical/chemical characteristics.


Crystal-chemical isotypism may be defined in different ways, depending on the number and nature of the physical/chemical characteristics that are taken into consideration, such as bond strength distribution, bond character, electronegativities assigned to atoms, radius ratios assigned to pairs of atoms, and electronic states.[*]

The use of the term `similar', in the definitions of configurational and crystal-chemical isotypism, arises from the inherent difficulty in defining a priori limits on the similarity of geometrical configurations or physical/chemical characteristics. These limits may differ between different categories of structures; they may also differ according to the purpose of a particular investigation or the physical or chemical property studied. Several approaches are possible in defining limits, such as a priori considerations (modelling) or statistical studies of known structure categories. Different approaches may yield different results. Examples of crystal-chemical isotypes are given in Table 1. Another example is the low-pressure and high-pressure forms of Ce which are crystal-chemically isotypic with regard to most crystal-chemical criteria; they are, however, not crystal-chemical isotypes with regard to electronic states.

 
Table 1: Examples of pairs of structures with different degrees of similarity
  Pnma $Pa\bar{3}$ I4/mmm $Ia\bar{3}d$ $Fm\bar{3}m$ $Fm\bar{3}m$ $Fm\bar{3}m$ $Pa\bar{3}$
  $2{\times}4(c),8(d)$-$4{\times}4(c)$ 4(a), 8(c)xxx 2(a),4(e) c/a=2.52-c/a=3.30 16(a),24(c), 24(d),96(h)xyz 4(a) 4(a),4(e) 4(a),8(c) 4(a),8(c)xxx
  LuRuB2-ScRhSi2 FeS2(pyrite)-CO2 ZrPd2-Zr2Pd Ca3Al2Si3O12-Y3Fe3+5O12 Cu-Ne NaCl-PbS CaF2-Li2O FeS2(pyrite)-PtP2
Isopointal No Yes Yes Yes Yes Yes Yes Yes
Isoconfigurational - No * Yes Yes Yes Yes Yes
Crystal-chemically isotypic according to            
  bond-strength distribution - - Yes No Yes Yes Yes Yes
  bond character - - Yes No No No Yes Yes
  radius ratios assigned to pairs of corresponding sites - - No Yes Yes Yes No Yes
  electronegativities assigned to sites - - Nearly yes Yes No Yes No Yes

*Notice that in this case the two structures which have c/a ratios differing by 30% are isoconfigurational if the limit of similarity is set above 30% and non-isoconfigurational if it is set below 30%.



I.4. Two structures represent a type and antitype if:

(i) they are isoconfigurational; and

(ii) some important physical/chemical characteristics of corresponding atoms are interchanged (reversed).


The characteristics usually considered in this context are electronegativities (positive versus negative charges) and larger versus smaller radii.

Examples are: CaF2-Li2O (Table 1), LaF3-Cu3P, CaCl2-Co2C, NaCl-RbF.


I.5. Two structures are defined as homeotypic if one or more of the following conditions required for isotypism are relaxed:

(i) identical or enantiomorphic space-group types, allowing for group-subgroup and group-supergroup relationships;

(ii) limitations imposed on the similarity of geometric properties, i.e. axial ratios, interaxial angles, values of adjustable positional parameters, and the coordination of corresponding atoms;

(iii) site occupancy limits, allowing given sites to be occupied by different atomic species.


The present definition narrows the original concept of Laves (1980). Two structures are considered as homeotypic if all essential features of topology are preserved between them. Relaxation of the geometric limits as in I.5(ii) without relaxation of the isosymmetry condition leads to structure type branches.


Examples of homeotypic structures are:

Distortion variants (or distortion derivatives): CaTiO3 (ideal perovskite) $\rightarrow$ KCuF3, BaTiO3, GdFeO3, etc . with subgroup symmetries.

Site-ordering variants (or substitution derivatives): C (diamond) $\rightarrow$ ZnS (sphalerite) $\rightarrow$ Cu3SbS4 (famatinite) $\rightarrow$ Cu2FeSnS4 (stannite); K(Al0.25Si0.75)4O8 (sanidine) $\rightarrow$ KAlSi3O8 (microcline).


I.6. Polytypic structures are defined in the Report of the IUCr Ad-hoc Committee on the Nomenclature of Disordered, Modulated and Polytype Structures (Guinier et al., 1984).


Examples are: closest-packed structures of chemical elements, SiC polytypes, Friauf-Laves phases, micas.


I.7. Interstitial (or `stuffed') derivatives represent compounds in which unoccupied `interstitial' sites (voids) of the basic structure are (progressively) filled by atoms in the derivative structure. In general, the relationship between the unfilled parent (basic) structure and the derivatives based on filling one specific interstitial site approaches homeotypism.


Examples are: ReO3 \rightarrow CaTiO3; Mg \rightarrow Mo2C; SiO2 (`ideal' tridymite) \rightarrow KNa3(AlSiO4)4 (nepheline).


I.8. 'Recombination' structures are formed when topologically simple parent structures are periodically divided into blocks,[*] rods or slabs which in turn are recombined into derivative structures by means of one or more structure building operations.


The most important of these operations are (1) unit-cell twinning, (2) crystallographic shear planes, (3) intergrowth of blocks, rods or slabs of different structure types, (4) periodic out-of-phase or antiphase boundaries, (5) rotation of rods (blocks) and (6) the vernier principle (Makovicky & Hyde, 1981). For most of these operations, not only parallel but also cyclic examples have been observed. In general, the sites on block, rod or slab interfaces differ in coordination and chemistry from those in the interior. This interface modulation can be accompanied or substituted by an overall long-range compositional modulation.

In cases (1) to (5), the frequency of structure building operators (or, conversely, the size of `undisturbed' structure blocks, rods or slabs between two consecutive operators) can vary by well defined increments so that these phases often occur as members of homologous series.

Examples are:

Twinning on unit-cell scale: PbS $\rightarrow$ lillianite homologous series (Pbn-1Bi2Sn+2), e.g. Pb3Bi2S6 (lillianite).

Shear derivatives: TiO2 (rutile) $\rightarrow$ TinO2n-1 (Magnéli phases) or TiO2 (rutile) $\rightarrow$ Nb2O5.

Intergrowth on unit-cell scale: olivine-norbergite homologous (polysomatic) series n(Mg,Fe)2SiO$_4{\cdot}$Mg(OH,F)2; biopyriboles, e.g. Mg3n+1Si4nO10n+2(OH)2n-2; MgCu2-type and CaCu5-type slabs $\rightarrow$ Ce2Ni7.

Antiphase boundaries: CuAu II, Dy5Cl11.

Block (rod) rotation: ReO$_3 \rightarrow $Nb8W9O47 or ReO$_3 \rightarrow $Mo5O14.

Vernier principle: slabs PbS (100) and PbS (111) $\rightarrow$Pb46Bi54S127 (cannizzarite), Y6O5F8, Pb2Bi2S5 (cosalite), NdCo4B$_4 \rightarrow$ Sm17(Fe4B4)15.

Compositional modulation: Pb46Bi54S127 (cannizzarite), FePb3Sn4Sb2S14 (cylindrite).


Note : In each example the sequence indicated is: parent(s) $\rightarrow$ derivative(s).


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Next: II. Coordination of the atoms Up: Nomenclature of Inorganic Structure Types Previous: Introduction

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