International
Tables for Crystallography Volume D Physical properties of crystals Edited by A. Authier © International Union of Crystallography 2006 |
International Tables for Crystallography (2006). Vol. D. ch. 3.2, pp. 380-381
Section 3.2.3.1. Sets, pairs, mappings and equivalence classes
a
Department of Physics, Technical University of Liberec, Hálkova 6, 461 17 Liberec 1, Czech Republic,bInstitut für Kristallographie, Rheinisch–Westfälische Technische Hochschule, D-52056 Aachen, Germany, and cMineralogisch-Petrologisches Institut, Universität Bonn, D-53113 Bonn, Germany |
Definition 3.2.3.1. A set is a collection of distinguishable objects. The objects constituting a set are called elements (or points) of the set.
In Chapter 3.4 we encounter mainly two types of sets: sets the elements of which are crystalline objects (domain states, domain twins, domain walls etc.), and sets, like groups, with elements of mathematical nature, e.g. rotations, transformations, operations etc. The sets of crystalline objects will be denoted by capital sans-serif letters, e.g. , and capital bold letters, e.g. or , will be used to denote elements of such sets. Groups will be denoted by capital italic letters, e.g. G, F etc., and their elements by lower-case italic letters, e.g. . The exposition of this section is given for sets the elements of which are (crystalline) objects, but all notions and relations hold for any other sets.
If an element belongs to the set , one writes , in the opposite case . Sets consisting of a small number of elements can be expressed explicitly by writing their elements between curly braces, . The order of elements in the symbol of the set is irrelevant. From the definition of a set it follows that there are no equal elements in the set, or in other words, any two equal elements coalesce into one:If a set contains many (or an infinite number of) elements, the elements are specified in another way, e.g. by stating that they have a certain property in common.
The number of elements in a set is the order of the set. A finite set consists of a finite number of elements and this number is denoted by . An infinite set contains infinite number of elements and an empty set, denoted by , contains no element. In what follows, the term `set' will mean a `finite nonempty set' unless explicitly stated otherwise.
A set is a subset of , or , if every element of is an element of . If each element of is an element of , and vice versa, then is equal to or identical with , or . If there exists at least one element of which is not contained in , then is a proper subset of , or . The subset is often defined by a restriction that specifies only some elements of as elements of . This is written in short as ; the expression means that consists of all elements of that satisfy the restriction given behind the sign |.
The intersection of two sets and , or , is a set comprising all elements that belong both to and to . If the sets and have no element in common, , then one says that the sets and are disjoint. The union of sets and , or , is a set consisting of all elements that belong either to or to . Sometimes the symbol is used instead of the symbol . The difference of set and , or the complement of in , , comprises those elements of that do not belong to .
A collection of two objects and constitutes an unordered pair. The objects of an unordered pair are called elements or points. A trivial unordered pair consists of two identical elements. A non-trivial unordered domain pair comprises two non-identical elements and is identical with a set of order two.
Note that we do not identify an unordered pair with a set of order two where, according to (3.2.3.1), two equal objects coalesce into one. In spite of this difference we shall use the same symbol for the unordered pair as for the set of order two, but reverse the symbol for the trivial unordered pair. With this reservation, the identityholds for both unordered pairs and for sets of order two.
An ordered pair, denoted , consists of the first and the second member of the pair. If , the ordered pair is called a trivial ordered pair, ; if the pair is a non-trivial ordered pair. The ordered pair with a reversed order of elements is called a transposed pair. In contrast to unordered pairs, initial and transposed non-trivial ordered pairs are different objects,
The members and of an ordered pair can either belong to one set, , or each to a different set, .
Two ordered pairs and are equal, , if and only if and .
We shall encounter ordered and unordered pairs in Sections 3.4.3 and 3.4.4 , where the members of pairs are domain states or domain twins. However, pairs are also essential in introducing further concepts of set theory. The starting point is the following construction of a set of pairs that are formed from two sets:
A Cartesian product of two sets and is a set of all ordered pairs , where . The sets and can be different or identical sets. If the sets and are finite, then the Cartesian product consists of ordered pairs.
A mapping of a set into a set is a rule which assigns to each element a unique element . This is written symbolically as or , and one says that is mapped to under the mapping . The element is called the image of the element S under . The assignment can be expressed by an ordered pair , if one ascribes to the first member of the pair and the element to the second member of the pair . Then the mapping of a set into a set , symbolically written as , can be identified with such a subset of ordered pairs of the Cartesian product in which each element of occurs exactly once as the first member of the pair . If is a finite set, then consists of ordered pairs.
We note that in a mapping several elements of may be mapped to the same element of . In such a case, the mapping is called a many-to-one mapping. If the mapping is such that each element of is the image of some element of , then the mapping is called a mapping of onto . If is a mapping of onto and, moreover, each element of is the image of exactly one element of , then the mapping becomes a one-to-one correspondence between and , . In this case, and are of the same order.
One often encounters a situation in which one assigns to each ordered pair an element , where all three elements are elements from the same set , symbolically ; or . Such a mapping is called a binary operation or a composition law on the set . A sum of two numbers or a product of two numbers , where belong to the set of all real numbers, are elementary examples of binary operations.
The notion of the ordered pair allows one to introduce another useful concept, namely the relation on a set. An example will illustrate this notion. Let be a set of integers, . For each ordered pair , , one can decide whether m is smaller than n, , or not. All pairs that fulfil the condition form a subset of all possible ordered pairs . In other words, the relation defines a subset of the set , . Similarly, the relation ( denotes absolute value of n) defines another subset of .
To indicate that an element is related to by , where , one writes , where the relation defines a subset of all ordered pairs , (the same letter is used for the subset and for the relation on ). The opposite also holds: Each subset of defines a certain relation on .
A relation is called an equivalence relation on the set if it satisfies three conditions: Thus, for example, it is easy to corroborate that the relation on the set of integers fulfils all three conditions (3.2.3.3) to (3.2.3.5) and is, therefore, an equivalence relation on the set . On the other hand, the relation is not an equivalence relation on since it fulfils neither the reflexivity (3.2.3.3) nor the symmetry condition (3.2.3.4).
Let be an equivalence relation on and ; all elements such that constitute a subset of denoted and called the equivalence class of with respect to (or the -equivalence class of S). The element is called the representative of the class . Any other member of the class can be chosen as its representative. Any two elements of the equivalence class are -equivalent elements of .
From the definition of the equivalence class, it follows that any two elements are either -equivalent elements of , , and thus belong to the same class, , or are not -equivalent, and thus belong to two different classes that are disjoint, . In this way, the equivalence relation divides the set into disjoint subsets (equivalence classes), the union of which is equal to the set itself. Such a decomposition is called a partition of the set associated with the equivalence relation . For a finite set this decomposition can be expressed as a union of equivalence classes, where are representatives of the equivalence classes.
Generally, any decomposition of a set into a system of disjoint non-empty subsets such that every element of the set is a member of just one subset is called a partition of the set. To any partition of a set there corresponds an equivalence relation such that the -equivalence classes of form that partition. This equivalence relation defines two elements as equivalent if and only if they belong to the same subset.
The term `equivalent' is often used when it is clear from the context what the relevant equivalence relation is. Similarly, the term `class' is used instead of `equivalence class'. Sometimes equivalence classes have names that do not explicitly indicate that they are equivalence classes. For example, in group theory, conjugate subgroups, left, right and double cosets form equivalence classes (see Section 3.2.3.2). Often instead of the expression `partition of a set ' an equivalent expression `classification of the elements of a set ' is used. The most important equivalence classes in the symmetry analysis of domain structures are called orbits and will be discussed in Section 3.2.3.3.
More details on set theory can be found in Kuratowski & Mostowski (1968), Lipschutz (1981), and Opechowski (1986).
References
Kuratowski, K. & Mostowski, A. (1968). Set theory. Amsterdam: North-Holland.Google ScholarLipschutz, S. (1981). Theory and problems of set theory and related topics. Singapore: McGraw-Hill.Google Scholar
Opechowski, W. (1986). Crystallographic and metacrystallographic groups. Amsterdam: North-Holland.Google Scholar