In mathematics, an equivalence relation is a binary relation that is reflexive, symmetric and transitive. The equipollence relation between line segments in geometry is a common example of an equivalence relation. A simpler example is equality. Any number is equal to itself (reflexive). If , then (symmetric). If and , then (transitive).
Each equivalence relation provides a partition of the underlying set into disjoint equivalence classes. Two elements of the given set are equivalent to each other if and only if they belong to the same equivalence class.
Various notations are used in the literature to denote that two elements and of a set are equivalent with respect to an equivalence relation the most common are "" and "a ≡ b", which are used when is implicit, and variations of "", "a ≡Rb", or "" to specify explicitly. Non-equivalence may be written "a ≁ b" or "".
A binary relation on a set is said to be an equivalence relation, if and only if it is reflexive, symmetric and transitive. That is, for all and in
together with the relation is called a setoid. The equivalence class of under denoted is defined as [1] [2]
In relational algebra, if and are relations, then the composite relation is defined so that if and only if there is a such that and . [note 1] This definition is a generalisation of the definition of functional composition. The defining properties of an equivalence relation on a set can then be reformulated as follows:
On the set , the relation is an equivalence relation. The following sets are equivalence classes of this relation:
The set of all equivalence classes for is This set is a partition of the set . It is also called the quotient set of by .
The following relations are all equivalence relations:
If is an equivalence relation on and is a property of elements of such that whenever is true if is true, then the property is said to be well-defined or a class invariant under the relation
A frequent particular case occurs when is a function from to another set if implies then is said to be a morphism for a class invariant under or simply invariant under This occurs, e.g. in the character theory of finite groups. The latter case with the function can be expressed by a commutative triangle. See also invariant. Some authors use "compatible with " or just "respects " instead of "invariant under ".
More generally, a function may map equivalent arguments (under an equivalence relation ) to equivalent values (under an equivalence relation ). Such a function is known as a morphism from to
Let , and be an equivalence relation. Some key definitions and terminology follow:
A subset of such that holds for all and in , and never for in and outside , is called an equivalence class of by . Let denote the equivalence class to which belongs. All elements of equivalent to each other are also elements of the same equivalence class.
The set of all equivalence classes of by denoted is the quotient set of by If is a topological space, there is a natural way of transforming into a topological space; see Quotient space for the details.[ undue weight? – discuss ]
The projection of is the function defined by which maps elements of into their respective equivalence classes by
The equivalence kernel of a function is the equivalence relation ~ defined by The equivalence kernel of an injection is the identity relation.
A partition of X is a set P of nonempty subsets of X, such that every element of X is an element of a single element of P. Each element of P is a cell of the partition. Moreover, the elements of P are pairwise disjoint and their union is X.
Let X be a finite set with n elements. Since every equivalence relation over X corresponds to a partition of X, and vice versa, the number of equivalence relations on X equals the number of distinct partitions of X, which is the nth Bell number Bn:
A key result links equivalence relations and partitions: [5] [6] [7]
In both cases, the cells of the partition of X are the equivalence classes of X by ~. Since each element of X belongs to a unique cell of any partition of X, and since each cell of the partition is identical to an equivalence class of X by ~, each element of X belongs to a unique equivalence class of X by ~. Thus there is a natural bijection between the set of all equivalence relations on X and the set of all partitions of X.
If and are two equivalence relations on the same set , and implies for all then is said to be a coarser relation than , and is a finer relation than . Equivalently,
The equality equivalence relation is the finest equivalence relation on any set, while the universal relation, which relates all pairs of elements, is the coarsest.
The relation " is finer than " on the collection of all equivalence relations on a fixed set is itself a partial order relation, which makes the collection a geometric lattice. [8]
Much of mathematics is grounded in the study of equivalences, and order relations. Lattice theory captures the mathematical structure of order relations. Even though equivalence relations are as ubiquitous in mathematics as order relations, the algebraic structure of equivalences is not as well known as that of orders. The former structure draws primarily on group theory and, to a lesser extent, on the theory of lattices, categories, and groupoids.
Just as order relations are grounded in ordered sets, sets closed under pairwise supremum and infimum, equivalence relations are grounded in partitioned sets, which are sets closed under bijections that preserve partition structure. Since all such bijections map an equivalence class onto itself, such bijections are also known as permutations. Hence permutation groups (also known as transformation groups) and the related notion of orbit shed light on the mathematical structure of equivalence relations.
Let '~' denote an equivalence relation over some nonempty set A, called the universe or underlying set. Let G denote the set of bijective functions over A that preserve the partition structure of A, meaning that for all and Then the following three connected theorems hold: [10]
In sum, given an equivalence relation ~ over A, there exists a transformation group G over A whose orbits are the equivalence classes of A under ~.
This transformation group characterisation of equivalence relations differs fundamentally from the way lattices characterize order relations. The arguments of the lattice theory operations meet and join are elements of some universe A. Meanwhile, the arguments of the transformation group operations composition and inverse are elements of a set of bijections, A → A.
Moving to groups in general, let H be a subgroup of some group G. Let ~ be an equivalence relation on G, such that The equivalence classes of ~—also called the orbits of the action of H on G—are the right cosets of H in G. Interchanging a and b yields the left cosets.
Related thinking can be found in Rosen (2008: chpt. 10).
Let G be a set and let "~" denote an equivalence relation over G. Then we can form a groupoid representing this equivalence relation as follows. The objects are the elements of G, and for any two elements x and y of G, there exists a unique morphism from x to y if and only if
The advantages of regarding an equivalence relation as a special case of a groupoid include:
The equivalence relations on any set X, when ordered by set inclusion, form a complete lattice, called ConX by convention. The canonical map ker : X^X → ConX, relates the monoid X^X of all functions on X and ConX. ker is surjective but not injective. Less formally, the equivalence relation ker on X, takes each function f : X → X to its kernel kerf. Likewise, ker(ker) is an equivalence relation on X^X.
Equivalence relations are a ready source of examples or counterexamples. For example, an equivalence relation with exactly two infinite equivalence classes is an easy example of a theory which is ω-categorical, but not categorical for any larger cardinal number.
An implication of model theory is that the properties defining a relation can be proved independent of each other (and hence necessary parts of the definition) if and only if, for each property, examples can be found of relations not satisfying the given property while satisfying all the other properties. Hence the three defining properties of equivalence relations can be proved mutually independent by the following three examples:
Properties definable in first-order logic that an equivalence relation may or may not possess include:
In mathematics, a binary relation associates elements of one set called the domain with elements of another set called the codomain. Precisely, a binary relation over sets and is a set of ordered pairs where is in and is in . It encodes the common concept of relation: an element is related to an element , if and only if the pair belongs to the set of ordered pairs that defines the binary relation.
In mathematics, when the elements of some set have a notion of equivalence, then one may naturally split the set into equivalence classes. These equivalence classes are constructed so that elements and belong to the same equivalence class if, and only if, they are equivalent.
In mathematics, especially in category theory and homotopy theory, a groupoid generalises the notion of group in several equivalent ways. A groupoid can be seen as a:
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