Group (mathematics)
In mathematics, a group is an algebraic structure consisting of a set of elements equipped with an operation that combines any two elements to form a third element and that satisfies four conditions called the group axioms, namely closure, associativity, identity and invertibility. One of the most familiar examples of a group is the set of integers together with the addition operation, but the abstract formalization of the group axioms, detached as it is from the concrete nature of any particular group and its operation, applies much more widely. It allows entities with highly diverse mathematical origins in abstract algebra and beyond to be handled in a flexible way while retaining their essential structural aspects. The ubiquity of groups in numerous areas within and outside mathematics makes them a central organizing principle of contemporary mathematics.^{[1]}^{[2]}
Groups share a fundamental kinship with the notion of symmetry. For example, a symmetry group encodes symmetry features of a geometrical object: the group consists of the set of transformations that leave the object unchanged and the operation of combining two such transformations by performing one after the other. Lie groups are the symmetry groups used in the Standard Model of particle physics; Poincaré groups, which are also Lie groups, can express the physical symmetry underlying special relativity; and point groups are used to help understand symmetry phenomena in molecular chemistry.
The concept of a group arose from the study of polynomial equations, starting with Évariste Galois in the 1830s. After contributions from other fields such as number theory and geometry, the group notion was generalized and firmly established around 1870. Modern group theory—an active mathematical discipline—studies groups in their own right.^{a[›]} To explore groups, mathematicians have devised various notions to break groups into smaller, betterunderstandable pieces, such as subgroups, quotient groups and simple groups. In addition to their abstract properties, group theorists also study the different ways in which a group can be expressed concretely, both from a point of view of representation theory (that is, through the representations of the group) and of computational group theory. A theory has been developed for finite groups, which culminated with the classification of finite simple groups, completed in 2004.^{aa[›]} Since the mid1980s, geometric group theory, which studies finitely generated groups as geometric objects, has become a particularly active area in group theory.
Algebraic structure → Group theory Group theory 



Infinite dimensional Lie group

Algebraic structures 

Definition and illustration
First example: the integers
One of the most familiar groups is the set of integers Z which consists of the numbers
 ..., −4, −3, −2, −1, 0, 1, 2, 3, 4, ...,^{[3]} together with addition.
The following properties of integer addition serve as a model for the abstract group axioms given in the definition below.
 For any two integers a and b, the sum a + b is also an integer. That is, addition of integers always yields an integer. This property is known as closure under addition.
 For all integers a, b and c, (a + b) + c = a + (b + c). Expressed in words, adding a to b first, and then adding the result to c gives the same final result as adding a to the sum of b and c, a property known as associativity.
 If a is any integer, then 0 + a = a + 0 = a. Zero is called the identity element of addition because adding it to any integer returns the same integer.
 For every integer a, there is an integer b such that a + b = b + a = 0. The integer b is called the inverse element of the integer a and is denoted −a.
The integers, together with the operation +, form a mathematical object belonging to a broad class sharing similar structural aspects. To appropriately understand these structures as a collective, the following abstract definition is developed.
Definition
A group is a set, G, together with an operation • (called the group law of G) that combines any two elements a and b to form another element, denoted a • b or ab. To qualify as a group, the set and operation, (G, •), must satisfy four requirements known as the group axioms:^{[5]}
 Closure
 For all a, b in G, the result of the operation, a • b, is also in G.^{b[›]}
 Associativity
 For all a, b and c in G, (a • b) • c = a • (b • c).
 Identity element
 There exists an element e in G such that, for every element a in G, the equation e • a = a • e = a holds. Such an element is unique (see below), and thus one speaks of the identity element.
 Inverse element
 For each a in G, there exists an element b in G, commonly denoted a^{−1} (or −a, if the operation is denoted "+"), such that a • b = b • a = e, where e is the identity element.
The result of an operation may depend on the order of the operands. In other words, the result of combining element a with element b need not yield the same result as combining element b with element a; the equation
 a • b = b • a
may not always be true. This equation always holds in the group of integers under addition, because a + b = b + a for any two integers (commutativity of addition). Groups for which the commutativity equation a • b = b • a always holds are called abelian groups (in honor of Niels Henrik Abel). The symmetry group described in the following section is an example of a group that is not abelian.
The identity element of a group G is often written as 1 or 1_{G},^{[6]} a notation inherited from the multiplicative identity. If a group is abelian, then one may choose to denote the group operation by + and the identity element by 0; in that case, the group is called an additive group. The identity element can also be written as id.
The set G is called the underlying set of the group (G, •). Often the group's underlying set G is used as a short name for the group (G, •). Along the same lines, shorthand expressions such as "a subset of the group G" or "an element of group G" are used when what is actually meant is "a subset of the underlying set G of the group (G, •)" or "an element of the underlying set G of the group (G, •)". Usually, it is clear from the context whether a symbol like G refers to a group or to an underlying set.
Second example: a symmetry group
Two figures in the plane are congruent if one can be changed into the other using a combination of rotations, reflections, and translations. Any figure is congruent to itself. However, some figures are congruent to themselves in more than one way, and these extra congruences are called symmetries. A square has eight symmetries. These are:
 the identity operation leaving everything unchanged, denoted id;
 rotations of the square around its center by 90° clockwise, 180° clockwise, and 270° clockwise, denoted by r_{1}, r_{2} and r_{3}, respectively;
 reflections about the vertical and horizontal middle line (f_{h} and f_{v}), or through the two diagonals (f_{d} and f_{c}).
These symmetries are represented by functions. Each of these functions sends a point in the square to the corresponding point under the symmetry. For example, r_{1} sends a point to its rotation 90° clockwise around the square's center, and f_{h} sends a point to its reflection across the square's vertical middle line. Composing two of these symmetry functions gives another symmetry function. These symmetries determine a group called the dihedral group of degree 4 and denoted D_{4}. The underlying set of the group is the above set of symmetry functions, and the group operation is function composition.^{[7]} Two symmetries are combined by composing them as functions, that is, applying the first one to the square, and the second one to the result of the first application. The result of performing first a and then b is written symbolically from right to left as
 b • a ("apply the symmetry b after performing the symmetry a").
The righttoleft notation is the same notation that is used for composition of functions.
The group table on the right lists the results of all such compositions possible. For example, rotating by 270° clockwise (r_{3}) and then reflecting horizontally (f_{h}) is the same as performing a reflection along the diagonal (f_{d}). Using the above symbols, highlighted in blue in the group table:
 f_{h} • r_{3} = f_{d}.
•  id  r_{1}  r_{2}  r_{3}  f_{v}  f_{h}  f_{d}  f_{c} 

id  id  r_{1}  r_{2}  r_{3}  f_{v}  f_{h}  f_{d}  f_{c} 
r_{1}  r_{1}  r_{2}  r_{3}  id  f_{c}  f_{d}  f_{v}  f_{h} 
r_{2}  r_{2}  r_{3}  id  r_{1}  f_{h}  f_{v}  f_{c}  f_{d} 
r_{3}  r_{3}  id  r_{1}  r_{2}  f_{d}  f_{c}  f_{h}  f_{v} 
f_{v}  f_{v}  f_{d}  f_{h}  f_{c}  id  r_{2}  r_{1}  r_{3} 
f_{h}  f_{h}  f_{c}  f_{v}  f_{d}  r_{2}  id  r_{3}  r_{1} 
f_{d}  f_{d}  f_{h}  f_{c}  f_{v}  r_{3}  r_{1}  id  r_{2} 
f_{c}  f_{c}  f_{v}  f_{d}  f_{h}  r_{1}  r_{3}  r_{2}  id 
The elements id, r_{1}, r_{2}, and r_{3} form a subgroup, highlighted in red (upper left region). A left and right coset of this subgroup is highlighted in green (in the last row) and yellow (last column), respectively. 
Given this set of symmetries and the described operation, the group axioms can be understood as follows:
 The closure axiom demands that the composition b • a of any two symmetries a and b is also a symmetry. Another example for the group operation is
 r_{3} • f_{h} = f_{c},
 The associativity constraint deals with composing more than two symmetries: Starting with three elements a, b and c of D_{4}, there are two possible ways of using these three symmetries in this order to determine a symmetry of the square. One of these ways is to first compose a and b into a single symmetry, then to compose that symmetry with c. The other way is to first compose b and c, then to compose the resulting symmetry with a. The associativity condition
 (a • b) • c = a • (b • c)
means that these two ways are the same, i.e., a product of many group elements can be simplified in any grouping. For example, (f_{d} • f_{v}) • r_{2} = f_{d} • (f_{v} • r_{2}) can be checked using the group table at the right
(f_{d} • f_{v}) • r_{2} = r_{3} • r_{2} = r_{1}, which equals f_{d} • (f_{v} • r_{2}) = f_{d} • f_{h} = r_{1}.  The identity element is the symmetry id leaving everything unchanged: for any symmetry a, performing id after a (or a after id) equals a, in symbolic form,
 id • a = a,
 a • id = a.
 An inverse element undoes the transformation of some other element. Every symmetry can be undone: each of the following transformations—identity id, the reflections f_{h}, f_{v}, f_{d}, f_{c} and the 180° rotation r_{2}—is its own inverse, because performing it twice brings the square back to its original orientation. The rotations r_{3} and r_{1} are each other's inverses, because rotating 90° and then rotation 270° (or vice versa) yields a rotation over 360° which leaves the square unchanged. In symbols,
 f_{h} • f_{h} = id,
 r_{3} • r_{1} = r_{1} • r_{3} = id.
In contrast to the group of integers above, where the order of the operation is irrelevant, it does matter in D_{4}: f_{h} • r_{1} = f_{c} but r_{1} • f_{h} = f_{d}. In other words, D_{4} is not abelian, which makes the group structure more difficult than the integers introduced first.
History
The modern concept of an abstract group developed out of several fields of mathematics.^{[8]}^{[9]}^{[10]} The original motivation for group theory was the quest for solutions of polynomial equations of degree higher than 4. The 19thcentury French mathematician Évariste Galois, extending prior work of Paolo Ruffini and JosephLouis Lagrange, gave a criterion for the solvability of a particular polynomial equation in terms of the symmetry group of its roots (solutions). The elements of such a Galois group correspond to certain permutations of the roots. At first, Galois' ideas were rejected by his contemporaries, and published only posthumously.^{[11]}^{[12]} More general permutation groups were investigated in particular by Augustin Louis Cauchy. Arthur Cayley's On the theory of groups, as depending on the symbolic equation θ^{n} = 1 (1854) gives the first abstract definition of a finite group.^{[13]}
Geometry was a second field in which groups were used systematically, especially symmetry groups as part of Felix Klein's 1872 Erlangen program.^{[14]} After novel geometries such as hyperbolic and projective geometry had emerged, Klein used group theory to organize them in a more coherent way. Further advancing these ideas, Sophus Lie founded the study of Lie groups in 1884.^{[15]}
The third field contributing to group theory was number theory. Certain abelian group structures had been used implicitly in Carl Friedrich Gauss' numbertheoretical work Disquisitiones Arithmeticae (1798), and more explicitly by Leopold Kronecker.^{[16]} In 1847, Ernst Kummer made early attempts to prove Fermat's Last Theorem by developing groups describing factorization into prime numbers.^{[17]}
The convergence of these various sources into a uniform theory of groups started with Camille Jordan's Traité des substitutions et des équations algébriques (1870).^{[18]} Walther von Dyck (1882) introduced the idea of specifying a group by means of generators and relations, and was also the first to give an axiomatic definition of an "abstract group", in the terminology of the time.^{[19]} As of the 20th century, groups gained wide recognition by the pioneering work of Ferdinand Georg Frobenius and William Burnside, who worked on representation theory of finite groups, Richard Brauer's modular representation theory and Issai Schur's papers.^{[20]} The theory of Lie groups, and more generally locally compact groups was studied by Hermann Weyl, Élie Cartan and many others.^{[21]} Its algebraic counterpart, the theory of algebraic groups, was first shaped by Claude Chevalley (from the late 1930s) and later by the work of Armand Borel and Jacques Tits.^{[22]}
The University of Chicago's 1960–61 Group Theory Year brought together group theorists such as Daniel Gorenstein, John G. Thompson and Walter Feit, laying the foundation of a collaboration that, with input from numerous other mathematicians, led to the classification of finite simple groups, with the final step taken by Aschbacher and Smith in 2004. This project exceeded previous mathematical endeavours by its sheer size, in both length of proof and number of researchers. Research is ongoing to simplify the proof of this classification.^{[23]} These days, group theory is still a highly active mathematical branch, impacting many other fields.^{a[›]}
Elementary consequences of the group axioms
Basic facts about all groups that can be obtained directly from the group axioms are commonly subsumed under elementary group theory.^{[24]} For example, repeated applications of the associativity axiom show that the unambiguity of
 a • b • c = (a • b) • c = a • (b • c)
generalizes to more than three factors. Because this implies that parentheses can be inserted anywhere within such a series of terms, parentheses are usually omitted.^{[25]}
The axioms may be weakened to assert only the existence of a left identity and left inverses. Both can be shown to be actually twosided, so the resulting definition is equivalent to the one given above.^{[26]}
Uniqueness of identity element and inverses
Two important consequences of the group axioms are the uniqueness of the identity element and the uniqueness of inverse elements. There can be only one identity element in a group, and each element in a group has exactly one inverse element. Thus, it is customary to speak of the identity, and the inverse of an element.^{[27]}
To prove the uniqueness of an inverse element of a, suppose that a has two inverses, denoted b and c, in a group (G, •). Then

b = b • e as e is the identity element = b • (a • c) because c is an inverse of a, so e = a • c = (b • a) • c by associativity, which allows to rearrange the parentheses = e • c since b is an inverse of a, i.e., b • a = e = c for e is the identity element
The term b on the first line above and the c on the last are equal, since they are connected by a chain of equalities. In other words, there is only one inverse element of a. Similarly, to prove that the identity element of a group is unique, assume G is a group with two identity elements e and f. Then e = e • f = f, hence e and f are equal.
Division
In groups, the existence of inverse elements implies that division is possible: given elements a and b of the group G, there is exactly one solution x in G to the equation x • a = b, namely b • a^{−1}.^{[27]} In fact, we have
 (b • a^{−1}) • a = b • (a^{−1} • a) = b • e = b.
Uniqueness results by multiplying the two sides of the equation x • a = b by a^{−1}. The element b • a^{−1}, often denoted b / a, is called the right quotient of b by a, or the result of the right division of b by a.
Similarly there is exactly one solution y in G to the equation a • y = b, namely y = a^{−1} • b. This solution is the left quotient of b by a, and is sometimes denoted a \ b.
In general b / a and a \ b may be different, but, if the group operation is commutative (that is, if the group is abelian), they are equal. In this case, the group operation is often denoted as an addition, and one talks of subtraction and difference instead of division and quotient.
A consequence of this is that multiplication by a group element g is a bijection. Specifically, if g is an element of the group G, the function (mathematics) from G to itself that maps h ∈ G to g • h is a bijection. This function is called the left translation by g . Similarly, the right translation by g is the bijection from G to itself, that maps h to h • g. If G is abelian, the left and the right translation by a group element are the same.
Basic concepts

The following sections use mathematical symbols such as X = {x, y, z} to denote a set X containing elements x, y, and z, or alternatively x ∈ X to restate that x is an element of X. The notation f : X → Y means f is a function assigning to every element of X an element of Y.
To understand groups beyond the level of mere symbolic manipulations as above, more structural concepts have to be employed.^{c[›]} There is a conceptual principle underlying all of the following notions: to take advantage of the structure offered by groups (which sets, being "structureless", do not have), constructions related to groups have to be compatible with the group operation. This compatibility manifests itself in the following notions in various ways. For example, groups can be related to each other via functions called group homomorphisms. By the mentioned principle, they are required to respect the group structures in a precise sense. The structure of groups can also be understood by breaking them into pieces called subgroups and quotient groups. The principle of "preserving structures"—a recurring topic in mathematics throughout—is an instance of working in a category, in this case the category of groups.^{[28]}
Group homomorphisms
Group homomorphisms^{g[›]} are functions that preserve group structure. A function a: G → H between two groups (G, •) and (H, ∗) is called a homomorphism if the equation
 a(g • k) = a(g) ∗ a(k)
holds for all elements g, k in G. In other words, the result is the same when performing the group operation after or before applying the map a. This requirement ensures that a(1_{G}) = 1_{H}, and also a(g)^{−1} = a(g^{−1}) for all g in G. Thus a group homomorphism respects all the structure of G provided by the group axioms.^{[29]}
Two groups G and H are called isomorphic if there exist group homomorphisms a: G → H and b: H → G, such that applying the two functions one after another in each of the two possible orders gives the identity functions of G and H. That is, a(b(h)) = h and b(a(g)) = g for any g in G and h in H. From an abstract point of view, isomorphic groups carry the same information. For example, proving that g • g = 1_{G} for some element g of G is equivalent to proving that a(g) ∗ a(g) = 1_{H}, because applying a to the first equality yields the second, and applying b to the second gives back the first.
Subgroups
Informally, a subgroup is a group H contained within a bigger one, G.^{[30]} Concretely, the identity element of G is contained in H, and whenever h_{1} and h_{2} are in H, then so are h_{1} • h_{2} and h_{1}^{−1}, so the elements of H, equipped with the group operation on G restricted to H, indeed form a group.
In the example above, the identity and the rotations constitute a subgroup R = {id, r_{1}, r_{2}, r_{3}}, highlighted in red in the group table above: any two rotations composed are still a rotation, and a rotation can be undone by (i.e., is inverse to) the complementary rotations 270° for 90°, 180° for 180°, and 90° for 270° (note that rotation in the opposite direction is not defined). The subgroup test is a necessary and sufficient condition for a nonempty subset H of a group G to be a subgroup: it is sufficient to check that g^{−1}h ∈ H for all elements g, h ∈ H. Knowing the subgroups is important in understanding the group as a whole.^{d[›]}
Given any subset S of a group G, the subgroup generated by S consists of products of elements of S and their inverses. It is the smallest subgroup of G containing S.^{[31]} In the introductory example above, the subgroup generated by r_{2} and f_{v} consists of these two elements, the identity element id and f_{h} = f_{v} • r_{2}. Again, this is a subgroup, because combining any two of these four elements or their inverses (which are, in this particular case, these same elements) yields an element of this subgroup.
Cosets
In many situations it is desirable to consider two group elements the same if they differ by an element of a given subgroup. For example, in D_{4} above, once a reflection is performed, the square never gets back to the r_{2} configuration by just applying the rotation operations (and no further reflections), i.e., the rotation operations are irrelevant to the question whether a reflection has been performed. Cosets are used to formalize this insight: a subgroup H defines left and right cosets, which can be thought of as translations of H by arbitrary group elements g. In symbolic terms, the left and right cosets of H containing g are
 gH = {g • h : h ∈ H} and Hg = {h • g : h ∈ H}, respectively.^{[32]}
The left cosets of any subgroup H form a partition of G; that is, the union of all left cosets is equal to G and two left cosets are either equal or have an empty intersection.^{[33]} The first case g_{1}H = g_{2}H happens precisely when g_{1}^{−1} • g_{2} ∈ H, i.e., if the two elements differ by an element of H. Similar considerations apply to the right cosets of H. The left and right cosets of H may or may not be equal. If they are, i.e., for all g in G, gH = Hg, then H is said to be a normal subgroup.
In D_{4}, the introductory symmetry group, the left cosets gR of the subgroup R consisting of the rotations are either equal to R, if g is an element of R itself, or otherwise equal to U = f_{c}R = {f_{c}, f_{v}, f_{d}, f_{h}} (highlighted in green). The subgroup R is also normal, because f_{c}R = U = Rf_{c} and similarly for any element other than f_{c}. (In fact, in the case of D_{4}, observe that all such cosets are equal, such that f_{h}R = f_{v}R = f_{d}R = f_{c}R.)
Quotient groups
In some situations the set of cosets of a subgroup can be endowed with a group law, giving a quotient group or factor group. For this to be possible, the subgroup has to be normal. Given any normal subgroup N, the quotient group is defined by
 G / N = {gN, g ∈ G}, "G modulo N".^{[34]}
This set inherits a group operation (sometimes called coset multiplication, or coset addition) from the original group G: (gN) • (hN) = (gh)N for all g and h in G. This definition is motivated by the idea (itself an instance of general structural considerations outlined above) that the map G → G / N that associates to any element g its coset gN be a group homomorphism, or by general abstract considerations called universal properties. The coset eN = N serves as the identity in this group, and the inverse of gN in the quotient group is (gN)^{−1} = (g^{−1})N.^{e[›]}
•  R  U 

R  R  U 
U  U  R 
The elements of the quotient group D_{4} / R are R itself, which represents the identity, and U = f_{v}R. The group operation on the quotient is shown at the right. For example, U • U = f_{v}R • f_{v}R = (f_{v} • f_{v})R = R. Both the subgroup R = {id, r_{1}, r_{2}, r_{3}}, as well as the corresponding quotient are abelian, whereas D_{4} is not abelian. Building bigger groups by smaller ones, such as D_{4} from its subgroup R and the quotient D_{4} / R is abstracted by a notion called semidirect product.
Quotient groups and subgroups together form a way of describing every group by its presentation: any group is the quotient of the free group over the generators of the group, quotiented by the subgroup of relations. The dihedral group D_{4}, for example, can be generated by two elements r and f (for example, r = r_{1}, the right rotation and f = f_{v} the vertical (or any other) reflection), which means that every symmetry of the square is a finite composition of these two symmetries or their inverses. Together with the relations
 r ^{4} = f ^{2} = (r • f)^{2} = 1,^{[35]}
the group is completely described. A presentation of a group can also be used to construct the Cayley graph, a device used to graphically capture discrete groups.
Sub and quotient groups are related in the following way: a subset H of G can be seen as an injective map H → G, i.e., any element of the target has at most one element that maps to it. The counterpart to injective maps are surjective maps (every element of the target is mapped onto), such as the canonical map G → G / N.^{y[›]} Interpreting subgroup and quotients in light of these homomorphisms emphasizes the structural concept inherent to these definitions alluded to in the introduction. In general, homomorphisms are neither injective nor surjective. Kernel and image of group homomorphisms and the first isomorphism theorem address this phenomenon.
Examples and applications
Examples and applications of groups abound. A starting point is the group Z of integers with addition as group operation, introduced above. If instead of addition multiplication is considered, one obtains multiplicative groups. These groups are predecessors of important constructions in abstract algebra.
Groups are also applied in many other mathematical areas. Mathematical objects are often examined by associating groups to them and studying the properties of the corresponding groups. For example, Henri Poincaré founded what is now called algebraic topology by introducing the fundamental group.^{[36]} By means of this connection, topological properties such as proximity and continuity translate into properties of groups.^{i[›]} For example, elements of the fundamental group are represented by loops. The second image at the right shows some loops in a plane minus a point. The blue loop is considered nullhomotopic (and thus irrelevant), because it can be continuously shrunk to a point. The presence of the hole prevents the orange loop from being shrunk to a point. The fundamental group of the plane with a point deleted turns out to be infinite cyclic, generated by the orange loop (or any other loop winding once around the hole). This way, the fundamental group detects the hole.
In more recent applications, the influence has also been reversed to motivate geometric constructions by a grouptheoretical background.^{j[›]} In a similar vein, geometric group theory employs geometric concepts, for example in the study of hyperbolic groups.^{[37]} Further branches crucially applying groups include algebraic geometry and number theory.^{[38]}
In addition to the above theoretical applications, many practical applications of groups exist. Cryptography relies on the combination of the abstract group theory approach together with algorithmical knowledge obtained in computational group theory, in particular when implemented for finite groups.^{[39]} Applications of group theory are not restricted to mathematics; sciences such as physics, chemistry and computer science benefit from the concept.
Numbers
Many number systems, such as the integers and the rationals enjoy a naturally given group structure. In some cases, such as with the rationals, both addition and multiplication operations give rise to group structures. Such number systems are predecessors to more general algebraic structures known as rings and fields. Further abstract algebraic concepts such as modules, vector spaces and algebras also form groups.
Integers
The group of integers Z under addition, denoted (Z, +), has been described above. The integers, with the operation of multiplication instead of addition, (Z, ·) do not form a group. The closure, associativity and identity axioms are satisfied, but inverses do not exist: for example, a = 2 is an integer, but the only solution to the equation a · b = 1 in this case is b = 1/2, which is a rational number, but not an integer. Hence not every element of Z has a (multiplicative) inverse.^{k[›]}
Rationals
The desire for the existence of multiplicative inverses suggests considering fractions
Fractions of integers (with b nonzero) are known as rational numbers.^{l[›]} The set of all such fractions is commonly denoted Q. There is still a minor obstacle for (Q, ·), the rationals with multiplication, being a group: because the rational number 0 does not have a multiplicative inverse (i.e., there is no x such that x · 0 = 1), (Q, ·) is still not a group.
However, the set of all nonzero rational numbers Q ∖ {0} = {q ∈ Q  q ≠ 0} does form an abelian group under multiplication, denoted (Q ∖ {0}, ·).^{m[›]} Associativity and identity element axioms follow from the properties of integers. The closure requirement still holds true after removing zero, because the product of two nonzero rationals is never zero. Finally, the inverse of a/b is b/a, therefore the axiom of the inverse element is satisfied.
The rational numbers (including 0) also form a group under addition. Intertwining addition and multiplication operations yields more complicated structures called rings and—if division is possible, such as in Q—fields, which occupy a central position in abstract algebra. Group theoretic arguments therefore underlie parts of the theory of those entities.^{n[›]}
Modular arithmetic
In modular arithmetic, two integers are added and then the sum is divided by a positive integer called the modulus. The result of modular addition is the remainder of that division. For any modulus, n, the set of integers from 0 to n − 1 forms a group under modular addition: the inverse of any element a is n − a, and 0 is the identity element. This is familiar from the addition of hours on the face of a clock: if the hour hand is on 9 and is advanced 4 hours, it ends up on 1, as shown at the right. This is expressed by saying that 9 + 4 equals 1 "modulo 12" or, in symbols,
 9 + 4 ≡ 1 modulo 12.
The group of integers modulo n is written Z_{n} or Z/nZ.
For any prime number p, there is also the multiplicative group of integers modulo p.^{[40]} Its elements are the integers 1 to p − 1. The group operation is multiplication modulo p. That is, the usual product is divided by p and the remainder of this division is the result of modular multiplication. For example, if p = 5, there are four group elements 1, 2, 3, 4. In this group, 4 · 4 = 1, because the usual product 16 is equivalent to 1, which divided by 5 yields a remainder of 1. for 5 divides 16 − 1 = 15, denoted
 16 ≡ 1 (mod 5).
The primality of p ensures that the product of two integers neither of which is divisible by p is not divisible by p either, hence the indicated set of classes is closed under multiplication.^{o[›]} The identity element is 1, as usual for a multiplicative group, and the associativity follows from the corresponding property of integers. Finally, the inverse element axiom requires that given an integer a not divisible by p, there exists an integer b such that
 a · b ≡ 1 (mod p), i.e., p divides the difference a · b − 1.
The inverse b can be found by using Bézout's identity and the fact that the greatest common divisor gcd(a, p) equals 1.^{[41]} In the case p = 5 above, the inverse of 4 is 4, and the inverse of 3 is 2, as 3 · 2 = 6 ≡ 1 (mod 5). Hence all group axioms are fulfilled. Actually, this example is similar to (Q ∖ {0}, ·) above: it consists of exactly those elements in Z/pZ that have a multiplicative inverse.^{[42]} These groups are denoted F_{p}^{×}. They are crucial to publickey cryptography.^{p[›]}
Cyclic groups
A cyclic group is a group all of whose elements are powers of a particular element a.^{[43]} In multiplicative notation, the elements of the group are:
 ..., a^{−3}, a^{−2}, a^{−1}, a^{0} = e, a, a^{2}, a^{3}, ...,
where a^{2} means a • a, and a^{−3} stands for a^{−1} • a^{−1} • a^{−1} = (a • a • a)^{−1} etc.^{h[›]} Such an element a is called a generator or a primitive element of the group. In additive notation, the requirement for an element to be primitive is that each element of the group can be written as
 ..., −a−a, −a, 0, a, a+a, ...
In the groups Z/nZ introduced above, the element 1 is primitive, so these groups are cyclic. Indeed, each element is expressible as a sum all of whose terms are 1. Any cyclic group with n elements is isomorphic to this group. A second example for cyclic groups is the group of nth complex roots of unity, given by complex numbers z satisfying z^{n} = 1. These numbers can be visualized as the vertices on a regular ngon, as shown in blue at the right for n = 6. The group operation is multiplication of complex numbers. In the picture, multiplying with z corresponds to a counterclockwise rotation by 60°.^{[44]} Using some field theory, the group F_{p}^{×} can be shown to be cyclic: for example, if p = 5, 3 is a generator since 3^{1} = 3, 3^{2} = 9 ≡ 4, 3^{3} ≡ 2, and 3^{4} ≡ 1.
Some cyclic groups have an infinite number of elements. In these groups, for every nonzero element a, all the powers of a are distinct; despite the name "cyclic group", the powers of the elements do not cycle. An infinite cyclic group is isomorphic to (Z, +), the group of integers under addition introduced above.^{[45]} As these two prototypes are both abelian, so is any cyclic group.
The study of finitely generated abelian groups is quite mature, including the fundamental theorem of finitely generated abelian groups; and reflecting this state of affairs, many grouprelated notions, such as center and commutator, describe the extent to which a given group is not abelian.^{[46]}
Symmetry groups
Symmetry groups are groups consisting of symmetries of given mathematical objects—be they of geometric nature, such as the introductory symmetry group of the square, or of algebraic nature, such as polynomial equations and their solutions.^{[47]} Conceptually, group theory can be thought of as the study of symmetry.^{t[›]} Symmetries in mathematics greatly simplify the study of geometrical or analytical objects. A group is said to act on another mathematical object X if every group element performs some operation on X compatibly to the group law. In the rightmost example below, an element of order 7 of the (2,3,7) triangle group acts on the tiling by permuting the highlighted warped triangles (and the other ones, too). By a group action, the group pattern is connected to the structure of the object being acted on.
In chemical fields, such as crystallography, space groups and point groups describe molecular symmetries and crystal symmetries. These symmetries underlie the chemical and physical behavior of these systems, and group theory enables simplification of quantum mechanical analysis of these properties.^{[48]} For example, group theory is used to show that optical transitions between certain quantum levels cannot occur simply because of the symmetry of the states involved.
Not only are groups useful to assess the implications of symmetries in molecules, but surprisingly they also predict that molecules sometimes can change symmetry. The JahnTeller effect is a distortion of a molecule of high symmetry when it adopts a particular ground state of lower symmetry from a set of possible ground states that are related to each other by the symmetry operations of the molecule.^{[49]}^{[50]}
Likewise, group theory helps predict the changes in physical properties that occur when a material undergoes a phase transition, for example, from a cubic to a tetrahedral crystalline form. An example is ferroelectric materials, where the change from a paraelectric to a ferroelectric state occurs at the Curie temperature and is related to a change from the highsymmetry paraelectric state to the lower symmetry ferroelectric state, accompanied by a socalled soft phonon mode, a vibrational lattice mode that goes to zero frequency at the transition.^{[51]}
Such spontaneous symmetry breaking has found further application in elementary particle physics, where its occurrence is related to the appearance of Goldstone bosons.
Buckminsterfullerene displays icosahedral symmetry, though the double bonds reduce this to pyritohedral symmetry. 
Ammonia, NH_{3}. Its symmetry group is of order 6, generated by a 120° rotation and a reflection. 
Cubane C_{8}H_{8} features octahedral symmetry. 
Hexaaquacopper(II) complex ion, [Cu(OH_{2})_{6}]^{2+}. Compared to a perfectly symmetrical shape, the molecule is vertically dilated by about 22% (JahnTeller effect).  The (2,3,7) triangle group, a hyperbolic group, acts on this tiling of the hyperbolic plane. 
Finite symmetry groups such as the Mathieu groups are used in coding theory, which is in turn applied in error correction of transmitted data, and in CD players.^{[52]} Another application is differential Galois theory, which characterizes functions having antiderivatives of a prescribed form, giving grouptheoretic criteria for when solutions of certain differential equations are wellbehaved.^{u[›]} Geometric properties that remain stable under group actions are investigated in (geometric) invariant theory.^{[53]}
General linear group and representation theory
Matrix groups consist of matrices together with matrix multiplication. The general linear group GL(n, R) consists of all invertible nbyn matrices with real entries.^{[54]} Its subgroups are referred to as matrix groups or linear groups. The dihedral group example mentioned above can be viewed as a (very small) matrix group. Another important matrix group is the special orthogonal group SO(n). It describes all possible rotations in n dimensions. Via Euler angles, rotation matrices are used in computer graphics.^{[55]}
Representation theory is both an application of the group concept and important for a deeper understanding of groups.^{[56]}^{[57]} It studies the group by its group actions on other spaces. A broad class of group representations are linear representations, i.e., the group is acting on a vector space, such as the threedimensional Euclidean space R^{3}. A representation of G on an ndimensional real vector space is simply a group homomorphism
 ρ: G → GL(n, R)
from the group to the general linear group. This way, the group operation, which may be abstractly given, translates to the multiplication of matrices making it accessible to explicit computations.^{w[›]}
Given a group action, this gives further means to study the object being acted on.^{x[›]} On the other hand, it also yields information about the group. Group representations are an organizing principle in the theory of finite groups, Lie groups, algebraic groups and topological groups, especially (locally) compact groups.^{[56]}^{[58]}
Galois groups
Galois groups were developed to help solve polynomial equations by capturing their symmetry features.^{[59]}^{[60]} For example, the solutions of the quadratic equation ax^{2} + bx + c = 0 are given by
Exchanging "+" and "−" in the expression, i.e., permuting the two solutions of the equation can be viewed as a (very simple) group operation. Similar formulae are known for cubic and quartic equations, but do not exist in general for degree 5 and higher.^{[61]} Abstract properties of Galois groups associated with polynomials (in particular their solvability) give a criterion for polynomials that have all their solutions expressible by radicals, i.e., solutions expressible using solely addition, multiplication, and roots similar to the formula above.^{[62]}
The problem can be dealt with by shifting to field theory and considering the splitting field of a polynomial. Modern Galois theory generalizes the above type of Galois groups to field extensions and establishes—via the fundamental theorem of Galois theory—a precise relationship between fields and groups, underlining once again the ubiquity of groups in mathematics.
Finite groups
A group is called finite if it has a finite number of elements. The number of elements is called the order of the group.^{[63]} An important class is the symmetric groups S_{N}, the groups of permutations of N letters. For example, the symmetric group on 3 letters S_{3} is the group consisting of all possible orderings of the three letters ABC, i.e., contains the elements ABC, ACB, BAC, BCA, CAB, CBA, in total 6 (factorial of 3) elements. This class is fundamental insofar as any finite group can be expressed as a subgroup of a symmetric group S_{N} for a suitable integer N, according to Cayley's theorem. Parallel to the group of symmetries of the square above, S_{3} can also be interpreted as the group of symmetries of an equilateral triangle.
The order of an element a in a group G is the least positive integer n such that a^{n} = e, where a^{n} represents
i.e., application of the operation • to n copies of a. (If • represents multiplication, then a^{n} corresponds to the nth power of a.) In infinite groups, such an n may not exist, in which case the order of a is said to be infinity. The order of an element equals the order of the cyclic subgroup generated by this element.
More sophisticated counting techniques, for example counting cosets, yield more precise statements about finite groups: Lagrange's Theorem states that for a finite group G the order of any finite subgroup H divides the order of G. The Sylow theorems give a partial converse.
The dihedral group (discussed above) is a finite group of order 8. The order of r_{1} is 4, as is the order of the subgroup R it generates (see above). The order of the reflection elements f_{v} etc. is 2. Both orders divide 8, as predicted by Lagrange's theorem. The groups F_{p}^{×} above have order p − 1.
Classification of finite simple groups
Mathematicians often strive for a complete classification (or list) of a mathematical notion. In the context of finite groups, this aim leads to difficult mathematics. According to Lagrange's theorem, finite groups of order p, a prime number, are necessarily cyclic (abelian) groups Z_{p}. Groups of order p^{2} can also be shown to be abelian, a statement which does not generalize to order p^{3}, as the nonabelian group D_{4} of order 8 = 2^{3} above shows.^{[64]} Computer algebra systems can be used to list small groups, but there is no classification of all finite groups.^{q[›]} An intermediate step is the classification of finite simple groups.^{r[›]} A nontrivial group is called simple if its only normal subgroups are the trivial group and the group itself.^{s[›]} The Jordan–Hölder theorem exhibits finite simple groups as the building blocks for all finite groups.^{[65]} Listing all finite simple groups was a major achievement in contemporary group theory. 1998 Fields Medal winner Richard Borcherds succeeded in proving the monstrous moonshine conjectures, a surprising and deep relation between the largest finite simple sporadic group—the "monster group"—and certain modular functions, a piece of classical complex analysis, and string theory, a theory supposed to unify the description of many physical phenomena.^{[66]}
Groups with additional structure
Many groups are simultaneously groups and examples of other mathematical structures. In the language of category theory, they are group objects in a category, meaning that they are objects (that is, examples of another mathematical structure) which come with transformations (called morphisms) that mimic the group axioms. For example, every group (as defined above) is also a set, so a group is a group object in the category of sets.
Topological groups
Some topological spaces may be endowed with a group law. In order for the group law and the topology to interweave well, the group operations must be continuous functions, that is, g • h, and g^{−1} must not vary wildly if g and h vary only little. Such groups are called topological groups, and they are the group objects in the category of topological spaces.^{[67]} The most basic examples are the reals R under addition, (R ∖ {0}, ·), and similarly with any other topological field such as the complex numbers or padic numbers. All of these groups are locally compact, so they have Haar measures and can be studied via harmonic analysis. The former offer an abstract formalism of invariant integrals. Invariance means, in the case of real numbers for example:
for any constant c. Matrix groups over these fields fall under this regime, as do adele rings and adelic algebraic groups, which are basic to number theory.^{[68]} Galois groups of infinite field extensions such as the absolute Galois group can also be equipped with a topology, the socalled Krull topology, which in turn is central to generalize the above sketched connection of fields and groups to infinite field extensions.^{[69]} An advanced generalization of this idea, adapted to the needs of algebraic geometry, is the étale fundamental group.^{[70]}
Lie groups
Lie groups (in honor of Sophus Lie) are groups which also have a manifold structure, i.e., they are spaces looking locally like some Euclidean space of the appropriate dimension.^{[71]} Again, the additional structure, here the manifold structure, has to be compatible, i.e., the maps corresponding to multiplication and the inverse have to be smooth.
A standard example is the general linear group introduced above: it is an open subset of the space of all nbyn matrices, because it is given by the inequality
 det (A) ≠ 0,
where A denotes an nbyn matrix.^{[72]}
Lie groups are of fundamental importance in modern physics: Noether's theorem links continuous symmetries to conserved quantities.^{[73]} Rotation, as well as translations in space and time are basic symmetries of the laws of mechanics. They can, for instance, be used to construct simple models—imposing, say, axial symmetry on a situation will typically lead to significant simplification in the equations one needs to solve to provide a physical description.^{v[›]} Another example are the Lorentz transformations, which relate measurements of time and velocity of two observers in motion relative to each other. They can be deduced in a purely grouptheoretical way, by expressing the transformations as a rotational symmetry of Minkowski space. The latter serves—in the absence of significant gravitation—as a model of space time in special relativity.^{[74]} The full symmetry group of Minkowski space, i.e., including translations, is known as the Poincaré group. By the above, it plays a pivotal role in special relativity and, by implication, for quantum field theories.^{[75]} Symmetries that vary with location are central to the modern description of physical interactions with the help of gauge theory.^{[76]}
Generalizations
Grouplike structures  

Totality^{α}  Associativity  Identity  Invertibility  Commutativity  
Semigroupoid  Unneeded  Required  Unneeded  Unneeded  Unneeded 
Category  Unneeded  Required  Required  Unneeded  Unneeded 
Groupoid  Unneeded  Required  Required  Required  Unneeded 
Magma  Required  Unneeded  Unneeded  Unneeded  Unneeded 
Quasigroup  Required  Unneeded  Unneeded  Required  Unneeded 
Loop  Required  Unneeded  Required  Required  Unneeded 
Semigroup  Required  Required  Unneeded  Unneeded  Unneeded 
Monoid  Required  Required  Required  Unneeded  Unneeded 
Group  Required  Required  Required  Required  Unneeded 
Abelian group  Required  Required  Required  Required  Required 
^α Closure, which is used in many sources, is an equivalent axiom to totality, though defined differently. 
In abstract algebra, more general structures are defined by relaxing some of the axioms defining a group.^{[28]}^{[77]}^{[78]} For example, if the requirement that every element has an inverse is eliminated, the resulting algebraic structure is called a monoid. The natural numbers N (including 0) under addition form a monoid, as do the nonzero integers under multiplication (Z ∖ {0}, ·), see above. There is a general method to formally add inverses to elements to any (abelian) monoid, much the same way as (Q ∖ {0}, ·) is derived from (Z ∖ {0}, ·), known as the Grothendieck group. Groupoids are similar to groups except that the composition a • b need not be defined for all a and b. They arise in the study of more complicated forms of symmetry, often in topological and analytical structures, such as the fundamental groupoid or stacks. Finally, it is possible to generalize any of these concepts by replacing the binary operation with an arbitrary nary one (i.e., an operation taking n arguments). With the proper generalization of the group axioms this gives rise to an nary group.^{[79]} The table gives a list of several structures generalizing groups.
See also
 Abelian group
 Cyclic group
 Euclidean group
 Finitely presented group
 Free group
 Fundamental group
 Grothendieck group
 Group algebra
 Group ring
 Heap (mathematics)
 List of small groups
 Nilpotent group
 Nonabelian group
 Quantum group
 Reductive group
 Solvable group
 Symmetry in physics
 Computational group theory
Notes
^ a: Mathematical Reviews lists 3,224 research papers on group theory and its generalizations written in 2005.
^ aa: The classification was announced in 1983, but gaps were found in the proof. See classification of finite simple groups for further information.
^ b: The closure axiom is already implied by the condition that • be a binary operation. Some authors therefore omit this axiom. However, group constructions often start with an operation defined on a superset, so a closure step is common in proofs that a system is a group. Lang 2002
^ c: See, for example, the books of Lang (2002, 2005) and Herstein (1996, 1975).
^ d: However, a group is not determined by its lattice of subgroups. See Suzuki 1951.
^ e: The fact that the group operation extends this canonically is an instance of a universal property.
^ f: For example, if G is finite, then the size of any subgroup and any quotient group divides the size of G, according to Lagrange's theorem.
^ g: The word homomorphism derives from Greek ὁμός—the same and μορφή—structure.
^ h: The additive notation for elements of a cyclic group would be t • a, t in Z.
^ i: See the Seifert–van Kampen theorem for an example.
^ j: An example is group cohomology of a group which equals the singular cohomology of its classifying space.
^ k: Elements which do have multiplicative inverses are called units, see Lang 2002, §II.1, p. 84.
^ l: The transition from the integers to the rationals by adding fractions is generalized by the quotient field.
^ m: The same is true for any field F instead of Q. See Lang 2005, §III.1, p. 86.
^ n: For example, a finite subgroup of the multiplicative group of a field is necessarily cyclic. See Lang 2002, Theorem IV.1.9. The notions of torsion of a module and simple algebras are other instances of this principle.
^ o: The stated property is a possible definition of prime numbers. See prime element.
^ p: For example, the DiffieHellman protocol uses the discrete logarithm.
^ q: The groups of order at most 2000 are known. Up to isomorphism, there are about 49 billion. See Besche, Eick & O'Brien 2001.
^ r: The gap between the classification of simple groups and the one of all groups lies in the extension problem, a problem too hard to be solved in general. See Aschbacher 2004, p. 737.
^ s: Equivalently, a nontrivial group is simple if its only quotient groups are the trivial group and the group itself. See Michler 2006, Carter 1989.
^ t: More rigorously, every group is the symmetry group of some graph; see Frucht's theorem, Frucht 1939.
^ u: More precisely, the monodromy action on the vector space of solutions of the differential equations is considered. See Kuga 1993, pp. 105–113.
^ v: See Schwarzschild metric for an example where symmetry greatly reduces the complexity of physical systems.
^ w: This was crucial to the classification of finite simple groups, for example. See Aschbacher 2004.
^ x: See, for example, Schur's Lemma for the impact of a group action on simple modules. A more involved example is the action of an absolute Galois group on étale cohomology.
^ y: Injective and surjective maps correspond to mono and epimorphisms, respectively. They are interchanged when passing to the dual category.
Citations
 ^ Herstein 1975, §2, p. 26
 ^ Hall 1967, §1.1, p. 1: "The idea of a group is one which pervades the whole of mathematics both pure and applied."
 ^ Lang 2005, App. 2, p. 360
 ^ Cook, Mariana R. (2009), Mathematicians: An Outer View of the Inner World, Princeton, N.J.: Princeton University Press, p. 24, ISBN 9780691139517
 ^ Herstein 1975, §2.1, p. 27
 ^ Weisstein, Eric W. "Identity Element". MathWorld.
 ^ Herstein 1975, §2.6, p. 54
 ^ Wussing 2007
 ^ Kleiner 1986
 ^ Smith 1906
 ^ Galois 1908
 ^ Kleiner 1986, p. 202
 ^ Cayley 1889
 ^ Wussing 2007, §III.2
 ^ Lie 1973
 ^ Kleiner 1986, p. 204
 ^ Wussing 2007, §I.3.4
 ^ Jordan 1870
 ^ von Dyck 1882
 ^ Curtis 2003
 ^ Mackey 1976
 ^ Borel 2001
 ^ Aschbacher 2004
 ^ Ledermann 1953, §1.2, pp. 4–5
 ^ Ledermann 1973, §I.1, p. 3
 ^ Lang 2002, §I.2, p. 7
 ^ ^{a} ^{b} Lang 2005, §II.1, p. 17
 ^ ^{a} ^{b} Mac Lane 1998
 ^ Lang 2005, §II.3, p. 34
 ^ Lang 2005, §II.1, p. 19
 ^ Ledermann 1973, §II.12, p. 39
 ^ Lang 2005, §II.4, p. 41
 ^ Lang 2002, §I.2, p. 12
 ^ Lang 2005, §II.4, p. 45
 ^ Lang 2002, §I.2, p. 9
 ^ Hatcher 2002, Chapter I, p. 30
 ^ Coornaert, Delzant & Papadopoulos 1990
 ^ for example, class groups and Picard groups; see Neukirch 1999, in particular §§I.12 and I.13
 ^ Seress 1997
 ^ Lang 2005, Chapter VII
 ^ Rosen 2000, p. 54 (Theorem 2.1)
 ^ Lang 2005, §VIII.1, p. 292
 ^ Lang 2005, §II.1, p. 22
 ^ Lang 2005, §II.2, p. 26
 ^ Lang 2005, §II.1, p. 22 (example 11)
 ^ Lang 2002, §I.5, p. 26, 29
 ^ Weyl 1952
 ^ Conway, Delgado Friedrichs & Huson et al. 2001. See also Bishop 1993
 ^ Bersuker, Isaac (2006), The JahnTeller Effect, Cambridge University Press, p. 2, ISBN 0521822122
 ^ Jahn & Teller 1937
 ^ Dove, Martin T (2003), Structure and Dynamics: an atomic view of materials, Oxford University Press, p. 265, ISBN 0198506783
 ^ Welsh 1989
 ^ Mumford, Fogarty & Kirwan 1994
 ^ Lay 2003
 ^ Kuipers 1999
 ^ ^{a} ^{b} Fulton & Harris 1991
 ^ Serre 1977
 ^ Rudin 1990
 ^ Robinson 1996, p. viii
 ^ Artin 1998
 ^ Lang 2002, Chapter VI (see in particular p. 273 for concrete examples)
 ^ Lang 2002, p. 292 (Theorem VI.7.2)
 ^ Kurzweil & Stellmacher 2004
 ^ Artin 1991, Theorem 6.1.14. See also Lang 2002, p. 77 for similar results.
 ^ Lang 2002, §I. 3, p. 22
 ^ Ronan 2007
 ^ Husain 1966
 ^ Neukirch 1999
 ^ Shatz 1972
 ^ Milne 1980
 ^ Warner 1983
 ^ Borel 1991
 ^ Goldstein 1980
 ^ Weinberg 1972
 ^ Naber 2003
 ^ Becchi 1997
 ^ Denecke & Wismath 2002
 ^ Romanowska & Smith 2002
 ^ Dudek 2001
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