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Mathematics / group-theory

Group Theory

Group theory studies algebraic structures that describe symmetry, reversible operations, and the relationships between transformations.

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Group theory is a branch of abstract algebra concerned with groups: sets equipped with an operation satisfying precise rules for composition, identity, and inverses. Groups provide a common language for symmetry, whether their elements are numbers, permutations, matrices, or geometric transformations. The subject investigates their internal structure, their relationships, and their actions on other objects, connecting algebra with geometry and many other areas of mathematics. (math.mit.edu)

Definition and basic examples

A group consists of a set GG and a binary operation, usually written as multiplication. Its defining axioms are:

  • Closure: abab belongs to GG whenever a,b∈Ga,b\in G.
  • Associativity: (ab)c=a(bc)(ab)c=a(bc).
  • Identity: an element ee satisfies ea=ae=aea=ae=a.
  • Inverses: each aa has an element a−1a^{-1} satisfying aa−1=a−1a=eaa^{-1}=a^{-1}a=e.

Closure can instead be incorporated into the definition of the operation as a map G×G→GG\times G\to G. The identity and each element’s inverse are unique. Commutativity is not required; a group satisfying ab=baab=ba for all elements is an abelian group. (math.mit.edu)

The integers form a group under addition, with identity 00 and inverse −a-a. In modular arithmetic, the residue classes modulo a positive integer nn form an additive group with nn elements. Both examples are cyclic groups, meaning that repeated application of the operation to one generator produces every element. Every cyclic group is abelian, although not every abelian group is cyclic. (ocw.mit.edu)

The symmetric group SnS_n consists of all permutations of nn objects, composed as functions, and has n!n! elements. The dihedral group of a regular nn-gon contains its nn rotations and nn reflections. Invertible square matrices of a fixed size over a field form a group under matrix multiplication. These examples demonstrate that the operation need not resemble ordinary numerical multiplication. (jmilne.org)

Subgroups, quotients, and structural maps

A subgroup is a subset that itself forms a group under the inherited operation. Its left cosets, gH={gh:h∈H}gH=\{gh:h\in H\}, partition the original group. For a finite group, this partition gives Lagrange’s theorem:

∣G∣=[G:H]∣H∣,|G|=[G:H]|H|,

where [G:H][G:H] is the number of left cosets. Consequently, a subgroup’s order divides the group’s order. (math.mit.edu)

A normal subgroup NN satisfies gNg−1=NgNg^{-1}=N for every g∈Gg\in G. Its cosets form a quotient group G/NG/N, with multiplication (gN)(hN)=ghN(gN)(hN)=ghN. Normality ensures that this operation does not depend on the representatives chosen. (math.mit.edu)

A group homomorphism is a map φ:G→K\varphi:G\to K preserving multiplication: φ(ab)=φ(a)φ(b)\varphi(ab)=\varphi(a)\varphi(b). Its kernel consists of elements mapped to the identity and is normal. A bijective homomorphism is an isomorphism, identifying groups with the same algebraic structure despite different descriptions. The first isomorphism theorem states that G/ker⁡φG/\ker\varphi is isomorphic to the image of φ\varphi. (jmilne.org)

Actions and finite-group structure

A group action assigns transformations of a set XX to group elements so that e⋅x=xe\cdot x=x and (gh)⋅x=g⋅(h⋅x)(gh)\cdot x=g\cdot(h\cdot x). An element’s orbit comprises all points reachable from it; its stabilizer comprises the group elements fixing it. For finite groups, the orbit–stabilizer formula relates these quantities:

∣Orb⁡(x)∣=∣G∣∣Stab⁡(x)∣.|\operatorname{Orb}(x)|=\frac{|G|}{|\operatorname{Stab}(x)|}.

Actions connect abstract groups to concrete symmetries and support counting arguments. (jmilne.org)

The Sylow theorems constrain finite groups through their prime-power subgroups. If ∣G∣=pam|G|=p^am, with pp prime and p∤mp\nmid m, subgroups of order pap^a exist. They are mutually conjugate, and their number divides mm and is congruent to 11 modulo pp. Such restrictions often establish whether a subgroup must be normal. (crypto.stanford.edu)

A simple group is nontrivial and has no proper nontrivial normal subgroup. A solvable group admits a finite series of subgroups, each normal in the next, whose successive quotients are abelian. These concepts describe different ways in which groups resist or permit decomposition. (math.mit.edu)

Representations and continuous symmetry

Representation theory studies homomorphisms from groups to groups of invertible linear transformations of a vector space. It translates group structure into linear algebra. An irreducible representation has no nonzero proper invariant subspace; decomposing representations into irreducible components reveals how symmetries act on different parts of a system. (math.mit.edu)

A Lie group is both a group and a smooth manifold, with smooth multiplication and inversion. Examples include rotation groups and invertible real or complex matrix groups. Its associated Lie algebra describes infinitesimal structure near the identity. This provides tools for studying continuous symmetries alongside the discrete symmetries of finite groups. (ocw.mit.edu)

Connections and applications

In Galois theory, groups of field automorphisms encode relationships among polynomial roots. Over a field of characteristic zero, a polynomial is solvable by radicals exactly when its Galois group is solvable. This explains why no radical formula solves every polynomial equation of degree five. (jmilne.org)

In crystallography, groups organize rotations, reflections, and translations preserving crystal structures. Three-dimensional periodic structures have 230 crystallographic space-group types. In quantum mechanics, representations describe how states transform under symmetry operations; Lie groups provide the mathematical framework for continuous symmetries in physical theories. (iucr.org)