Editing Character theory

{{Short description|Concept in mathematical group theory}}
{{About|the use of the term character theory in mathematics|related senses of the word character|Character (mathematics)}}
In [[mathematics]], more specifically in [[group theory]], the '''character''' of a [[group representation]] is a [[function (mathematics)|function]] on the [[group (mathematics)|group]] that associates to each group element the [[trace (linear algebra)|trace]] of the corresponding [[matrix (mathematics)|matrix]]. The character carries the essential information about the representation in a more condensed form. [[Georg Frobenius]] initially developed [[representation theory of finite groups]] entirely based on the characters, and without any explicit matrix realization of representations themselves. This is possible because a [[complex number|complex]] representation of a [[finite group]] is determined (up to [[isomorphism]]) by its character. The situation with representations over a [[field (mathematics)|field]] of positive [[characteristic (algebra)|characteristic]], so-called "modular representations", is more delicate, but [[Richard Brauer]] developed a powerful theory of characters in this case as well. Many deep theorems on the structure of finite groups use characters of [[modular representation theory|modular representations]].

== Applications ==
Characters of [[irreducible representation]]s encode many important properties of a group and can thus be used to study its structure. Character theory is an essential tool in the [[classification of finite simple groups]]. Close to half of the [[mathematical proof|proof]] of the [[Feit–Thompson theorem]] involves intricate calculations with character values. Easier, but still essential, results that use character theory include [[Burnside's theorem]] (a purely group-theoretic proof of Burnside's theorem has since been found, but that proof came over half a century after Burnside's original proof), and a theorem of [[Richard Brauer]] and [[Michio Suzuki (mathematician)|Michio Suzuki]] stating that a finite [[simple group]] cannot have a [[generalized quaternion group]] as its [[Sylow theorems|Sylow {{math|2}}-subgroup]].

==Definitions==
Let {{mvar|V}} be a [[dimension (vector space)|finite-dimensional]] [[vector space]] over a [[field (mathematics)|field]] {{mvar|F}} and let {{math|''ρ'' : ''G'' → GL(''V'')}} be a [[group representation|representation]] of a group {{mvar|G}} on {{mvar|V}}. The '''character''' of {{mvar|ρ}} is the function {{math|''χ<sub>ρ</sub>'' : ''G'' → ''F''}} given by

:<math>\chi_{\rho}(g) = \operatorname{Tr}(\rho(g))</math>

where {{math|Tr}} is the [[trace (linear algebra)|trace]].

A character {{math|''χ<sub>ρ</sub>''}} is called '''irreducible''' or '''simple''' if {{mvar|ρ}} is an [[irreducible representation]].  The '''degree''' of the character {{mvar|χ}} is the [[dimension of a representation|dimension]] of {{mvar|ρ}}; in characteristic zero this is equal to the value {{math|''χ''(1)}}. A character of degree 1 is called '''linear'''. When {{mvar|G}} is finite and {{mvar|F}} has characteristic zero, the '''kernel''' of the character {{math|''χ<sub>ρ</sub>''}} is the [[normal subgroup]]:

:<math>\ker \chi_\rho := \left \lbrace g \in G \mid \chi_{\rho}(g) = \chi_{\rho}(1) \right \rbrace, </math>

which is precisely the kernel of the representation {{mvar|ρ}}. However, the character is ''not'' a group homomorphism in general.

==Properties==
* Characters are [[class function]]s, that is, they each take a constant value on a given [[conjugacy class]]. More precisely, the set of irreducible characters of a given group {{mvar|G}} into a field {{mvar|F}} form a [[basis (linear algebra)|basis]] of the {{mvar|F}}-vector space of all class functions {{math|''G'' → ''F''}}.
* [[Representation_theory#Equivariant_maps_and_isomorphisms|Isomorphic]] representations have the same characters. Over a field of [[characteristic (algebra)|characteristic]] {{math|0}}, two representations are isomorphic [[if and only if]] they have the same character.<ref>Nicolas Bourbaki, ''Algèbre'', Springer-Verlag, 2012, Chap. 8, p392</ref>
* If a representation is the [[direct sum of representations|direct sum]] of [[subrepresentation]]s, then the corresponding character is the sum of the characters of those subrepresentations.
* If a character of the finite group {{mvar|G}} is restricted to a [[subgroup]] {{mvar|H}}, then the result is also a character of {{mvar|H}}.
* Every character value {{math|''χ''(''g'')}} is a sum of {{mvar|n}} {{mvar|m}}-th [[roots of unity]], where {{mvar|n}} is the degree (that is, the dimension of the associated vector space) of the representation with character {{mvar|χ}} and {{mvar|m}} is the [[order (group theory)|order]] of {{mvar|g}}. In particular, when {{math|1=''F'' = '''C'''}}, every such character value is an [[algebraic integer]].
* If {{math|1=''F'' = '''C'''}} and {{mvar|χ}} is irreducible, then  <math display="block">[G:C_G(x)]\frac{\chi(x)}{\chi(1)}</math> is an [[algebraic integer]] for all {{mvar|x}} in {{mvar|G}}.
* If {{mvar|F}} is [[algebraically closed]] and {{math|[[characteristic of a ring|char]](''F'')}} does not divide the [[order of a group|order]] of {{mvar|G}}, then the number of irreducible characters of {{mvar|G}} is equal to the number of [[conjugacy class]]es of {{mvar|G}}. Furthermore, in this case, the degrees of the irreducible characters are divisors of the order of {{mvar|G}} (and they even divide {{math|[''G'' : ''Z''(''G'')]}} if {{math|''F'' {{=}} '''C'''}}).

===Arithmetic properties===
Let ρ and σ be representations of {{mvar|G}}. Then the following identities hold:
*<math>\chi_{\rho \oplus \sigma} = \chi_\rho + \chi_\sigma</math>
*<math>\chi_{\rho \otimes \sigma} = \chi_\rho \cdot \chi_\sigma</math>
*<math>\chi_{\rho^*} = \overline {\chi_\rho}</math>
*<math>\chi_{{\scriptscriptstyle \rm{Alt}^2} \rho}(g) = \tfrac{1}{2}\! \left[ \left(\chi_\rho (g) \right)^2 - \chi_\rho (g^2) \right]</math>
*<math>\chi_{{\scriptscriptstyle \rm{Sym}^2} \rho}(g) = \tfrac{1}{2}\! \left[ \left(\chi_\rho (g) \right)^2 + \chi_\rho (g^2) \right]</math>
where {{math|''ρ''⊕''σ''}} is the [[direct sum of representations|direct sum]], {{math|''ρ''⊗''σ''}} is the [[tensor product]], {{math|''ρ''<sup>∗</sup>}} denotes the [[conjugate transpose]] of {{mvar|ρ}}, and {{math|Alt<sup>2</sup>}} is the [[exterior algebra|alternating product]] {{math|Alt<sup>2</sup>''ρ'' {{=}} ''ρ'' ∧ ''ρ''}} and {{math|Sym<sup>2</sup>}} is the [[symmetric square]], which is determined by
<math display="block">\rho \otimes \rho = \left(\rho \wedge \rho \right) \oplus \textrm{Sym}^2 \rho.</math>

==Character tables==
{{Further|Character table}}
The irreducible [[complex number|complex]] characters of a finite group form a '''character table''' which encodes much useful information about the group {{mvar|G}} in a compact form.  Each row is labelled by an irreducible representation and the entries in the row are the characters of the representation on the respective conjugacy class of {{mvar|G}}. The columns are labelled by (representatives of) the conjugacy classes of {{mvar|G}}. It is customary to label the first row by the character of the '''[[trivial representation]]''', which is the trivial action of {{mvar|G}} on a 1-dimensional vector space by <math> \rho(g)=1</math> for all <math> g\in G </math>. Each entry in the first row is therefore 1. Similarly, it is customary to label the first column by the identity. Therefore, the first column contains the degree of each irreducible character.

Here is the character table of

:<math>C_3 = \langle u \mid u^{3} = 1 \rangle,</math>

the [[cyclic group]] with three elements and generator ''u'':

{| class="wikitable"
|-
|&nbsp;
|{{math|(1)}}
|{{math|(''u'')}}
|{{math|(''u''<sup>2</sup>)}}
|-
|{{math|'''1'''}}
|{{math|1}}
|{{math|1}}
|{{math|1}}
|-
|{{math|''χ''<sub>1</sub>}}
|{{math|1}}
|{{mvar|ω}}
|{{math|''ω''<sup>2</sup>}}
|-
|{{math|''χ''<sub>2</sub>}}
|{{math|1}}
|{{math|''ω''<sup>2</sup>}}
|{{mvar|ω}}
|-
|}

where {{mvar|ω}} is a [[primitive root of unity|primitive]] third root of unity.

The character table is always square, because the number of irreducible representations is equal to the number of conjugacy classes.<ref>Serre, §2.5</ref>

===Orthogonality relations===
{{main|Schur orthogonality relations}}
The space of complex-valued [[class function]]s of a finite group {{mvar|G}} has a natural [[inner product]]:

:<math>\left \langle \alpha, \beta\right \rangle := \frac{1}{|G|}\sum_{g \in G} \alpha(g) \overline{\beta(g)}</math>

where {{math|{{overline|''β''(''g'')}}}} is the [[complex conjugate]] of {{math|''β''(''g'')}}. With respect to this inner product, the irreducible characters form an [[orthonormal basis]] for the space of class-functions, and this yields the orthogonality relation for the rows of the character table:

:<math>\left \langle \chi_i, \chi_j \right \rangle  = \begin{cases} 0 & \mbox{ if } i \ne j, \\ 1 & \mbox{ if } i = j. \end{cases}</math>

For {{math|''g'', ''h''}} in {{mvar|G}}, applying the same inner product to the columns of the character table yields:

:<math>\sum_{\chi_i} \chi_i(g) \overline{\chi_i(h)} = \begin{cases} \left | C_G(g) \right |, & \mbox{ if } g, h \mbox{ are conjugate } \\ 0 & \mbox{ otherwise.}\end{cases}</math>

where the sum is over all of the irreducible characters {{math|''χ<sub>i</sub>''}} of {{mvar|G}} and the symbol {{math|{{pipe}}''C<sub>G</sub>''(''g''){{pipe}}}} denotes the order of the [[centralizer]] of {{mvar|g}}. Note that since {{mvar|g}} and {{mvar|h}} are conjugate iff they are in the same column of the character table, this implies that the columns of the character table are orthogonal.

The orthogonality relations can aid many computations including:
* Decomposing an unknown character as a linear combination of irreducible characters.
* Constructing the complete character table when only some of the irreducible characters are known.
* Finding the orders of the centralizers of representatives of the conjugacy classes of a group.
* Finding the order of the group.

===Character table properties===
Certain properties of the group {{mvar|G}} can be deduced from its character table:

* The order of {{mvar|G}} is given by the sum of the squares of the entries of the first column (the degrees of the irreducible characters). More generally, the sum of the squares of the [[absolute value]]s of the entries in any column gives the order of the centralizer of an element of the corresponding conjugacy class.
*All normal subgroups of {{mvar|G}} (and thus whether or not {{mvar|G}} is simple) can be recognised from its character table. The [[Kernel (group theory)|kernel]] of a character {{mvar|χ}} is the set of elements {{mvar|g}} in {{mvar|G}} for which {{math|''χ''(''g'') {{=}} ''χ''(1)}}; this is a normal subgroup of {{mvar|G}}. Each normal subgroup of {{mvar|G}} is the intersection of the kernels of some of the irreducible characters of {{mvar|G}}.
*The [[commutator subgroup]] of {{mvar|G}} is the intersection of the kernels of the linear characters of {{mvar|G}}.
*If {{mvar|G}} is finite, then since the character table is square and has as many rows as conjugacy classes, it follows that {{mvar|G}} is [[abelian group|abelian]] iff each conjugacy class is a singleton iff the character table of {{mvar|G}} is <math>|G| \!\times\! |G|</math> iff each irreducible character is linear.
*It follows, using some results of [[Richard Brauer]] from [[modular representation theory]], that the prime divisors of the orders of the elements of each conjugacy class of a finite group can be deduced from its character table (an observation of [[Graham Higman]]).

The character table does not in general determine the group [[up to]] [[group isomorphism|isomorphism]]: for example, the [[quaternion group]] {{mvar|Q}} and the [[dihedral group]] of {{math|8}} elements, {{math|''D''<sub>4</sub>}}, have the same character table. Brauer asked whether the character table, together with the knowledge of how the powers of elements of its conjugacy classes are distributed, determines a finite group up to isomorphism. In 1964, this was answered in the negative by [[E. C. Dade]].

The linear representations of {{mvar|G}} are themselves a group under the [[tensor product]], since the tensor product of 1-dimensional vector spaces is again 1-dimensional. That is, if <math>\rho_1:G\to V_1</math> and <math> \rho_2:G\to V_2</math> are linear representations, then <math> \rho_1\otimes\rho_2 (g)=(\rho_1(g)\otimes\rho_2(g))</math> defines a new linear representation. This gives rise to a group of linear characters, called the [[character group]] under the operation <math> [\chi_1*\chi_2](g)=\chi_1(g)\chi_2(g)</math>. This group is connected to [[Dirichlet character]]s and [[Fourier analysis]].

==Induced characters and Frobenius reciprocity==
{{main|Induced character|Frobenius reciprocity}}
The characters discussed in this section are assumed to be complex-valued. Let {{mvar|H}} be a subgroup of the finite group {{mvar|G}}. Given a character {{mvar|χ}} of {{mvar|G}}, let {{math|''χ<sub>H</sub>''}} denote its restriction to {{mvar|H}}. Let {{mvar|θ}} be a character of {{mvar|H}}. [[Ferdinand Georg Frobenius]] showed how to construct a character of {{mvar|G}} from {{mvar|θ}}, using what is now known as ''[[Frobenius reciprocity]]''. Since the irreducible characters of {{mvar|G}} form an orthonormal basis for the space of complex-valued class functions of {{mvar|G}}, there is a unique class function {{math|''θ<sup>G</sup>''}} of {{mvar|G}} with the property that

:<math> \langle \theta^{G}, \chi \rangle_G = \langle \theta,\chi_H \rangle_H </math>

for each irreducible character {{mvar|χ}} of {{mvar|G}} (the leftmost inner product is for class functions of {{mvar|G}} and the rightmost inner product is for class functions of {{mvar|H}}). Since the restriction of a character of {{mvar|G}} to the subgroup {{mvar|H}} is again a character of {{mvar|H}}, this definition makes it clear that {{math|''θ<sup>G</sup>''}} is a non-negative [[integer]] combination of irreducible characters of {{mvar|G}}, so is indeed a character of {{mvar|G}}. It is known as ''the character of'' {{mvar|G}} ''induced from'' {{mvar|θ}}. The defining formula of Frobenius reciprocity can be extended to general complex-valued class functions.

Given a matrix representation {{mvar|ρ}} of {{mvar|H}}, Frobenius later gave an explicit way to construct a matrix representation of {{mvar|G}}, known as the representation [[induced representation|induced from]] {{mvar|ρ}}, and written analogously as {{math|''ρ<sup>G</sup>''}}. This led to an alternative description of the induced character {{math|''θ<sup>G</sup>''}}. This induced character vanishes on all elements of {{mvar|G}} which are not conjugate to any element of {{mvar|H}}. Since the induced character is a class function of {{mvar|G}}, it is only now necessary to describe its values on elements of {{mvar|H}}. If one writes {{mvar|G}} as a [[disjoint union]] of right [[coset]]s of {{mvar|H}}, say

:<math>G = Ht_1 \cup \ldots \cup Ht_n,</math>

then, given an element {{mvar|h}} of {{mvar|H}}, we have:

:<math> \theta^G(h) = \sum_{i \ : \ t_iht_i^{-1} \in H} \theta \left (t_iht_i^{-1} \right ).</math>

Because {{mvar|θ}} is a class function of {{mvar|H}}, this value does not depend on the particular choice of coset representatives.

This alternative description of the induced character sometimes allows explicit computation from relatively little information about the embedding of {{mvar|H}} in {{mvar|G}}, and is often useful for calculation of particular character tables. When {{mvar|θ}} is the trivial character of {{mvar|H}}, the induced character obtained is known as the '''permutation character''' of {{mvar|G}} (on the cosets of {{mvar|H}}).

The general technique of character induction and later refinements found numerous applications in [[Group_theory#Finite_group_theory|finite group theory]] and elsewhere in mathematics, in the hands of mathematicians such as [[Emil Artin]], [[Richard Brauer]], [[Walter Feit]] and [[Michio Suzuki (mathematician)|Michio Suzuki]], as well as Frobenius himself.

==Mackey decomposition==
The Mackey decomposition was defined and explored by [[G. Mackey|George Mackey]] in the context of [[Lie group]]s, but is a powerful tool in the character theory and representation theory of finite groups. Its basic form concerns the way a character (or module) induced from a subgroup {{mvar|H}} of a finite group {{mvar|G}} behaves on restriction back to a (possibly different) subgroup {{mvar|K}} of {{mvar|G}}, and makes use of the decomposition of {{mvar|G}} into {{math|(''H'', ''K'')}}-double cosets.

If <math display="inline"> G = \bigcup_{t \in T} HtK </math> is a disjoint union, and {{mvar|θ}} is a complex class function of {{mvar|H}}, then Mackey's formula states that

:<math>\left( \theta^{G}\right)_K = \sum_{ t \in T} \left(\left [\theta^{t} \right ]_{t^{-1}Ht \cap K}\right)^{K},</math>

where {{math|''θ<sup>t</sup>''}} is the class function of {{math|''t''<sup>−1</sup>''Ht''}} defined by {{math|''θ<sup>t</sup>''(''t''<sup>−1</sup>''ht'') {{=}} ''θ''(''h'')}} for all {{mvar|h}} in {{mvar|H}}. There is a similar formula for the restriction of an induced module to a subgroup, which holds for representations over any [[ring (mathematics)|ring]], and has applications in a wide variety of algebraic and [[topology|topological]] contexts.

Mackey decomposition, in conjunction with Frobenius reciprocity, yields a well-known and useful formula for the inner product of two class functions {{mvar|θ}} and {{mvar|ψ}} induced from respective subgroups {{mvar|H}} and {{mvar|K}}, whose utility lies in the fact that it only depends on how conjugates of {{mvar|H}} and {{mvar|K}} intersect each other. The formula (with its derivation) is:

:<math>\begin{align}
\left \langle \theta^{G},\psi^{G} \right \rangle &= \left \langle \left(\theta^{G}\right)_{K},\psi \right \rangle \\
&= \sum_{ t \in T} \left \langle \left( \left [\theta^{t} \right ]_{t^{-1}Ht \cap K}\right)^{K}, \psi \right \rangle \\
&= \sum_{t \in T} \left \langle \left(\theta^{t} \right)_{t^{-1}Ht \cap K},\psi_{t^{-1}Ht \cap K} \right \rangle, 
\end{align}</math>

(where {{mvar|T}} is a full set of {{math|(''H'', ''K'')}}-double coset representatives, as before). This formula is often used when {{mvar|θ}} and {{mvar|ψ}} are linear characters, in which case all the inner products appearing in the right hand sum are either {{math|1}} or {{math|0}}, depending on whether or not the linear characters {{math|''θ<sup>t</sup>''}} and {{mvar|ψ}} have the same restriction to {{math|''t''<sup>−1</sup>''Ht'' ∩ ''K''}}. If {{mvar|θ}} and {{mvar|ψ}} are both trivial characters, then the inner product simplifies to {{math|{{pipe}}''T''{{pipe}}}}.

=="Twisted" dimension==
One may interpret the character of a representation as the "twisted" [[dimension (vector space)|dimension of a vector space]].<ref name="Gannon">{{Harv|Gannon|2006}}</ref> Treating the character as a function of the elements of the group {{math|''χ''(''g'')}}, its value at the [[Identity element|identity]] is the dimension of the space, since {{math|''χ''(1) {{=}} Tr(''ρ''(1)) {{=}} Tr(''I<sub>V</sub>'') {{=}} dim(''V'')}}. Accordingly, one can view the other values of the character as "twisted" dimensions.{{clarify|date=June 2011|reason=recursive definition}}

One can find analogs or generalizations of statements about dimensions to statements about characters or representations. A sophisticated example of this occurs in the theory of [[monstrous moonshine]]: the [[j-invariant|{{mvar|j}}-invariant]] is the [[graded dimension]] of an infinite-dimensional graded representation of the [[Monster group]], and replacing the dimension with the character gives the [[McKay–Thompson series]] for each element of the Monster group.<ref name="Gannon" />

==Characters of Lie groups and Lie algebras==
{{See also|Weyl character formula|Algebraic character}}

If <math>G</math> is a [[Lie group]] and <math>\rho</math> a finite-dimensional representation of <math>G</math>, the character <math>\chi_\rho</math> of <math>\rho</math> is defined precisely as for any group as
:<math>\chi_\rho(g)=\operatorname{Tr}(\rho(g))</math>.
Meanwhile, if <math>\mathfrak g</math> is a [[Lie algebra]] and <math>\rho</math> a finite-dimensional representation of <math>\mathfrak g</math>, we can define the character <math>\chi_\rho</math> by
:<math>\chi_\rho(X)=\operatorname{Tr}(e^{\rho(X)})</math>.
The character will satisfy <math>\chi_\rho(\operatorname{Ad}_g(X))=\chi_\rho(X)</math> for all <math>g</math> in the associated Lie group <math> G</math> and all <math>X\in\mathfrak g</math>. If we have a Lie group representation and an associated Lie algebra representation, the character <math>\chi_\rho</math> of the Lie algebra representation is related to the character <math>\Chi_\rho</math> of the group representation by the formula
:<math>\chi_\rho(X)=\Chi_\rho(e^X)</math>.

Suppose now that <math>\mathfrak g</math> is a complex [[semisimple Lie algebra]] with Cartan subalgebra <math>\mathfrak h</math>. The value of the character <math>\chi_\rho</math> of an irreducible representation <math>\rho</math> of <math>\mathfrak g</math> is determined by its values on <math>\mathfrak h</math>. The restriction of the character to <math>\mathfrak h</math> can easily be computed in terms of the [[weight space (representation theory)|weight space]]s, as follows:
:<math>\chi_\rho(H) = \sum_\lambda m_\lambda e^{\lambda(H)},\quad H\in\mathfrak h</math>,
where the sum is over all [[weight (representation theory)|weights]] <math>\lambda</math> of <math>\rho</math> and where <math>m_\lambda</math> is the multiplicity of <math>\lambda</math>.<ref>{{harvnb|Hall|2015}} Proposition 10.12</ref>

The (restriction to <math>\mathfrak h</math> of the) character can be computed more explicitly by the Weyl character formula.

==See also==
*{{slink|Irreducible representation|Applications in theoretical physics and chemistry}}
* [[Association scheme]]s, a combinatorial generalization of group-character theory.
* [[Clifford theory]], introduced by [[A. H. Clifford]] in 1937, yields information about the restriction of a complex irreducible character of a finite group {{mvar|G}} to a normal subgroup {{mvar|N}}.
* [[Frobenius formula]]
* [[Real element]], a group element ''g'' such that ''χ''(''g'') is a real number for all characters ''χ''

==References==
{{Reflist}}
{{refbegin}}
* Lecture 2 of {{Fulton-Harris}}  [http://isites.harvard.edu/fs/docs/icb.topic1381051.files/fulton-harris-representation-theory.pdf   online]
*{{Cite book | first = Terry | last = Gannon | title = Moonshine beyond the Monster: The Bridge Connecting Algebra, Modular Forms and Physics | year = 2006 | publisher = Cambridge University Press | isbn = 978-0-521-83531-2 }}
* {{Citation| last=Hall|first=Brian C.|title=Lie groups, Lie algebras, and representations: An elementary introduction|edition=2nd|series=Graduate Texts in Mathematics|volume=222|publisher=Springer|year=2015|isbn=978-3319134666}}
* {{cite book| last = Isaacs | first = I.M. | title=Character Theory of Finite Groups | publisher=Dover | year=1994 | isbn=978-0-486-68014-9 | edition=Corrected reprint of the 1976 original, published by Academic Press.}}
* {{cite book | last1 = James | first1 = Gordon |authorlink2=Martin Liebeck| last2 = Liebeck | first2 = Martin | title=Representations and Characters of Groups (2nd ed.) | year=2001 | publisher=Cambridge University Press | isbn=978-0-521-00392-6}}
* {{cite book | author-link=J.-P. Serre | first=Jean-Pierre | last=Serre | title=Linear Representations of Finite Groups | publisher=Springer-Verlag | year=1977 | isbn=978-0-387-90190-9 | location=New York-Heidelberg | series=Graduate Texts in Mathematics | volume=42 | others=Translated from the second French edition by Leonard L. Scott | mr=0450380 | doi=10.1007/978-1-4684-9458-7 | url-access=registration | url=https://archive.org/details/linearrepresenta1977serr }}
{{refend}}

==External links==
* {{PlanetMath|urlname=Character|title=Character}}

{{Authority control}}

[[Category:Representation theory of groups]]