Number Theory: An Introduction to Mathematics

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4 Representations of Arbitrary Finite Groups 411

It is easily verified that ifs→A(s)is a matrix representation of degreenof a
groupG,thens→A(s−^1 )t(the transpose ofA(s−^1 )) is a representation of the same
degree, thecontragredient representation.Furthermore,s→detA(s)is a representa-
tion of degree 1.
Again, ifρ:s→A(s)andσ:s→B(s)are matrix representations of a group
G, of degreesmandnrespectively, then the Kronecker product mapping

s→A(s)⊗B(s)

is also a representation ofG,ofdegreemn,since

(A(s)⊗B(s))(A(t)⊗B(t))=A(st)⊗B(st).

We will call this representation simply theproductof the representationsρandσ,and
denote it byρ⊗σ.
The basic problem of representation theory is to determine all possible representa-
tions of a given group. As we will see, all representations may in fact be built up from
certain ‘irreducible’ ones.
Letρbe a representation of a groupGby linear transformations of a vector space
V. If a subspaceUofVisinvariantunderG,i.e.if


ρ(s)U⊆U for everys∈G,

then the restrictions toUof the given linear transformations provide a representation
ρUofGby linear transformations of the vector spaceU. If it happens that there exists
another subspaceWinvariant underGsuch thatVis the direct sum ofUandW,i.e.
V=U+WandU∩W={ 0 }, then the representationρis completely determined by
the representationsρUandρWand will be said simply to be theirsum.
A representationρof a groupGby linear transformations of a vector spaceVis
said to beirreducibleif no nontrivial proper subspace ofVis invariant underG,and
reducibleotherwise. Evidently any representation of degree 1 is irreducible.
A matrix representations→A(s),ofdegreen, of a groupGis reducible if it is
equivalent to a representation in which all matrices have the block form
(
P(s) Q(s)
0 R(s)

)


,


whereP(s)is a square matrix of orderm, 0 <m<n.Thens→P(s)ands→R(s)
are representations ofGof degreesmandn−mrespectively. The given representation
is the sum of these representations if there exists a non-singular matrixTsuch that

T−^1 A(s)T=

(


P(s) 0
0 R(s)

)


for everys∈G.

The following theorem of Maschke (1899) reduces the problem of finding all
representations of afinitegroup to that of finding all irreducible representations.

Proposition 9Every representation of a finite group is (equivalent to) a sum of
irreducible representations.
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