For a nonzero finite-dimensional complex vector space , a unital matrix algebra acting irreducibly on is the full endomorphism algebra. Its Jacobson radical annihilates : otherwise the radical times is all of , contradicting nilpotence. Faithfulness kills the radical, and the Artin–Wedderburn theorem then leaves one simple matrix factor acting on its standard column module. This is a matrix-algebra theorem, distinct from the orbit-counting Burnside lemma and the finite-group Burnside's theorem.
If is the character of , then Burnside lemma applied to the diagonal action on gives
For a transitive action , this also equals the number of double cosets in .
For a group action, the orbit of a group action of is , and its stabilizer subgroup is . The orbit-stabilizer theorem gives : the map is a well-defined bijection from stabilizer cosets to the orbit.
Within one orbit, the stabilizer subgroups are conjugate, since . Their sizes are therefore equal. Summing stabilizer sizes over a single orbit gives , and summing over all orbits yields
Now count the pairs fixed by the action in two ways. Holding fixed gives choices of , whereas holding fixed gives choices of . Thus
Combining the two identities proves Burnside lemma:
The finiteness hypotheses justify these cardinality sums. If is empty, every sum and the orbit count are zero, so the formula still applies.
Centre the cube at the origin with faces having normals . Every rotational symmetry fixes the centre and permutes these normals, so its rotation matrix is a signed permutation matrix of determinant one. Conversely any such matrix permutes the cube’s coordinates up to signs and preserves the cube. For each of coordinate permutations, four of the eight choices of signs give determinant one. Consequently the rotational symmetry group of a cube has
This counts the rotations directly, without an unverified stabilizer calculation. The TeX’s is damaged transcription: the PDF prints 24.
Let be the face colourings. A colouring fixed by a rotation must be constant on each permutation cycle of faces, giving fixed colourings if the rotation has face cycles. The rotation types are:
RotationNumberFace cycle typeFixed colourings
Identity1
Quarter-turn about opposite face centres6
Half-turn about opposite face centres3
Half-turn about opposite edge midpoints6
Third-turn about opposite vertices8
There are three face axes, each with two quarter-turns and one half-turn; six edge axes, each with one half-turn; and four vertex axes, each with two nonidentity third-turns. These rotations are distinct and, with the identity, total 24, so the table is exhaustive. Face-axis rotations fix their two axial faces; the remaining four faces cycle or pair. Edge half-turns pair all faces, while vertex third-turns form two triples.
Burnside lemma now gives
The three colours are labelled, orthogonal reflections are excluded, and no condition requires every colour to appear.
The singleton orbits are exactly . Every other orbit represented by has size by the orbit-stabilizer theorem. Partitioning into its orbits of a group action therefore gives
For the second identity, count
in two ways. Holding fixed gives
Holding fixed gives . Each orbit contributes points, each with stabilizer size , and hence contributes . Thus , proving Burnside lemma:
For the rotation group , the identity fixes all colorings. Because five is prime, each of the four nonidentity rotations is a single five-cycle and fixes exactly the constant colorings. Burnside lemma therefore gives the number of coloring necklaces
For the dihedral group , the five reflections each fix one vertex and interchange two pairs of vertices, so each fixes colorings. Adding these to the identity and rotation contributions gives the number of coloring bracelets
Burnside lemma says that the number of orbits of a finite group on a finite set is
Indeed, double-count the set . Counting first by gives the numerator. Counting first by gives ; each orbit contributes by the orbit-stabilizer theorem, proving the formula.
Let be the character of the permutation representation. Then
is, by Burnside's lemma, the number of orbits on . A two-transitive group action has exactly two such orbits: the diagonal and the ordered pairs of distinct points. Hence . Transitivity also gives . If is its irreducible character decomposition, then , so exactly one nontrivial irreducible character occurs, with multiplicity one. Thus the permutation character has precisely two distinct irreducible summands.
The Burnside lemma states that for a finite group acting on a finite set ,
To prove it, count
Counting by gives . Counting by gives
using the orbit-stabilizer theorem on each orbit . Dividing by proves the formula.
Let be the character of the permutation representation . Then , and a second application of Burnside's lemma gives
For a two-transitive action there are exactly two orbits on : the diagonal and the ordered pairs of distinct points. Hence . Transitivity says the trivial representation occurs once. Since the squared multiplicities of the irreducible constituents sum to two, there is exactly one further constituent, with multiplicity one, and it is irreducible and nontrivial. Thus
as in the permutation representation of a two-transitive action.
For permutation characters, Burnside lemma on a product gives
Two pairs and lie in the same -orbit exactly when
When , every value is possible because . Therefore the symmetric-group subset permutation representation satisfies
For , the inclusion map between subset permutation modules embeds into , so
is a character. Its norm is
By character orthogonality, is the character of an irreducible representation.
For , complementation is an -equivariant bijection , so
Consequently
the negative of one of the irreducible characters just found, and is not itself the character of a representation.