Linear representation theory of alternating group:A4

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This article gives specific information, namely, linear representation theory, about a particular group, namely: alternating group:A4.
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This article discusses the linear representation theory of the alternating group of degree four. For convenience, the underlying set is {1,2,3,4}, and permutations are written using the cycle decomposition notation.

See alternating group:A4 and subgroup structure of alternating group:A4 for background information on the group structure.

Representations

The trivial representation

The trivial representation works over all fields. It is a one-dimensional representation that sends every element of the group to the identity matrix.

The three-dimensional irreducible representation

There is a unique three-dimensional irreducible representation that works over any field of chracteristic not equal to 2. Here is one way of describing this representation. Consider the action of the alternating group on a four-dimensional vector space, by permuting the basis vectors through its action on a set of size four. This action hsa an invariant subspace of codimension one: the subspace comprising vectors whose coordinates add to zero. This gives a three-dimensional vector space on which the alternating group acts, and this is an irreducible representation.

The two one-dimensional representations with kernel of order four

The alternating group of degree four has a unique proper nontrivial normal subgroup. This is a subgroup of order four, and equals the commutator subgroup. It is explicitly given by:

K:={(),(1,2)(3,4),(1,3)(2,4),(1,4)(2,3)}.

There are two one-dimensional representations with kernel K. These correspond to the two one-dimensional representations of the quotient group, which is cyclic of order three (see linear representation theory of cyclic group:Z3 for details). The two representations are, explicitly as follows:

  • One representation sends (1,2,3),(3,2,4),(4,2,1),(1,3,4) to e2πi/3 and (1,3,2),(3,4,2),(4,1,2),(1,4,3) to e2πi/3.
  • The other representation sends (1,2,3),(3,2,4),(4,2,1),(1,3,4) to e2πi/3 and (1,3,2),(3,4,2),(4,1,2),(1,4,3) to e2πi/3.

The analogues of these representations work over any field that has characteristic not equal to 3 and has primitive cuberoots of unity.

A two-dimensional irreducible representation over fields not having primitive cuberoots of unity

If the field has characteristic not equal to 3 and does not have a primitive cuberoot of unity, the two representations described in the previous section have no analogue. Instead, there is an irreducible two-dimensional representation, corresponding to the irreducible two-dimensional representation of the cyclic group of order three over such fields. For instance, over the field of real numbers, such a representation is given by the rotation of multiples of 2π/3.

Character table

Representation/conjugacy class representative () (1,2)(3,4) (1,2,3) (1,3,2)
trivial representation 1 1 1 1
first nontrivial one-dimensional representation 1 1 e2πi/3 e2πi/3
second nontrivial one-dimensional representation 1 1 e2πi/3 e2πi/3
three-dimensional irreducible representation 3 -1 0 0

Here are the characters multiplied by conjugacy class size and divided by the degree of the representation. Note that size-degree-weighted characters are algebraic integers:

Representation/conjugacy class representative () (1,2)(3,4) (1,2,3) (1,3,2)
trivial representation 1 3 4 4
first nontrivial one-dimensional representation 1 3 4e2πi/3 4e2πi/3
second nontrivial one-dimensional representation 1 3 4e2πi/3 4e2πi/3
three-dimensional irreducible representation 1 -1 0 0

Degrees of irreducible representations

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Realization information

Smallest ring of realization

Representation Smallest ring of realization Smallest set of elements that can be used as matrix entries for the ring
trivial representation Z -- ring of integers {1}
first nontrivial irreducible representation Z[e2πi/3] {1,e2πi/3,e2πi/3}
second nontrivial irreducible representation Z[e2πi/3] {1,e2πi/3,e2πi/3}
irreducible three-dimensional representation Z {1,0,1}
irreducible two-dimensional representation over fields not containing a primitive cuberoot of unity Z {1,0,1}