Linear representation theory of alternating group:A4: Difference between revisions

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===A two-dimensional irreducible representation over fields not having 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 <math>3</math> 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 [[cyclic group:Z3|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 <math>2\pi/3</math>.
Suppose a field <math>F</math> has characteristic not equal to <math>3</math> 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 over <math>F</math> with kernel the derived subgroup, corresponding to the irreducible two-dimensional representation of [[cyclic group:Z3|the cyclic group of order three]] over <math>F</math>. For instance, over the field of real numbers, such a representation is given by the rotation of multiples of <math>2\pi/3</math> (note that although the description as rotations requires the use of <math>\sqrt{3}</math>, there is an alternative description that uses only integers and hence works in any field).
 
For more on this representation, see [[linear representation theory of cyclic group:Z3]].
 
This representation is not absolutely irreducible. In fact, if we take a quadratic extension of <math>F</math> by a primitive cube root of unity, the representation splits in this extension as a sum of the two one-dimensional irreducible representations with the same kernel mentioned earlier.


==Character table==
==Character table==

Revision as of 00:35, 13 April 2011

This article gives specific information, namely, linear representation theory, about a particular group, namely: alternating group:A4.
View linear representation theory of particular groups | View other specific information about alternating group:A4

This article discusses the linear representation theory of the alternating group of degree four, a group of order 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.

Summary

Item Value
Degrees of irreducible representations over a splitting field 1,1,1,3
Maximum degree of irreducible representation over a splitting field 3
lcm of degrees of irreducible representations over a splitting field 3
Smallest ring of realization of all representations (characteristic zero) Z[e2πi/3)]
Smallest field of realization of all representations (characteristic zero) Q(e2πi/3)
Criterion for a field to be a splitting field Any field of characteristic not 2 or 3 that contains a primitive cube root of unity (sufficient, also necessary?)
Degrees of irreducible representations over a non-splitting field 1,2,2,3
Maximum of degrees of irreducible representations over a non-splitting field 3
lcm of degrees of irreducible representations over a non-splitting field 6

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, namely V4 in A4. This is a subgroup of order four isomorphic to the Klein four-group, and equals the derived 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

Suppose a field F 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 over F with kernel the derived subgroup, corresponding to the irreducible two-dimensional representation of the cyclic group of order three over F. For instance, over the field of real numbers, such a representation is given by the rotation of multiples of 2π/3 (note that although the description as rotations requires the use of 3, there is an alternative description that uses only integers and hence works in any field).

For more on this representation, see linear representation theory of cyclic group:Z3.

This representation is not absolutely irreducible. In fact, if we take a quadratic extension of F by a primitive cube root of unity, the representation splits in this extension as a sum of the two one-dimensional irreducible representations with the same kernel mentioned earlier.

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

Described below for a field of characteristic not 2 or 3:

Type of field Condition on polynomial Condition on q for field of size q Degrees of irreducible representations
Contains a primitive cuberoot of unity x2+x+1 splits 3 divides q1 1,1,1,3
Does not contain a primitive cuberoot of unity x2+x+1 does not split 3 does not divide q1 1,2,3

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}