geometric representation theory
representation, 2-representation, ∞-representation
Grothendieck group, lambda-ring, symmetric function, formal group
principal bundle, torsor, vector bundle, Atiyah Lie algebroid
Eilenberg-Moore category, algebra over an operad, actegory, crossed module
In representation theory, Mackey theory refers to a set of tools for constructing and classifying irreducible representations of a group from that of a normal subgroup , by using induction from the stabilizer groups of the adjoint action of on the set of irreps of .
(Also referred to as little group-methods, cf. Wigner classification.)
Consider
and denote:
the dual group of group characters, hence, since is abelian, of irreducible representations of ,
the adjoint action of on and the induced action on :
a set of representatives of the resulting orbits of in ,
the corresponding stabilizer subgroups of ,
the corresponding subgroups of
Finally, denote
which is a group character on , by the definition of .
Similarly, for an irrep of , write
and consider the induced representations of the tensor products:
The representations (1) are irreducible.
If then and .
Every irrep of is of the form , up to isomorphism.
Consider the semidirect product group , with
the cyclic group of order ,
the cyclic group of order 2 acting on via the sign involution.
In order find all the (complex) irreps of we unwind the statement of Prop. :
(We denote congruence classes by square brackets: .)
First, the complex irreps of the normal subgroup are themselves labeled by and given by
On these, the nontrivial element acts by :
From this we have two kinds of orbits:
the singleton orbits with stabilizer :
, which always exists
and , which exists when is an even number,
the pairs with stabilizer the trivial group :
, for (with the floor).
The first singleton in the first case gives rise to two irreps, corresponding to the two irreps of (the trivial representation and the sign representation):
and
while the second singleton in the first case similarly gives
and
The second case gives rise to one irrep for each :
These latter irreps are 2-dimensional, with an evident matrix representation given by
As a consistency check that we found all irreps, we verify that the sum of squares formula holds:
We have found two 1-dimensional irreps when is odd and four of them when is even, together with irreps of dimension 2, whence the sum of their squares of dimensions is,
for odd :
and for even :
correctly coinciding with the order of our group :
For construction of irreps of wreath products of groups see there.
The original article:
General discussion:
Review for the case of finite groups:
Charles Curtis, Irving Reiner, around Prop. 11.8 of: Representation theory of finite groups and associative algebras, AMS (1962) [ISBN:978-0-8218-4066-5]
Jean-Pierre Serre, section 8.2 of: Linear Representations of Finite Groups, Graduate Texts in Mathematics 42, Springer (1977) [doi:10.1007/978-1-4684-9458-7, pdf]
Brian Conrad: Mackey theory and applications [pdf, pdf]
Amirtanshu Prasad, M. K. Vemuri: Mackey’s Little Group Method [pdf, pdf]
S. Martin: Mackey Theory, chapter 12 of Representation Theory, notes by Dexter Chua (2016) [pdf]
Further developments:
Review for the case of Lie groups (cf. Wigner classification):
Last revised on May 11, 2025 at 17:29:19. See the history of this page for a list of all contributions to it.