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
Given a group with subgroup then the evident operation of restricting linear representations of to -representations has both a left adjoint (2) and a right adjoint functor (5). For , the image is called the left induced representation and the image is called the right induced representation or co-induced representation of .
Often this is considered for finite groups or at least for subgroups of finite index, in which case these left and right adjoints agree to make an ambidextrous adjunction (Prop. ) and then are both traditionally denoted and just called the induced representation. The hom-isomorphism of the adjunction in this case is traditionally known as Frobenius reciprocity.
Consider:
a group,
a ground field (or ground ring),
the -linear span of the elements of , hence with linear basis , and equipped with the structure of the group algebra of over , to be regarded canonically as a module (bimodule) over itself,
the category of -linear representations of ,
with intertwiners between them as morphisms,
equivalently the category of -modules, with hom-spaces to be denoted
a subgroup inclusion.
Write
for the functor forming restricted representations along (letting act on a given -representation via its inclusion into ).
(left induced representation) The functor (1) has a left adjoint given by
where on the right we have the -vector space (or -module) underlying the tensor product of (right-with-left) -modules equipped with the -group action given by
We claim that the hom-isomorphism is given by evaluation at the neutral element :
To see this, just observe that
where the first equality is by definition of the tensor product, the second-but-last is (3) and the last one is by the -equivariance of . This shows that is -equivariant and that it uniquely determines , hence that we have a bijection of hom-sets
Finally, it is manifest that this bijection is natural in and , and so this establishes a hom-isomorphism exhibiting the claimed adjunction .
The counit of the left adjunction (Prop. ) is given by inserting the neutral element:
The adjunction unit is (see there) the adjunct of the identity map:
hence is its image under the hom-isomorphism (4). From that formula (4) we have indeed
(right induced representation) The functor (1) has a right adjoint given by
where on the right we have the -vector space (or -module) of -equivariant -linear maps equipped with the -group action given by
We claim that the hom-isomorphism is given by evaluation at the neutral element :
To see this, just observe that
where the first equality is the -equivariance of , the second is (6) and the last one is the -equivariance of . This shows that is -equivariant and that it uniquely determines , hence that we have a bijection of hom-sets:
Finally, it is manifest that this bijection is natural in and , and so this establishes a hom-isomorphism exhibiting the claimed adjunction .
The counit of the right adjunction (Prop. ) is given by evaluation at the neutral element:
The adjunction counit is (see there) the adjunct of the identity map:
hence is its image under the hom-isomorphism (7). From that formula (7) we have indeed
A first step towards a deeper understanding for what’s going on with induced representations above is to resolve the subgroup inclusion to a (Kan) fibration of groupoids, which will show that left/right induced representations are about forming (direct) sums/products of contributions over the homotopy fiber of .
To that end, recall for any group action on a set the action groupoid
Examples are delooping groupoids and “homotopy double coset groupoids” like :
where our variance convention is such that functors are equivalent to left group actions in , and in particular functors are directly identified with linear representations of :
Accordingly, for any groupoid, functors are linear groupoid representations.
For a subgroup inclusion:
the homotopy double coset groupoid is equivalent to the delooping groupoid of :
such that the canonical functor
is a resolution of by a surjective Kan fibration,
thus exhibiting its ordinary fiber as the homotopy fiber of ,
the induced equivalence of representation-categories
is exhibited by sending a given -representation to the groupoid representation given by
Note that on the left is (the name of) an object of the groupoid , while on the right it is the actual set of right -translates of the element .
The following functor is evidently both essentially surjective as well as fully faithful, therefore is an equivalence of groupoids:
The claim that this factors through a surjective Kan fibration is now immediate from inspection.
Moreover, the following inspection shows that the claimed operation extends to a functor which is a strict right inverse to precomposition with the previous resolution functor:
(To note here that the natural transformation in the middle is indeed well-defined, due to the the intertwining-property of the homomorphism of linear representations.)
Hence by the 2-out-of-3-property enjoyed by equivalences of groupoids (cf. the canonical model structure on groupoids) it follows that is an equivalence, as claimed.
With this in hand we have an equivalent but “more obvious” re-statement of the existence of left induced representations (2):
(resolved left induced representation) The functor (8) has a left adjoint given by
where on the right we let act in the evident way between direct summands.
The hom-isomorphism is essentially tautologous:
where we don’t display the -action, which is however evident and evidently respected.
Under the identification of -representations with groupoid representations according to Prop. , their left induced representations (9) are simply the direct sum of the contributions of over the homotopy fiber of :
We formulate induction and coinduction of representations abstractly in homotopy type theory. (Hence the following is automatically the (∞,1)-category theory-version, which in parts is sometimes referred to as cohomological induction.)
Let be an ambient (∞,1)-topos. By the discussion at ∞-action, for a group object in , hence an ∞-group, the slice (∞,1)-topos over its delooping is the (∞,1)-category of -∞-actions
(A genuine ∞-representation/∞-module over may be taken to be a an abelian -group object in , but we can just as well work in the more general context of possibly non-linear representations, hence of actions.)
Accordingly, for a homomorphism of ∞-groups, hence for a morphism of their deloopings, there is the corresponding base change geometric morphism
Here
the inverse image/(∞,1)-pullback functor produces the “restricted” -representations along ;
the dependent sum is the induced representation ∞-functor;
the dependent product is the coinduced representation ∞-functor.
For the case of permutation representations of discrete groups this perspective is made explicit by Lawvere 1969 p. 14, 1970 p. 5.
We show that for subgroup inclusions of finite index the left and right induced representations (above) agree.
(comparison map between left and right induced representations)
For a subgroup inclusion and , we have a -equivariant linear injection from the left (2) into the right induced representation (5)
natural in , which is an isomorphism if the subgroup inclusion has finite index.
Define to take homogeneous elements of the form , for , to the linear map which, in turn, is given on basis elements by
First to observe that this construction is well defined, in that
is -equivariant,
which is immediate from the form of the above formula;
is independent of the choice of representative ,
which is seen from
whence indeed
is -equivariant,
which is seen by computing for as follows:
It is also immediate that the construction is natural in .
Now the -equivariance implies that for any choice of section of the coset quotient coprojection (in Sets) the range of is spanned by the combinations .
For this to vanish on all clearly all the must vanish separately, which shows that the kernel of is , hence that we have an injection.
At the same time, if has finite index in then both this range as well as the codomain have finite dimension, both equal to the number of -cosets of elements of . This means (by the rank-nullity theorem, if you wish) that in the case of finite index the injection is moreover surjective and hence an isomorphism, as claimed.
Hence:
(induction along finite-index inclusions is ambidextrous)
When the subgroup inclusion has finite index (in particular if is already a finite group) then the left (2) and right induced representation functors (5) are naturally isomorphic , constituting with an ambidextrous adjunction.
This statement is mentioned for instance in Hristova 2019 p 1.
The situation generalizes to representations of Hopf algebras, cf. Flake et al. 2024.
(Brauer induction theorem)
Over the complex numbers, the virtual representations of a finite group are all virtual combinations of induced representations of 1-dimensional representations.
if is the trivial representation of dimension 1 then its induced representation is the basic permutation representation spanned by the coset-space :
For more see at induced representation of the trivial representation.
(cf. tom Dieck 2009, Chapter 4)
Let
be a group homomorphism (often assumed to be a subgroup inclusion, and sometimes with assumed to be a finite group). For some -representation (often taken to be the trivial -representation), let be the induced -representation. Then the endomorphism ring of in is called the centralizer algebra or also the Hecke algebra or Iwahori-Hecke algebra? of the induced representation. (Basics are in Woit, def. 2, details are in Curtis & Reiner 1981, section 67, a quick survey of related theory is given by Srinivasan.
In terms of the notation in General abstract formulation above and for any homomorphism of -groups, we have the ∞-monoid
where is the internal hom in the slice (∞,1)-topos .
For any other representation, there is a canonical ∞-action of on . If here is the trivial representation then by adjointness this is the invariants of and hence the Hecke algebra acts on the invariants. (See for instance Woit, def. 2). This is sometimes called the Hecke algebra action on the Iwahori fixed vectors (e.g. here, p. 9)
Coinduction on Harish-Chandra modules is referred to as Zuckerman induction. See there for more details.
The identification of representation induction as the extra left adjoint in a base change morphism, as discussed in the General abstract discussion above, puts induced representations in the same general abstract framework as existential quantification in logic and generally of dependent sum in dependent type theory (see there for more details). This relation has first been amplified in (Lawvere).
If the modules over a group are considered as comodules over the function Hopf algebra over the group, then one can instead consider the induction for comodules. See cotensor product.
The derived functor of the representation induction functor is often referred to as cohomological induction.
The character of an induced representation is an induced character.
representation theory and equivariant cohomology in terms of (∞,1)-topos theory/homotopy type theory (FSS 12 I, exmp. 4.4):
Original articles:
George Mackey, Induced representations of locally compact groups I, Annals of Mathematics 55 1 (1952) 101-139 [doi:10.2307/1969423, jstor:1969423]
George Mackey: Induced representations of locally compact groups II, Annals of Mathematics 58 2 (1953) 193-221 [doi:10.2307/1969786, jstor:1969786]
George Mackey: Induced representations of groups and quantum mechanics, W. A. Benjamin, New York (1968) [ark:/13960/t6841m201]
(cf. Wigner classification)
Textbook accounts:
Jean-Pierre Serre, section 3.3 of: Linear Representations of Finite Groups, Graduate Texts in Mathematics 42, Springer (1977) [doi:10.1007/978-1-4684-9458-7, pdf]
Charles Curtis, Irving Reiner: Induced Representations, chapter VII in: Representation theory of finite groups and associative algebras, AMS (1962) [ISBN:978-0-8218-4066-5]
Charles Curtis, Irving Reiner: Methods of representation theory – With applications to finite groups and orders – Vol. I, Wiley (1981) [ark:/13960/t8gf4wd3x]
William Fulton, Joe Harris, section 3.3 of: Representation Theory: a First Course, Springer (1991) [doi:10.1007/978-1-4612-0979-9]
Pavel Etingof, Dmitry Vaintrob, et al., section 4.8 of: Introduction to representation theory, Student Mathematical Library 59, AMS (2011) [arXiv:0901.0827, ams:stml-59]
Benjamin Steinberg, section 8.2 of: Representation Theory of Finite Groups – An Introductory Approach, Springer (2012) [doi:10.1007/978-1-4614-0776-8]
Lecture notes:
See also:
Wikipedia: Induced representation
Wrong-way Frobenius reciprocity for finite groups representations [MO:q/132272]
Bhama Srinivasan; Modular Representations, Old and New, [pdf, pdf]
The general abstract formulation above is mentioned (for discrete groups and their permutation representations) in
William Lawvere: Adjointness in Foundations, Dialectica 23 (1969) 281-296, Reprints in Theory and Applications of Categories, 16 (2006) 1-16 [pdf]
William Lawvere: Equality in hyperdoctrines and comprehension schema as an adjoint functor, Proceedings of the AMS Symposium on Pure Mathematics XVII (1970) 1-14 [pdf]
Last revised on May 3, 2025 at 07:55:53. See the history of this page for a list of all contributions to it.