Inertia groups of codimension-one primes of a symmetric algebra #
Let ρ be a representation of a group G on a module M, acting on the symmetric algebra
Sym M by Representation.symmetricAlgebraMulSemiringAction. The inertia group P.inertia G of
an ideal P of Sym M is the subgroup of elements acting trivially modulo P (Mathlib's
Ideal.inertia). Since Sym M is generated by M, an element lies in it exactly when it moves
every vector by an element of P. For the prime ideal spanned by a degree-one element ι ℓ, this
says that g moves every vector by a multiple of ℓ.
Over a field K, these are the only height-one primes whose inertia group acts nontrivially on
M: if g acts nontrivially and lies in the inertia group of a height-one prime P, then P
contains the nonzero degree-one element ι (ρ g m - m) for some m, which is prime, so P is
spanned by it. Conversely, for finite-dimensional M each nonzero ι ℓ spans a prime of height
one (SymmetricAlgebra.height_span_singleton_ι). If moreover G is finite of order invertible in
K and ρ is faithful, the inertia group of ι ℓ acts on the line K ∙ ℓ through an injective
character, so it is cyclic.
For polynomial functions on a vector space V, take M = V* with the contragredient action
ρ.dual. A nonzero linear form ℓ spans the ideal of the hyperplane ker ℓ, and the inertia
group of that ideal is the pointwise stabilizer of ker ℓ. Thus a height-one prime of Sym(V*)
whose inertia group acts nontrivially on V is the ideal of a hyperplane ker ℓ, its inertia
group is the pointwise stabilizer of ker ℓ, and each element of it acting nontrivially on V is
a pseudoreflection whose fixed hyperplane is exactly ker ℓ. If moreover G is finite of order
invertible in K and acts faithfully, these inertia groups are cyclic.
Consequently the inertia group of every height-one prime of Sym(V*) lies in the subgroup
generated by the pseudoreflections together with the kernel of ρ. When ρ is faithful it lies
in the subgroup H generated by the pseudoreflections alone
(Representation.pseudoreflectionSubgroup, in TauCeti.RepresentationTheory.Pseudoreflection).
Let G be finite and V finite-dimensional, and let ρ be faithful. The normal subgroup H
gives the factorization V → V/H → V/G of the quotient map, and G ⧸ H acts on the invariants
Sym(V*)^H with invariants Sym(V*)^G. Every height-one prime P of Sym(V*)^H lies under a
height-one prime Q of Sym(V*), since Sym(V*) is integral over the finitely generated algebra
Sym(V*)^H and contraction preserves heights. The inertia group of P in G ⧸ H is the image of
the inertia group of Q in G (Ideal.inertia_quotient_eq_bot_iff), so it is trivial. Thus the
residual quotient V/H → V/G has trivial inertia at every codimension-one point.
Main results #
Representation.symmetricAlgebra_mem_inertia_iff:glies in the inertia group ofPexactly whenι (ρ g m - m) ∈ Pfor everym.Representation.symmetricAlgebra_mem_inertia_span_singleton_ι_iff: the inertia group ofι ℓconsists of the elements moving every vector by a multiple ofℓ.Representation.exists_eq_span_singleton_ι_of_mem_inertia: a height-one prime whose inertia group acts nontrivially is spanned by a nonzero degree-one element.Representation.isCyclic_inertia_span_singleton_ιandRepresentation.isCyclic_inertia_of_height_eq_one: for a faithful representation of a finite group of order invertible inK, these inertia groups are cyclic.Representation.mem_dual_inertia_span_singleton_ι_iff_le_fixedSubmodule: for polynomial functions onV, the inertia group of the ideal ofker ℓis its pointwise stabilizer.Representation.exists_eq_span_singleton_ι_and_ker_eq_of_mem_inertia: an element of the inertia group of a height-one prime ofSym(V*)acting nontrivially onVis a pseudoreflection, whose fixed hyperplane cuts out that prime.Representation.inertia_le_pseudoreflectionSubgroup_sup_kerandRepresentation.inertia_le_pseudoreflectionSubgroup: the inertia group of a height-one prime ofSym(V*)lies in the pseudoreflection subgroup, together with the kernel ofρin general.Representation.inertia_quotient_pseudoreflectionSubgroup_eq_bot: for a faithful representation of a finite group,G ⧸ Hhas trivial inertia at every height-one prime ofSym(V*)^H.
References #
- R. Kane, Reflection Groups and Invariant Theory, CMS Books in Mathematics, Springer (2001), § 18.
- L. Smith, Polynomial Invariants of Finite Groups, A K Peters (1995), § 7.4.
An element g lies in the inertia group of an ideal P of Sym M for the induced action
exactly when it moves every degree-one element by an element of P.
An element g lies in the inertia group of the ideal spanned by a degree-one element ι ℓ
exactly when it moves every vector by a multiple of ℓ.
If an element g acting nontrivially on M lies in the inertia group of a height-one prime
P of Sym M, then P is spanned by a nonzero degree-one element.
For a faithful representation of a finite group whose order is invertible in K, the
inertia group of the ideal spanned by a nonzero degree-one element ι ℓ is cyclic: it acts on the
line K ∙ ℓ through an injective character.
For a faithful representation of a finite group whose order is invertible in K, the inertia
group of every height-one prime of Sym M is cyclic.
For polynomial functions on V, the inertia group of the ideal spanned by a linear form ℓ
is the pointwise stabilizer of the hyperplane ker ℓ.
Let P be a height-one prime of the polynomial functions Sym(V*) on V, and let g lie in
its inertia group and act nontrivially on V. Then P is spanned by a nonzero linear form ℓ,
and g is a pseudoreflection fixing exactly the hyperplane ker ℓ.
The inertia group of a height-one prime of the polynomial functions Sym(V*) lies in the
subgroup generated by the pseudoreflections of ρ and the kernel of ρ: each of its elements
either acts trivially on V or is a pseudoreflection.
For a faithful representation, the inertia group of a height-one prime of the polynomial
functions Sym(V*) lies in the subgroup generated by the pseudoreflections.
The residual quotient has trivial inertia in codimension one. Let ρ be a faithful
representation of a finite group G on a finite-dimensional space V, and let H be its
pseudoreflection subgroup. Then G ⧸ H acts on the polynomial invariants Sym(V*)^H, and the
inertia group of every height-one prime of Sym(V*)^H for this action is trivial. Geometrically,
the residual quotient V/H → V/G by G ⧸ H has trivial inertia at every codimension-one point.