Dimension shifting in Tate cohomology #
For a finite group G, the connecting maps of the canonical sequences
0 ⟶ A ⟶ Coind_⊥^G A ⟶ dimensionShiftUp A ⟶ 0 and
0 ⟶ dimensionShiftDown A ⟶ Ind_⊥^G A ⟶ A ⟶ 0
are isomorphisms in every integer Tate degree. The same is true after restriction to any finite
subgroup of G, even when G itself is infinite. These subgroupwise shifts allow a vanishing
condition in consecutive degrees to be moved to other degrees simultaneously on all subgroups,
as required in Tate's cohomological triviality and cup-product criteria.
The two sequences stay short exact after tensoring on the left with any representation M, and
the middle terms M ⊗ Coind_⊥^G A and M ⊗ Ind_⊥^G A still have vanishing Tate cohomology, so
their connecting maps are isomorphisms as well (tensorDimensionShiftUpIso,
tensorDimensionShiftDownIso). These tensored shifts take the target degree as a parameter, so
that a construction proceeding by recursion on the degree, such as the cup product in all
bidegrees, needs no transport along equalities of degrees between its recursive steps; the cup
product transports its result once, at the end, to the requested target degree.
The composites of two consecutive upward shifts, on the group (dimensionShiftUpTwoIso, from
degree 0 to degree 2) and on a finite subgroup (dimensionShiftUpTwoResIso), present a
degree-two class as the double shift of a degree-zero class.
Each isomorphism below has Mathlib's connecting homomorphism TateCohomology.δ as its forward
map. Thus its naturality in a morphism of the short exact sequences is the existing theorem
TateCohomology.δ_naturality; no choices of abstract isomorphisms enter the construction.
The naturality statements here apply both to a shift and to its tensor with a fixed
representation, so they transport cup products along coefficient maps.
The unrestricted constructions adapt δUpIsoTate and δDownIsoTate from
ClassFieldTheory/Cohomology/Functors/UpDown.lean in kbuzzard/ClassFieldTheory, commit
ccc3323c6750abca25b49b35106f54eb3a398509. The restricted constructions use the vanishing of
restricted induced and coinduced representations proved in TateCohomology.Coinduced.
All four reuse Mathlib's CategoryTheory.ShortComplex.ShortExact.δIso.
References #
- J. S. Milne, Class Field Theory, Chapter II, §3 (dimension shifting and Theorem 3.10).
The upward dimension-shifting sequence identifies Tate cohomology of dimensionShiftUp A
in degree n with Tate cohomology of A in degree n + 1.
Equations
- TauCeti.TateCohomology.dimensionShiftUpIso A n = ⋯.δIso n (n + 1) ⋯ ⋯ ⋯
Instances For
The upward dimension shift is the connecting map of the coinduced short exact sequence.
The downward dimension-shifting sequence identifies Tate cohomology of A in degree n
with Tate cohomology of dimensionShiftDown A in degree n + 1.
Equations
- TauCeti.TateCohomology.dimensionShiftDownIso A n = ⋯.δIso n (n + 1) ⋯ ⋯ ⋯
Instances For
The downward dimension shift is the connecting map of the induced short exact sequence.
Two upward dimension shifts identify degree-zero Tate cohomology of the twice-shifted representation with degree-two Tate cohomology of the representation itself.
Equations
Instances For
The double shift is the composite of the two upward dimension shifts.
Upward dimension shifting commutes with a morphism of coefficient representations.
Upward dimension shifting commutes with a morphism of coefficient representations.
The inverse upward shift commutes with a coefficient morphism.
The inverse upward shift commutes with a coefficient morphism.
Downward dimension shifting commutes with a morphism of coefficient representations.
Downward dimension shifting commutes with a morphism of coefficient representations.
The inverse downward shift commutes with a coefficient morphism.
The inverse downward shift commutes with a coefficient morphism.
Vanishing in degree n of an upward shift is vanishing in degree n + 1 of the original
module.
Vanishing in degree n + 1 of a downward shift is vanishing in degree n of the original
module.
Tensoring the upward dimension-shifting sequence of A on the left with M identifies Tate
cohomology of M ⊗ dimensionShiftUp A in degree i with Tate cohomology of M ⊗ A in degree
j = i + 1.
Equations
- TauCeti.TateCohomology.tensorDimensionShiftUpIso A M i j hij = ⋯.δIso i j hij ⋯ ⋯
Instances For
The tensored upward dimension shift is the connecting map of the tensored coinduced short exact sequence.
Tensoring the downward dimension-shifting sequence of A on the left with M identifies Tate
cohomology of M ⊗ A in degree i with Tate cohomology of M ⊗ dimensionShiftDown A in degree
j = i + 1.
Equations
- TauCeti.TateCohomology.tensorDimensionShiftDownIso A M i j hij = ⋯.δIso i j hij ⋯ ⋯
Instances For
The tensored downward dimension shift is the connecting map of the tensored induced short exact sequence.
The tensored upward dimension shift is natural in its shifting representation.
The tensored upward dimension shift is natural in its shifting representation.
The inverse tensored upward shift is natural in its shifting representation.
The inverse tensored upward shift is natural in its shifting representation.
The tensored downward dimension shift is natural in its shifting representation.
The tensored downward dimension shift is natural in its shifting representation.
The inverse tensored downward shift is natural in its shifting representation.
The inverse tensored downward shift is natural in its shifting representation.
The tensored upward dimension shift is natural in the tensoring representation.
The tensored upward dimension shift is natural in the tensoring representation.
The inverse tensored upward shift is natural in the tensoring representation.
The inverse tensored upward shift is natural in the tensoring representation.
The tensored downward dimension shift is natural in the tensoring representation.
The tensored downward dimension shift is natural in the tensoring representation.
The inverse of the tensored downward dimension shift is natural in the tensoring representation.
The inverse of the tensored downward dimension shift is natural in the tensoring representation.
Upward dimension shifting after restriction to a finite subgroup. The shift is constructed
over G, so the same coefficient representation works for every finite subgroup.
Equations
- TauCeti.TateCohomology.dimensionShiftUpResIso A S n = ⋯.δIso n (n + 1) ⋯ ⋯ ⋯
Instances For
Restricted upward dimension shifting is the connecting map of the restricted sequence.
Downward dimension shifting after restriction to a finite subgroup. The shift is constructed
over G, so the same coefficient representation works for every finite subgroup.
Equations
- TauCeti.TateCohomology.dimensionShiftDownResIso A S n = ⋯.δIso n (n + 1) ⋯ ⋯ ⋯
Instances For
Restricted downward dimension shifting is the connecting map of the restricted sequence.
Two upward dimension shifts after restriction to a finite subgroup identify Tate cohomology
of the twice-shifted representation in degree n with Tate cohomology of the representation
itself in degree n + 1 + 1.
Equations
Instances For
The restricted double shift is the composite of the two restricted upward dimension shifts.
Vanishing in degree n of an upward shift is vanishing in degree n + 1 of the original
module, also on a finite subgroup.
Vanishing in degree n + 1 of a downward shift is vanishing in degree n of the original
module, also on a finite subgroup.