Unnormalized cubical chains with local coefficients #
Let L be a local coefficient system on a space X. The cubical n-chains of X with
coefficients in L are the direct sum, over the singular n-cubes c of X, of the fibre of
L at the origin c 0 of the cube. The boundary of a cube c carrying a coefficient a is the
alternating sum of its faces,
∂ (c, a) = Σᵢ (-1) ^ i ((face i 0 c, a) - (face i 1 c, τᵢ a)),
where τᵢ transports a from the origin of c to the origin of its face face i 1 c along the
image under c of a path in the cube. The cube is simply connected, so the path class it
transports along is determined by its endpoints (ContinuousMap.pathClass); this is what
makes the boundary square to zero, exactly as for constant coefficients. This is the cubical
version of the singular chains with local coefficients of
TauCeti.AlgebraicTopology.Singular.Twisted.Basic, and the complex on which Serre's spectral
sequence of a fibre space is built.
Chains are functorial in the coefficient system (coefficientMap) and in the space: a continuous
map f : X → Y sends the chains of X with coefficients in the pulled back system f⁎L to the
chains of Y with coefficients in L (map). In degree zero, a cocone s over L, for
instance the colimit of L or the module M of a constant system, gives an augmentation
C^□_0(X; L) → s.pt which vanishes on boundaries.
Main definitions #
TauCeti.LocalCoefficientSystem.TwistedCubicalChain L n: the cubicaln-chains with coefficients inL, withofCube L c, the inclusion of the summand of a cube.TauCeti.LocalCoefficientSystem.TwistedCubicalChain.boundary L n: the boundary.TauCeti.LocalCoefficientSystem.TwistedCubicalChain.coefficientMap η n,TauCeti.LocalCoefficientSystem.TwistedCubicalChain.map f L n: functoriality in the coefficient system and in the space.TauCeti.LocalCoefficientSystem.TwistedCubicalChain.augment s: the augmentation into a cocone.
Main results #
TauCeti.LocalCoefficientSystem.TwistedCubicalChain.boundary_boundary:∂ ∘ ∂ = 0.TauCeti.LocalCoefficientSystem.TwistedCubicalChain.map_boundary,TauCeti.LocalCoefficientSystem.TwistedCubicalChain.coefficientMap_boundary: the boundary is natural.TauCeti.LocalCoefficientSystem.TwistedCubicalChain.map_id,TauCeti.LocalCoefficientSystem.TwistedCubicalChain.map_comp,TauCeti.LocalCoefficientSystem.TwistedCubicalChain.coefficientMap_map: functoriality.TauCeti.LocalCoefficientSystem.TwistedCubicalChain.augment_boundary:ε ∘ ∂ = 0.
References #
- J.-P. Serre, Homologie singulière des espaces fibrés. Applications, Ann. of Math. 54 (1951), Chapter II.
- W. S. Massey, Singular Homology Theory, GTM 70, Springer, 1980, Chapters II and XIV.
- J.-F. Barraud, M. Damian, V. Humilière, A. Oancea, Floer homology with DG coefficients. Applications to cotangent bundles, arXiv:2404.07953, §7.2.
The cubical n-chains with coefficients in a local system L: the direct sum, over the
singular n-cubes c, of the fibre of L at the origin of c.
Instances For
The inclusion of the summand of a singular cube into the cubical chains.
Instances For
The inclusion of the summand of a singular cube is the direct-sum inclusion.
Equal cubes carrying corresponding coefficients, in the fibres of L at their equal origins,
are equal chains.
The linear map out of the cubical chains with prescribed values on each summand.
Instances For
The map with prescribed values on summands restricts to the prescribed map on each summand.
Two linear maps out of the cubical chains agree as soon as they agree on every summand.
Induction on cubical chains: a property of chains which holds for 0, for each cube with
a coefficient, and is stable under sums, holds for every chain.
The summand of the subcube c ∘ ι of a cube c, with the coefficient transported from the
origin of c to the origin of the subcube along the path class inside c.
Instances For
A subcube with a coefficient is the summand of the subcube with the transported coefficient.
The cube itself is the subcube along the identity.
A subcube of a subcube is a subcube.
The boundary of cubical chains with local coefficients.
Instances For
The boundary of a cube is the alternating sum of its faces, the subcubes
c ∘ face i t id, with the coefficient transported along the path classes inside the cube to the
origins of the faces.
The map of cubical chains induced by a morphism of local coefficient systems.
Instances For
A morphism of local systems acts on the summand of each cube by its component at the origin.
The identity of a local system induces the identity on cubical chains.
A composite of morphisms of local systems induces the composite map on cubical chains.
A morphism of local systems sends a subcube with a coefficient to the same subcube with the image coefficient.
The boundary commutes with the maps induced by a morphism of local systems.
The map of cubical chains induced by a continuous map f, from the chains with coefficients
in the pulled back system f⁎L to the chains with coefficients in L.
Instances For
A continuous map sends the summand of a cube identically onto the summand of the image cube.
A continuous map sends a subcube with a coefficient to the image subcube.
The identity map induces on cubical chains the map coming from the identification of a system with its pullback along the identity.
A composite of continuous maps induces on cubical chains the composite of the two induced maps, after the identification of the pullback along the composite with the iterated pullback.
The augmentation of the cubical 0-chains into a cocone s over the local system: a
point x with a coefficient a goes to the image of a under the leg of s at x. For the
colimit cocone it takes values in colimit L; for a constant system with fibre M and the cocone
of identities it is the sum of the coefficients.
Instances For
The augmentation sends a 0-cube, a point, with a coefficient to the image of the coefficient
under the leg of the cocone at that point.
The augmentation of a point of a subcube, a vertex of the cube, is the image of the coefficient at the origin of the cube.
The augmentation vanishes on boundaries: a path with a coefficient contributes the images of the coefficient at both of its end points, which agree in the cocone.
The augmentation is natural in the coefficient system.
The augmentation is natural in the space.