nLab bivariant cohomology theory

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Where a homology theory is a covariant functor and a cohomology theory is a contravariant functor on some category of spaces, a bivariant cohomology theory is a bifunctor, hence a functor of two variables, contravariant in the first, and covariant in the second.

Examples:

Axiomatization in homotopy theory

Here are some notes on a proposal for how to usefully formalize bivariant cohomology theory in stable homotopy theory. (This is in generalization of the structure of KK-theory, while the original axioms of (Fulton-MacPherson 81) are a little different1. Aspects of the following appear in (Nuiten 13, Schreiber 14). See also at dependent linear type theory the section on secondary integral transforms).

\,

Let EE be an E-∞ ring, write GL 1(E)GL_1(E) for its ∞-group of units. With H\mathbf{H} the ambient (∞,1)-topos, write H /BGL 1(E)\mathbf{H}_{/\mathbf{B}GL_1(E)} for the slice (∞,1)-topos over the delooping of this abelian ∞-group. This is the (∞,1)-category of spaces equipped with (∞,1)-line bundles over EE. Consider an (∞,1)-functor

Γ *:H /BGL 1(E)→EMod \Gamma^\ast \;\colon \; \mathbf{H}_{/\mathbf{B}GL_1(E)} \to E Mod

to the (∞,1)-category of (∞,1)-modules over EE, which form EE-modules of co-sections of EE-(∞,1)-module bundles (generalized Thom spectra).

This is well understood for H=\mathbf{H} = ∞Grpd in which case Γ≃lim→∘i\Gamma \simeq \underset{\to}{\lim} \circ i is the (∞,1)-functor homotopy colimits in EModE Mod under the canonical embedding BGL 1(E)≃ELine↪EMod\mathbf{B} GL_1(E) \simeq E Line \hookrightarrow E Mod. But one can consider similar constructions Γ\Gamma for more general ambient (∞,1)-toposes H\mathbf{H}.

Definition

For χ i:X i→BGL 1(E)\chi_i \colon X_i \to \mathbf{B}GL_1(E) two objects of H /BGL 1(E)\mathbf{H}_{/\mathbf{B}GL_1(E)}, the (χ 1,χ 2)(\chi_1,\chi_2)-twisted bivariant EE-cohomology on (X 1,X 2)(X_1,X_2) is

E •+χ 2−χ 1(X 1,X 2)≔Hom EMod(Γ X 1 *(χ 1),Γ X 2 *(χ 2))∈EMod. E^{\bullet + \chi_2 - \chi_1}(X_1,X_2) \;\coloneqq\; Hom_{E Mod}\left(\Gamma^\ast_{X_1}\left(\chi_1\right), \Gamma^\ast_{X_2}\left(\chi_2\right)\right) \in E Mod \,.
Example

By the general discussion at twisted cohomology, following (ABG, def. 5.1) we have

  • for X 2=*X_2 = \ast the point, the above bivariant cohomology is the χ 1\chi_1-twisted EE-cohomology of X 1X_1;

    E •+χ 1(X 1,*)≃E •+χ 1(X 1). E^{\bullet + \chi_1}(X_1, \ast) \simeq E^{\bullet + \chi_1}(X_1) \,.
  • for X 1=*X_1 = \ast the point, the above bivariant cohomology is the χ 2\chi_2-twisted EE-homology of X 2X_2;

    E •+χ 2(*,X 2)≃E •+χ 2(X 2). E^{\bullet + \chi_2}(\ast, X_2) \simeq E_{\bullet + \chi_2}(X_2) \,.
Example

KK-theory is a model for bivariant twisted topological K-theory over differentiable stacks (hence 1-truncated suitably representable objects in H=\mathbf{H} = Smooth∞Grpd, see Tu-Xu-LG 03). According to (Joachim-Stolz 09, around p. 4) the category KKKK first of all is naturally an enriched category 𝕂𝕂\mathbb{KK} over the category 𝒮\mathcal{S} of symmetric spectra and as such comes with a symmetric monoidal enriched functor

𝕂𝕂→KUMod. \mathbb{KK} \to KU Mod \,.

This sends an object to its operator K-theory spectrum, hence to the EE-dual of the EE-module of co-sections.

Remark

Generally, one may want to consider in def. the dualized co-section functor

Γ=[Γ *(−),E]:(H /BGL 1(E)) op→EMod. \Gamma = [\Gamma^\ast(-), E] \;\colon\; \left(\mathbf{H}_{/\mathbf{B}GL_1(E)}\right)^{op} \to E Mod \,.
Example

A correspondence in H /BGL 1(E)\mathbf{H}_{/\mathbf{B}GL_1(E)}

Q i 1↙ ↘ i 2 X 1 ⇙ ξ X 2 χ 1↘ ↙ χ 2 BGL 1(E) \array{ && Q \\ & {}^{\mathllap{i_1}}\swarrow && \searrow^{\mathrlap{i_2}} \\ X_1 && \swArrow_{\xi} && X_2 \\ & {}_{\mathllap{\chi_1}}\searrow && \swarrow_{\mathrlap{\chi_2}} \\ && \mathbf{B}GL_1(E) }

is a morphism of “twisted EE-motives” in that it is a correspondence in H\mathbf{H} between the spaces X 1X_1 and X 2X_2 equipped with an (i 1 *χ 1,i 2 *χ 2)(i_1^\ast \chi_1, i_2^\ast \chi_2)-twisted bivariant EE-cohomology cocycle ξ\xi on the correspondence space QQ. Under the co-sections / Thom spectrum functor this is sent to a correspondence

Γ X 1(χ 1)→ξΓ Q(i 2 *χ 2)←i 2 *Γ X 2(χ 2) \Gamma_{X_1}(\chi_1) \stackrel{\xi}{\rightarrow} \Gamma_Q(i_2^\ast \chi_2) \stackrel{i_2^\ast}{\leftarrow} \Gamma_{X_2}(\chi_2)

in EModE Mod. If the wrong-way map of this is orientable in EE-cohomology then we may form its dual morphism/Umkehr map to obtain the corresponding “index”

Γ X 1(χ 1)→(i 2) !ξΓ X 2(χ 2) \Gamma_{X_1}(\chi_1) \stackrel{(i_2)_! \xi}{\to} \Gamma_{X_2}(\chi_2)

in EModE Mod. Identifying correspondences that yield the same “index” this way yields a presentation of bivariant cohomology by motive-like structures. This is how (equivariant) bivariant K-theory is presented, at least over manifolds, see at KK-theory – References – In terms of correspondences.

References

A general introduction to bivariant cohomology theories is in

A general construction of bivariant theories on smooth manifolds from cohomology theories by geometric cycles, generalizing the construction of K-homology by Baum-Douglas geometric cycles, is in

  • Martin Jakob, Bivariant theories for smooth manifolds, Applied Categorical Structures 10 no. 3 (2002)

A similar construction for PL manifolds is in

  • S. Buoncristiano, C. P. Rourke and B. J. Sanderson, A geometric approach to homology theory, Cambridge Univ. Press, Cambridge, Mass. (1976)

A study of bivariant theories in the context of motivic stable homotopy theory, and more generally in the broader framework of Grothendieck six functors formalism is in

  • F. Déglise, Bivariant theories in motivic stable homotopy, (arXiv:1705.01528)

References related to the discussion in Axiomatization in homotopy theory above include the following


  1. Thanks to Thomas Nikolaus for patiently emphasizing this. ↩

Last revised on April 11, 2018 at 02:16:42. See the history of this page for a list of all contributions to it.