nLab
cosmic cube

Context

Higher category theory

higher category theory

Basic concepts

Basic theorems

Applications

Models

Morphisms

Functors

Universal constructions

Extra properties and structure

1-categorical presentations

Contents

Idea

The Cosmic Cube of higher category theory is the name for a diagram whose vertices correspond to special types of n-categories. The cube looks like this:

We may take n= here as well, and we may also consider a version for (n,r)-categories. The three axes correspond to:

  • making n-categories ‘groupoidal’ — that is, making morphisms invertible, thus passing from general n-categories to n-groupoids;

  • making n-categories strict, thus passing from general n-categories to strict n-categories;

  • making n-categories symmetric monoidal or ‘stable’, thus passing from general n-categories to symmetric monoidal n-categories.

In terms of homotopy theory

Each vertex of the cube can also be understood as corresponding to a version of homotopy theory:

-groupoids yield ordinary homotopy theory, symmetric monoidal and groupal -groupoids correspond to stable homotopy theory, strictly abelian strict -groupoids correspond to homological algebra. -Categories that are not -groupoids correspond to directed homotopy theory.

Vertices of the cube

Here we list the 8 vertices of the cube in the case of -categories.

Strict -categories

Strict -groupoids

Stably monoidal -categories

Stably monoidal -groupoids

Strictly stably monoidal strict -groupoids

Etc.

(…)

Edges of the cube

Strict -groupoids in all -groupoids

A strict ∞-groupoid is modeled by a crossed complex. Under ω-nerve it embeds into all ∞-groupoids, modeled as Kan complexes.

CrsCplx N Δ KanCplx StrGrpd Grpd.\array{ CrsCplx &\stackrel{N^\Delta}{\hookrightarrow}& KanCplx \\ \downarrow && \downarrow \\ Str \infty Grpd &\hookrightarrow& \infty Grpd } \,.

Strictly stable strict -groupoids in strict -groupoids

A strictly stable strict ∞-groupoid is modeled by a bounded-below chain complex of abelian groups. Under the embedding Θ of complexes into crossed complexes it embeds into strict ∞-groupoids.

ChnCplx Θ CrsCplx StrAbStrGrpd StrGrpd.\array{ ChnCplx &\stackrel{\Theta}{\hookrightarrow}& CrsCplx \\ \downarrow && \downarrow \\ StrAb Str \infty Grpd &\hookrightarrow& Str \infty Grpd } \,.

For the definition of Θ see Nonabelian Algebraic Topology , section Crossed complexes from chain complexes.

Strictly stable strict -groupoids in all -groupoids

Combining the above inclusions

ChainCplx Θ CrossedCplx N Δ KanCplx StrAbStrGrpd StrGrpd Grpd\array{ ChainCplx &\stackrel{\Theta}{\hookrightarrow}& CrossedCplx &\stackrel{N^\Delta}{\hookrightarrow}& KanCplx \\ \downarrow^{\mathrlap{\simeq}} && \downarrow^{\mathrlap{\simeq}} && \downarrow^{\mathrlap{\simeq}} \\ StrAb Str\infty Grpd &\hookrightarrow& Str \infty Grpd &\hookrightarrow& \infty Grpd }

yields in total the map ChnCplxsAb from chain complexes to simplicial abelian groups (followed by the forgetful sAbKanCpx) of the Dold-Kan correspondence.

Strictly stable strict -groupoids in strictly stable -groupoids

A strictly stable strict ∞-groupoid is modeled by a bounded-below chain complex of abelian groups. Under ω-nerve it embeds into all (connective) spectras, modeled as spectrum objects in Kan complexes.

ChnCplx + Σ N ΔΘ Sp(KanCplx) StrAbStrGrpd Sp(Grpd).\array{ ChnCplx^+ &\stackrel{\Sigma^\infty \N^\Delta \Theta}{\hookrightarrow}& Sp(KanCplx) \\ \downarrow && \downarrow \\ StrAb Str \infty Grpd &\hookrightarrow& Sp(\infty Grpd) } \,.

Strictly stable -groupoids in all -groupoids

A strictly stable ∞-groupoid is modeled by a connective spectrum. The forgetful functor to ∞-groupoids is also called Ω or the “zeroth-space functor.”

References

Revised on October 6, 2010 22:55:34 by Urs Schreiber (87.212.203.135)