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higher Klein geometry

Context

Geometry

Differential geometry

Contents

Idea

Higher Klein geometry is the generalization of Klein geometry from traditional (differential) geometry to higher geometry:

where Klein geometry is about (Lie) groups and their quotients, higher Klein geometry is about (smooth) ∞-groups and their ∞-quotients.

The way that the generalization proceeds is clear after the following observation.

Observation

Let G be a discrete group and HG a subgroup. Write BG and BH for the corresponding delooping groupoids with a single object. Then the action groupoid G//H is the homotopy fiber of the inclusion functor

BHBG\mathbf{B}H \to \mathbf{B}G

in the (2,1)-category Grpd: we have a fiber sequence

G//HBHBGG//H \to \mathbf{B}H \to \mathbf{B}G

that exhibits G//H as the G-principal bundle over BH which is classified by the cocycle BHBG.

Moreover, the decategorification of the action groupoid (its 0-truncation) is the ordinary quotient

τ 0(G//H)=G/H.\tau_0 (G//H) = G/H \,.
Proof

This should all be explained in detail at action groupoid.

The fact that a quotient is given by a homotopy fiber is a special case of the general theorem discussed at ∞-colimits with values in ∞Grpd

Remark

That fiber sequence continues to the left as

HGG//HBHBG.H \to G \to G//H \to \mathbf{B}H \to \mathbf{B}G \,.
Observation

The above statement remains true verbatim if discrete groups are generalized to Lie groups – or other cohesive groups – if only we pass from the (2,1)-topos Grpd of discrete groupoids to the (2,1)-topos SmoothGrpd of smooth groupoids .

This follows with the discussion at smooth ∞-groupoid -- structures.

Since the quotient G/H is what is called a Klein geometry and since by the above observations we have analogs of these quotients for higher cohesive groups, there is then an evident definition of higher Klein geometry :

Definition

Let H be a choice of cohesive structure. For instance choose

Definition

An -Klein geometry in H is a fiber sequence in H

G//HBHiBGG//H \to \mathbf{B}H \stackrel{i}{\to} \mathbf{B}G

for i any morphism between two connected objects, as indicated, hence Ωi:HG any morphism of ∞-group objects.

Remark

For X an object equipped with a G-action and f:YX any morphism, the higher Klein geometry induced by “the shape Y in X” is given by taking i:HG be the stabilizer ∞-group Stab(f)G of f in X.

Remarks

Examples

Higher super Poincaré Klein geometry

Let H= SuperSmooth∞Grpd be the context for synthetic higher supergeometry.

Write 𝔰𝔲𝔤𝔯𝔞 11 for the super L-∞ algebra called the supergravity Lie 6-algebra. This has a sub-super L -algebra of the form

B(𝔰𝔬(10,1)bb 5)B𝔰𝔲𝔤𝔯𝔞 11,\mathbf{B}(\mathfrak{so}(10,1) \oplus b \mathbb{R} \oplus b^{5}\mathbb{R}) \hookrightarrow \mathbf{B}\mathfrak{sugra}_11 \,,

where

The quotient

𝔰𝔲𝔤𝔯𝔞 11/((𝔰𝔬(10,1)bb 5))\mathfrak{sugra}_11 / ((\mathfrak{so}(10,1) \oplus b \mathbb{R} \oplus b^{5}\mathbb{R}))

is the super translation Lie algebra in 11-dimensions.

This higher Klein geometry is the local model for the higher Cartan geometry that describes 11-dimensional supergravity. See D'Auria-Fre formulation of supergravity for more on this.

local modelglobal geometry
Klein geometryCartan geometry
Klein 2-geometryCartan 2-geometry
higher Klein geometryhigher Cartan geometry

Revised on January 16, 2012 20:09:53 by David Corfield (86.152.177.169)