structures in a cohesive (∞,1)-topos
This is a subsection of the entry cohesive (∞,1)-topos. See there for background and context.
A cohesive (∞,1)-topos is a context of ∞-groupoids that are equipped with a geometric notion of cohesion on their collections of objects and k-morphisms, for instance topological cohesion or smooth cohesion.
While the axioms of cohesion do imply the intrinsic existence of exponentiated infinitesimal spaces, they do not admit access to an explicit synthetic notion of infinitesimal extension.
Here we consider one extra axiom on a cohesive (∞,1)-topos that does imply a good intrinsic notion of synthetic differential extension, compatible with the given notion of cohesion. We speak of infinitesimal cohesion .
In a cohesion -topos with infinitesimal cohesion there are for instance good intrinsic notions of formal smoothness and of de Rham spaces of objects.
We discuss extra structure on a cohesive (∞,1)-topos that encodes a refinement of the corresponding notion of cohesion to infinitesimal cohesion . More precisely, we consider inclusions of cohesive -toposes that exhibit the objects of as infinitesimal cohesive neighbourhoods of objects in .
Given a cohesive -topos we say that an infinitesimal cohesive neighbourhood of is another cohesive -topos equipped with an adjoint quadruple of adjoint (∞,1)-functors
where is
that preserves the terminal object.
This definition is an abstraction of similar situations considered in (SimpsonTeleman) and in Kontsevich-Rosenberg. See also the section Infinitesimal thickenings at Q-category.
This implies that also is a full and faithful (∞,1)-functor.
By the characterizaton of full and faithful adjoint (∞,1)-functors the condition on is equivalent to . Since it follows by essential uniqueness of adjoint (∞,1)-functors that also .
This definition captures the characterization of an infinitesimal object as having a single global point surrounded by an infinitesimal neighbourhood: as we shall see in more detail below, the (∞,1)-functor may be thought of as contracting away any infinitesimal extension of an object. Thus being an infinitesimal object amounts to , and the (∞,1)-adjunction then indeed guarantees that has only a single global point, since
The inclusion into the infinitesimal neighbourhood is necessarily a morphism of (∞,1)-toposes over ∞Grpd.
as is the induced geometric morphism
Moreover is necessarily a full and faithful (∞,1)-functor.
By essential uniqueness of th global section geometric morphism: In both cases the direct image functor has as left adjoint that preserves the terminal object. Therefore
Analogously in the second case.
We shall write
so that the global section geometric moprhism of factors as
Let for the remainder of this section an infinitesimal neighbourhood be fixed.
We give a presentation of classes of infinitesimal neighbourhoods by simplicial presheaves on suitable sites.
Let be an ∞-cohesive site. We say a site
equipped with a coreflective embedding
such that
is an infinitesimal neighbourhood site of .
Let be an ∞-cohesive site and an infinitesimal neighbourhood site.
Then the (∞,1)-category of (∞,1)-sheaves on is a cohesive -topos and the restriction along exhibits it as an infinitesimal neighbourhood of the cohesive -topos over .
Moreover, restricts on representables to the (∞,1)-Yoneda embedding factoring through :
We present the (∞,1)-sheaf (∞,1)-category by the projective model structure on simplicial presheaves left Bousfield localized at the covering sieve inclusions
(as discussed at models for (∞,1)-sheaf (∞,1)-toposes).
Consider the right Kan extension of simplicial presheaves along the functor . On an object it is given by the end-expression
where in the last step we use the Yoneda reduction-form of the Yoneda lemma.
This shows that the right adjoint to is itself given by precomposition with a functor, and hence has itself a further right adjoint, which gives us a total of four adjoint functors
From this are directly induced the corresponding simplicial Quillen adjunctions on the global projective and injective model structure on simplicial presheaves
Observe that , being a left Kan extension, sends representables to representables: we have
and by Yoneda reduction (more explicitly: observing that this is equivalently the formula for left Kan extension of the non-corepresentable along the identity functor) this is
By the discussion at simplicial Quillen adjunction for the above Quillen adjunctions to descend to the Cech-local model structure on simplicial presheaves it suffices that the right adjoints preserve locally fibrant objects.
We first check that sends locally fibrant objects to locally fibrant objects.
To that end, let be a covering family in . Write for its Cech nerve, where denotes the Yoneda embedding. Recall by the definition of the ∞-cohesive site that all the fiber products of representable presheaves here are again themselves representable, hence . This means that the left adjoint preserves not only the coend and tensoring, but by the remark in the previous paragraph and the assumption that preserves pullbacks along covers we have that
By the assumption that preserves covers, this is the Cech nerve of a covering family in . Therefore for fibrant we have for all coverings in that the descent morphism
is a weak equivalence, hence that is locally fibrant.
To see that preserves locally fibrant objects, we apply the analogous reasoning after observing that its left adjoint preserves all limits and colimits of simplicial presheaves (as these are computed objectwise) and by observing that for a covering family in we have that its image under is its image under , by the Yoneda lemma:
and using that preserves covers by assumption.
Therefore is a left and right local Quillen functor with left local Quillen adjoint and right local Quillen adjoint .
It follows that is given by the left derived functor of restriction along , and is given by the right derived functor of restriction along .
Finally to see that also preserves locally fibrant objects by the same reasoning as above, notice that for every covering family in and every morphism in we may find a covering of such that we find commuting diagrams on the left of
because by adjunction these correspond to commuting diagrams as indicated on the right, which exist by definition of coverage on and lift through by assumption on .
This implies that is a generalized cover in the terminology at model structure on simplicial presheaves, which by the discussion there implies that the corresponding Cech nerve equivalent to the sieve inclusion is a weak equivalence.
This establishes the quadruple of adjoint (∞,1)-functors as claimed.
It remains to see that is full and faithful.
For that notice the general fact that left Kan extension (see the propeties discussed there) along a full and faithful functor satisfies . It remains to observe that since is not only right but also left Quillen by the above, we have that applied to a cofibrant object is already the derived functor of the composite.
Conversely this implies that is an ∞-connected (∞,1)-topos over Smooth∞Grpd, exhibited by the triple of adjunctions
We discuss structures that are canonically present in a cohesive -topos equipped with infinitesimal cohesion. These structures parallel the structures in a general cohesive (∞,1)-topos.
In the presence of infinitesimal cohesion there is an infinitesimal analog of the geometric paths ∞-groupoids.
Define the adjoint triple of adjoint (∞,1)-functors corresponding to the adjoint quadruple :
For we say that
In traditional contexts see (SimpsonTeleman, p. 7) the object is called the de Rham space of or the de Rham stack of . Here we may tend to avoid this terminology, since by the discussion at cohesive (∞,1)-topos -- de Rham cohomology we have a good notion of intrinsic de Rham cohomology in any cohesive (∞,1)-topos already without equipping it with infinitesimal cohesion. From this point of view the object is not primarily characterized by the fact that (in some models, see below) it does co-represent de Rham cohomology – because the object from above does, too – but by the fact that it does so in an explicitly (synthetic) infinitesimal way.
There is a canonical natural transformation
that factors the finite path inclusion through the infinitesimal one
Notice that for any morphism in any (∞,1)-topos , there is the corresponding base change geometric morphism between the over-(∞,1)-toposes
For any object write
for the base change geometric morphism induced by the constant infinitesimal path inclusion , def. 3.
For we call as well as its pullback (depending on context) the jet bundle of .
We say an object is formally smooth if the constant infinitesimal path inclusion, , def. 3, is an effective epimorphism.
In this form this is the evident -categorical analog of the conditions as they appear for instance in (SimpsonTeleman, page 7).
An object is formally smooth according to def. 5 precisely if the canonical morphism
(induced from the adjoint quadruple , see there) is an effective epimorphism.
The canonical morphism is the composite
By the condition that is a full and faithful (∞,1)-functor the second morphism here in an equivalence, as indicated, and hence the component of the composite on being an effective epimorphism is equivalent to the component being an effective epimorphism.
In this form this characterization of formal smoothness is the evident generalization of the condition given in (Kontsevich-Rosenberg, section 4.1). See the section Formal smoothness at Q-category for more discussion. Notice that by this remark the notation there is related to the one used here by , and .
Therefore we have the following more general definition.
For a morphism in , we say that
is a formally smooth morphism if the canonical morphism
is an effective epimorphism.
is a formally unramified morphism if this is a (-1)-truncated morphism. More generally, is an order- formally unramified morphisms for if this is a k-truncated morphism.
is a formally étale morphism if this morphism is an equivalence, hence if
is an (∞,1)-pullback square.
An order-(-2) formally unramified morphism is equivalently a formally étale morphism.
Only for 0-truncated does formal smoothness together with formal unramifiedness imply formal étaleness.
The collection of formally étale morphisms in , def. 6, is closed under the following operations.
Every equivalence is formally étale.
The composite of two formally étale morphisms is itself formally étale.
If
is a diagram such that and are formally étale, then also is formally étale.
Any retract of a formally étale morphisms is itself formally étale.
The (∞,1)-pullback of a formally étale morphisms is formally étale if the pullback is preserved by .
The statements about closure under composition and pullback appears as(KontsevichRosenberg, prop. 5.4, prop. 5.6). Notice that the extra assumption that preserves the pullback is implicit in their setup, by remark 2.
The first statement follows since -pullbacks are well defined up to quivalence.
The second two statements follow by the pasting law for (∞,1)-pullbacks: let and be two morphisms and consider the pasting diagram
If and are formally étale then both small squares are pullback squares. Then the pasting law says that so is the outer rectangle and hence is formally étale. Similarly, if and are formally étale then the right square and the total reactangle are pullbacks, so the pasting law says that also the left square is a pullback and so also is formally étale.
For the fourth claim, let be a retract in the arrow (∞,1)-category . By applying the natural transformation we obtain a retract
in the category of squares . We claim that generally, if the middle piece in a retract in is an (∞,1)-pullback square, then so is its retract sqare. This implies the fourth claim.
To see this, we use that
(∞,1)-limits are computed by homotopy limits in any presentable (∞,1)-category presenting ;
homotopy limits in may be computed by the left and right adjoints provided by the derivator associated to .
From this the claim follows as described in detail at retract in the section retracts of diagrams .
For the last claim, consider an (∞,1)-pullback diagram
where is formally étale.
Applying the natural transformation to this yields a square of squares. Two sides of this are the pasting composite
and the other two sides are the pasting composite
Counting left to right and top to bottom, we have that
the first square is a pullback by assumption that preserves the given pullback;
the second square is a pullback, since is formally étale.
the total top rectangle is therefore a pullback, by the pasting law;
the fourth square is a pullback since is right adjoint and so also preserves pullbacks;
also the total bottom rectangle is a pullback, since it is equal to the top total rectangle;
therefore finally the third square is a pullback, by the other clause of the pasting law. Hence is formally étale.
The properties listed in prop. 5 correspond to the axioms on the open maps (“admissible maps”) in a geometry (for structured (∞,1)-toposes) (Lurie, def. 1.2.1). This means that a notion of formally étale morphisms induces a notion of locally algebra-ed (∞,1)toposes/structured (∞,1)-toposes in a cohesive context. This is discuss in
In order to interpret the notion of formal smoothness, we turn now to the discussion of infinitesimal reduction.
By definition of infinitesimal neighbourhood we have that is a full and faithful (∞,1)-functor. It follows that and hence
For every , we have that is formally smooth according to def. 5.
By prop. 6 we have that
is an equivalence. As such it is in particular an effective epimorphism.
An ordinary topological/Lie étale groupoid is one whose source/target map is an étale map. We consider now a notion that can be formulated in the presence of infinitesimal cohesion which generalizes this.
Let be an infinitesimal cohesive neighbourhood.
An object is called a cohesive étale -groupoid if there exists an atlas – an effective epimorphism out of a 0-truncated object – which is also a formally étale morphism def. 6.
We discuss the intrinsic flat cohomology in an infinitesimal neighbourhood.
For we say that
(where is given by def. 3) is the infinitesimal flat cohomology of with coefficient in .
In traditional contexts this is also called crystalline cohomology or just de Rham cohomology . Since we already have an intrinsic notion of de Rham cohomology in any cohesive (∞,1)-topos, which is similar to but may slightly differ from infinitesimal flat differential cohomology, we shall say synthetic de Rham cohomology for the notion of def. 8 if we wish to honor traditional terminology. In this case we shall write
By the above observation we have canonical morphisms
The objects on the left are principal ∞-bundles equipped with flat ∞-connection . The first morphism forgets their higher parallel transport along finite volumes and just remembers the parallel transport along infinitesimal volumes. The last morphism finally forgets also this connection information.
For an abelian ∞-group object we say that the de Rham theorem for -coefficients holds in if for all the infinitesimal path inclusion
is an equivalence in -cohomology, hence if for all we have that
is an isomorphism.
If we follow the notation of note 5 and moreover write for the intrinsic geometric realization, then this becomes
where on the right we have ordinary cohomology in Top (for instance realized as singular cohomology) with coefficients in the discrete group underlying the cohesive group .
In certain contexts of infinitesimal neighbourhoods of cohesive -toposes the de Rham theorem in this form has been considered in (SimpsonTeleman).
The genuine infinitesimal analog of exponentiated ∞-Lie algebras are formal cohesive ∞-groupoids.
An object is an infinitesimal cohesive -groupoid if .
An ∞-group object that is infinitesimal we call an formal ∞-group .
For any object, we say is a formal cohesive ∞-groupoid over if ; equivalently: if there is a morphism
that serves as the -unit on , hence as the infinitesimal path inclusion for .
An infinitesimal cohesive -groupoid is both geometrically contractible and has as underlying discrete -groupoid the point:
.
The first statement is implied by the fact that both as well as are full and faithful. This means that if then already . Since and preserves the terminal object by cohesiveness, this implies the first claim.
The second statement follows by
For all , we have that and are formal cohesive ∞-groupoids over , the first by the constant infinitesmal path inclusion, the second by the identity.
For this is tautological, for it follows from the idempotency of Red and the -zig-zag identity.
The delooping of an formal cohesive ∞-group is an formal cohesive ∞-groupoid over the point.
Since both and are right adjoint, the infinitesimal path ∞-groupoid functor commutes with delooping. Therefore
An infinitesimal cohesive ∞-groupoid is both geometrically contractible and has as underlying discrete ∞-groupoid the point:
.
This follows with using the above observation from the full and faithfulness of and .
The former implies that with already . Since and since preserves the point by cohesiveness, this implies the first claim.
For the latter we compute
(…)
For any (∞,1)-site the construction of the tangent (∞,1)-category provides a canonical infinitesimal thickening of :
where the -functor pair on the right forms a -relative (∞,1)-adjunction. The composite is the cotangent complex functor for and is fiberwise the canonical map out of the stabilization.
The image of is contained in that of . Therefore we may restrict the -adjunction on the right to the full sub-(∞,1)-category of on thise objects in the image of . This yields an infinitesimal neighbourhood of (∞,1)-sites
(…)
(…)
The category-theoretic definition of cohesive topos was proposed by Bill Lawvere. See the references at cohesive topos.
The observation that the further left adjoint in a locally ∞-connected (∞,1)-topos defines an intrinsic notion of paths and geometric homotopy groups in an (∞,1)-topos was suggested by Richard Williamson.
The observation that the further right adjoint in a local (∞,1)-topos serves to characterize concrete (∞,1)-sheaves was amplified by David Carchedi.
Several aspects of the discussion here are, more or less explicitly, in
For instance something analogous to the notion of ∞-connected site and the fundamental ∞-groupoid in a locally ∞-connected (∞,1)-topos is the content of section 2.16. The infinitesimal path ∞-groupoid adjunction is essentially discussed in section 3.
The characterization of infinitesimal extensions and formal smoothness by adjoint functors is considered in
in the context of Q-categories .
Some of the material discussed here is in section 2.4 of
A commented list of related references is at