nLab
cohesive (infinity,1)-topos -- infinitesimal cohesion

Context

Cohesive -Toposes

cohesive topos

cohesive (∞,1)-topos

cohesive homotopy type theory

Backround

Definition

Presentation over a site

Structures in a cohesive (,1)-topos

structures in a cohesive (∞,1)-topos

Structures with infinitesimal cohesion

infinitesimal cohesion

Models

This is a subsection of the entry cohesive (∞,1)-topos. See there for background and context.


Contents

Idea

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 (,1)-topos with infinitesimal cohesion there are for instance good intrinsic notions of formal smoothness and of de Rham spaces of objects.

Infinitesimal cohesion

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 HH th of cohesive (,1)-toposes that exhibit the objects of H th as infinitesimal cohesive neighbourhoods of objects in H.

Definition

Definition

Given a cohesive (,1)-topos H we say that an infinitesimal cohesive neighbourhood of H is another cohesive (,1)-topos H th equipped with an adjoint quadruple of adjoint (∞,1)-functors

(i !i *i *i !):Hi !i *i *i !H th(i_! \dashv i^* \dashv i_* \dashv i^!) : \mathbf{H} \stackrel{\overset{i_!}{\hookrightarrow}}{\stackrel{\overset{i^*}{\leftarrow}}{\stackrel{\overset{i_*}{\hookrightarrow}}{\underset{i^!}{\leftarrow}}}} \mathbf{H}_{th}

where i ! is

This definition is an abstraction of similar situations considered in (SimpsonTeleman) and in Kontsevich-Rosenberg. See also the section Infinitesimal thickenings at Q-category.

Observation

This implies that also i * is a full and faithful (∞,1)-functor.

Proof

By the characterizaton of full and faithful adjoint (∞,1)-functors the condition on i ! is equivalent to i *i !Id. Since (i *i !i *i *) it follows by essential uniqueness of adjoint (∞,1)-functors that also i *i *Id.

Note

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 i * may be thought of as contracting away any infinitesimal extension of an object. Thus X being an infinitesimal object amounts to i *X*, and the (∞,1)-adjunction (i !i *) then indeed guarantees that X has only a single global point, since

H th(*,X) H th(i !*,X) H(*,i *X) H(*,*) *.\begin{aligned} \mathbf{H}_{th}(*, X) & \simeq \mathbf{H}_{th}(i_! *, X) \\ & \simeq \mathbf{H}(*, i^* X) \\ & \simeq \mathbf{H}(*, *) \\ & \simeq * \end{aligned} \,.
Proposition

The inclusion into the infinitesimal neighbourhood is necessarily a morphism of (∞,1)-toposes over ∞Grpd.

H (i *i *) H th Γ Γ Grpd\array{ \mathbf{H} && \stackrel{(i^* \dashv i_*)}{\to} && \mathbf{H}_{th} \\ & {}_{\mathllap{\Gamma}}\searrow && \swarrow_{\mathrlap{\Gamma}} \\ && \infty Grpd }

as is the induced geometric morphism (i *i !):H thH

H th (i *i !) H Γ Γ Grpd.\array{ \mathbf{H}_{th} && \stackrel{(i_* \dashv i^!)}{\to} && \mathbf{H} \\ & {}_{\mathllap{\Gamma}}\searrow && \swarrow_{\mathrlap{\Gamma}} \\ && \infty Grpd } \,.

Moreover i * is necessarily a full and faithful (∞,1)-functor.

Proof

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

Γ H th(i *X) H th(*,i *X) H(i **,X) H(*,X) Γ H(X).\begin{aligned} \Gamma_{\mathbf{H}_{th}}( i_* X ) & \simeq \mathbf{H}_{th}(*, i_* X) \\ & \simeq \mathbf{H}(i^* *, X) \\ & \simeq \mathbf{H}(*, X) \\ & \simeq \Gamma_{\mathbf{H}}(X) \end{aligned} \,.

Analogously in the second case.

We shall write

(Π infDisc infΓ inf):=(i *i *i !)(\Pi_{inf} \dashv Disc_{inf} \dashv \Gamma_{inf}) := (i^* \dashv i_* \dashv i^!)

so that the global section geometric moprhism of H th factors as

(Π H thDisc H thΓ H th):H thΓ infDisc infΠ infHΓ HDisc HΠ HGrpd.(\Pi_{\mathbf{H}_{th}} \dashv Disc_{\mathbf{H}_{th}} \dashv \Gamma_{\mathbf{H}_{th}}) : \mathbf{H}_{th} \stackrel{\overset{\Pi_{inf}}{\to}}{\stackrel{\overset{Disc_{inf}}{\leftarrow}}{\underset{\Gamma_{inf}}{\to}}} \mathbf{H} \stackrel{\overset{\Pi_{\mathbf{H}}}{\to}}{\stackrel{\overset{Disc_{\mathbf{H}}}{\leftarrow}}{\underset{\Gamma_{\mathbf{H}}}{\to}}} \infty Grpd \,.

Let for the remainder of this section an infinitesimal neighbourhood HH th be fixed.

Properties

We give a presentation of classes of infinitesimal neighbourhoods by simplicial presheaves on suitable sites.

Definition

Let C be an ∞-cohesive site. We say a site C th

  • equipped with a coreflective embedding

    (ip):CpiC th(i \dashv p) : C \stackrel{\overset{i}{\hookrightarrow}}{\underset{p}{\leftarrow}} C_{th}
  • such that

    • i preserves pullbacks along morphisms in covering families;

    • both i and p send covering families to covering families;

    • for all U in C th and covering families {U ip(U)} there is a lift through p to a covering family {U iU}

is an infinitesimal neighbourhood site of C.

Proposition

Let C be an ∞-cohesive site and (ip):CpiC th an infinitesimal neighbourhood site.

Then the (∞,1)-category of (∞,1)-sheaves on C th is a cohesive (,1)-topos and the restriction i * along i exhibits it as an infinitesimal neighbourhood of the cohesive (,1)-topos over C.

(i !i *i *i !):Sh (,1)(C)i !i *i *i !Sh (,1)(C th).( i_! \dashv i^* \dashv i_* \dashv i^! ) : Sh_{(\infty,1)}(C) \stackrel{\overset{i_!}{\hookrightarrow}}{\stackrel{\overset{i^*}{\leftarrow}}{\stackrel{\overset{i_*}{\to}}{\stackrel{i^!}{\leftarrow}}}} Sh_{(\infty,1)}(C^{th}) \,.

Moreover, i ! restricts on representables to the (∞,1)-Yoneda embedding factoring through i:

C Sh (,1)(C) i i ! C th Sh (,1)(C th).\array{ C &\hookrightarrow& Sh_{(\infty,1)}(C) \\ \downarrow^{\mathrlap{i}} && \downarrow^{\mathrlap{i_!}} \\ C_{th} &\hookrightarrow& Sh_{(\infty,1)}(C_{th}) } \,.
Proof

We present the (∞,1)-sheaf (∞,1)-category Sh (,1)(C th) by the projective model structure on simplicial presheaves left Bousfield localized at the covering sieve inclusions

Sh (,1)(C th)([C th op,sSet] loc) Sh_{(\infty,1)}(C_{th}) \simeq ([C_{th}^{op}, sSet]_{loc})^\circ

(as discussed at models for (∞,1)-sheaf (∞,1)-toposes).

Consider the right Kan extension Ran i:[C op,sSet][C th op,sSet] of simplicial presheaves along the functor i. On an object K×DC th it is given by the end-expression

Ran iF:K UCsSet(C th(i(U),K),F(U)) UCsSet(C(U,p(K)),F(U)) F(p(K)) =:(p *F)(K),\begin{aligned} \mathrm{Ran}_{i} F : \mathbf{K} & \mapsto \int_{U \in C} \mathrm{sSet}( C_{\mathrm{th}}(i(U), \mathbf{K}) , F(U)) \\ & \simeq \int_{U \in C} \mathrm{sSet}( C(U, p(\mathbf{K})) , F(U)) \\ & \simeq F(p(\mathbf{K})) \\ & =: (p^* F)(\mathbf{K}) \end{aligned} \,,

where in the last step we use the Yoneda reduction-form of the Yoneda lemma.

This shows that the right adjoint to ()i 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

[C op,sSet]Ran p()p()iLan i[C th op,sSet].[C^{op}, sSet] \stackrel{\overset{Lan_i}{\to}}{\stackrel{\overset{(-)\circ i}{\leftarrow}}{\stackrel{\overset{(-)\circ p}{\to}}{\underset{Ran_p}{\leftarrow}}}} [C_{th}^{op}, sSet] \,.

From this are directly induced the corresponding simplicial Quillen adjunctions on the global projective and injective model structure on simplicial presheaves

(Lan i()i):[C op,sSet] proj()iLan i[C th op,sSet] proj;(Lan_i \dashv (-) \circ i) : [C^{op}, sSet]_{proj} \stackrel{\overset{Lan_i}{\to}}{\underset{(-)\circ i}{\leftarrow}} [C_{th}^{op}, sSet]_{proj} \,;
(()i()p):[C op,sSet] proj()p()i[C th op,sSet] proj;((-)\circ i \dashv (-) \circ p) : [C^{op}, sSet]_{proj} \stackrel{\overset{(-)\circ i}{\leftarrow}} {\underset{(-)\circ p}{\to}} [C_{th}^{op}, sSet]_{proj} \,;
(()pRan p):[C op,sSet] injRan p()p[C th op,sSet] inj.((-) \circ p \dashv Ran_p) : [C^{op}, sSet]_{inj} \stackrel{\overset{(-)\circ p}{\to}}{\underset{Ran_p}{\leftarrow}} [C_{th}^{op}, sSet]_{inj} \,.

Observe that Lan i, being a left Kan extension, sends representables to representables: we have

Lan iC(,T):K UCC th(K,i(U))C(U,T)Lan_i C(-,T) : \mathbf{K} \mapsto \int^{U \in C} C_{th}(\mathbf{K}, i(U)) \cdot C(U,T)

and by Yoneda reduction (more explicitly: observing that this is equivalently the formula for left Kan extension of the non-corepresentable C th(K×D,i()):CsSet along the identity functor) this is

C th(K,i(T)).\cdots \simeq C_{th}(\mathbf{K}, i(T)) \,.

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 ()i sends locally fibrant objects to locally fibrant objects.

To that end, let {U iU} be a covering family in C. Write [k]ΔΔ[k] i 0,,i k(j(U i 0)× j(U)j(U i 1)× j(U)× j(U)j(U k)) for its Cech nerve, where j denotes the Yoneda embedding. Recall by the definition of the ∞-cohesive site C that all the fiber products of representable presheaves here are again themselves representable, hence = [k]ΔΔ[k] i 0,,i k(j(U i 0× UU i 1× U× UU k)). This means that the left adjoint Lan i preserves not only the coend and tensoring, but by the remark in the previous paragraph and the assumption that i preserves pullbacks along covers we have that

Lan iC({U iU}) [k]ΔΔ[k] i 0,,i kLan i(j(U i 0× UU i 1× U× UU k)) [k]ΔΔ[k] i 0,,i kji(U i 0× UU i 1× U× UU k) [k]ΔΔ[k] i 0,,i kj(i(U i 0)× i(U)i(U i 1)× i(U)× i(U)i(U k)).\begin{aligned} Lan_i C(\{U_i \to U\}) & \simeq \int^{[k] \in \Delta} \Delta[k] \cdot \coprod_{i_0, \cdots, i_k} Lan_i (j(U_{i_0} \times_U U_{i_1} \times_U \cdots \times_U U_k)) \\ & \simeq \int^{[k] \in \Delta} \Delta[k] \cdot \coprod_{i_0, \cdots, i_k} j i (U_{i_0} \times_U U_{i_1} \times_U \cdots \times_U U_k) \\ & \simeq \int^{[k] \in \Delta} \Delta[k] \cdot \coprod_{i_0, \cdots, i_k} j (i(U_{i_0}) \times_{i(U)} i(U_{i_1}) \times_{i(U)} \cdots \times_{i(U)} i(U_k)) \end{aligned} \,.

By the assumption that i preserves covers, this is the Cech nerve of a covering family in C th. Therefore for F[C th op,sSet] proj,loc fibrant we have for all coverings {U iU} in C that the descent morphism

(i *F)(U)=F(i(U))[C th op,sSet](C({i(U i)}),F)=[C op,sSet](C({U i}),i *F)(i^* F)(U) = F(i(U)) \stackrel{}{\to} [C_{th}^{op}, sSet](C(\{i(U_i)\}), F) = [C^{op}, sSet](C(\{U_i\}), i^* F)

is a weak equivalence, hence that i *F is locally fibrant.

To see that ()p preserves locally fibrant objects, we apply the analogous reasoning after observing that its left adjoint ()i preserves all limits and colimits of simplicial presheaves (as these are computed objectwise) and by observing that for {U ip iU} a covering family in C th we have that its image under ()i is its image under p, by the Yoneda lemma:

[C op,sSet](K,(()i)(U)) C th(i(K),U) C(K,p(U))\begin{aligned} [C^{op}, sSet](K, ((-)\circ i) (\mathbf{U})) & \simeq C_{th}(i(K), \mathbf{U}) \\ & \simeq C(K, p(\mathbf{U})) \end{aligned}

and using that p preserves covers by assumption.

Therefore ()i is a left and right local Quillen functor with left local Quillen adjoint Lan i and right local Quillen adjoint ()p.

It follows that i *:Sh (,1)(C th)Sh (,1)(C) is given by the left derived functor of restriction along i, and i *:Sh (,1)(C)Sh (,1)(C th) is given by the right derived functor of restriction along p.

Finally to see that also Ran p preserves locally fibrant objects by the same reasoning as above, notice that for every covering family {U iU} in C and every morphism Kp *U in C th we may find a covering {K jK} of K such that we find commuting diagrams on the left of

K j p *U i(j) K p *Up(K j) = i *(K j) U i(j) p(K) = i *(K) U,\array{ \mathbf{K}_j &\to& p^* U_{i(j)} \\ \downarrow && \downarrow \\ \mathbf{K} &\to& p^* U } \;\;\; \leftrightarrow \;\;\; \array{ p(\mathbf{K}_j) & =& i^*(\mathbf{K}_j) &\to& U_{i(j)} \\ \downarrow && \downarrow && \downarrow \\ p(\mathbf{K}) &= & i^*(\mathbf{K}) &\to& U } \,,

because by adjunction these correspond to commuting diagrams as indicated on the right, which exist by definition of coverage on C and lift through p by assumption on C th.

This implies that {p *U ip *U} 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 i ! 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 i satisfies Lan iiid. It remains to observe that since ()i is not only right but also left Quillen by the above, we have that i *Lan i applied to a cofibrant object is already the derived functor of the composite.

Note

Conversely this implies that Sh (,1)(C th) is an ∞-connected (∞,1)-topos over Smooth∞Grpd, exhibited by the triple of adjunctions

(i *i *i !):SynthDiffGrpdSmoothGrpd.(i^* \dashv i_* \dashv i^!) : SynthDiff \infty Grpd \to Smooth \infty Grpd \,.

Structures in the presence of infinitesimal cohesion

We discuss structures that are canonically present in a cohesive (,1)-topos equipped with infinitesimal cohesion. These structures parallel the structures in a general cohesive (∞,1)-topos.

Infinitesimal paths and de Rham spaces

In the presence of infinitesimal cohesion there is an infinitesimal analog of the geometric paths ∞-groupoids.

Infinitesimal path -groupoid
Definition

Define the adjoint triple of adjoint (∞,1)-functors corresponding to the adjoint quadruple (i !i *i *i !):

(RedΠ inf dR):(i !i *i *i *i *i !):H thH th.(\mathbf{Red} \dashv \mathbf{\Pi}_{inf} \dashv \mathbf{\flat}_{dR}) : (i_! i^* \dashv i_* i^* \dashv i_* i^! ) : \mathbf{H}_{th} \to \mathbf{H}_{th} \,.

For XH th we say that

  • Π inf(X) is the infinitesimal path -groupoid of X;

    The (i *i *)-unit

    XΠ inf(X)X \to \mathbf{\Pi}_{inf}(X)

    we call the constant infinitesimal path inclusion.

  • Red(X) is the reduced cohesive -groupoid underlying X.

    The (i *i *)-counit

    RedXX\mathbf{Red} X \to X

    we call the inclusion of the reduced part of X.

Remark

In traditional contexts see (SimpsonTeleman, p. 7) the object Π inf(X) is called the de Rham space of X or the de Rham stack of X . 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 Π inf(X) is not primarily characterized by the fact that (in some models, see below) it does co-represent de Rham cohomology – because the object Π dR(X) from above does, too – but by the fact that it does so in an explicitly (synthetic) infinitesimal way.

Observation

There is a canonical natural transformation

Π inf(X)Π(X)\mathbf{\Pi}_{inf}(X) \to \mathbf{\Pi}(X)

that factors the finite path inclusion through the infinitesimal one

Π inf(X) X Π(X).\array{ && \mathbf{\Pi}_{inf}(X) \\ & \nearrow && \searrow \\ X &&\to&& \mathbf{\Pi}(X) } \,.
Proof

This is the formula for the unit of the composite adjunction H thDisc infΠ infHDiscΠGrpd:

Xi infXDisc infΠ infXDisc inf(i HΠ infX)Disc HDisc infΠ HΠ infX=Disc H thΠ H th.X \stackrel{i_{inf}X}{\to} Disc_{inf}\Pi_{inf} X \stackrel{Disc_{inf}(i_{\mathbf{H}}\Pi_{inf}X)}{\to} Disc_{\mathbf{H}} Disc_{inf} \Pi_{\mathbf{H}} \Pi_{inf} X = Disc_{\mathbf{H}_{th}} \Pi_{\mathbf{H}_{th}} \,.
Jet -bundles

Notice that for f:XY any morphism in any (∞,1)-topos H, there is the corresponding base change geometric morphism between the over-(∞,1)-toposes

(f *f *):H/Xf *f *H/Y.(f^* \dashv f_*) : \mathbf{H}/X \stackrel{\overset{f^*}{\leftarrow}}{\underset{f_*}{\to}} \mathbf{H}/Y \,.
Definition

For any object XH write

Jet:H/Xi *i *H/Π inf(X)Jet : \mathbf{H}/X \stackrel{\overset{i^*}{\leftarrow}}{\underset{i_*}{\to}} \mathbf{H}/\mathbf{\Pi}_{inf}(X)

for the base change geometric morphism induced by the constant infinitesimal path inclusion i:XΠ inf(X), def. 3.

For (EX)H/X we call Jet(E)Π inf(X) as well as its pullback i *Jet(E)X (depending on context) the jet bundle of EX.

Formally smooth/étale/unramified morphisms
Definition

We say an object XH th is formally smooth if the constant infinitesimal path inclusion, XΠ inf(X), def. 3, is an effective epimorphism.

In this form this is the evident (,1)-categorical analog of the conditions as they appear for instance in (SimpsonTeleman, page 7).

Note

An object XH th is formally smooth according to def. 5 precisely if the canonical morphism

i !Xi *Xi_! X \to i_* X

(induced from the adjoint quadruple (i !i *i *i !), see there) is an effective epimorphism.

Proof

The canonical morphism is the composite

(i !i *):=i !ηi !Π infi !:=i *i *i !i *.(i_! \to i_*) := i_! \stackrel{\eta i_!}{\to} \mathbf{\Pi}_{inf} i_! := i_* i^* i_! \stackrel{\simeq}{\to} i_* \,.

By the condition that i ! is a full and faithful (∞,1)-functor the second morphism here in an equivalence, as indicated, and hence the component of the composite on X being an effective epimorphism is equivalent to the component i !XΠi !X being an effective epimorphism.

Remark

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 u *=i !, u *=i * and u !=i *.

Therefore we have the following more general definition.

Definition

For f:XY a morphism in H, we say that

  1. f is a formally smooth morphism if the canonical morphism

    i !Xi !Y i *Yi *Yi_! X \to i_! Y \prod_{i_* Y} i_* Y

    is an effective epimorphism.

  2. f is a formally unramified morphism if this is a (-1)-truncated morphism. More generally, f is an order-k formally unramified morphisms for (2)k if this is a k-truncated morphism.

  3. f is a formally étale morphism if this morphism is an equivalence, hence if

    i !X i !f i !Y i *X i *f i *Y\array{ i_! X &\stackrel{i_! f}{\to}& i_! Y \\ \downarrow && \downarrow \\ i_* X &\stackrel{i_* f}{\to}& i_* Y }

    is an (∞,1)-pullback square.

Note

An order-(-2) formally unramified morphism is equivalently a formally étale morphism.

Only for 0-truncated X does formal smoothness together with formal unramifiedness imply formal étaleness.

Proposition

The collection of formally étale morphisms in H, def. 6, is closed under the following operations.

  1. Every equivalence is formally étale.

  2. The composite of two formally étale morphisms is itself formally étale.

  3. If

    Y f g X h Z\array{ && Y \\ & {}^{\mathllap{f}}\nearrow &\swArrow_{\simeq}& \searrow^{\mathrlap{g}} \\ X &&\stackrel{h}{\to}&& Z }

    is a diagram such that g and h are formally étale, then also f is formally étale.

  4. Any retract of a formally étale morphisms is itself formally étale.

  5. The (∞,1)-pullback of a formally étale morphisms is formally étale if the pullback is preserved by i !.

The statements about closure under composition and pullback appears as(KontsevichRosenberg, prop. 5.4, prop. 5.6). Notice that the extra assumption that i ! preserves the pullback is implicit in their setup, by remark 2.

Proof

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 f:XY and g:YZ be two morphisms and consider the pasting diagram

i !X i !f i !Y i !g Z i *X i *f i *Y i *g i *Z.\array{ i_! X &\stackrel{i_! f }{\to}& i_! Y &\stackrel{i_! g}{\to}& Z \\ \downarrow && \downarrow && \downarrow \\ i_* X &\stackrel{i_* f }{\to}& i_* Y &\stackrel{i_* g}{\to}& i_* Z } \,.

If f and g are formally étale then both small squares are pullback squares. Then the pasting law says that so is the outer rectangle and hence gf is formally étale. Similarly, if g and gf 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 f is formally étale.

For the fourth claim, let Id(gfg) be a retract in the arrow (∞,1)-category H I. By applying the natural transformation ϕ:i !I * we obtain a retract

Id((i !gi *g)(i !fi *f)(i !gi *g))Id \simeq ((i_! g \to i_*g) \to (i_! f \to i_*f) \to (i_! g \to i_*g))

in the category of squares H . We claim that generally, if the middle piece in a retract in H is an (∞,1)-pullback square, then so is its retract sqare. This implies the fourth claim.

To see this, we use that

  1. (∞,1)-limits are computed by homotopy limits in any presentable (∞,1)-category C presenting H;

  2. homotopy limits in C may be computed by the left and right adjoints provided by the derivator Ho(C) associated to C.

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

A× YX X p f A Y\array{ A \times_Y X &\to& X \\ {}^{\mathllap{p}}\downarrow && \downarrow^{\mathrlap{f}} \\ A &\to& Y }

where f is formally étale.

Applying the natural transformation ϕ:i !i * to this yields a square of squares. Two sides of this are the pasting composite

i !A× YX i !X ϕ X i *X i !p i !f i *f i !A i !Y ϕ Y i *Y\array{ i_! A \times_Y X &\to& i_! X &\stackrel{\phi_X}{\to}& i_* X \\ \downarrow^{\mathrlap{i_! p}} && \downarrow^{\mathrlap{i_! f}} && \downarrow^{\mathrlap{i_* f}} \\ i_! A &\to& i_! Y &\stackrel{\phi_Y}{\to}& i_* Y }

and the other two sides are the pasting composite

i !A× YX ϕ A× YX i *A× YA i *X i !p i *p i *f i !A ϕ A i *A i *Y.\array{ i_! A \times_Y X &\stackrel{\phi_{A \times_Y X}}{\to}& i_* A \times_Y A &\stackrel{}{\to}& i_* X \\ \downarrow^{\mathrlap{i_! p}} && \downarrow^{\mathrlap{i_* p}} && \downarrow^{\mathrlap{i_* f}} \\ i_! A &\stackrel{\phi_A}{\to}& i_* A &\to& i_* Y } \,.

Counting left to right and top to bottom, we have that

  • the first square is a pullback by assumption that i ! preserves the given pullback;

  • the second square is a pullback, since f is formally étale.

  • the total top rectangle is therefore a pullback, by the pasting law;

  • the fourth square is a pullback since i * 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 p is formally étale.

Remark

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.

Proposition

The operation Red is an idempotent projection of H th onto the image of H

RedRedRed.\mathbf{Red} \mathbf{Red} \simeq \mathbf{Red} \,.

Accordingly also

Π infΠ infΠ inf\mathbf{\Pi}_{inf} \mathbf{\Pi}_{inf} \simeq \mathbf{\Pi}_{inf}

and

inf inf inf.\mathbf{\flat}_{inf} \mathbf{\flat}_{inf} \simeq \mathbf{\flat}_{inf} \,.
Proof

By definition of infinitesimal neighbourhood we have that i ! is a full and faithful (∞,1)-functor. It follows that i *i !Id and hence

RedRed i !i *i !i * i !i * Red.\begin{aligned} \mathbf{Red} \mathbf{Red} & \simeq i_! i^* i_! i^* \\ & \simeq i_! i^* \\ & \simeq \mathbf{Red} \end{aligned} \,.
Observation

For every XH th, we have that Π inf(X) is formally smooth according to def. 5.

Proof

By prop. 6 we have that

Π inf(X)Π infΠ infX\mathbf{\Pi}_{inf}(X) \to \mathbf{\Pi}_{inf} \mathbf{\Pi}_{inf}X

is an equivalence. As such it is in particular an effective epimorphism.

Cohesive étale -groupoids

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.

Definition

Let i:HH th be an infinitesimal cohesive neighbourhood.

An object XH is called a cohesive étale -groupoid if there exists an atlas X 0X – an effective epimorphism out of a 0-truncated object – which is also a formally étale morphism def. 6.

Flat -connections and infinitesimal local systems

We discuss the intrinsic flat cohomology in an infinitesimal neighbourhood.

Definition

For X,AH th we say that

H infflat(X,A):=π 0H(Π inf(X),A)π 0H(X, infA)H_{infflat}(X,A) := \pi_0 \mathbf{H}(\mathbf{\Pi}_{inf}(X), A) \simeq \pi_0 \mathbf{H}(X, \mathbf{\flat}_{inf}A)

(where (Π inf inf) is given by def. 3) is the infinitesimal flat cohomology of X with coefficient in A.

Note

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

H dR,synth(X,A):=π 0H th(Π inf(X),A).H_{dR,synth}(X,A) := \pi_0 \mathbf{H}_{th}(\mathbf{\Pi}_{inf}(X), A) \,.
Note

By the above observation we have canonical morphisms

H flat(X,A)H infflat(X,A)H(X,A)\mathbf{H}_{flat}(X,A) \to \mathbf{H}_{infflat}(X,A) \to \mathbf{H}(X,A)

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.

Definition

For AH th an abelian ∞-group object we say that the de Rham theorem for A-coefficients holds in H th if for all XH th the infinitesimal path inclusion

Π inf(X)Π(X)\mathbf{\Pi}_{inf}(X) \to \mathbf{\Pi}(X)

is an equivalence in A-cohomology, hence if for all n we have that

π 0H th(Π(X),B nA)π 0H th(Π inf(X),B nA)\pi_0 \mathbf{H}_{th}(\mathbf{\Pi}(X), \mathbf{B}^n A) \to \pi_0 \mathbf{H}_{th}(\mathbf{\Pi}_{inf}(X), \mathbf{B}^n A)

is an isomorphism.

If we follow the notation of note 5 and moreover write X=ΠX for the intrinsic geometric realization, then this becomes

H dR,synth (X,A)H (X,A disc),H^{\bullet}_{dR, synth}(X,A) \simeq H^\bullet(|X|, A_{disc}) \,,

where on the right we have ordinary cohomology in Top (for instance realized as singular cohomology) with coefficients in the discrete group A disc:=ΓA underlying the cohesive group A.

In certain contexts of infinitesimal neighbourhoods of cohesive -toposes the de Rham theorem in this form has been considered in (SimpsonTeleman).

Formal cohesive -groupoids

The genuine infinitesimal analog of exponentiated ∞-Lie algebras are formal cohesive ∞-groupoids.

Definition

An object XH th is an infinitesimal cohesive -groupoid if Π infX*.

An ∞-group object 𝔤H th that is infinitesimal we call an formal ∞-group .

For XH any object, we say 𝔞H th is a formal cohesive ∞-groupoid over X if Π inf(𝔞)Π inf(X); equivalently: if there is a morphism

𝔞Π inf(X)\mathfrak{a} \to \mathbf{\Pi}_{inf}(X)

that serves as the (i *i *)-unit on 𝔞, hence as the infinitesimal path inclusion for 𝔞.

Proposition

An infinitesimal cohesive -groupoid is both geometrically contractible and has as underlying discrete -groupoid the point:

  • ΠX*

  • ΓX*.

Proof

The first statement is implied by the fact that both i ! as well as i * are full and faithful. This means that if Π inf(X)* then already i *X=Π inf(X)*. Since Π H thΠ HΠ inf and Π H preserves the terminal object by cohesiveness, this implies the first claim.

The second statement follows by

ΓX H th(*,X) H th(Red*,X) H th(*,Π inf(X)) H th(*,*) *.\begin{aligned} \Gamma X & \simeq \mathbf{H}_{\mathrm{th}}(*,X) \\ & \simeq \mathbf{H}_{\mathrm{th}}(\mathbf{Red}*, X) \\ & \simeq \mathbf{H}_{\mathrm{th}}(*, \mathbf{\Pi}_{\mathrm{inf}}(X)) \\ & \simeq \mathbf{H}_{\mathrm{th}}(*,*) \\ & \simeq * \end{aligned} \,.
Observation

For all XH, we have that X and Π inf(X) are formal cohesive ∞-groupoids over X, the first by the constant infinitesmal path inclusion, the second by the identity.

Proof

For X this is tautological, for Π(X) it follows from the idempotency of Red and the (i *i *)-zig-zag identity.

Proposition

The delooping B𝔤 of an formal cohesive ∞-group 𝔤 is an formal cohesive ∞-groupoid over the point.

Proof

Since both i * and i * are right adjoint, the infinitesimal path ∞-groupoid functor commutes with delooping. Therefore

Π infB𝔤 BΠ inf𝔤 B* * Π inf*.\begin{aligned} \mathbf{\Pi}_{inf} \mathbf{B}\mathfrak{g} & \simeq \mathbf{B} \mathbf{\Pi}_{inf} \mathfrak{g} \\ & \simeq \mathbf{B} * \\ & \simeq * \\ & \simeq \mathbf{\Pi}_{inf} * \end{aligned} \,.
Proposition

An infinitesimal cohesive ∞-groupoid XH th is both geometrically contractible and has as underlying discrete ∞-groupoid the point:

  • ΠX*

  • ΓX*.

Proof

This follows with using the above observation from the full and faithfulness of i ! and i *.

The former implies that with Π inf(X)* already i *X=Π infX=*. Since Π H thΠ HΠ inf and since Π H preserves the point by cohesiveness, this implies the first claim.

For the latter we compute

ΓX H th(*,X) H th(Red*,X) H th(*,Π inf(X)) H th(*,*) *.\begin{aligned} \Gamma X & \simeq \mathbf{H}_{th}(*,X) \\ & \simeq \mathbf{H}_{th}(\mathbf{Red}*, X) \\ & \simeq \mathbf{H}_{th}(*, \mathbf{\Pi}_{inf}(X)) \\ & \simeq \mathbf{H}_{th}(*,*) \\ & \simeq * \end{aligned} \,.

Lie theory

(…)

Deformation theory

For C op any (∞,1)-site the construction of the tangent (∞,1)-category T CC provides a canonical infinitesimal thickening of C:

CdomΔcodC Δ[1]Ω L,C \stackrel{\overset{cod}{\leftarrow}}{\stackrel{\overset{\Delta}{\to}}{\underset{dom}{\leftarrow}}} C^{\Delta[1]} \stackrel{\overset{L}{\to}}{\underset{\Omega^\infty}{\leftarrow}} \,,

where the -functor pair on the right forms a cod-relative (∞,1)-adjunction. The composite Li is the cotangent complex functor for C and Ω is fiberwise the canonical map out of the stabilization.

The image of i is contained in that of Ω . Therefore we may restrict the (codi)-adjunction on the right to the full sub-(∞,1)-category T˜ C of C Δ[1] on thise objects in the image of Ω . This yields an infinitesimal neighbourhood of (∞,1)-sites

C opcodi(T˜ C) op.C^{op} \stackrel{\overset{i}{\hookrightarrow}}{\underset{cod}{\leftarrow}} (\tilde T_C)^{op} \,.

(…)

(…)

Examples

References

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 Π 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 coDisc 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 (RedΠ inf inf) 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