1. Introduction
1.1 Motivation
In their seminal paper, Donaldson and Thomas [Reference Donaldson and ThomasDT98] proposed a definition of gauge-theoretic invariants for a compact Calabi–Yau threefold
$X$
. Writing
$\unicode {x03BD}_X$
for the volume form on
$X$
, these invariants would count the critical points of a holomorphic Chern–Simons functional
on spaces of connections on vector bundles on
$X$
, taken up to the action of a suitable gauge group. Defining such invariants directly in this infinite dimensional setup proved difficult, which led Thomas [Reference ThomasTho00] to pursue an algebraic setup involving moduli spaces of finite type. In the study of Donaldson–Thomas (DT) type invariants that followed [Reference Kontsevich and SoibelmanKS08, Reference Brav and DyckerhoffBD19, Reference Joyce and SongJS12], the moduli space of interest is the moduli stack of semistable sheaves
$\mathcal{M}_X$
, and the invariants are defined by expressing
$\mathcal{M}_X$
locally as a critical locus of a finite type potential [Reference JoyceJoy15].
The link between the gauge-theoretic and the algebraic setups was explored by Toda [Reference TodaTod18], who showed that the moduli space
$\mathcal{M}_X$
is locally controlled by a gauge problem associated to a polystable sheaf
$\mathcal{F} \in \mathsf{coh}\; X$
. Concretely, one takes a locally free resolution
$\mathcal{E}^\bullet \to \mathcal{F}$
and considers the DG algebra
of Dolbeault forms, whose Maurer–Cartan locus represents the critical locus of the Chern–Simons functional. The gauge problem is made finite dimensional by transferring the DG algebra structure to a minimal model, given by an
$A_\infty$
-structure on the Ext-algebra
Toda [Reference TodaTod18] shows that the Maurer–Cartan locus of
$\mathcal{H}_{\mathcal{E}}$
is an analytic space whose quotient by the gauge group presents an analytic neighbourhood of
$\mathcal{F}$
in
$\mathcal{M}_X$
. Under the assumption that
$X$
is 3 Calabi–Yau, it is, moreover, a critical locus
$\{{\rm d} \mathcal{W}_{\mathcal{F}} = 0\}$
of the associated analytic potential
where
$\unicode {x03C3}\colon {\rm Ext}^\bullet (\mathcal{F},\mathcal{F}) \xrightarrow {\ \sim \ } {\rm Ext}^{\dim X-\bullet }(\mathcal{F},\mathcal{F})^\vee$
is the Serre duality pairing. The potential is the desired replacement for the Chern–Simons functional in this finite dimensional model, and is the correct function for defining refined versions of the DT invariants [Reference Kontsevich and SoibelmanKS08, Reference Morrison, Mozgovoy, Nagao and SzendrőiMMN+12, Reference TodaTod21].
These results suggest that it should be possible to study the enumerative geometry of
$X$
by directly manipulating the
$A_\infty$
-algebra
$\mathcal{H}_{\mathcal{E}}$
using algebraic methods. However, for this to work there are two additional structures which need to be considered:
-
• an analytic structure on
$\mathfrak{g}_{\mathcal{E}}$
and
$\mathcal{H}_{\mathcal{E}}$
, in the form of a norm
${\left \|\cdot \right \|}$
for which (as shown by Tu [Reference TuTu14]) the higher products satisfy a geometric series bound(1)
\begin{align} {\left \|\unicode {x03BC}_n\right \|} \lt C^n\quad \forall n\geqslant 1; \text { and} \end{align}
-
• a cyclic structure on
$\mathcal{H}_{\mathcal{E}}$
, in the form of the isomorphism
$\unicode {x03C3} \colon \mathcal{H}_{\mathcal{E}} \to \mathcal{H}_{\mathcal{E}}^*$
which (as shown by Polishchuk [Reference PolishchukPol01]) is compatible with the natural
$A_\infty$
-bimodule structures on
$\mathcal{H}_{\mathcal{E}}$
and
$\mathcal{H}_E^*$
.
Neither the cyclic nor the analytic structure is compatible with arbitrary
$A_\infty$
-algebra morphisms. Instead, one should consider morphisms of cyclic
$A_\infty$
-algebras (defined in [Reference KajiuraKaj07, Reference Kontsevich and SoibelmanKS09]), and morphisms of analytic
$A_\infty$
-algebras (appearing implicitly in [Reference TuTu14, Reference TodaTod18]), respectively.
The aim of this paper is to develop the theory of
$A_\infty$
-algebras carrying both a cyclic and an analytic structure. The main goal is to find a general method for constructing analytic cyclic minimal models for a given analytic
$A_\infty$
-algebra, with the motivating example being the analytic DG algebra
$\mathfrak{g}_{\mathcal{E}}$
and its analytic cyclic minimal model
$(\mathcal{H}_{\mathcal{E}},\unicode {x03C3})$
. To do this we study the behaviour of right Calabi–Yau structures on such analytic
$A_\infty$
-algebras.
1.2 Main result
In what follows,
$A$
denotes an
$A_\infty$
-algebra defined over a separable
$\mathbb{C}$
-algebra
$\ell$
, which includes
$A_\infty$
-structures on vector spaces and quivers.
Recall that a right
$d$
-CY structure (often also called a proper or compact CY structure; see e.g. [Reference Kontsevich and SoibelmanKS09]) on
$A$
is a cocycle in the negative cyclic complex of
$A$
satisfying a certain nondegeneracy condition [Reference Behrend, Bryan and SzendrőiBBS13]. In this paper, we take the Connes complex
$\mathsf{C}_\lambda ^\bullet (A)$
as our model for negative cyclic cohomology
${\rm HC}_\lambda ^\bullet (A)$
, and a
$d$
-CY structure will be a cocycle in
$\mathsf{C}_\lambda ^{-d}(A)$
. Given an analytic structure
${{\left \|\cdot \right \|}} \colon A \to \mathbb{R}$
as above, we define the subcomplex
and we call a right CY structure analytic if it lies in
$\mathsf{C}_\lambda ^{{\rm an},\bullet }(A)$
. We show that the subcomplex
$\mathsf{C}_\lambda ^{{\rm an},\bullet }(A)$
admits pullbacks with respect to
$A_\infty$
-morphisms satisfying a bound analogous to (1), and that it is therefore a good cohomology theory on a category of analytic
$A_\infty$
-algebras. Working inside this category, we find the following main theorem.
Theorem A (Theorem4.23). Let
$A$
be an analytic
$A_\infty$
-algebra admitting an analytic minimal model
${\rm H}(A)$
which is finite dimensional and unital. Then every analytic right
$d$
-CY structure
$\unicode {x03D5} \in \mathsf{C}_\lambda ^{{\rm an},-d}(A)$
defines a
$d$
-cyclic analytic minimal model
which depends only on the class
$[\unicode {x03D5}]_{{\rm an}} \in {\rm HC}_\lambda ^{{\rm an},-n}(A)$
up to an isomorphism of cyclic analytic
$A_\infty$
-algebras. If
$B$
is a second such
$A_\infty$
-algebra, then every analytic quasi-isomorphism
$f\colon B \to A$
induces a cyclic analytic
$A_\infty$
-isomorphism
The proof of our main theorem follows the work of Amorim and Tu [Reference Amorim and TuAT25], proving a type of ‘analytic Darboux theorem’ for the homotopy-invariant version of cyclic structures [Reference ChoCho08], which are related to the noncommutative symplectic structures of [Reference Kontsevich and SoibelmanKS09].
Cyclic
$A_\infty$
-algebras are especially interesting in the 3-CY setting, because a cyclic
$A_\infty$
-structure is captured by a potential: given such a 3-cyclic
$A_\infty$
-algebra
$(A,\unicode {x03C3})$
there is an associated noncommutative potential
$W \in \widehat {\mathsf{T}} V := \prod _{n\geqslant 0} V^{\otimes n}$
in the completed tensor algebra over
$V = (A^1)^\vee$
. If
$A$
is, moreover, equipped with an analytic structure, this potential lies in an analytic subring
and is therefore an analytic potential in the framework of Hua and Keller [Reference Hua and KellerHK19]. Analytic morphisms induce algebra morphisms between these analytic subrings, so in the 3-CY setting our theorem can be interpreted as follows.
Corollary B (Corollary4.24). In the situation of Theorem
A
suppose that
$\unicode {x03D5}$
is a right 3-CY structure, and write
$V_A = {\rm H}^1(A)^\vee$
. Then there is a canonical analytic potential
which is well defined up to an automorphism of
$\widetilde {\mathsf{T}} V_A$
. Moreover, if
$f\colon B\to A$
is a quasi-isomorphism and
$V_B = {\rm H}^1(B)^\vee$
then there is an induced isomorphism
$g\colon \widetilde {\mathsf{T}} V_A \to \widetilde {\mathsf{T}} V_B$
such that
The main theorem and its corollary provide a bridge between infinite dimensional settings, involving, for example, normed DG algebras, and finite dimensional settings, such as those considered in [Reference Hua and KellerHK19]. In particular, it applies to the gauge-theoretic setup mentioned above.
1.3 Analytic CY structures in complex geometry
We apply TheoremA to describe the cyclic analytic minimal models of Toda’s DGA
$\mathfrak{g}_{\mathcal{E}}$
for a perfect complex
$\mathcal{E}$
of vector bundles on a smooth projective variety
$X$
of dimension
$d$
. If
$X$
is Calabi–Yau with holomorphic volume form
${\unicode {x03BD}_X}\in {\rm H}^0(X,\Omega ^d_X)$
, then there is an induced right CY structure: the bounded linear functional
defines a cocycle
$\unicode {x03D5}^{\unicode {x03BD}_X} \in \mathsf{C}_\lambda ^{{\rm an},-d}(\mathfrak{g}_{\mathcal{E}})$
which is nondegenerate in the appropriate sense. The associated cyclic analytic minimal model
$(\mathcal{H}_{\mathcal{E}}^{\unicode {x03BD}_X},\unicode {x03C3}^{\unicode {x03BD}_X})$
recovers that found in [Reference PolishchukPol01, Reference TuTu14, Reference TodaTod18].
There are, in general, many other choices of analytic right CY structures, each of which yields a cyclic analytic minimal model of
$\mathfrak{g}_{\mathcal{E}}$
. We identify a family of such CY structures corresponding to holomorphic volume germs along the support
$Z = {\rm \mathsf{supp}}\; \mathcal{E}$
, by which we mean the equivalence class of a differential form
on analytic open neighbourhoods
$U\supset Z$
, which is nonvanishing when
$U$
is sufficiently small. Such a germ determines a bounded linear functional on the DG subalgebra
of Dolbeault forms with compact support in any sufficiently small neighbourhood
$U\supset Z$
. This functional induces an analytic right CY structure on
$\mathfrak{g}_{\mathcal{E}|_U,c}$
, which we transfer to a right CY structure on
$\mathfrak{g}_{\mathcal{E}}$
using an explicit
$A_\infty$
-quasi-isomorphism. This leads to the following theorem.
Theorem C (Theorem5.10). Let
$X$
be a smooth projective variety of dimension
$d$
, and
$\mathcal{E} \in \mathsf{D}^{{\rm perf}}(X)$
a complex with support
$Z\subset X$
. Then every volume germ
$\unicode {x03BD} \in (\Omega ^d_X)_Z$
determines a class
$[\unicode {x03D5}^{\unicode {x03BD}}]_{{\rm an}} \in {\rm HC}_\lambda ^{{\rm an},-d}(\mathfrak{g}_{\mathcal{E}})$
of an analytic right
$d$
-CY structure, and hence a
$d$
-cyclic analytic minimal model
which is uniquely defined up to an isomorphism of cyclic analytic
$A_\infty$
-algebras. Moreover,
$\mathcal{H}_{\mathcal{E}}^{\unicode {x03BD}}$
is isomorphic to
$\mathcal{H}_{\mathcal{E}}$
as an ordinary (non-cyclic) analytical
$A_\infty$
-algebra.
The above theorem applies to the setting of [Reference TodaTod18] when
$\mathcal{E}$
is a resolution of a polystable sheaf
$\mathcal{F} \in \mathsf{coh}\; X$
whose support does not meet the canonical divisor
$K_X$
. Some examples considered in the enumerative geometry literature are point sheaves [Reference BehrendBeh09] and sheaves on contractible curves [Reference SzendrőiSze08, Reference KatzKat08]. If
$X$
is a threefold, then there is a noncommutative analytic potential
whose abelianisation
$\mathcal{W}^{\unicode {x03BD}}_{\mathcal{E}} = (W^{\unicode {x03BD}}_{\mathcal{E}})^{{\rm ab}}$
is an ordinary analytic function whose critical locus describes the moduli space of semistable sheaves around
$\mathcal{F}$
. Hence, the gauge-theoretic setup can be generalised from the projective CY-3 case in [Reference TodaTod18] to open analytic neighbourhoods of projective CY-3 folds equipped with a choice of volume form.
In our setup, both the
$A_\infty$
-algebra structure on the Ext-algebra of
$\mathcal{E}$
and the volume germ
$\unicode {x03BD}$
are determined in terms of analytic-local geometry around the support of
$\mathcal{E}$
in
$X$
. One would therefore expect that the cyclic
$A_\infty$
-algebra
$(\mathcal{H}_{\mathcal{E}}^{\unicode {x03BD}},\unicode {x03C3}^{\unicode {x03BD}})$
is not sensitive to the global geometry of
$X$
. To show this we consider embeddings of such neighbourhoods into other projective varieties.
Theorem D (Theorem5.13). Let
$X,X'$
be smooth projective varieties of dimension
$d$
, and let
$Y$
be an open submanifold of
$X$
with an open embedding into
$X'$
, as in the following diagram.

Let
$\mathcal{E}'$
be a perfect complex on
$X'$
with cohomological support
$f(Z) \subset f(Y)$
for some compact
$Z\subset Y$
, and let
$\unicode {x03BD} \in (\Omega ^d_{X'})_Z$
be a volume germ. Then for any
$\mathcal{E} \in \mathsf{D}^{{\rm perf}}(X)$
such that
$\mathcal{E}|_Y \simeq f^*\mathcal{E}'$
, there exists an analytic quasi-isomorphism
which identifies the classes
$[\unicode {x03D5}^{\unicode {x03BD}}]$
and
$[\unicode {x03D5}^{f^*\unicode {x03D5}}]$
via pullback. In particular, there is an analytic cyclic
$A_\infty$
-isomorphism between the
$d$
-cyclic analytic minimal models
Corollary E (Corollary5.14). If
$X,X'$
are threefolds, then the noncommutative potentials
$W_{\mathcal{E}'}^{\unicode {x03BD}}$
and
$W_{\mathcal{E}}^{f^*\unicode {x03BD}}$
are related by an analytic change of variables
$\widetilde {\mathsf{T}}{\rm Ext}^1(\mathcal{E},\mathcal{E})^\vee \xrightarrow {\sim } \widetilde {\mathsf{T}}{\rm Ext}^1(\mathcal{E}',\mathcal{E}')$
.
One implication of TheoremD is that there is a canonical cyclic
$A_\infty$
-structure on the Ext-algebra of a compactly supported sheaf
$\mathcal{F}$
on a quasi-projective Calabi–Yau threefold
$Y$
equipped with a fixed volume form. Indeed, applying TheoremC to a resolution of
$\mathcal{F}$
on any compactification
$X = \overline Y$
, it follows from TheoremD that the cyclic
$A_\infty$
-algebra obtained does not depend on these choices.
For the reader who is exclusively interesting in projective Calabi–Yau geometry, we stress that TheoremD also allows one to compare the cyclic analytic
$A_\infty$
-structure (hence the enumerative geometry) of different projective CY varieties on a common analytic neighbourhood. As a motivating example, we compute the cyclic analytic
$A_\infty$
-structure on the Ext-algebra of an arbitrary point sheaf.
Proposition F (Proposition5.18). Let
$p\in X$
be a point on a smooth projective variety
$X$
of dimension
$d$
, and
$\mathcal{F} \to \mathcal{O}_p$
a locally free resolution for the associated point sheaf. Then for every volume germ
$\unicode {x03BD} \in (\Omega ^d_Y)_p$
there is an isomorphism of cyclic analytic
$A_\infty$
-algebras
\begin{align*} \mathcal{H}^{\unicode {x03BD}}_{\mathcal{F}} \cong _{{\rm an},{\rm cyc}} \left (\ \bigwedge ^\bullet T_{\kern -.5pt o\kern .5pt}{\mathbb{A}}^d,\ \unicode {x03C3}^\lambda \colon \xi \mapsto \lambda (\xi \wedge -)\ \right ), \end{align*}
where the right-hand side denotes the graded algebra of polyvectors at the origin
$o\in {\mathbb{A}}^d$
with cyclic structure induced by some linear form
$\lambda \colon \bigwedge ^d T_{\kern -.5pt o\kern .5pt}{\mathbb{A}}^d \xrightarrow {\sim } {\mathbb{C}}$
.
1.4 Structure of the paper
In § 2 we recall the definition of (analytic)
$A_\infty$
-algebras, and prove some new results about inverses of analytic morphisms that are used in later sections.
In § 3 we define analytic
$A_\infty$
-bimodules and analytic Hochschild cohomology, and we prove some new results about the invertibility of analytic
$A_\infty$
-bimodule maps.
In § 4 we define analytic (homotopy) cyclic structures, used to prove TheoremA.
In § 5 we apply these results to the DG algebras of Dolbeault differential forms, which is used to prove TheoremsC and D, and PropositionF. This section is largely self-contained.
2. Analytic
$A_\infty$
-algebras
In this section we recall the definitions of
$A_\infty$
-algebras and morphisms, and introduce the relevant category of analytic
$A_\infty$
-algebras based on the convergence conditions of [Reference TuTu14, Reference TodaTod18]. The
$A_\infty$
-algebras we will use in § 5 have a natural structure of a quiver (possibly with multiplicity), since the
$A_\infty$
-algebras encode a certain noncommutative multi-pointed deformation theory. In order to preserve this structure in all our constructions, we work in a general setup of
$A_\infty$
-algebras over a separable algebra rather than over a field, following the example of [Reference Van den BerghVdB15].
In what follows let
$\ell$
be a separable
$\mathbb{C}$
-algebra (i.e. a product of matrix algebras) and
$\operatorname {\mathsf{grMod}} \ell ^e$
the graded
$\mathbb{C}$
-linear category of graded bimodules
$V = V^\bullet$
which are nonzero in finitely many degrees. Given
$V,W\in \operatorname {\mathsf{grMod}} \ell ^e$
we denote the graded vector space of
$\ell ^e$
-linear maps by
and write
${{\rm Hom}}_{\ell ^e}(V,W)$
for the subspace of graded morphisms. We write
$|f|$
for the degree of a homogeneous element
$f\in \hom _{\ell ^e}^\bullet (V,W)$
. The category
$\operatorname {\mathsf{grMod}} \ell ^e$
carries the usual graded tensor product
$\otimes := \otimes _\ell$
and shift functor
$[1]\colon \operatorname {\mathsf{grMod}} \ell ^e \to \operatorname {\mathsf{grMod}} \ell ^e$
. We write
$s\in \hom ^{-1}_{\ell ^e}(V,V[1])$
for the shift map, acting as the identity
$V^i \to V^i = (V[1])^{i-1}$
on each graded component.
2.1
$A_\infty$
-algebras and morphisms
$A_\infty$
-algebras are commonly defined as sequences of multilinear maps either of the form
$V^{\otimes n} \to W$
with varying degrees or of the form
$V[1]^{\otimes n} \to W[1]$
, with all maps being homogeneous. In this section we adopt the latter convention, adopting the notation
\begin{align*} \mathcal{M}^\bullet (V,W) := \prod _{n=0}^\infty \hom _{\ell ^e}^\bullet (V[1]^{\otimes n}, W[1]) \end{align*}
for the graded vector space of these sequences
$f = (f_n)_{n\in \mathbb{N}}$
, and we write
$\overline {\mathcal{M}}(V,W) \subset \mathcal{M}(V,W)$
for the subspace of sequences with
$f_0=0$
. There exist various compositions between sequences in
$\mathcal{M}(V,W)$
, which are most cleanly described using the bar construction
\begin{align*} \mathsf{B} V := \left (\bigoplus _{n\in \mathbb{N}} V[1]^{\otimes n}, \Delta \right ) \end{align*}
which is a cofree coaugmented conilpotent coalgebra over
$\ell$
with the decomposition coproduct
$\Delta$
. The cofreeness implies that every sequence
$f \in \mathcal{M}(V,V) \simeq \hom _{\ell ^e}(\mathsf{B} V,V[1])$
induces a unique coderivation
$\widetilde f \colon \mathsf{B} V \to \mathsf{B} V$
via the formula (see [Reference TradlerTra08, Lemma 2.3])
and likewise every coderivation defines a sequence in
$\mathcal{M}(V,V)$
by composing with the obvious projection
$\unicode {x03C0} \colon \mathsf{B} V \to V[1]$
. In terms of the bar construction,
$A_\infty$
-algebras are defined as follows.
Definition 2.1. An
$A_\infty$
-algebra is a pair
$(A,\unicode {x03BC})$
of
$A\in \operatorname {\mathsf{grMod}} \ell ^e$
and a map
$\unicode {x03BC} \in \overline {\mathcal{M}}^1(A, A)$
satisfying the condition
${\widetilde {\unicode {x03BC}}}^2=0$
, or equivalently
$\unicode {x03BC} \circ \widetilde {\unicode {x03BC}} = 0$
.
The
$A_\infty$
-condition implies that
$\unicode {x03BC}_1^2=0$
, so that
$\unicode {x03BC}_1$
makes
$A[1]$
into a cochain complex. We say an
$A_\infty$
-algebra is compact if the cohomology with respect to
$\unicode {x03BC}_1$
is finite dimensional over
$\mathbb{C}$
.
Example 2.2. If
$(A,{\rm d}, \cdot )$
is a DG algebra, then the associated
$A_\infty$
-structure is given by the compositions
$\unicode {x03BC}_1 = -s\circ {\rm d} \circ s^{-1}$
and
$\unicode {x03BC}_2 = -s^{-1} \circ (-\cdot -) \circ (s^{-1}\otimes s^{-1})$
.
Given
$V,W\in \operatorname {\mathsf{grMod}} \ell ^e$
, every sequence
$f \in \mathcal{M}(V,W) \simeq \hom _{\ell ^e}(\mathsf{B} V,W[1])$
induces a cohomomorphism
$\widehat f \colon \mathsf{B} V \to \mathsf{B} W$
between the associated coalgebras via the formula
and every cohomomorphism between bar-coalgebras can be described in this way. These lifts are used to define (pre-)morphisms of
$A_\infty$
-algebras.
Definition 2.3. A pre-morphism between
$A_\infty$
-algebras
$A$
and
$B$
is an element
$f\in \overline {\mathcal{M}}^0(A,B)$
. A pre-morphism is a morphism if it satisfies
$\widetilde {\unicode {x03BC}}_B \circ \widehat f = \widehat f \circ \widetilde {\unicode {x03BC}}_A$
, or equivalently
$\unicode {x03BC}_B \circ \widehat f=f\circ \widetilde {\unicode {x03BC}}_A$
.
The morphism condition implies that
$f_1\colon A[1] \to B[1]$
is a morphism of cochain complexes. A morphism
$f\in {{\rm Hom}}_{\mathsf{Alg}^\infty }(A,B)$
is called a quasi-isomorphism if
$f_1$
is a quasi-isomorphism.
By lifting pre-morphisms to cohomomorphisms, one obtains an associative composition between (pre-)morphisms which we will write as
With this composition,
$A_\infty$
-algebras form a category
$\mathsf{Alg}^\infty$
with morphism spaces
${{\rm Hom}}_{\mathsf{Alg}^\infty }(A,B)$
. We remark that the composition of two quasi-isomorphisms is again a quasi-isomorphism.
Definition 2.4. A unit for an
$A_\infty$
-algebra
$A = (A,\unicode {x03BC})$
is an injective map
$\unicode {x1D7D9} \colon \ell [1] \to A[1]$
such that
\begin{align*} \begin{aligned} \unicode {x03BC}_2(\unicode {x1D7D9}(l),a) = la,\quad \unicode {x03BC}_2(a,\unicode {x1D7D9}(l)) = (-1)^{|a|+1} al \quad &\textrm{for all}\; l\in \ell [1],\ a\in A[1]\\[5pt] \unicode {x03BC}_n(\ldots ,\unicode {x1D7D9}(l),\ldots ) = 0 \quad &\textrm{for all}\; n\neq 2, \end{aligned} \end{align*}
and a triple
$(A,\unicode {x03BC},\unicode {x1D7D9})$
is called a unital
$A_\infty$
-algebra.
If
$A$
and
$B$
are unital
$A_\infty$
-algebras, with units
$\unicode {x1D7D9}_A$
and
$\unicode {x1D7D9}_B$
, then one can consider the subset
${{\rm Hom}}_{\mathsf{Alg}^\infty }^{{\rm un}}(A,B) \subset {{\rm Hom}}_{\mathsf{Alg}^\infty }(A,B)$
of morphisms
$f$
satisfying
\begin{align*} \begin{aligned} f_1 \circ \unicode {x1D7D9}_A &= \unicode {x1D7D9}_B,\\[5pt] f_{i+j+1} \circ ({\rm id}^{\otimes i} \otimes \unicode {x1D7D9}_A \otimes {\rm id}^{\otimes j}) &= 0\quad \textrm{for all}\; i+j \gt 0, \end{aligned} \end{align*}
which are called unital
$A_\infty$
-morphisms. The composition of two unital morphisms is again unital, so unital
$A_\infty$
-algebras again form a category
$\mathsf{Alg}^{\infty ,{\rm un}}$
. Finally, we consider a weakening of the unital condition in cohomology.
Definition 2.5. A weak unit, or cohomological unit, is a map
$\unicode {x1D7D9}\colon \ell [1] \to A[1]$
for which the image is
$\unicode {x03BC}_1$
-closed and which satisfies the following relations in
$\unicode {x03BC}_1$
-cohomology:
One can likewise define a category of cohomologically unital
$A_\infty$
-algebras, with morphisms consisting of
$A_\infty$
-morphisms
$f$
for which
$[f_1(\unicode {x1D7D9}(l))] = [\unicode {x1D7D9}(l)]$
.
2.2 Homotopies
$A_\infty$
-algebras are a model for homotopical algebra, and it is therefore natural to consider morphisms up to homotopy. There are various definitions, ranging from algebraic [Reference Lefèvre-HasegawaLH03, Reference KellerKel01] to more continuous variants [Reference Flajolet and SedgewickFS09], which lead to equivalent theories of homotopy. Below we use a variation of the piecewise-smooth model in [Reference Flajolet and SedgewickFS09, § 4.2.1].
Definition 2.6. Let
$\mathsf{PC}^\infty ([0,1]) \subset L^\infty ([0,1])$
denote the ring of equivalence classes of bounded real functions on
$f\colon [0,1] \to \mathbb{R}$
that are smooth outside of a discrete set, with two functions identified if they agree almost everywhere. We call elements of
$\mathsf{PC}^\infty ([0,1])$
piecewise-smooth functions.
Remark 2.7. Any
$f \in \mathsf{PC}^\infty ([0,1])$
has well-defined one-sided limits at every
$t\in [0,1]$
. If the one-sided limits agree everywhere, then
$f$
is the class of the continuous function
$\lim _{t'\to t} f(t')$
. This recovers the more restrictive definition of ‘piecewise-smooth function’ as a continuous function with smoothness imposed on a dense set, which may be common in other texts.
For each
$f\in \mathsf{PC}^\infty ([0,1])$
, the derivative
${\partial x}/{\partial t}$
is by definition well defined on the smooth locus, and therefore extends to a unique equivalence class in
$\mathsf{PC}^\infty ([0,1])$
if it is bounded. We can therefore consider the DG algebra of piecewise differential forms
with the usual wedge product and differential
${\rm d} \colon x+y {\rm d} t \mapsto {\partial x}/{\partial t} {\rm d} t$
. Then we consider, for any
$A_\infty$
-algebra
$(A,\unicode {x03BC})$
, the tensor product
$A_\infty$
-algebra
where the
$A_\infty$
-algebra structure is defined as in [Reference LodayLod11, Proposition 3.7] by
where
$(-\cdots -)$
denotes the multiplication on
$k$
elements in
$\Omega ^\bullet _{[0,1]}$
, and maps are applied along the isomorphism
$(\Omega _{[0,1]}^\bullet \otimes A[1])^{\otimes k} \cong (\Omega _{[0,1]}^\bullet )^{\otimes k} \otimes A[1]^{\otimes k}$
observing the usual Koszul sign conventions. The tensor product fits into a diagram of three quasi-isomorphisms
where
$\mathsf{ev}_t((x+y{\rm d} t)\otimes a) = \lim _{t'\to t} x(t') \cdot a$
. These maps make
$\Omega ^\bullet _{[0,1]} \otimes A$
into a path-space object as in [Reference Flajolet and SedgewickFS09, Definition 4.2.1], which leads to the following notion of a homotopy.
Definition 2.8. A homotopy between two morphisms
$f,g\in {{\rm Hom}}_{\mathsf{Alg}^\infty }(A,B)$
is an
$A_\infty$
-morphism
$H\in {{\rm Hom}}_{\mathsf{Alg}^\infty }(A,\Omega ^\bullet _{[0,1]}\otimes B)$
such that
$\mathsf{ev}_0\circ H=f$
and
$\mathsf{ev}_1 \circ H=g$
.
To make the condition more explicit we can write
$H \in \overline {\mathcal{M}}^0(A,\Omega ^\bullet _{[0,1]}\otimes B)$
as
$H = H_x + H_y {\rm d} t$
for some coefficient functions
$t\mapsto H_x^t\in \overline {\mathcal{M}}^0(A,B)$
and
$t\mapsto H_y^t \in \overline {\mathcal{M}}^{-1}(A,B)$
. Then, as observed in [[Reference Flajolet and SedgewickFS09, (4.2.41)], the map
$H$
is a homotopy if and only if the following two conditions hold:
It follows from a general argument [Reference Flajolet and SedgewickFS09, Proposition 4.2.37] that homotopy defines an equivalence relation between
$A_\infty$
-morphisms, which is compatible with the composition. We give a direct proof below, which will also apply in the analytic setting.
Lemma 2.9.
Homotopy defines an equivalence relation
$\sim$
on
${{\rm Hom}}_{\mathsf{Alg}^\infty }(A,B)$
.
Proof.
It is clear that
$f\sim f$
for any
$f\in {{\rm Hom}}_{\mathsf{Alg}^\infty }(A,B)$
via the constant homotopy
$H^t = f$
. Likewise, if
$f\sim g$
via a homotopy
$H = H_x + H_y {\rm d} t$
then
$G^t = H^{1-t}_x - H_y^{1-t} {\rm d} t$
defines a homotopy
$g\sim f$
. Now if
$f\sim g$
and
$g\sim h$
via homotopies
$H = H_x + H_y{\rm d} t$
and
$G= G_x + G_y{\rm d} t$
, then we consider the pre-morphism
$G*H \in \overline {\mathcal{M}}^0(A,\Omega ^\bullet _{[0,1]}\otimes B)$
with
\begin{align*} (G*H)^t = \left\{\begin{array}{l@{\quad}l} H_x^{2t} + 2 H_y^{2t}{\rm d} t & t\leqslant 1/2\\[5pt] G_x^{2t-1} + 2 G_y^{2t-1} & t\gt 1/2. \end{array} \right.\end{align*}
We remark that this is well defined: the coefficient functions are piecewise-smooth,
$(G*H)_x$
is continuous since
$H_x^1 = g=G_x^0$
by assumption, and the derivative of
$(G*H)_x$
is bounded by the derivatives of
$G_x$
and
$H_x$
. By construction,
$(G*H)_x^t \in {{\rm Hom}}_{\mathsf{Alg}^\infty }(A,B)$
for all
$t\in [0,1]$
, showing (5). The identity (6) holds for almost all
$t \in [0,1/2)$
since
\begin{align*} \begin{aligned} \frac {\partial }{\partial t} (G*H)_x^t &= 2\cdot \left(\unicode {x03BC} \circ \left(\widehat H_x^{2t} \otimes H_y^{2t} \otimes \widehat H_x^{2t}\right) + H_y^{2t} \circ \widetilde {\unicode {x03BC}}\right) \\[5pt] &= \unicode {x03BC} \circ \left({\widehat {(G*H)}}_x^t \otimes (G*H)_y^t \otimes {\widehat {(G*H)}}_x^t\right) + (G*H)_y^t \circ \widetilde {\unicode {x03BC}}, \end{aligned} \end{align*}
and a similar computation shows that the identity holds for almost all
$t\in (1/2,1]$
. Hence
$G*H$
is a homotopy between
$f = \mathsf{ev}_0 \circ (G*H)$
and
$h = \mathsf{ev}_1\circ (G*H)$
.
Lemma 2.10.
If
$f\sim f'$
and
$g\sim g'$
then
$f\diamond g \sim f'\diamond g'$
.
Proof.
Let
$H$
and
$G$
be the homotopies for
$f\sim f'$
and
$g\sim g'$
. Then
$H\diamond g$
is clearly a homotopy between
$f\diamond g \sim f'\diamond g$
. Now
$f'$
lifts to an
$A_\infty$
-morphism
${\rm id} \otimes f'$
between the path objects, providing a homotopy
$({\rm id}\otimes f')\diamond G$
between
$f'\diamond g$
and
$f'\diamond g'$
.
We say that two morphisms
$f,g$
in
$\mathsf{Alg}^\infty$
are homotopy inverse if
$f\diamond g$
and
$g\diamond f$
are homotopic to the identity. In this case
$f$
and
$g$
are said to be homotopy equivalences and their source/target
$A_\infty$
-algebras are homotopy equivalent.
2.3 Minimal models
Recall that an
$A_\infty$
-algebra
$(A,\unicode {x03BC})$
is called minimal if
$\unicode {x03BC}_1=0$
. It is often convenient to replace an
$A_\infty$
-algebra by a homotopy equivalent minimal one: a minimal model.
Definition 2.11. A minimal model for
$A$
is a minimal
${\rm H}(A) \in {\mathsf{Alg}^\infty }$
with quasi-isomorphisms
$P = P_A \in {{\rm Hom}}_{\mathsf{Alg}^\infty }(A,{\rm H}(A))$
and
$I = I_A \in {{\rm Hom}}_{\mathsf{Alg}^\infty }({\rm H}(A),A)$
such that:
It is well known that every
$A_\infty$
-algebra admits a minimal model, which can be constructed explicitly using Kadeishvili’s homotopy transfer formula [Reference KadeishviliKad80] applied to the cohomology algebra of
$A$
.
Given
$A_\infty$
-algebras
$A,B\in {\mathsf{Alg}^\infty }$
with a fixed choice of minimal models
${\rm H}(A)$
and
${\rm H}(B)$
, we obtain for every morphism
$f\in {{\rm Hom}}_{\mathsf{Alg}^\infty }(A,B)$
an induced map
It is well known that if
$f$
is a quasi-isomorphism, then
${\rm H}(f)$
is an isomorphism. The inverse at the level of minimal models can be constructed using a ‘tree formula’ that we recall below.
Definition 2.12. We use
$\mathcal{O}(n)$
to denote the set of planar rooted trees on
$n$
leaves in which every internal node has valency
$\geqslant 3$
, and we use
$\mathcal{O}(n,d) \subset \mathcal{O}(n)$
to denote the subset of trees with
$d$
internal nodes.
Note that there is a unique tree in
$\mathcal{O}(1) = \mathcal{O}(1,0)$
and that for
$n\gt 1$
each tree
$T\in \mathcal{O}(n)$
is uniquely determined by the ordered list of rooted subtrees
$T_1,\ldots ,T_k$
starting in the internal node of
$T$
connected to the root.
For any pre-morphism
$f\in \overline {\mathcal{M}}^0(A,B)$
and map
$g_1 \colon B[1]\to A[1]$
we define a map for every
$T\in \mathcal{O}(n)$
as follows: for the unique tree
$T\in \mathcal{O}(1)$
we set
$g_T = g_1$
and for general
$T\in \mathcal{O}(n)$
we set
where
$T_1,\ldots ,T_k$
are the subtrees starting in the internal node of
$T$
connected to the root. The following result is classical, and can be easily verified using the recursive formula.
Proposition 2.13.
Let
$f\in \overline {\mathcal{M}}^0(A,B)$
be a pre-morphism such that
$f_1\colon A[1]\to B[1]$
admits an inverse
$g_1\colon B[1]\to A[1]$
. Then the pre-morphism
$g\in \overline {\mathcal{M}}(B,A)$
defined by
is an inverse to
$f$
. If
$f$
is, moreover, an
$A_\infty$
-morphism, then
$g$
is again an
$A_\infty$
-morphism.
Lemma 2.14. Every quasi-isomorphism induces an isomorphism between minimal models.
Proof.
Fix minimal models
${\rm H}(A)$
and
${\rm H}(B)$
with maps
$I_A,I_B,P_A,P_B$
as in (7). Then given any quasi-isomorphism
$f\in {{\rm Hom}}_{\mathsf{Alg}^\infty }(A,B)$
, the induced map
${\rm H}(f) = P_B \diamond f \diamond I_A$
is again a quasi-isomorphism, because
$P_B$
and
$I_A$
are quasi-isomorphisms. But then
${\rm H}(f)_1$
is an isomorphism by minimality, and the inverse
${\rm H}(f)^{-1}$
exists by Proposition2.13.
Corollary 2.15.
Minimal models are unique up to
$A_\infty$
-isomorphism.
Proof.
This follows directly from Lemma2.14 when taking
${\rm H}(A)$
and
${\rm H}(B)$
to be two different minimal models of
$A=B$
with morphism
$f={\rm id}_A$
.
Given a quasi-isomorphism
$f$
, the composition
$g = I_A \diamond {\rm H}(f)^{-1}\diamond P_B$
is a homotopy inverse to
$f$
. To see this, note that there are identities
induced by the homotopies
$I_A\circ P_A \sim {\rm id}_A$
and
$I_B\circ P_B \sim {\rm id}_B$
. Hence, every quasi-isomorphism is also a homotopy equivalence.
2.4 Analytic algebras and morphisms
We now consider the category
$\operatorname {\mathsf{grNMod}} {\ell ^e}$
of graded normed
$\ell ^e$
-bimodules, by which we mean pairs
$(V,{{\left \|\cdot \right \|}}_V)$
of a bimodule
$V\in \operatorname {\mathsf{grMod}} \ell ^e$
and a norm
${{\left \|\cdot \right \|}}_V \colon V\to \mathbb{R}$
on the underlying ungraded vector space such that for any
$l,r\in \ell$
the multiplication
$v \mapsto l v r$
is bounded in
${{\left \|\cdot \right \|}}_\ell$
. Between any
$V,W \in \operatorname {\mathsf{grNMod}} {\ell ^e}$
there is a graded normed vector space
of bounded morphisms with respect to the operator norm
${\left \|f\right \|}_{{\rm op}} := \sup _{\|v\|_V=1} \|f(v)\|_W$
. The shift naturally extends to a functor
$[1]\colon \operatorname {\mathsf{grNMod}} {\ell ^e} \to \operatorname {\mathsf{grNMod}}{\ell ^e}$
, and for any pair
$V,W\in \operatorname {\mathsf{grNMod}} {\ell ^e}$
the tensor product
$V\otimes W$
is again normed via the projective tensor norm
where the infimum is over all presentations of an element
$z\in V\otimes W$
as a sum of pure tensors in the tensor product
$V\otimes _{\mathbb{C}} W$
over
$\mathbb{C}$
. If
$f_i\colon V_i \to W_i$
are bounded bimodule morphisms between
$V_1,V_2,W_1,W_2 \in \operatorname {\mathsf{grNMod}}{\ell ^e}$
, the tensor product
$f_1\otimes f_2$
has operator norm
and is therefore a bounded bimodule map
$V_1\otimes V_2 \to W_1\otimes W_2$
. Henceforth, we will drop the subscripts on the above norms to reduce clutter.
Now given a normed
$\ell$
-bimodule
$V\in \operatorname {\mathsf{grNMod}} {\ell ^e}$
and
$r \in \mathbb{R}$
with
$r \gt 0$
we consider the following normed version of the bar construction:
noting that the supremum in the definition of
${{\left \|\cdot \right \|}}_r$
is finite for any finite sum in
$\mathsf{B} V$
. Bounded maps out of these normed
$\ell$
-bimodules are characterised by the following lemma.
Lemma 2.16.
Let
$V,W\in \operatorname {\mathsf{grNMod}} {\ell ^e}$
and let
$f \in \mathcal{M}(V,W)$
. Then the following are equivalent:
-
(i) there exists
$C\gt 0$
such that
${\left \|f_n\right \|} \lt C^n$
for all
$n\geqslant 1$
; and
-
(ii) there exists
$r\gt 0$
such that
$f\colon \mathsf{B}(V,r) \to W[1]$
is bounded.
If additionally
$f_0=0$
then this is also equivalent to:
-
(iii) for every
$r'\gt 0$
there exists an
$r\gt 0$
such that
$\widehat f \colon \mathsf{B}(V,r) \to \mathsf{B}(W,r')$
is bounded.
If additionally
$V=W$
then this is also equivalent to:
-
(iv) for every
$r'\gt 0$
there exists an
$r\gt 0$
such that
$\widetilde f \colon \mathsf{B}(V,r) \to \mathsf{B}(V,r')$
is bounded.
Proof.
(i)
$\implies$
(ii). Without loss of generality we may assume that
$f_0=0$
. Let
$C\gt 0$
be such that
${\left \|f_n\right \|} \lt C^n$
for all
$n\geqslant 1$
, and fix some
$r \lt C^{-1}$
. Then the map
$f \colon \mathsf{B}(V,r) \to W[1]$
satisfies, for every
$v = \sum _{n\geqslant 1} v_n \in \mathsf{B}(V,r)$
,
\begin{align*} {\left \|f(v)\right \|} \leqslant \sum _{n\geqslant 1} {\left \|f_n(v_n)\right \|} \lt \sum _{n\geqslant 1} C^n {\left \|v_n\right \|} \leqslant \sum _{n\in \mathbb{N}} (Cr)^n {\left \|v\right \|}_r = \frac {{\left \|v\right \|}_r}{1-Cr}, \end{align*}
where the final equality for the geometric series holds because
$Cr \lt 1$
. It follows that
$f$
has operator norm bounded by
$(1-Cr)^{-1} \lt \infty$
.
(ii)
$\implies$
(i). If
$f \colon \mathsf{B}(V,r) \to W[1]$
is bounded in the operator norm by some constant
$K\gt 1$
, then for each
$n\geqslant 1$
and
$v_n \in V[1]^{\otimes n}$
the map
$f_n$
satisfies
Hence, picking any
$C\gt K/r$
it follows that
${\left \|f_n\right \|} \lt C^n$
for all
$n\geqslant 1$
.
(i)
$\implies$
(iii). Let
$C\gt 0$
be such that
${\left \|f_n\right \|} \lt C^n$
for all
$n\geqslant 1$
, fix
$r'\gt 0$
and let
$K = \min \{r',1\}$
. Then assuming
$f_0=0$
and expanding the formula for
$\widehat f$
, we find that, for every
$v = \sum _{n\in \mathbb{N}} v_n \in \mathsf{B} V$
,
\begin{align*} \begin{aligned} {\left \|\widehat f(v)\right \|}_{r'} &\leqslant \sum _{n\geqslant 1} \sum _{n_1+\cdots +n_k = n} {\left \|f_{n_1}\otimes \cdots \otimes f_{n_k}(v_n)\right \|} (r')^{-k} \\[5pt] &\leqslant \sum _{n\in \mathbb{N}} \sum _{n_1+\cdots +n_k = n} C^n K^{-k} {\left \|v_n\right \|} \\[5pt] &\leqslant \sum _{n\in \mathbb{N}} ({\#}\textrm{ partitions of n})\cdot \left (\frac CK\right )^n {\left \|v_n\right \|}. \end{aligned} \end{align*}
The number of partitions of
$n$
is bounded by the number of ordered partitions (also known as compositions), of which there are
$2^{n-1}$
, and it is therefore, in particular, bounded by
$2^n$
. Picking
$r\lt {K}/{2C}$
, the geometric series with terms
$({2rC}/{K})^n$
again converges, which shows that
\begin{align*} {\left \|\widehat f(v)\right \|}_{r'} \leqslant \sum _{n\in \mathbb{N}} \left (\frac {2rC}{K}\right )^n {\left \|v\right \|}_r = \frac {K}{K-2rC} {\left \|v\right \|}_r. \end{align*}
As
$r$
can be chosen independently of
$v$
, it follows that
$\widehat f \colon \mathsf{B}(V,r) \to \mathsf{B}(V,r')$
is bounded.
(i)
$\implies$
(iv). Let
$C\gt 1$
be such that
${\left \|f_n\right \|}\lt C^n$
for all
$n\in \mathbb{N}$
, fix
$r'\gt 0$
and let
$K=\min \{r',1\}$
. Then assuming
$f_0=0$
and expanding the formula for
$\widetilde f$
yields, for every
$v=\sum _{n\in \mathbb{N}} v_n \in \mathsf{B} V$
,
\begin{align*} \begin{aligned} {\left \|\widetilde f(v)\right \|}_{r'} &\leqslant \sum _{n\in \mathbb{N}} \sum _{i+k+j=n} {\left \|({\rm id}^{\otimes i} \otimes f_k \otimes {\rm id}^{\otimes j})(v_n)\right \|} (r')^{-(i+j+1)} \\[5pt] &\leqslant \sum _{n\in \mathbb{N}} \sum _{i+k+j=n} C^k K^{-(i+j+1)}{\left \|v_n\right \|} \\[5pt] &\leqslant \sum _{n\in \mathbb{N}} n^3 \left (\frac CK\right )^n{\left \|v_n\right \|}. \end{aligned} \end{align*}
Picking
$q\gt 0$
such that
$n^3 \lt q^n$
for all
$n$
and an
$r\lt {K}/{qC}$
, it again follows that
\begin{align*} {\left \|\widetilde f(v)\right \|}_{r'} \leqslant \sum _{n\in \mathbb{N}} \left (\frac {rqC}{K}\right )^n {\left \|v\right \|}_r = \frac {K}{K - rqC}{\left \|v\right \|}_r, \end{align*}
and hence
$\widetilde f$
is bounded when considered as a linear map
$\mathsf{B}(V,r) \to \mathsf{B}(V,r')$
.
(iii), (iv)
$\implies$
(ii). For any
$r'$
, the projection
$\unicode {x03C0}\colon \mathsf{B}(V,r') \to V[1]$
is obviously bounded, so if a map
$\widehat f$
or
$\widetilde f$
is bounded it follows that
$f = \unicode {x03C0} \circ \widehat f = \unicode {x03C0} \circ \widetilde f$
is again bounded.
We define the space of analytic sequences of multilinear maps between
$V$
and
$W$
as
and note that its elements are sequences
$f = (f_n)_{n\in \mathbb{N}}$
satisfying one of the equivalent conditions in the above lemma. As before, we write
$\overline {\mathcal{A}}(V,W) \subset {\mathcal{A}}(V,W)$
for the sequences with
$f_0=0$
.
Definition 2.17.
An analytic
$A_\infty$
-algebra is a pair
$(A,\unicode {x03BC})$
of
$A\in \operatorname {\mathsf{grNMod}}{\ell ^e}$
and
$\unicode {x03BC}\in \overline {\mathcal{A}}^1(A,A)$
which satisfies
${\widetilde {\unicode {x03BC}}}^2=0$
.
Example 2.18. Let
$(A,{\rm d})$
be a DG algebra, and suppose
${{\left \|\cdot \right \|}}\colon A \to \mathbb{R}$
is any norm on the underlying vector space. Then the differential and multiplication define an analytic
$A_\infty$
-algebra structure if and only if both are bounded. In particular, this includes the case of Banach DG algebras.
Example 2.19. Let
$(A,\unicode {x03BC})$
be a finite dimensional
$A_\infty$
-algebra such that
$\unicode {x03BC}_n=0$
for
$n\gg 0$
. Then
$(A,\unicode {x03BC})$
is analytic for any choice of norm on
$A$
.
Remark 2.20. It follows from Lemma 2.16 that the definition given above is equivalent to the
$A_\infty$
-algebras satisfying the convergence condition used in [Reference TuTu14, Reference TodaTod18].
Given two analytic
$A_\infty$
-algebras
$A$
and
$B$
, we say that a pre-morphism
$f$
is analytic if it lies in the subspace
$f\in {\mathcal{A}}^0(A,B)$
. Lemma2.16 implies that the composition of analytic pre-morphisms is well defined.
Lemma 2.21.
For any three analytic
$A_\infty$
-algebras
$A,B,C$
, the composition restricts to a map
Proof.
Given
$f\in {\mathcal{A}}^0(A,B)$
and
$g\in {\mathcal{A}}^0(B,C)$
, it follows from Lemma2.16 that there exist
$r_1,r_2\gt 0$
such that the maps
are bounded. Then the composition
$g \diamond f=g \circ \widehat f$
is also bounded.
We conclude that analytic
$A_\infty$
-algebras again form a category
$\mathsf{Alg}^{\infty ,{\rm an}}$
, with morphism spaces
with an obvious forgetful functor
${\mathsf{Alg}^{\infty ,{\rm an}}} \to {\mathsf{Alg}^\infty }$
.
2.5 Analytic homotopies
To generalise the definition of homotopies to analytic
$A_\infty$
-algebras we introduce a norm on the path object. The algebra
$\mathsf{PC}^\infty ([0,1])$
is bounded for the essential supremum norm
${{\left \|\cdot \right \|}}_{\infty }$
on
$L^\infty ([0,1])$
, and likewise
$\Omega ^\bullet _{[0,1]}$
is bounded in the norm
For
$A\in {\mathsf{Alg}^{\infty , {\rm an}}}$
there is an induced tensor norm on
$\Omega ^\bullet _{[0,1]}\otimes A$
and one checks easily that this is an analytic
$A_\infty$
-algebra, using (3) and (4). The following is then a natural generalisation of homotopy between analytic
$A_\infty$
-morphisms.
Definition 2.22. For
$A,B\in {\mathsf{Alg}^{\infty ,{\rm an}}}$
, a homotopy
$H\in {{\rm Hom}}_{\mathsf{Alg}^\infty }(A,\Omega ^\bullet _{[0,1]}\otimes B)$
is analytic if it lies in the subspace
${{\rm Hom}}_{\mathsf{Alg}^\infty }^{{\rm an}}(A,\Omega ^\bullet _{[0,1]}\otimes B)$
.
We will use an explicit sufficient condition for a homotopy to be analytic in terms of the coefficient functions. Suppose
$H = H_x + H_y {\rm d} t$
, then for all
$k\geqslant 1$
we have a bound
where
${{\left \|\cdot \right \|}}_\infty$
denotes the essential supremum of the operator norms over the interval, and bounds
Hence
$H$
is analytic if and only if there is a
$C\gt 0$
such that for each
$k\geqslant 1$
the functions
$H_{x,k}$
,
$\tfrac {\partial }{\partial t} H_{x,k}$
, and
$H_{y,k}$
are bounded almost everywhere by
$C^k$
. We use this to prove the following.
Lemma 2.23.
Analytic homotopy defines an equivalence relation
$\sim _{{\rm an}}$
on
${{\rm Hom}}_{\mathsf{Alg}^\infty }^{{\rm an}}(A,B)$
.
Proof.
Given
$f\in {{\rm Hom}}_{\mathsf{Alg}^\infty }^{{\rm an}}(A,B)$
, the constant homotopy
$H=1\otimes f$
has norms
${\left \|(1\otimes f)_k\right \|} = {\left \|f_k\right \|}$
and is therefore analytic. Hence
$f\sim _{{\rm an}} f$
always holds. Likewise, if
$f\sim _{{\rm an}} g$
with analytic homotopy
$H = H_x + H_y {\rm d} t$
, then the coefficient functions of the homotopy
$G^t = H_x^{1-t} - H_y^{1-t} {\rm d} t$
have norms
Hence
$G$
is again analytic and provides an analytic homotopy
$g\sim _{{\rm an}} f$
. Finally, suppose
$f\sim _{{\rm an}} g$
and
$g\sim _{{\rm an}} h$
via analytic homotopies
$H$
and
$G$
, then we have
\begin{align*} \begin{gathered} {\left \|(G*H)_{x,k}\right \|}_\infty = \max \{{\left \|H_{x,k}\right \|}_\infty ,{\left \|G_{x,k}\right \|}_\infty \},\quad {\left \|(G*H)_{x,k}\right \|}_\infty=2 \max \{{\left \|\tfrac {\partial }{\partial t}H_{x,k}\right \|}_\infty ,{\left \|\tfrac {\partial }{\partial t}G_{x,k}\right \|}_\infty \},\\[5pt] {\left \|(G*H)_{x,k}\right \|}_\infty=2 \max \{{\left \|H_{y,k}\right \|}_\infty ,{\left \|G_{y,k}\right \|}_\infty \}.\quad \end{gathered} \end{align*}
Since the coefficient functions of
$H$
and
$G$
are essentially bounded by
$C^k$
for some
$C\gt 0$
, the coefficient functions of
$G*H$
are essentially bounded by
$(2C)^k$
. Hence,
$G*H$
is an analytic homotopy
$f\sim _{{\rm an}} h$
.
The relation
$\sim _{{\rm an}}$
is again compatible with
$\diamond$
, because the compositions used in Lemma2.10 are analytic. Hence we obtain an equivalence relation on morphisms in
$\mathsf{Alg}^{\infty ,{\rm an}}$
which is compatible with composition. In particular, we can speak of analytic homotopy inverse maps and analytic homotopy equivalences as before.
2.6 Analytic minimal models
We define an analogue of a minimal model in the analytic setting by requiring all the structures involved to be analytic.
Definition 2.24. An analytic minimal model for
$A\in {\mathsf{Alg}^{\infty ,{\rm an}}}$
is a minimal
${\rm H}(A) \in {\mathsf{Alg}^{\infty ,{\rm an}}}$
with quasi-isomorphisms
$P \in {{\rm Hom}}_{\mathsf{Alg}^\infty }^{{\rm an}}(A,{\rm H}(A))$
and
$I \in {{\rm Hom}}_{\mathsf{Alg}^\infty }^{{\rm an}}({\rm H}(A),A)$
such that:
In contrast to the non-analytic case, not every analytic
$A_\infty$
-algebra has an analytic minimal model. Indeed, it is in general not even possible to find chain maps
$I_1$
and
$P_1$
providing a bounded splitting of its cohomology. Nonetheless, the construction in [Reference TuTu14] shows that the homotopy transfer formula can be used to construct analytic minimal models in geometric settings, which we will see in § 5.
We conclude by generalising some results about (homotopy) inverses from § 2.3.
Lemma 2.25.
Let
$f \in \overline {\mathcal{A}}^0(A,B)$
be an analytic pre-morphism such that
$f_1\colon A[1]\to B[1]$
admits a bounded inverse
$g_1$
. Then the inverse
$g$
of Proposition
2.13
is again analytic.
Proof.
By assumption there exists a common constant
$C\gt 1$
such that
${\left \|g_1\right \|} \lt C$
and
${\left \|f_n\right \|} \lt C^n$
for all
$n\geqslant 1$
. We now claim that for any tree
$T \in \mathcal{O}(n,d)$
the norm of
$g_T$
is bounded by
${\left \|g_T\right \|} \lt C^{2n+2d-1}$
. This follows by induction: for the base case
$T\in \mathcal{O}(1) = \mathcal{O}(1,0)$
, we have
while for
$n\gt 1$
any tree
$T\in \mathcal{O}(n)$
determined by subtrees
$T_i \in \mathcal{O}(n_i,d_i)$
such that
$\sum n_i = n$
and
$\sum d_i = d-1$
, we have
assuming the claim holds for all
$n_i\lt n$
and
$d_i \lt d$
; this shows the identity for each
$T$
. To derive the analytic bound we note that any
$T\in \mathcal{O}(n)$
has valency
$\geqslant 3$
at internal nodes, and therefore has at most
$n-1$
internal nodes. Hence,
$\mathcal{O}(n)$
consists of the subsets
$\mathcal{O}(n,d)$
with
$d=1,\ldots , n-1$
internal nodes. Any
$T\in \mathcal{O}(n,d)$
has
$n+d$
total vertices, and is therefore bounded by the Catalan number
$\mathcal{C}_{n+d-1} = {1}/{n+d}\binom {2n+2d}{n+d}$
, which counts the number of all planar rooted trees with
$n+d$
vertices (see e.g. [Reference FukayaFuk09, § I.3.21]). The cardinality of
$\mathcal{O}(n)$
is therefore bounded by
\begin{align*} |\mathcal{O}(n)| \leqslant \sum _{d=1}^{n-1} \mathcal{C}_{n+d-1} \leqslant (n-1) \mathcal{C}_{2n-2} = \tfrac {n-1}{2n-1}\binom {4n-4}{2n-2} \leqslant \sum _{j=0}^{4n-4} \binom {4n-4}{j} = 2^{4n-4} \leqslant 16^n. \end{align*}
We therefore find the following bound on the norm of
$g_n$
:
\begin{align*} {\left \|g_n\right \|} \leqslant \sum _{d=0}^{n-1} \sum _{T\in \mathcal{O}(n,d)} \|g_T\| \lt \sum _{d=0}^{n-1} \sum _{T\in \mathcal{O}(n,d)} C^{2n+2d-1} \leqslant |\mathcal{O}(n)| \cdot C^{4n} \lt (16C^4)^n. \end{align*}
Because the constant
$16C^4$
is independent of
$n$
, it follows that
$g$
is analytic.
Note that if the
$A_\infty$
-algebras
$A$
and
$B$
are finite dimensional, then the continuity of
$g_1$
is automatic. The above now implies that the morphism between minimal models induced by an analytic quasi-isomorphism is invertible in the analytic category.
Lemma 2.26.
Suppose
$A,B\in {\mathsf{Alg}^{\infty ,{\rm an}}}$
are compact and admit analytic minimal models. Then every analytic quasi-isomorphism induces an analytic isomorphism between the minimal models.
Proof.
By assumption there are minimal models
${\rm H}(A)$
,
${\rm H}(B)$
such that the maps
$I_A,I_B,P_A,P_B$
are analytic, and hence the morphism
${\rm H}(f) := P_B \diamond f \diamond I_A$
is again analytic. By assumption
${\rm H}(A)$
and
${\rm H}(B)$
are finite dimensional, so the inverse of
${\rm H}(f)_1$
is bounded and therefore the inverse
${\rm H}(f)^{-1}$
is analytic by Lemma2.25.
Corollary 2.27.
Analytic minimal models of compact analytic
$A_\infty$
-algebras are unique up to analytic isomorphism.
If
$f$
is an analytic quasi-isomorphism between compact analytic
$A_\infty$
-algebras admitting minimal models, then
$g = I_A \diamond {\rm H}(f)^{-1} \diamond P_B$
is an analytic homotopy inverse, since the homotopies (8) and (9) are again analytic. Hence for such analytic
$A_\infty$
-algebras, analytic quasi-isomorphisms and analytic homotopy equivalences are the same.
Finally, we show that the existence of minimal models only depends on the analytic homotopy equivalence class of an
$A_\infty$
-algebra.
Lemma 2.28.
Suppose
$A,B\in {\mathsf{Alg}^{\infty ,{\rm an}}}$
are analytic
$A_\infty$
-algebras which are analytically homotopy equivalent. Then
$A$
admits an analytic minimal model if and only if
$B$
does.
Proof.
By assumption there are maps
$f \in {{\rm Hom}}_{\mathsf{Alg}^\infty }^{{\rm an}}(A,B)$
and
$g\in {{\rm Hom}}_{\mathsf{Alg}^\infty }^{{\rm an}}(B,A)$
which are homotopy inverse. Then the composition
$g\diamond f \in {{\rm Hom}}_{{\mathsf{Alg}^\infty }}^{{\rm an}}(A,A)$
is a homotopy equivalence, and hence a quasi-isomorphism. If
$A$
admits a minimal model, it follows from Lemma2.26 that
$g\diamond f$
admits an analytic homotopy inverse
$T = I_A \diamond {\rm H}(g\diamond f)^{-1} \diamond P_A$
. We see that
so that
$P_A\diamond T\diamond g$
is left-inverse to
$f\diamond I_A$
. To show it is homotopy right-inverse, first note that
$g\diamond f \sim _{{\rm an}} {\rm id}_A$
implies that
$T$
is homotopic to the identity via
Since
$f\diamond g\sim _{{\rm an}} {\rm id}_B$
also holds, the claim then follows from the chain of homotopies
Hence the maps
$I_B = f\diamond I_A$
and
$P_B = P_A\diamond T\diamond g$
make
${\rm H}(A)$
into a minimal model for
$B$
.
3. Analytic
$A_\infty$
-bimodules
In this section we define
$A_\infty$
-bimodules and morphisms over an analytic
$A_\infty$
-algebra by imposing an analogous condition on sequences of multilinear maps. We start by recalling the definition of such bimodules using a bar construction, for which we again follow Tradler [Reference TradlerTra08].
3.1
$A_\infty$
-bimodules
Given an
$A_\infty$
-algebra
$A \in {\mathsf{Alg}^\infty }$
,
$A$
-bimodules and the morphisms between them can be defined via double sequences of morphisms in the graded vector space
\begin{align*} \mathcal{M}_A(M,N) := \prod _{i,j=0}^\infty \hom _{\ell ^e}(A[1]^{\otimes i} \otimes M[1] \otimes A[1]^{\otimes j}. N[1]). \end{align*}
We will use the notation
$\unicode {x03C1} = (\unicode {x03C1}_{i,j})_{i,j\in \mathbb{N}}$
for homogeneous elements of
$\mathcal{M}_A(M,N)$
, and when applying such a map to elements we will underline the element in
$M[1]$
for clarity. As before, this space of sequences can be identified with the morphisms out of a bar construction
\begin{align*} \mathsf{B}_A M := \mathsf{B} A \otimes M[1] \otimes \mathsf{B} A = \bigoplus _{i,j=0}^\infty A[1]^{\otimes i} \otimes M[1]\otimes A[1]^{\otimes j}, \end{align*}
which is naturally a cofree cobimodule over the coalgebra
$\mathsf{B} A$
. In [Reference TradlerTra08, Lemmas 3.3, 4.2] it is shown that one can lift any map
$\unicode {x03C1} \in \mathcal{M}_A(M,N)$
to a cohomomorphism
$\widehat {\unicode {x03C1}}\colon \mathsf{B}_AM \to \mathsf{B}_AN$
, and to a coderivation
$\widetilde {\unicode {x03C1}} \colon \mathsf{B}_AM \to \mathsf{B}_A M$
if
$M=N$
. These maps are explicitly given by the following formulas:
\begin{align*} \begin{aligned} \widehat {\unicode {x03C1}} &:= \sum _{i,j\geqslant 0} {\rm id}^{\otimes i} \otimes \underline {\unicode {x03C1}} \otimes {\rm id}^{\otimes j} \\[5pt] \widetilde {\unicode {x03C1}} &:= \sum _{i,j} {\rm id}^{\otimes i} \otimes \underline {\unicode {x03C1}} \otimes {\rm id}^{\otimes j} + \sum _{i,j,k\geqslant 0} {\rm id}^{\otimes i} \otimes \unicode {x03BC}_A \otimes {\rm id}^{\otimes k} \otimes \underline {{\rm id}}_{M[1]} \otimes {\rm id}^{\otimes j} \\[5pt] &\quad + \sum _{i,j,k\geqslant 0}{\rm id}^{\otimes i} \otimes \underline {{\rm id}}_{M[1]} \otimes {\rm id}^{\otimes k} \otimes \unicode {x03BC}_A \otimes {\rm id}^{\otimes j}, \end{aligned} \end{align*}
where the part of the maps landing in
$M[1]$
is again underlined. These lifts are used to define
$A_\infty$
-bimodule structures and their morphisms, as follows.
Definition 3.1. An
$A_\infty$
-bimodule over an
$A_\infty$
-algebra
$A$
is pair
$(M,\unicode {x03BD})$
of a bimodule
$M \in \operatorname {\mathsf{grMod}} \ell ^e$
and a map
$\unicode {x03BD} \in \mathcal{M}_A^0(M, M)$
satisfying
$\widetilde {\unicode {x03BD}}^2=0$
, or equivalently
$\unicode {x03BD} \circ \widetilde {\unicode {x03BD}} = 0$
.
The main examples of bimodules which we will consider are the following; proofs that these are bimodules can be found in [Reference TradlerTra08, Lemma 5.1].
Example 3.2. The diagonal bimodule
$A_\Delta = (A,\unicode {x03BD}_\Delta )$
is defined by the map
Example 3.3. The dual bimodule
$A^\vee = ({{\rm Hom}}_{\mathbb{C}}(A,{\mathbb{C}}), \unicode {x03BD}_\Delta ^\vee )$
is defined by the sequence of maps
where
$K= |a|(|b| + |c| + |d|) + |b|$
is a Koszul sign.
Bimodules over an
$A_\infty$
-algebra
$A$
form a DG category with the following morphism complexes.
Definition 3.4. A pre-morphism between
$A_\infty$
-bimodules
$(M,\unicode {x03BD}_M)$
and
$(N,\unicode {x03BD}_N)$
is a cochain in
The degree
$0$
cocycles form the subspace of morphisms
${{\rm Hom}}_{A-A}(M,N) \subset \hom _{A-A}^0(M,N)$
.
Given
$\unicode {x03C1} \in \hom _{A-A}(M,N)$
and
$\unicode {x03C4} \in \hom _{A-A}(L,M)$
the composition is defined as
$\unicode {x03C1} \diamond \unicode {x03C4} = \unicode {x03C1} \circ \widehat {\unicode {x03C4}}$
. This composition then yields a well-defined DG category
$\operatorname {\mathsf{Mod}}^\infty _{A-A}$
of
$A_\infty$
-bimodules.
Given a morphism
$f \in {{\rm Hom}}_{{\mathsf{Alg}^\infty }}(A,B)$
of
$A_\infty$
-algebras
$A,B\in {\mathsf{Alg}^\infty }$
, there is a DG functor
mapping a
$B$
-bimodule
$(M,\unicode {x03BD})$
to
$(M,f^\sharp \unicode {x03BD}) = (M,\unicode {x03BD} \circ (\widehat f \otimes \underline {{\rm id}}_{M[1]} \otimes \widehat f))$
and mapping a
$B$
-bimodule pre-morphism
$\unicode {x03C1}$
to the map
$f^\sharp \unicode {x03C1}$
defined by the composition
For a proof that this defines a DG functor
$f^\sharp$
and that this is functorial in
$f$
, see [Reference GanatraGan12, § 2.8].
For any
$f \in {{\rm Hom}}_{{\mathsf{Alg}^\infty }}(A,B)$
, there are
$A_\infty$
-bimodule morphisms
$f_\Delta \in {{\rm Hom}}_{A-A}(A_\Delta ,f^\sharp B_\Delta )$
and
$f_\Delta ^\vee \in {{\rm Hom}}_{A-A}(f^\sharp B_\Delta ^\vee , A_\Delta ^\vee )$
defined in components by
\begin{align*} \begin{aligned} (f_\Delta )_{i,j}(a,b,c) &= f_{i+1+j}(a,b,c),\\[5pt] (f_\Delta ^\vee )_{i,j}(a,\underline {b},c)(d) &= (-1)^K b (f_{i+1+j} (c, d, a)), \end{aligned} \end{align*}
where
$a \in A^{\otimes i}$
,
$c\in A^{\otimes j}$
, and
$K = |a|(|b|+|c|+|d|)$
is a Koszul sign. Given any pre-morphism
$\unicode {x03C1} \in \hom _{B-B}(B_\Delta ,B_\Delta ^\vee )$
there is a pre-morphism
$f^*\unicode {x03C1} \in \hom _{A-A}(A_\Delta ,A_\Delta ^\vee )$
given by
This defines a chain map
$f^*\colon \hom _{B-B}(B_\Delta ,B_\Delta ^\vee ) \to \hom _{A-A}(A_\Delta ,A_\Delta ^\vee )$
for each
$f$
, since
$f^\sharp$
is a DG functor and
$f_\Delta$
and
$f_\Delta ^\vee$
commute with the differential. One can check that this is also functorial.
3.2 Hochschild cohomology
Given an
$A_\infty$
-algebra
$A$
, one can define the Hochschild cohomology with values in any
$A_\infty$
-bimodule
$M$
. The Hochschild complex can again be modelled using the bar construction: following Tradler [Reference TradlerTra08, Lemma 2.3], each
$\unicode {x03BE} \in \mathcal{M}(A,M)$
defines a map
which is a coderivation
$\overline {\unicode {x03BE}}\colon \mathsf{B} A \to \mathsf{B}_AM$
with values in the comodule
$\mathsf{B}_AM$
. As before, the underlining signifies the component mapping to the factor
$M$
. Using this lift, the Hochschild cochain complex can be defined as follows.
Definition 3.5. Let
$(A,\unicode {x03BC})$
be an
$A_\infty$
-algebra and
$(M,\unicode {x03BD})$
an
$A$
-bimodule. Then the
$M$
-valued Hochschild cochain complex is the complex
$\mathsf{C}^\bullet (A,M) := \left (\mathcal{M}(A,M)[-1],\ {\bf b}\right )$
with differential
The cohomology of the complex is denoted
${{\rm HH}}^\bullet (A,M)$
, and, if
$M = A_\Delta$
, the complex and its cohomology are denoted as
$\mathsf{C}^\bullet (A) := \mathsf{C}^\bullet (A,A_\Delta )$
and
${{\rm HH}}^\bullet (A) := {{\rm HH}}^\bullet (A,A_\Delta )$
, respectively.
The Hochschild complex is functorial in each factor: any morphisms
$f\in {{\rm Hom}}_{{\mathsf{Alg}^\infty }}(A,B)$
or
$\unicode {x03C1}\in {{\rm Hom}}_{A-A}(M,N)$
induce respective chain maps
\begin{align*} \begin{aligned} \mathsf{C}^\bullet (B,M) &\to \mathsf{C}^\bullet (A,f^\sharp M)\quad &\unicode {x03BE} \mapsto \unicode {x03BE} \circ \widehat f,\\[5pt] \mathsf{C}^\bullet (A,M) &\to \mathsf{C}^\bullet (A,N)\quad &\unicode {x03BE} \mapsto \unicode {x03C1} \circ \overline {\unicode {x03BE}}. \end{aligned} \end{align*}
In particular, for
$M= A_\Delta ^\vee$
and
$\unicode {x03C1} = f_\Delta ^\vee$
the combination of these constructions yields a chain map
$f^* \colon \mathsf{C}^\bullet (B,B_\Delta ^\vee ) \to \mathsf{C}^\bullet (A,A_\Delta ^\vee )$
, sending
$\xi \mapsto f_\Delta ^\vee \circ \overline {\xi \circ \widehat f}$
. Explicitly, this map is given by
\begin{align*} f^*\xi (a_1,\ldots ,a_n)(a_0) = \sum _{\substack {i,j\geqslant 0\\[5pt] i+j \leqslant n}} (-1)^{K_i} \xi (\widehat f(a_{i+1},\ldots ,a_{n-j}))(f(a_{n-j+1},\ldots ,a_n,a_0,a_1,\ldots ,a_i)), \end{align*}
where
$K_i = (|a_1|+\cdots +|a_i|)(|a_{i+1}|+\cdots +|a_n| + |a_0|)$
is the Koszul sign obtained from permuting the
$a_i$
. This map is natural with respect to
$f$
and induces a map
$[f^*] \colon {{\rm HH}}^\bullet (B,B_\Delta ^\vee ) \to {{\rm HH}}^\bullet (A,A_\Delta ^\vee )$
, making the Hochschild cohomology with values in the dual bimodule functorial.
A variation of Hochschild cohomology is negative cyclic cohomology, which can be realised using Connes’ complex. An element
$\unicode {x03BE} = (\xi _n)_{n\in \mathbb{N}} \in \mathsf{C}^\bullet (A,A^\vee _\Delta )$
is called cyclic if for each
$n\geqslant 1$
and all
$a_0,\ldots ,a_n \in A[1]$
the following relation holds:
One checks that the Hochschild differential preserves cyclic cochains, yielding a subcomplex
which is called Connes’ complex. The cohomology of this complex is denoted
${\rm HC}_\lambda ^\bullet (A)$
. We remark that the pullback along any morphism
$f\in {{\rm Hom}}_{{\mathsf{Alg}^\infty }}(A,B)$
preserves cyclic cocycles, and therefore restricts to a map
$f^*\colon \mathsf{C}^\bullet _\lambda (B) \to \mathsf{C}^\bullet _\lambda (A)$
and an induced map
$[f^*] \colon {\rm HC}_\lambda ^\bullet (B) \to {\rm HC}_\lambda ^\bullet (A)$
.
It is well known that Hochschild cohomology and negative cyclic cohomology are invariant under homotopy equivalences. Below we include a proof using the definition of homotopy in § 2.2, which will also apply in the analytic setting.
Proposition 3.6.
Let
$f,g\in {{\rm Hom}}_{\mathsf{Alg}^\infty }(A,B)$
with
$f\sim g$
. Then
$f$
and
$g$
induce the same morphisms
Proof.
If
$f\sim g$
then
$f = \mathsf{ev}_0 \circ H$
and
$g=\mathsf{ev}_1 \circ H$
for some homotopy
$H\in {{\rm Hom}}_{\mathsf{Alg}^\infty }(A,\Omega ^\bullet _{[0,1]}\otimes B)$
, and the induced maps are therefore given by
Therefore, it is sufficient to prove that the maps
$\mathsf{ev}_0,\mathsf{ev}_1 \in {{\rm Hom}}_{\mathsf{Alg}^\infty }(\Omega ^\bullet _{[0,1]} \otimes B, B)$
induce the same map
$[\mathsf{ev}_0^*] = [\mathsf{ev}_1^*]$
on Hochschild/negative cyclic cohomology, which we do below.
Let
$\unicode {x03BE} \in Z^k\mathsf{C}(B,B^\vee _\Delta )$
be any fixed cocycle. Then the pullback along
$\mathsf{ev}_t$
for any
$t\in [0,1]$
is given by a cocycle
$\mathsf{ev}_t^*\unicode {x03BE} \in Z^k\mathsf{C}(\Omega ^\bullet _{[0,1]} \otimes B,(\Omega ^\bullet _{[0,1]} \otimes B)^\vee _\Delta )$
, given on pure tensors of the form
$\omega _i = (x_i+y_i{\rm d} t) \otimes b_i$
by
We claim that the difference
$\mathsf{ev}_1^*\unicode {x03BE} - \mathsf{ev}_0^*\unicode {x03BE}$
is the
${\bf b}$
-image
$\unicode {x03B6}\in \mathsf{C}^{k-1}(\Omega ^\bullet _{[0,1]} \otimes B, (\Omega ^\bullet _{[0,1]} \otimes B)^\vee _\Delta )$
defined on pure tensors
$\omega _i = (x_i+y_i{\rm d} t) \otimes b_i$
as
\begin{equation} \begin{aligned} \zeta _n(\omega _1,\ldots ,\omega _n)(\omega _{n+1}) &= \sum _{j=1}^n(-1)^{|\unicode {x03BE}|+|b_1|+\cdots +|b_{j-1}|} \int _0^1 x_1\cdots y_j \cdots x_{n+1} {\rm d} t \cdot \xi _n(b_1,\ldots ,b_n)(b_{n+1})\\[5pt] &\quad + (-1)^{|\unicode {x03BE}|+1+|b_1|+\cdots +|b_n|} \int _0^1 x_1\cdots x_n y_{n+1} {\rm d} t \cdot \xi _n(b_1,\ldots ,b_n)(b_{n+1}). \end{aligned} \end{equation}
For brevity we decompose the
$A_\infty$
-structure defined in (3) and (4) as
$\unicode {x03BC}^\otimes = {\rm d} + \unicode {x03BC}$
, using the abbreviation
${\rm d} = {\rm d} \otimes {\rm id}$
and
$\unicode {x03BC} = \sum _{k\geqslant 1} (-\cdots -) \otimes \unicode {x03BC}_k$
. Then we have the following:
By inspection, the value of (12) on variables
$\omega _i = (x_i+y_i{\rm d} t) \otimes b_i$
is
\begin{align*} \begin{aligned} &({\rm d}^\vee \circ \unicode {x03B6} - (-1)^{|\unicode {x03B6}|} \cdot \unicode {x03B6} \circ \widetilde {{\rm d}})(\omega _1,\ldots ,\omega _n)(\omega _{n+1})\\[5pt] &\quad = (-1)^{|\unicode {x03B6}|+|b_1|+\cdots + |b_n|} \unicode {x03B6}(x_1\otimes b_1,\ldots ,x_n\otimes b_n)({\rm d} x_{n+1}\otimes b_{n+1}) \\[5pt] &\quad \quad - \sum _{j=1}^n (-1)^{|\unicode {x03B6}|+|b_1|+\cdots +|b_{j-1}|} \cdot \unicode {x03B6}_n(x_1\otimes b_1,\ldots , {\rm d} x_j\otimes b_j , \ldots , x_n\otimes b_n)(x_{n+1}\otimes b_{n+1}) \\[5pt] &\quad = \sum _{j=1}^{n+1} \int _0^1 \left (x_0\cdots \tfrac {\partial x_j}{\partial t} \cdots x_n\right ) {\rm d} t \cdot \unicode {x03BE}_n(b_1,\ldots ,b_n)(b_{n+1}) \\[5pt] &\quad = (x_0(1)\cdots \cdots x_n(1) - x_0(0)\cdots \cdots x_n(0))\cdot \unicode {x03BE}_n(b_1,\ldots ,b_n)(b_0) \\[5pt] &\quad = (\mathsf{ev}_1^*\unicode {x03BE})_n (\omega _1,\ldots ,\omega _n)(\omega _0) - (\mathsf{ev}_0^*\unicode {x03BE})_n (\omega _1,\ldots ,\omega _n)(\omega _0). \end{aligned} \end{align*}
Conversely, the motivated reader may check that the value of (13) on pure tensors
$\omega _i$
is equal to
\begin{align*} \begin{aligned} &(\unicode {x03BC}_\Delta ^\vee \circ \overline {\unicode {x03B6}} - (-1)^{|\unicode {x03B6}|} \unicode {x03B6} \circ \widetilde {\unicode {x03BC}})(\omega _1,\ldots ,\omega _n)(\omega _{n+1}) \\[5pt] &=\quad \sum _{j=1}^{n} (-1)^{|\unicode {x03BE}|+|b_1|+\cdots +|b_{j-1}|} \cdot \int _0^1 x_1\cdots y_j \cdots x_n {\rm d} t \cdot {\bf b}(\unicode {x03BE})(b_1,\ldots ,b_n)(b_{n+1}), \end{aligned} \end{align*}
which always vanishes because
$\unicode {x03BE}$
is assumed to be a cocycle. We conclude that
To see that the same is true for the cyclic classes, it suffices to show that
$\unicode {x03B6}$
is cyclic whenever
$\unicode {x03BE}$
is cyclic. If
$\unicode {x03BE}$
is cyclic, then given homogeneous pure tensors
$\omega _i$
with
$\omega _j = y_j {\rm d} t \otimes b_j$
for some fixed
$j\leqslant n$
and
$\omega _i = x_i \otimes b_i$
for all
$i\neq j$
, we have
\begin{align*} \begin{aligned} &\zeta _n(\omega _{n+1},\omega _1,\ldots ,\omega _{n-1})(\omega _n) \\[5pt] &\quad = (-1)^{|\unicode {x03BE}|+|b_{n+1}| + |b_1|+\cdots +|b_{j-1}|} \int _0^1 x_1\cdots y_j \cdots x_{n+1} {\rm d} t \cdot \xi _n(b_{n+1},b_1,\ldots ,b_{n-1})(b_n) \\[5pt] &\quad = (-1)^{|b_{n+1}| + |b_1|+\cdots +|b_{j-1}| + |b_{n+1}|(|b_1|+\cdots +|b_n|)} \int _0^1 x_1\cdots y_j \cdots x_{n+1} {\rm d} t \cdot \xi _n(b_1,\ldots ,b_n)(b_{n+1}) \\[5pt] &\quad = (-1)^{|b_{n+1}|(|b_1|+\cdots +(|b_j|+1)+\cdots +|b_n|)}\unicode {x03B6}(\omega _1,\ldots ,\omega _n)(\omega _{n+1}) \\[5pt] &\quad = (-1)^{|\omega _{n+1}|(|\omega _1|+\cdots +|\omega _n|)}\unicode {x03B6}(\omega _1,\ldots ,\omega _n)(\omega _{n+1}). \end{aligned} \end{align*}
A similar computation shows that the cyclic identity holds when
$\omega _{n+1} = y_{n+1}{\rm d} t \otimes b_{n+1}$
. This shows that
$\mathsf{ev}_0$
and
$\mathsf{ev}_1$
induce the same classes on Hochschild and negative cyclic cohomology, as claimed.
Corollary 3.7.
For an
$A_\infty$
-algebra
$A$
with minimal model
${\rm H}(A)$
there are isomorphisms
Proof.
The maps induced by the morphisms
$I$
and
$P$
satisfy
$I^*P^* = (P\diamond I)^* = {\rm id}$
, and the existence of a homotopy
$I\diamond P \sim {\rm id}_A$
implies that
$[P^*][I^*] = [(I\diamond P)^*] = [({\rm id}_A)^*] = {\rm id}$
.
3.3 Analytic
$A_\infty$
-bimodules
Given
$A\in {\mathsf{Alg}^{\infty ,{\rm an}}}$
and
$M\in \operatorname {\mathsf{grNMod}}{\ell ^e}$
we consider a family of norms as in § 2.4: for each
$r\gt 0$
we define
where
$m = \sum _{i,j} m_{i,j} \in \mathsf{B}_AM$
is a decomposition into elements
$m_{i,j} \in A[1]^{\otimes i} \otimes M[1] \otimes A[1]^{\otimes j}$
. Boundedness of linear maps out of these normed bar constructions can again be characterised in various ways, analogously to Lemma2.16.
Lemma 3.8.
For
$\unicode {x03C1}\in \mathcal{M}_A(M,N)$
the following are equivalent:
-
(i) there exists
$C\gt 0$
such that
${\left \|\unicode {x03C1}_{i,j}\right \|} \leqslant C^{i+j+1}$
for all
$i,j\in \mathbb{N}$
, -
(ii) there exists
$r\gt 0$
such that
$\unicode {x03C1}\colon \mathsf{B}_A(M,r) \to N[1]$
is bounded, and
-
(iii) for every
$r'\gt 0$
there exists
$r\gt 0$
such that
$\widehat {\unicode {x03C1}} \colon \mathsf{B}_A(M,r) \to \mathsf{B}_A(N,r')$
is bounded.
If, moreover,
$M=N$
, then this is also equivalent to:
-
(iv) for every
$r'\gt 0$
there exists
$r\gt 0$
such that
$\widetilde {\unicode {x03C1}} \colon \mathsf{B}_A(M,r) \to \mathsf{B}_A(M,r')$
is bounded.
Proof.
(i)
$\implies$
(ii). Suppose there exists
$C\gt 0$
such that
${\left \|\unicode {x03C1}_{i,j}\right \|} \leqslant C^{i+j+1}$
for all
$i,j\in \mathbb{N}$
, and fix
$0\lt r\lt C^{-1}$
. Then an element
$m = \sum _{i,j} m_{i,j} \in \mathsf{B}_A(M,r)$
of norm
${\left \|m\right \|}_r=1$
satisfies
${\left \|m_{i,j}\right \|} \leqslant r^{i+j+1}$
for all
$i,j\in \mathbb{N}$
and therefore
Because the power series
$\sum _n n z^{n+1}$
has radius of convergence
$1$
, it converges at
$z = Cr \lt 1$
. In particular, the norm
$\unicode {x03C1}$
is bounded.
(ii)
$\implies$
(i). Let
$K\gt 1$
be a constant bounding the norm of
$\unicode {x03C1}\colon \mathsf{B}_A(M,r) \to N[1]$
and pick
$C \geqslant {K}/{r}$
. Then for all
$i,j\in \mathbb{N}$
and
$m_{i,j}\in A[1]^{\otimes i} \otimes M[1] \otimes A[1]^{\otimes j}$
of norm
${\left \|m_{i,j}\right \|} = 1$
, the map
$\unicode {x03C1}_{i,j}$
satisfies
which shows that, in particular,
${\left \|\unicode {x03C1}_{i,j}\right \|} \leqslant C^{i+j+1}$
.
(i)
$\implies$
(iii). Suppose there exists
$C\gt 1$
such that
${\left \|\unicode {x03C1}_{i,j}\right \|} \leqslant C^{i+j+1}$
for all
$i,j\in \mathbb{N}$
, and fix
$r'\gt 0$
. Then we choose a constant
$q\gt 0$
such that
$ij \lt q^{i+j+1}$
for all
$i,j\in \mathbb{N}$
, a constant
$K=\min \{r',1\}$
, and a radius
$r\lt {K}/{qC}$
. Then for any element
$m = \sum m_{i,j} \in \mathsf{B}_A M$
of norm
${\left \|m\right \|}_r=1$
one has
${\left \|m_{i,j}\right \|} \leqslant r^{i+j+1}$
and hence
\begin{align*} \begin{aligned} {\left \|\widehat {\unicode {x03C1}}(m)\right \|}_{r'} &\leqslant \sum _{i,j\geqslant 0} \sum _{\substack {0\leqslant i\leqslant n\\[5pt] 0\leqslant j\leqslant m}} {\left \|({\rm id}^{\otimes i} \otimes \unicode {x03C1}_{n-i,m-j} \otimes {\rm id}^{\otimes j})(m_{i,j})\right \|} (r')^{-i-j-1} \\[5pt] &\leqslant \sum _{i,j\geqslant 0} \sum _{\substack {0\leqslant i\leqslant n\\[5pt] 0\leqslant j\leqslant m}} C^{i+j-i-j+1} K^{-i-j-1} r^{i+j+1} \\[5pt] &\leqslant \sum _{i,j\geqslant 0} nm \left (\frac {rC}{K}\right )^{i+j+1} \\[5pt] &\leqslant \sum _{N\geqslant 1} (N-1) \left (\frac {rq C}{K}\right )^N .\end{aligned} \end{align*}
Then the norm is bounded by the value of the power series
$\sum _N (N-1) z^N$
at
$z={rqC}/{K} \lt 1$
.
(i)
$\implies$
(iv). This follows in an analogous way to the previous implication. We leave the details up to the reader.
(iii), (iv)
$\implies$
(ii). The projection
$\unicode {x03C0} \colon \mathsf{B}_A(N,r') \to N[1]$
is clearly bounded for any
$r'\gt 0$
, so the boundedness of
$\widehat {\unicode {x03C1}}\colon \mathsf{B}_A(M,r) \to \mathsf{B}_A(N,r')$
implies that
$\unicode {x03C1} = \unicode {x03C0}\circ \widehat {\unicode {x03C1}}$
is bounded. Likewise,
$\unicode {x03C1} = \unicode {x03C0} \circ \widetilde {\unicode {x03C1}}$
is bounded when
$\widetilde {\unicode {x03C1}}\colon \mathsf{B}_A(M,r) \to \mathsf{B}_A(M,r')$
is bounded.
Hence, as in the algebra case we find that the union over the spaces
$\hom _{\ell ^e}^{{\rm cont}}(\mathsf{B}_A(M,r),N[1])$
is given by a graded vector space of double sequences
whose elements we again call analytic. In particular, we obtain a definition of analytic
$A_\infty$
-bimodules over an analytic
$A_\infty$
-algebra.
Definition 3.9. Let
$(A,\unicode {x03BC})$
be an analytic
$A_\infty$
-algebra. Then an analytic
$A$
-bimodule is a pair
$(M,\unicode {x03BD})$
of
$M\in \operatorname {\mathsf{grNMod}}({\ell ^e})$
and
$\unicode {x03BD} \in {\mathcal{A}}_A^1(M,M)$
satisfying
$\widetilde {\unicode {x03BD}}^2=0$
.
Example 3.10. The diagonal bimodule
$A_\Delta$
is analytic for any analytic
$A_\infty$
-algebra when endowed with the induced norm, as
${\left \|\unicode {x03BD}_{\Delta ,i,j}\right \|} = {\left \|\unicode {x03BC}_{i+j+1}\right \|}$
satisfies the appropriate bound.
Example 3.11. The dual bimodule
$A^\vee$
is not analytic in general, as the dual space is not endowed with a natural norm. However, one can consider the continuous dual bimodule
where the components of
$\unicode {x03BD}'_\Delta$
are defined by the same formula as the components of
$\unicode {x03BD}_\Delta ^\vee$
. It is again straightforward to check that
${\left \|\unicode {x03BD}^\vee _{\Delta ,i,j}\right \|} = {\left \|\unicode {x03BC}_{i+j+1}\right \|}$
is bounded by a geometric series. If
$A$
is finite dimensional, then
$A'_\Delta$
is equal to
$A^\vee _\Delta$
in
$\mathsf{Mod}_{A-A}^\infty$
, but in general it is only a submodule.
As before, we call a (pre-)morphism
$\unicode {x03C1} \in \hom _{A-A}^{\bullet }(M,N)$
between
$A$
-bimodules
$(M,\unicode {x03BD}_M)$
and
$(N,\unicode {x03BD}_N)$
analytic if it lies in the subspace
${\mathcal{A}}_A(M,N) \subset \mathcal{M}_A(M,N)$
. It follows from Lemma3.8 that
is a bounded operator on this space, and hence gives rise to a complex of analytic pre-morphisms
which is a subcomplex of
$\hom _{A-A}^\bullet (M,N)$
. As before, we denote the subspace of analytic morphisms by
${{\rm Hom}}_{A-A}^{{\rm an}}(M,N) \subset {{\rm Hom}}_{A-A}(M,N)$
. It follows from Lemma3.8 that the composition of analytic bimodule pre-morphisms is again analytic, and therefore defines morphism complexes for a DG category
$\operatorname {\mathsf{NMod}}^{\infty ,{\rm an}}_{A-A}$
of analytic bimodules over
$A$
.
Given an analytic
$A_\infty$
-morphism
$f$
one can again consider the functor
$f^*$
, and the pullback map
$f^\sharp$
on the Hom-spaces between the diagonal bimodule and its continuous dual.
Lemma 3.12.
Let
$f\in {{\rm Hom}}^{{\rm an}}_{{\mathsf{Alg}^\infty }}(A,B)$
be an analytic morphism. Then there is a well-defined functor
which induces a pullback
$f^*\colon \hom _{B-B}^{{\rm an}}(B_\Delta ,B_\Delta ') \to \hom _{A-A}^{{\rm an}}(A_\Delta ,A_\Delta ')$
.
Proof.
Given
$f \in {{\rm Hom}}^{{\rm an}}_{{\mathsf{Alg}^\infty }}(A,B)$
, for any
$N,M\in \operatorname {\mathsf{grNMod}} {\ell ^e}$
and
$\unicode {x03C1}\in {\mathcal{A}}_B(M,N)$
there exists a common constant
$C\gt 0$
such that
${\left \|f_n\right \|} \lt C^n$
for all
$n\in \mathbb{N}$
and
${\left \|\unicode {x03C1}_{i,j}\right \|} \lt C^{i+j+1}$
for all
$i,j\in \mathbb{N}$
. Then the construction
$f^\sharp \unicode {x03C1}$
has components satisfying
\begin{align*} \begin{aligned} {\left \|(f^\sharp \unicode {x03C1})_{i,j}\right \|} &\leqslant \sum _{\substack {i_1+\cdots +i_n = i\\[5pt] j_1+\cdots +j_n = j}} {\left \|\unicode {x03C1}_{n,m}\right \|} {\left \|f_{i_1}\right \|} \cdots {\left \|f_{i_n}\right \|} {\left \|f_{j_1}\right \|} \cdots {\left \|f_{j_m}\right \|} \\[5pt] &\lt \sum _{\substack {i_1+\cdots +i_n = i\\[5pt] j_1+\cdots +j_n = j}} C^{n+m+i+j+1} \\[5pt] &\leqslant ({\#} \textrm{ of partitions of $i$}) \cdot ({\#} \textrm{ of partitions of $j$})) \cdot C^{2(i+j)+1}. \end{aligned} \end{align*}
Picking some constant
$q\gt 1$
such that
$q^n$
bounds the number of partitions of
$n$
, it follows that
${\left \|(f^\sharp \unicode {x03C1})_{i,j}\right \|} \lt q^{i+j}C^{2(i+j)+1} \leqslant (qC^2)^{i+j+1}$
, which shows that
$f^\sharp \unicode {x03C1} \in {\mathcal{A}}_A(M,N)$
. If follows that
$f^\sharp$
maps every analytic bimodule structure
$\unicode {x03BD}$
to an analytic bimodule structure
$f^\sharp \unicode {x03BD}$
, and an analytic (pre-)morphism
$\unicode {x03C1} \in \hom ^{{\rm an}}_{A-A}(M,N)$
between analytic bimodules to an analytic bimodule map
$f^\sharp \unicode {x03C1}$
. Hence
$f^\sharp$
is a well-defined functor between categories of analytic bimodules.
It follows that
$f^\sharp B_\Delta$
is an analytic bimodule, and it follows directly from the definition that the map
$f_\Delta \colon A \to f^\sharp B_\Delta$
is analytic. The bimodule
$f^\sharp B_\Delta '$
is likewise analytic, and it follows easily that the formula for
$f^\vee _\Delta$
defines an analytic map
$f_\Delta ' \colon f^\sharp B_\Delta ' \to A_\Delta '$
. Hence, if
$\unicode {x03C1} \in \hom _{B-B}^{{\rm an}}(B_\Delta ,B_\Delta ')$
is an analytic bimodule map, the composition
$f^*\unicode {x03C1} = f_\Delta ' \diamond f^\sharp \unicode {x03C1} \diamond f_\Delta$
is again analytic.
3.4 Analytic Hochschild cohomology
Given an analytic
$A_\infty$
-algebra
$(A,\unicode {x03BC})$
and an analytic
$A$
-bimodule
$(M,\unicode {x03BD}) \in \operatorname {\mathsf{NMod}}^{\infty ,{\rm an}}_{A-A}$
, we call a Hochschild cochain
$\unicode {x03BE} \in \mathsf{C}^\bullet (A,M) = (\mathcal{M}(A,M)[-1],{\bf b})$
analytic if it lies in the subspace
${\mathcal{A}}(A,M)[-1] \subset \mathcal{M}(A,M)[-1]$
. This analytic condition can again be characterised in multiple ways.
Lemma 3.13.
Let
$\unicode {x03BE} \in \mathsf{C}^\bullet (A,M)$
. Then the following are equivalent:
-
(i)
$\unicode {x03BE}$
is analytic; and
-
(ii) for every
$r'\gt 0$
there exists
$r\gt 0$
such that
$\overline {\unicode {x03BE}}\colon \mathsf{B}(A,r) \to \mathsf{B}_A(M,r')$
is bounded.
Proof.
The implication (ii)
$\implies$
(i) is obvious, and hence we only check the other implication. Given
$\unicode {x03BE}\in \mathsf{C}^{\bullet ,{\rm an}}(A,M)$
, there exists
$C\gt 1$
such that
${\left \|\xi _n\right \|} \lt C^n$
for all
$n\geqslant 1$
. Fix
$r'\gt 0$
, and let
$r \lt \min \{r',1/C\}$
. Then for every element
$\sum _{n\in \mathbb{N}} a_n \in \mathsf{B}(A,r)$
of norm
${\left \|a\right \|}_r \leqslant 1$
\begin{align*} \begin{aligned} {\left \|\overline {\unicode {x03BE}}(a)\right \|}_{r'} &\leqslant \sum _{i,j,k\geqslant 0} \sum _{k\geqslant 0} {\left \|({\rm id}^i\otimes \underline {\xi _k}\otimes {\rm id}^{\otimes j})(a_{i+k+j})\right \|} (r')^{-i-j-1} \\[5pt] &\leqslant \sum _{i,j\geqslant 0} {\left \|\unicode {x03BE}_0(1)\right \|} {\left \|a_{i+j}\right \|} (r')^{-i-j-1} + \sum _{i,j\geqslant 0}\sum _{k\geqslant 1} C^{i+k+j} {\left \|a_{i+k+j}\right \|} \cdot (r')^{-i-j-1} \\[5pt] &\leqslant {\left \|\unicode {x03BE}_0(1)\right \|}(r')^{-1} \sum _{n\geqslant 0} (n+1) (r/r')^n + (r')^{-1}\sum _{i,j\geqslant 0}\sum _{k\geqslant 1} (Cr)^{k} \cdot (r/r')^{i+j} \\[5pt] &\leqslant \frac {{\left \|\unicode {x03BE}_0(1)\right \|}}{r'(1-(r/r'))^2} + \frac {1}{r'(1-Cr)(1-(r/r'))^2} \lt \infty . \end{aligned} \end{align*}
It follows that the operator
$\overline {\unicode {x03BE}}$
is bounded.
As a corollary, it follows that the differential maps an analytic cochain
$\unicode {x03BE} \in \mathsf{C}^{\bullet ,{\rm an}}(A,M)$
to a cochain
which is bounded as a map
$\mathsf{B}(A,r) \to M$
for some
$r$
, and hence analytic by Lemma2.16. It follows that the analytic cochains form a well-defined subcomplex, which we denote by
For
$M=A_\Delta$
we again abbreviate
$\mathsf{C}^{\bullet ,{\rm an}}(A) := \mathsf{C}^{\bullet ,{\rm an}}(A,A_\Delta )$
. Similarly, we define the analytic version of Connes’ complex as the intersection
which will play the role of the negative cyclic cohomology in the analytic setting.
The analytic Hochschild complex is again functorial in each argument with respect to analytic maps: given
$f\in {{\rm Hom}}_{{\mathsf{Alg}^\infty }}^{{\rm an}}(A,B)$
it follows directly from Lemma2.16 that there is a well-defined map
and likewise for any
$\unicode {x03C1}\in {{\rm Hom}}_{A-A}^{{\rm an}}(M,N)$
it follows from Lemma3.13 that
is well defined. In particular, composition with
$\widehat f$
and
$f'_\Delta$
induces maps
$f^*\colon \mathsf{C}^{\bullet ,{\rm an}}(B,B_\Delta ') \to \mathsf{C}^{\bullet ,{\rm an}}(A,A_\Delta ')$
and
$f^*\colon \mathsf{C}^{\bullet ,{\rm an}}_\lambda (B) \to \mathsf{C}^{\bullet ,{\rm an}}_\lambda (A)$
for any analytic
$A_\infty$
-morphism
$f\in {{\rm Hom}}_{{\mathsf{Alg}^\infty }}^{{\rm an}}(A,B)$
. As before, we have a compatibility with homotopies.
Lemma 3.14.
Let
$f,g\in {{\rm Hom}}_{\mathsf{Alg}^\infty }^{{\rm an}}(A,B)$
with
$f\sim _{{\rm an}} g$
, then
$f$
and
$g$
induce the same morphism on analytic Hochschild cohomology and analytic cyclic cohomology.
Proof.
If
$f\sim _{{\rm an}} g$
then
$f = \mathsf{ev}_0 \circ H$
and
$g=\mathsf{ev}_1\circ H$
for an analytic map
$H\in {{\rm Hom}}_{\mathsf{Alg}^\infty }^{{\rm an}}(A,\Omega ^\bullet _{[0,1]}\otimes B)$
. Hence, as in Proposition3.6, it suffices to show that the analytic maps
$\mathsf{ev}_0$
and
$\mathsf{ev}_1$
induce the same map on the analytic versions of Hochschild/negative cyclic cohomology. For this, it suffices to show that if
$\unicode {x03BE} \in Z^k\mathsf{C}^{\bullet ,{\rm an}}(B,B'_\Delta )$
is an analytic cocycle then the cochain (11) is analytic. However, this is straightforward: for any fixed
$n$
and elements
$\omega _i = \sum _{k_i} (x_i^{k_i} + y_i^{k_i}{\rm d} t) \otimes b^{k_i}_i$
, we have
\begin{align*} \begin{aligned} {\left \|\zeta _n(\omega _1,\ldots ,\omega _n)(\omega _{n+1})\right \|} &\leqslant \sum _{k_1,\ldots ,k_{n+1}}\sum _{j=1}^n \int _0^1 x_1^{k_1}\cdots y_j^{k_j}\cdots x_{n+1}^{k_{n+1}}{\rm d} t \cdot {\left \|\xi _n(b_1,\ldots ,b_n)(b_{n+1})\right \|} \\[5pt] &\leqslant {\left \|\xi _n\right \|} \cdot \sum _{k_1,\ldots ,k_{n+1}} \sum _{j=1}^n {\left \|x_1^{k_1}\right \|}_\infty \cdots {\left \|y_j^{k_j}\right \|}_\infty \cdots {\left \|x_{n+1}^{k_{n+1}}\right \|}_\infty \cdot {\left \|b_1\right \|}\cdots {\left \|b_{n+1}\right \|}. \\[5pt] &\leqslant {\left \|\xi _n\right \|} \cdot \sum _{k_1} {\left \|(x_1^{k_1} + y_1^{k_1}{\rm d} t) \otimes b^{k_1}_1\right \|} \cdots \sum _{k_{n+1}} {\left \|(x_{n+1}^{k_{n+1}} + y_{n+1}^{k_{n+1}}{\rm d} t) \otimes b^{k_{n+1}}_{n+1}\right \|}. \end{aligned} \end{align*}
Taking the infimum over all such decompositions of
$\omega _i$
into pure tensors, we see that
${\left \|\zeta _n\right \|} \leqslant {\left \|\xi _n\right \|}$
, and it follows that
$\unicode {x03B6}$
is again an analytic cochain. Hence
$[\mathsf{ev}_1^*\unicode {x03BE}] = [\mathsf{ev}_0^*\unicode {x03BE}]$
also holds in the analytic versions of the Hochschild and negative cyclic cohomology.
Corollary 3.15.
For every analytic
$A_\infty$
-algebra
$A$
admitting an analytic minimal model
${\rm H}(A)$
there are isomorphisms
${{\rm HH}}^{{\rm an}}(A,A^\vee _\Delta ) \cong {{\rm HH}}^{{\rm an}}({\rm H}(A),{\rm H}(A)^\vee _\Delta )$
and
${\rm HC}^{{\rm an}}_\lambda (A) \cong {\rm HC}^{{\rm an}}_\lambda ({\rm H}(A))$
.
3.5 Analytic inverses for bimodule morphisms
In the remainder of this section we show the analogue of Lemma2.25 for bimodule morphisms: given
$\unicode {x03C1} \in {{\rm Hom}}_{A-A}^{{\rm an}}(M,N)$
such that
$\unicode {x03C1}_{0,0}$
is invertible in
$\operatorname {\mathsf{grNMod}} {\ell ^e}$
, we show that it admits an analytic inverse
$\unicode {x03C4} \in {{\rm Hom}}_{A-A}^{{\rm an}}(N,M)$
. To check the growth condition on
$\unicode {x03C4}$
, we define it explicitly using a tree formula and a special kind of planar tree.

Figure 1. Left: an example of a tree
$T \in \mathsf{Catp}(3,4,2)$
with the root at the bottom. Right: the string diagram for the corresponding map
$\unicode {x03C4}_T \colon A[1]^{\otimes 3} \otimes M[1] \otimes A[1]^{\otimes 4} \to N[1]$
.
Definition 3.16. A caterpillar is a rooted planar tree
$T$
with one of the leaves marked, such that all internal nodes have valency
$\geqslant 3$
and lie on a central path between the root and the marked leaf. The set of caterpillars for which
$n_1$
unmarked leaves lie to the left of this central path and
$n_2$
unmarked leaves lie to the right of the central path is denoted
$\mathsf{Catp}(n_1,n_2)$
. The subset of caterpillars with
$d$
internal nodes is denoted
$\mathsf{Catp}(n_1,n_2,d)$
.
A typical example of a caterpillar tree is given in Figure 1. There is a unique tree
$T\in \mathsf{Catp}(0,0)$
which has
$d=0$
internal nodes. For
$n\gt 1$
one has
$d\gt 1$
and every tree
$T\in \mathsf{Catp}(n_1,n_2,d)$
can be uniquely decomposed into an internal node and a subtree in two ways:

so
$T$
is uniquely determined by a pair of numbers
$(l_1,l_2)$
and a tree
$T_r \in \mathsf{Catp}(n_1-l_1,n_2-l_2,d-1)$
, and also by a pair of numbers
$(r_1,r_2)$
and a tree
$T_l \in \mathsf{Catp}(n_1-r_1,n_2-r_2,d-1)$
. Hence we have bijections
\begin{align*} \begin{aligned} \mathsf{Catp}(n_1,n_2) &\cong \{(l_1,l_2,T_r) \mid l_1+l_2\gt 0,\ T_r \in \mathsf{Catp}(n_1-l_1,n_2-l_2)\} \\[5pt] &\cong \{(T_l,r_1,r_2) \mid r_1+r_2\gt 0,\ T_l \in \mathsf{Catp}(n_1-r_1,n_2-r_2)\}. \end{aligned} \end{align*}
Given
$\unicode {x03C1}\in \hom _{A-A}(M,N)$
and
$\unicode {x03C4}_{0,0} \in \hom _{{\ell ^e}}^{{\rm cont}}(N,M)$
we then define, for every
$T\in \mathsf{Catp}(n_1,n_2)$
, a bimodule pre-morphism as follows. For
$n_1=n_2=0$
we set
$\unicode {x03C4}_T = \unicode {x03C4}_{0,0}$
, and otherwise we define
$\unicode {x03C4}_T$
via the following equivalent recursive formulas:
\begin{equation} \begin{aligned} \unicode {x03C4}_T &= - \unicode {x03C4}_{0,0} \circ \unicode {x03C1}_{l_1,l_2} \circ ({\rm id}^{\otimes l_1} \otimes \underline {\unicode {x03C4}_{T_r}}\otimes {\rm id}^{\otimes l_2})\\[5pt] &= - \unicode {x03C4}_{T_l} \circ ({\rm id}^{\otimes (n_1-r_1)} \otimes \underline {(\unicode {x03C1}_{r_1,r_2}\circ \unicode {x03C4}_{0,0})} \otimes {\rm id}^{\otimes (n_2-r_2)}). \end{aligned} \end{equation}
See again Figure 1 for an example of the map
$\unicode {x03C4}_T$
. If
$\unicode {x03C4}_{0,0}$
is an inverse for
$\unicode {x03C1}_{0,0}$
then the sum of these maps determines an inverse bimodule map.
Lemma 3.17.
Let
$\unicode {x03C1} \in \hom _{A-A}(M,N)$
be a pre-morphism such that
$\unicode {x03C1}_{0,0}$
admits a left-/right-inverse
$\unicode {x03C4}_{0,0}$
. Then
$\unicode {x03C1}$
admits a left-/right-inverse
$\unicode {x03C4} \in \hom _{A-A}(N,M)$
with components
where the maps
$\unicode {x03C4}_T$
are defined as above.
Proof.
Suppose
$\unicode {x03C4}_{0,0}$
is a right-inverse for
$\unicode {x03C1}_{0,0}$
, then we claim that
$\unicode {x03C4}$
is a right-inverse for
$\unicode {x03C1}$
. The base case
$i=j=0$
is trivial as
For
$i+j\gt 0$
it follows from the recursive definition of the maps
$\unicode {x03C4}_T$
that
\begin{align*} \begin{aligned} (\unicode {x03C1}\diamond \unicode {x03C4})_{i,j} &= \unicode {x03C1}_{0,0} \circ \unicode {x03C4}_{i,j} + \sum _{l_1+l_2\gt 0}\sum _{T_r\in \mathsf{Catp}(i-l_1,j-l_2)} \unicode {x03C1}_{l_1,l_2} \circ ({\rm id}^{\otimes l_1} \otimes \unicode {x03C1}_{T_r} \otimes {\rm id}^{\otimes l_2}) \\[5pt] &= \unicode {x03C1}_{0,0} \circ \unicode {x03C4}_{i,j} + \sum _{l_1+l_2\gt 0}\sum _{T_r\in \mathsf{Catp}(i-l_1,j-l_2)} \unicode {x03C1}_{0,0} \circ \unicode {x03C4}_{0,0} \circ \unicode {x03C1}_{l_1,l_2} \circ ({\rm id}^{\otimes l_1} \otimes \unicode {x03C1}_{T_r} \otimes {\rm id}^{\otimes l_2}) \\[5pt] &= \unicode {x03C1}_{0,0} \circ \unicode {x03C4}_{i,j} - \sum _{T \in \mathsf{Catp}(i,j)} \unicode {x03C1}_{0,0} \circ \unicode {x03C4}_{T} = 0, \end{aligned} \end{align*}
where the final line uses the bijection between trees in
$\mathsf{Catp}(i,j)$
and triples
$(l_1,l_2,T_r)$
discussed above. It follows that
$\unicode {x03C1}\diamond \unicode {x03C4} = {\rm id}$
, so
$\unicode {x03C4}$
is a right-inverse. The case where
$\unicode {x03C4}_{0,0}$
is a left-inverse is similar, using the other decomposition into triples
$(T_l,r_1,r_2)$
. In particular,
$\unicode {x03C4}$
is a two-sided inverse if
$\unicode {x03C4}_{0,0}$
is.
We remark that if
$\unicode {x03C1}$
is a morphism and
$\unicode {x03C4}=\unicode {x03C1}^{-1}$
is a two-sided inverse, then the latter is again a morphism by the equality
We claim that the map
$\unicode {x03C4}$
is, moreover, analytic when
$\unicode {x03C1}$
is analytic.
Proposition 3.18.
Let
$\unicode {x03C1} \in \hom _{A-A}^{{\rm an}}(M,N)$
be an analytic pre-morphism, and suppose that
$\unicode {x03C1}_{0,0}$
admits a continuous left-/right-inverse
$\unicode {x03C4}_{0,0}$
. Then
$\unicode {x03C1}$
admits an analytic left-/right-inverse.
Proof.
Because
$\unicode {x03C1}$
is analytic and
$\unicode {x03C4}_{0,0}$
is continuous, there exists
$C\gt 0$
such that
${\left \|\unicode {x03C4}_{0,0}\right \|} \lt C$
and
${\left \|\unicode {x03C1}_{i,j}\right \|} \lt C^{i+j+1}$
for all
$i,j\in \mathbb{N}$
. We claim that for
$T\in \mathsf{Catp}(n_1,n_2,d)$
the map
$\unicode {x03C4}_T$
satisfies
${\left \|\unicode {x03C4}_T\right \|} \lt C^{n_1+n_2+2d+1}$
. For
$n_1=n_2=0$
and
$d=0$
one has
Now let
$n_1,n_2$
and
$d\gt 0$
be arbitrary, then assuming the bound holds for all
$d' \lt d$
it follows by the recursive formula that there exists
$(l_1,l_2)$
and a tree
$T_r\in \mathsf{Catp}(n_1-l_1,n_2-l_2,d-1)$
such that
As the number of internal nodes satisfies
$d\leqslant i+j$
, it follows that
${\left \|\unicode {x03C4}_T\right \|} \lt C^{3(i+j)+3}$
for
$i+j\gt 0$
. Hence, taking the sum over all trees in
$\mathsf{Catp}(i,j)$
one finds that
Each
$T\in \mathsf{Catp}(i,j)$
corresponds to a unique planar tree with less than
$3(i+j)+3$
total nodes, so the cardinality of the set
$\mathsf{Catp}(i,j)$
is clearly bounded by the Catalan number
$\mathcal{C}_{3(i+j)+3}$
. Taking again a constant
$q\gt 1$
such that
$\mathcal{C}_n \lt q^n$
for
$n\gg 0$
, it follows that
${\left \|\unicode {x03C4}_{i,j}\right \|} \lt (qC)^{i+j+1}$
for
$i+j\gg 0$
. Hence
$\unicode {x03C4}$
is analytic.
4. Cyclic structures and analytic Calabi–Yau structures
The notion of a cyclic structure on an
$A_\infty$
-algebra was introduced in [Reference KajiuraKaj07, Reference Kontsevich and SoibelmanKS09]. A cyclic structure is defined as a non-degenerate skew-symmetric pairing
$\langle -,-\rangle \colon A[1] \otimes A[1] \to \ell [2-d]$
satisfying the condition
where
$K = |a_1|(|a_2|+\ldots +|a_n|)$
is a Koszul sign. In particular, a cyclic
$A_\infty$
-algebra is always finite dimensional. In practice, it is easier to work with the following alternative characterisation of a cyclic structure as a bimodule map [Reference TradlerTra08, Reference ChoCho08].
Definition 4.1. A
$d$
-cyclic structure on
$A\in {\mathsf{Alg}^\infty }$
is a morphism
$\unicode {x03C3} \in {{\rm Hom}}_{A-A}(A_\Delta ,A_\Delta ^\vee [-d])$
such that
$\unicode {x03C3}_{0,0}\colon A_\Delta [1] \to A_\Delta [1-d]$
is a skew-symmetric isomorphism and
$\unicode {x03C3}_{i,j} = 0$
for
$i+j \gt 0$
.
A pair
$(A,\unicode {x03C3}_A)$
of an
$A_\infty$
-algebra and a cyclic
$A_\infty$
-structure is called a cyclic
$A_\infty$
-algebra, and, given two such cyclic
$A_\infty$
-algebras
$(A,\unicode {x03C3}_A)$
and
$(B,\unicode {x03C3}_B)$
, a morphism
$f\in {{\rm Hom}}_{{\mathsf{Alg}^\infty }}(A,B)$
is said to be cyclic precisely if
$f^* \unicode {x03C3}_B = \unicode {x03C3}_A$
.
A case of special interest is when
$A$
is
$d$
-cyclic for
$d=3$
, and
$A^0 \cong \ell$
. In this case, the structure of the cyclic
$A_\infty$
-algebra
$(A,\unicode {x03C3}_A)$
can be recovered from a potential: setting
$V_A = (A^1)^*$
, the cyclic structure defines an element
in the completed tensor algebra
$\widehat {\mathsf{T}}_\ell V_A := \prod _{n\geqslant 0} V_A^{\otimes n}$
on
$V_A$
, which can be used to recover the
$A_\infty$
-structure (see e.g. [Reference Van den BerghVdB15]). Likewise, given an
$\ell$
-bimodule
$V$
and an element
$W = \sum _n W_n \in \widehat {\mathsf{T}}_\ell V$
such that each
$W_n$
is invariant under cyclic permutation, there is a well-defined cyclic
$A_\infty$
-algebra structure on
Any morphism
$f\in {{\rm Hom}}_{{\mathsf{Alg}^\infty }}(A,B)$
induces a graded algebra morphism
$f^* \colon \widehat {\mathsf{T}}_\ell V_B \to \widehat {\mathsf{T}}_\ell V_A$
, and if such a morphism is cyclic then
$f^*(W_B) = W_A$
by [Reference KajiuraKaj07, Proposition 4.16].
In this section we consider cyclic analytic
$A_\infty$
-algebras, by which we mean pairs
$(A,\unicode {x03C3}_A)$
with
$A\in {\mathsf{Alg}^{\infty ,{\rm an}}}$
and
$\unicode {x03C3}_A$
a cyclic structure in the above sense. In the case of
$d=3$
the analytic requirement yields an analytic potential in the sense of [Reference Hua and KellerHK19].
Proposition 4.2.
Let
$(A,\unicode {x03C3})$
be a 3-cyclic analytic
$A_\infty$
-algebra with
$A^0 \cong \ell$
, and pick a basis
$v_1,\ldots v_m$
for
$V_A$
. Then the potential
$W_A$
lies in the analytic subring
\begin{align*} \widetilde {\mathsf{T}}_\ell V_A := \left \{\sum _{n=0}^\infty \sum _{i_1,\ldots ,i_n} c_{i_1,\ldots ,i_n} \cdot v_{i_1}\otimes \ldots \otimes v_{i_n} \in \widehat {\mathsf{T}}_\ell V_A \ \middle |\ \begin{gathered} \textit{there exists}\; C\gt 0\; \textit{such that} \\[5pt] |c_{i_1,\ldots ,i_n}| \lt C^n \;\textit{for all}\; i_1,\ldots ,i_n \end{gathered} \right \}. \end{align*}
Proof.
Let
$a_1,\ldots ,a_m \in A^1$
be a dual basis to
$v_1,\ldots ,v_m \in V_A = (A^1)^*$
with
${\left \|a_i\right \|} \leqslant 1$
. Then the coefficient
$c_{i_1,\ldots ,i_n}$
of
$W_A$
in
$\widehat {\mathsf{T}}_\ell V_A$
is given by
$c_{i_1,\ldots ,i_n} =1/{n+1} \unicode {x03C3}(\unicode {x03BC}_{n-1}(a_{i_1},\ldots ,a_{i_{n-1}}))(a_{i_n})$
. Because
$\unicode {x03BC}$
is analytic by assumption, there exists
$C_0 \gt 1$
such that
${\left \|\unicode {x03C3}\right \|} \lt C_0$
and
${\left \|\unicode {x03BC}_n\right \|} \lt C_0^n$
for all
$n\geqslant 1$
. It follows that there is a bound for all
$i_1,\ldots ,i_n$
:
Therefore if we set
$C = C_0$
, the result follows.
Remark 4.3. Hua and Keller [Reference Hua and KellerHK19] use the language of quivers to define their potential. Here the base is a product
$\ell = \prod _{v\in Q_0} {\mathbb{C}} v$
over the nodes of a quiver
$Q$
, and the
$\ell$
-bimodule
$V$
should be seen as the span of the arrows in
$Q$
. This identifies
$\widehat {\mathsf{T}}_\ell V$
with the completed path algebra
$\widehat {{\mathbb{C}} Q}$
, and identifies the subring
$\widetilde {\mathsf{T}}_\ell V_A$
with the analytic path algebra
$\widetilde {{\mathbb{C}} Q} \subset \widehat {{\mathbb{C}} Q}$
in [Reference Hua and KellerHK19, § 3.3].
In the rest of this section we will show how to obtain a cyclic structure on analytic minimal models of analytic
$A_\infty$
-algebras that satisfy a Calabi–Yau property. This requires us to consider a ‘homotopic’ generalisation of cyclic structures, called a strong homotopy inner product.
4.1 Strong homotopy inner products
If
$\unicode {x03C3}$
is a cyclic structure on an
$A_\infty$
-algebra
$B$
then the pullback
$f^*\unicode {x03C3}$
along a quasi-morphism
$f\in {{\rm Hom}}_{{\mathsf{Alg}^\infty }}(A,B)$
will, in general, not be a cyclic structure on
$A$
because both the condition
and the requirement that
$(f^*\unicode {x03C3})_{0,0}$
is an isomorphism may be violated; one says that cyclic structures are strict. For this reason it is better to use a homotopy-invariant alternative which relaxes the cyclic conditions. One such alternative was define by Cho [Reference ChoCho08], and we recall it here following the setup of [Reference Amorim and TuAT25].
Definition 4.4. Given
$A \in {\mathsf{Alg}^\infty }$
, a closed 2-form is an element of the subcomplex
$\Omega ^{2,{\rm cl}}(A)\subset \hom _{A-A}^\bullet (A_\Delta ,A_\Delta ^\vee )[-2]$
of shifts of bimodule morphisms
$\unicode {x03C1}$
satisfying:
-
• skew-symmetry: for any
$i,j\in \mathbb{N}$
and
$a_0\otimes \cdots \otimes a_{i+j+1} \in (A[1])^{\otimes i+j+1}$
the relationholds, where
\begin{align*} \unicode {x03C1}(a_1\otimes \cdots \otimes \underline a_{i+1}\otimes \cdots \otimes a_n)(a_0) = (-1)^{K} \unicode {x03C1}(a_{i+2}\otimes \cdots \otimes \underline a_0\otimes \cdots \otimes a_i)(a_{i+1}) \end{align*}
$K$
is obtained from the Koszul sign rule after cyclic permutation; and
-
• closedness: for any
$a_0\otimes \cdots \otimes a_n \in (A[1])^{\otimes n}$
and indices
$1\leqslant i \lt j \lt k \leqslant n$
the relationholds, where
\begin{align*} \begin{aligned} (-1)^{K_i}\unicode {x03C1}(a_{j+1}\otimes \cdots \otimes \underline a_i\otimes \cdots \otimes a_{j-1})(a_j) &+ (-1)^{K_j}\unicode {x03C1}(a_{k+1}\otimes \cdots \otimes \underline a_j\otimes \cdots \otimes a_{k-1})(a_k) \\[5pt] &+ (-1)^{K_k}\unicode {x03C1}(a_{i+1}\otimes \cdots \otimes \underline a_k\otimes \cdots \otimes a_{i-1})(a_i)=0 \end{aligned} \end{align*}
$K_i,K_j,K_k$
are obtained from the Koszul sign rule after cyclic permutation.
Definition 4.5. A strong homotopy inner product (SHIP) of degree
$2-d$
is a cocycle
$\unicode {x03C1}\in Z^{2-d}\Omega ^{2,{\rm cl}}(A)$
for which the map
$\unicode {x03C1}_{0,0} \colon A_\Delta [1] \to A_\Delta ^\vee [1-d]$
is a quasi-isomorphism.
Any cyclic structure defines a SHIP, but the latter class is much better behaved under
$A_\infty$
-morphisms: given
$f\in {{\rm Hom}}_{{\mathsf{Alg}^\infty }}(A,B)$
the pullback
$f^*$
on bimodule morphisms restricts to a chain map
which maps SHIPs to SHIPs when
$f$
is a quasi-isomorphism. Following the philosophy of [Reference Kontsevich and SoibelmanKS09], a SHIP can be viewed as a type of noncommutative shifted-symplectic structure: one can view the Hochschild cohomologies
$\mathsf{C}^\bullet (A)$
and
$\mathsf{C}^\bullet (A,A^\vee )$
as vector fields and differential 1-forms on a noncommutative space, and any cocycle
$\unicode {x03C1} \in \Omega ^{2,{\rm cl}}(A)$
defines a contraction map
which is a quasi-isomorphism if
$\unicode {x03C1}$
is a SHIP. We now generalise the notion of strong homotopy inner products to analytic
$A_\infty$
-algebras, as follows.
For an analytic
$A_\infty$
-algebra
$A\in {\mathsf{Alg}^{\infty ,{\rm an}}}$
, we define the complex of analytic closed 2-forms
where we view
${\mathcal{A}}(A_\Delta ,A_\Delta ')$
as a subspace of
$\mathcal{M}(A_\Delta ,A_\Delta ^\vee )$
via the inclusion
$A_\Delta ' \hookrightarrow A_\Delta ^\vee$
. The assignment
$A\mapsto \Omega ^{2,{\rm cl},{\rm an}}(A)$
is again functorial, as Lemma3.12 guarantees that there is a chain map
for every analytic
$A_\infty$
-morphism
$f\in {{\rm Hom}}_{{\mathsf{Alg}^\infty }}^{{\rm an}}(A,B)$
. We define the following analogue of a SHIP for an analytic
$A_\infty$
-algebra admitting an analytic minimal model.
Definition 4.6. Let
$A$
be an analytic
$A_\infty$
-algebra
$A$
with minimal model
${\rm H}(A)$
. Then an analytic SHIP is a cocycle
$\unicode {x03C1}\in \Omega ^{2,{\rm cl},{\rm an}}(A)$
such that the map
admits a continuous inverse.
As before, an analytic SHIP can be thought of as a noncommutative shifted-symplectic structure with contraction map
which is well defined by the discussion in § 3.4. If
${\rm H}(A)$
is a strong minimal model, one can again show that this map is a quasi-isomorphism. In what follows, we consider finite dimensional minimal
$A_\infty$
-algebras, for which it suffices that
$\unicode {x03C1}_{0,0}$
is invertible and the contraction map is an isomorphism.
Proposition 4.7.
Suppose
$A$
is a finite dimensional minimal
$A_\infty$
-algebra and
$\unicode {x03C1}\in \Omega ^{2,{\rm cl},{\rm an}}(A)$
is a cocycle with
$\unicode {x03C1}_{0,0}$
invertible in
$\operatorname {\mathsf{grMod}}{\ell ^e}$
. Then
$\unicode {x03C1}$
is an analytic SHIP and
$\iota _-\unicode {x03C1}$
is an isomorphism.
Proof.
Continuity of
$\unicode {x03C1}_{0,0}^{-1}$
is automatic if
$A$
is finite dimensional, and hence
$\unicode {x03C1}$
is an analytic SHIP. It then follows from Proposition3.18 that
$\unicode {x03C1}$
admits an analytic inverse
$\unicode {x03C4} \in {{\rm Hom}}_{A-A}^{{\rm an}}(A'_\Delta ,A_\Delta )$
, and the induced map
is then inverse to the contraction map by bi-functoriality of the Hochschild cochain complex.
4.2 An analytic Darboux lemma
Kontsevich and Soibelman [Reference Kontsevich and SoibelmanKS09] showed that, when interpreted in the language of noncommutative symplectic geometry, any SHIP can be put into a standard Darboux form. In the algebraic setup we use here, this means that any SHIP
$\unicode {x03C1}\in \Omega ^{2,{\rm cl}}(A)$
on a minimal
$A_\infty$
-algebra
$A = (A^\bullet ,\unicode {x03BC})$
can be strictified to a genuine cyclic structure
where
$A^{{\rm pert}} = (A^\bullet ,\unicode {x03BC}^{{\rm pert}})$
is a perturbation of the
$A_\infty$
-structure and
$f\in {{\rm Hom}}_{{\mathsf{Alg}^\infty }}(A^{{\rm pert}},A)$
is an
$A_\infty$
-morphism with first order term
$f_1 = {\rm id}_A$
. A Darboux lemma of this form was first shown by Cho and Lee [Reference Cho and LeeCL11]. More recently, Amorim and Tu [Reference Amorim and TuAT25, Lemma 2.33] have shown that the morphism
$f$
can be obtained as
$f=f^1$
from a solution of a differential equation
\begin{equation} \left \{ \begin{aligned} \frac {{\rm d}}{{\rm d} t} f^t &= \unicode {x03B1}^t \diamond f^t\\[5pt] f^0 &= {\rm id}, \end{aligned} \right . \end{equation}
where
$t\mapsto \unicode {x03B1}^t$
is a certain one-parameter family of Hochschild cocycles interpolating between
$\unicode {x03C1}$
and
$\unicode {x03C3}$
, chosen such that the solution satisfies
$f^1 = f$
. In what follows we give an analytic version of this result using an explicit tree expression for the solution.
Fix a finite dimensional minimal
$A \in {\mathsf{Alg}^{\infty ,{\rm an}}}$
and let
$\unicode {x03B1} \in \mathcal{M}(A,A\otimes \mathsf{PC}^\infty ([0,1]))[-1]$
be a continuous family of Hochschild cochains
$\unicode {x03B1}^t \in \mathsf{C}_\bullet (A)$
. Then we define, for every
$T\in \mathcal{O}(n)$
, a continuous family
as follows. The unique tree
$T\in \mathcal{O}(1)$
determines the constant map
$f_T^t = {\rm id}_{A[1]}$
, and for
$T\in \mathcal{O}(n)$
with
$n\gt 1$
the map
$f_T$
is given by the recursive formula
where
$(T_1,\ldots ,T_k)$
are the subtrees emanating from the first internal node, as in Lemma2.25. The following lemma shows that this yields a solution for the differential equation of [Reference Amorim and TuAT25, Lemma 2.33].
Lemma 4.8.
Suppose
$\unicode {x03B1}^t_0 = \unicode {x03B1}^t_1=0$
. Then the family
$f \in \overline {\mathcal{M}}(A,A\otimes \mathsf{PC}^\infty ([0,1]))$
defined by
is a solution to the differential equation (15).
Proof.
For
$t=0$
we have
$f^0_T = {\rm id}_{A[1]}$
for the unique tree
$T\in \mathcal{O}(1)$
and
$f_T^0=0$
for
$T\in \mathcal{O}(n)$
with
$n\gt 1$
, as the latter are given by an empty integral. Hence
$f$
satisfies the initial condition
$f^0 = {\rm id}$
in (15) and it just remains to check that it satisfies the differential equation
\begin{align} \frac {{\rm d}}{{\rm d} t} f^t_n = (\unicode {x03B1}^t\diamond f^t)_n := \sum _{k=1}^n \sum _{n_1+\cdots +n_k = n} \unicode {x03B1}_k^t \circ (f_{n_1} \otimes \cdots \otimes f_{n_k}). \end{align}
Applying the recursive formula for
$f_T$
it follows that
\begin{align*} \begin{aligned} \frac {{\rm d}}{{\rm d} t} f^t_n &= \sum _{T\in \mathcal{O}(n)} \frac {{\rm d}}{{\rm d} t} f_T^t \\[5pt] &= \sum _{k=2}^{n} \sum _{n_1+\cdots + n_k = n} \sum _{T_i\in \mathcal{O}(n_i)} \unicode {x03B1}_k^t \circ (f_{T_1}^t \otimes \cdots \otimes f_{T_k}^t) \\[5pt] &= \sum _{k=2}^n\sum _{n_1+\cdots + n_k = n} \unicode {x03B1}_k^t \circ \left (\left (\sum _{T_1\in \mathcal{O}(n_1)} f_{T_1}^t\right ) \otimes \cdots \otimes \left (\sum _{T_k\in \mathcal{O}(n_k)} f_{T_k}^t\right )\right ) \\[5pt] &= \sum _{k=2}^n\sum _{n_1+\cdots + n_k = n} \unicode {x03B1}_k^t \circ (f_{n_1} \otimes \cdots \otimes f_{n_k}), \end{aligned} \end{align*}
which is equal to (16) under the assumption
$\unicode {x03B1}^t_1=0$
. Hence
$f$
is a solution to (15) as claimed.
Let
$\mathsf{PC}^\infty ([0,1])$
again be endowed with the essential supremum norm. Then a continuous pre-morphism
$f\in \mathcal{M}(A,A\otimes \mathsf{PC}^\infty ([0,1])$
is analytic if and only if there exists
$C\gt 0$
such that, for all
$n\geqslant 1$
,
where
${{\left \|\cdot \right \|}}_\infty$
denotes the supremum of the operator norms
$\left \|f_n^t\right \|$
for
$t\in [0,1]$
. We can use this to prove the following.
Lemma 4.9.
In the situation of Theorem
4.8
, suppose that
$\unicode {x03B1}$
is analytic. Then
$f$
is also analytic.
Proof.
Let
$C\gt 0$
be such that
${\left \|\unicode {x03B1}_n\right \|}_\infty \lt C^n$
for all
$n\in \mathbb{N}$
. We will show that
${\left \|f_T\right \|}_\infty \leqslant C^{n+d-1}$
holds for each
$T \in \mathcal{O}(n,d)$
by induction over
$n$
. For the unique tree
$T \in \mathcal{O}(1) = \mathcal{O}(1,0)$
we have
which establishes the base case. For the induction step let
$n\gt 1$
and assume the statement holds for all
$T\in \mathcal{O}(m,d)$
with
$m\lt n$
. Then
$T\in \mathcal{O}(n,d)$
is built out of
$l\geqslant 2$
subtrees
$T_1,\ldots ,T_l\subset T$
with
$T_i \in \mathcal{O}(n_i,d_i)$
satisfying
$n_i\neq 0$
,
$\sum n_i = n$
, and
$\sum _{i=1}^k d_i = d-1$
. Then, because each
$n_i$
is less than
$n$
, it follows by the induction hypothesis that
\begin{align*} \begin{aligned} {\left \|f_T\right \|}_\infty &= \sup _{t\in [0,1]}{\left \|\int _0^t \unicode {x03B1}^{\unicode {x03C4}}_k \circ (f_{T_1}^{\unicode {x03C4}} \otimes \cdots \otimes f_{T_l}^{\unicode {x03C4}}) {\rm d} \unicode {x03C4}\right \|} \\[5pt] &\leqslant \sup _{\unicode {x03C4} \in [0,1]} {\left \|\unicode {x03B1}^{\unicode {x03C4}}_k\right \|} {\left \|f_{T_1}^{\unicode {x03C4}}\right \|} \cdots {\left \| f_{T_k}^{\unicode {x03C4}} \right \|} \\[5pt] &\leqslant {\left \|\unicode {x03B1}_k\right \|}_\infty {\left \|f_{T_1}\right \|}_\infty \cdots {\left \|f_{T_k}\right \|}_\infty \\[5pt] &\leqslant C^k\cdot C^{n_1+d_1-1} \cdots C^{n_k+d_k-1} = C^{n+d-1} \end{aligned} \end{align*}
which verifies the induction. Because the valency of every internal node of a tree in
$\mathcal{O}(n)$
is at least
$3$
, one easily verifies that the maximal number of internal nodes is
$d\leqslant n$
. Hence, the sum over all trees is bounded by
where
$|\mathcal{O}(n)|$
denotes the cardinality of
$\mathcal{O}(n)$
, which is bounded by the Catalan number
$\mathcal{C}_{2n}$
. These Catalan numbers are bounded by
$q^n$
for some fixed
$q\gt 0$
, so we obtain a bound
which shows that
$f$
is uniformly analytic.
Using the above and the results of the previous section, we arrive at an analytic generalisation of the Darboux lemma appearing in [Reference Kontsevich and SoibelmanKS08, Reference Cho and LeeCL11, Reference Amorim and TuAT25].
Lemma 4.10 (Analytic Darboux). Let
$A \in {\mathsf{Alg}^{\infty ,{\rm an}}}$
be minimal and finite dimensional, and suppose that
$\unicode {x03C1} \in \Omega ^{2,{\rm cl},{\rm an}}(A)$
is a SHIP of degree
$2-d$
. Then:
-
(i) there exists an
$A_\infty$
-algebra
$A^{\unicode {x03C1}}$
and an analytic
$A_\infty$
-isomorphism
$f \in {{\rm Hom}}_{{\mathsf{Alg}^\infty }}^{{\rm an}}(A^{\unicode {x03C1}},A)$
such that
is a cyclic structure; and
\begin{align*} \unicode {x03C3}^{\unicode {x03C1}} := f^*\unicode {x03C1} \end{align*}
-
(ii) if
$\unicode {x03C4} \in \Omega ^{2,{\rm cl},{\rm an}}(A)$
is another SHIP such that the image
$\unicode {x03C4} - \unicode {x03C1}$
along the inclusion
$\Omega ^{2,{\rm cl},{\rm an}}(A) \to \Omega ^{2,{\rm cl}}(A)$
is exact, then there is a cyclic analytic
$A_\infty$
-isomorphism
\begin{align*} (A^{\unicode {x03C1}},\unicode {x03C3}^{\unicode {x03C1}}) \cong _{{\rm an},{\rm cyc}} (A^{\unicode {x03C4}},\unicode {x03C3}^{\unicode {x03C4}}). \end{align*}
Effectively, every class in
${\rm H}^{2-d}\Omega ^{2,{\rm cl}}(A)$
admitting an analytic lift defines a cyclic analytic model.
Proof.
(i) Let
$\unicode {x03C3} := \unicode {x03C1}_{0,0}$
and consider, for each
$t\in [0,1]$
, the analytic closed 2-form
Use Lemma4.17 to fix an analytic Hochschild cocycle
$\unicode {x03BE} \in \mathsf{C}^{{\rm an},\bullet }(A,A_\Delta ')$
with image
$S(\unicode {x03BE}) = \unicode {x03C1} - \unicode {x03C3}$
along the surjective map
$S\colon \mathsf{C}^{{\rm an},\bullet }(A,A_\Delta ') \to \Omega ^{2,{\rm cl},{\rm an}}(A)[1]$
. It follows from (20) that
$\unicode {x03BE}_1$
is given on generators by
so
$\unicode {x03BE}_1=0$
, and likewise
$\unicode {x03BE}_0=0$
. Because
$A$
is minimal the component
$\unicode {x03C1}^t_{0,0} = \unicode {x03C1}_{0,0}$
is invertible, and hence
$\unicode {x03C1}^t$
is an isomorphism by Proposition3.18. Hence, for every
$t$
the Hochschild cocycle
$\unicode {x03B1}^t \in \mathsf{C}^{{\rm an},\bullet }(A)$
defined by the equation
satisfies the equation
$\iota _{\unicode {x03B1}^t}\unicode {x03C1}^t = \unicode {x03BE}$
. It is straightforward to verify that the sequence
$\unicode {x03B1} = (\unicode {x03B1}_n)_{n\in \mathbb{N}}$
of functions
$\unicode {x03B1}_n\colon t\mapsto \unicode {x03B1}^t_n$
is in
$\mathcal{M}_{[0,1]}(A,A)$
. Indeed, each component
$\unicode {x03C1}^t_n$
varies linearly in
$t$
, and it is easy to verify from the recursive identity (17) that the function
$t\mapsto (\unicode {x03C1}^t)_n^{-1}$
is a polynomial of degree at most
$n$
in
$t$
. Hence,
$\unicode {x03B1}$
is a well-defined family of Hochschild cocycles, which satisfies
because
$\unicode {x03BE}_1=0$
, and likewise
$\unicode {x03B1}^t_0 = ((\unicode {x03C1}^t)^{-1} \circ \overline {\unicode {x03BE}})_0=0$
by definition. To show that it is analytic we note that for each
$t\in [0,1]$
we have
so that
${\left \|\unicode {x03C1}^t_n\right \|} \lt C_1^n$
for a uniform choice of constant
$C_1\gt 0$
independent of
$t$
. It then follows from the proof of Proposition3.18 that there is a uniform constant
$C_2\gt 0$
such that
${\left \|(\unicode {x03C1}^t)^{-1}_n\right \|} \lt C_2^n$
for all
$t$
, and because
$\unicode {x03BE}$
is analytic there is some
$C_3\gt 0$
bounding the composition
for all
$t$
. Therefore
$\unicode {x03B1} = (\unicode {x03B1}_n)_{n\in \mathbb{N}}$
is uniformly analytic, and it follows from Lemmas4.8 and 4.9 that there exists a uniformly analytic family of pre-morphisms
$f = (f_n)_{n\in \mathbb{N}}$
satisfying the differential equation (15). It then follows from [Reference Amorim and TuAT25, Proposition 2.32] that for each
$t$
the pullback
$(f^t)^* \colon \Omega ^{2,{\rm cl},{\rm an}}(A) \to \Omega ^{2,{\rm cl},{\rm an}}(A)$
satisfies
so, in particular,
$f^1$
pulls back
$\unicode {x03C1}^1 = \unicode {x03C1}$
to the constant 2-form
$(f^1)^*\unicode {x03C1} = \unicode {x03C3}$
. Because
$f_1^1 = {\rm id}$
, the pre-morphism
$f^1_1$
admits an analytic inverse by Lemma2.25. Hence if we define
$A^{\unicode {x03C1}}$
as the
$A_\infty$
-algebra with product defined by the analytic Hochschild cocycle
it follows, as in [Reference Amorim and TuAT25, Proposition 2.32], that
$f^1\in {{\rm Hom}}_{{\mathsf{Alg}^\infty }}^{{\rm an}}(A^{\unicode {x03C1}},A)$
is an isomorphism and
$\unicode {x03C3}^{\unicode {x03C1}} = \unicode {x03C3} = (f^1)^*\unicode {x03C1}$
is a cyclic structure as claimed.
(ii) Now let
$\unicode {x03C4}$
be another analytic SHIP defining a cyclic analytic
$A_\infty$
-algebra
$(A^{\unicode {x03C4}},\unicode {x03C3}^{\unicode {x03C4}})$
, and let
$g \in {{\rm Hom}}_{{\mathsf{Alg}^\infty }}^{{\rm an}}(A^{\unicode {x03C4}},A)$
denote the isomorphism for which
$\unicode {x03C3}^{\unicode {x03C4}} = g^*\unicode {x03C4}$
is cyclic. Suppose that
$\unicode {x03C4} - \unicode {x03C1}$
is exact in the complex
$\Omega ^{2,{\rm cl}}(A)$
, then, as in [Reference Amorim and TuAT25, Lemma 2.33], we note that
$\unicode {x03C4}_{0,0} = \unicode {x03C1}_{0,0}$
, so that for every
$t\in [0,1]$
the analytic closed 2-form
has
$\unicode {x03C1}^t_{0,0} = \unicode {x03C4}_{0,0} = \unicode {x03C1}_{0,0}$
an isomorphism, and is therefore a SHIP. Fixing a cocycle
$\unicode {x03BE} \in \mathsf{C}^{{\rm an},\bullet }(A,A'_\Delta )$
such that
$S(\unicode {x03BE}) = \unicode {x03C1} - \unicode {x03C4}$
as before, there again exists a family of Hochschild cocycles
$\unicode {x03B1}$
which satisfy the equation
$\iota _{\unicode {x03B1}^t}\unicode {x03C1}^t = \unicode {x03BE}$
for each
$t\in [0,1]$
. The norms of
$\unicode {x03C1}^t_n$
are bounded by
$\max \{{\left \|\unicode {x03C4}_n\right \|},{\left \|\unicode {x03C1}_n\right \|}\}$
for all
$t$
, so it again follows that
$\unicode {x03B1}$
is uniformly analytic. Hence there exists a family of pre-morphisms
$h$
with
$h^0 = {\rm id}$
solving the differential equation
Because
$\unicode {x03C1} - \unicode {x03C4}$
is exact in
$\Omega ^{2,{\rm cl}}(A)$
it follows that
$\unicode {x03BE}$
is exact in
$\mathsf{C}^\bullet (A,A^\vee )$
. Therefore [Reference Amorim and TuAT25, Lemma 2.33] implies that the analytic pre-morphism
$h^1$
is an
$A_\infty$
-morphism such that
$(h^1)^*\unicode {x03C4} = \unicode {x03C1}$
and hence lies in
$h^1\in {{\rm Hom}}_{{\mathsf{Alg}^\infty }}^{{\rm an}}(A,A)$
. Now the composition
$g^{-1} \circ h^1 \circ f^1 \in {{\rm Hom}}_{{\mathsf{Alg}^\infty }}^{{\rm an}}(A^{\unicode {x03C4}},A^{\unicode {x03C1}})$
is an analytic
$A_\infty$
-isomorphism satisfying
4.3 Analytic Calabi–Yau structures and SHIPs
Cyclic structures express a type of Calabi–Yau symmetry, which can be formalised using the notion of a right Calabi–Yau structure in the terminology of [Reference Behrend, Bryan and SzendrőiBBS13]. For ordinary
$A_\infty$
-algebras, these structures can be defined as follows.
Definition 4.11. A right
$d$
-Calabi–Yau structure on an
$A_\infty$
-algebra
$A = (A,\unicode {x03BC}) \in {\mathsf{Alg}^\infty }$
is a cocycle
$\unicode {x03D5} \in Z^{-d}\mathsf{C}_\lambda ^\bullet (A)$
for which the map
$A \to A^\vee [-d] \colon a \mapsto \unicode {x03D5}_0(\unicode {x03BC}_2(a,-))$
is a quasi-isomorphism.
It was shown by Cho and Lee [Reference Cho and LeeCL11] (and in [Reference Kontsevich and SoibelmanKS08] in the symplectic language) that right CY structures and SHIPs on an
$A_\infty$
-algebra
$A$
are equivalent notions. More precisely, the two structures are identified up to homotopy by a map
$\Omega ^{2,{\rm cl}}(A)[1] \to \mathsf{C}_\lambda ^\bullet (A)$
. This map can be constructed in two steps.
Proposition 4.12 ([Reference Amorim and TuAT25, Lemma 2.14, Proposition 2.18]). The map
$S\colon \mathsf{C}^\bullet (A,A_\Delta ^\vee ) \to \Omega ^{2,{\rm cl}}(A)[1]$
defined by
defines a chain map fitting into a short exact sequence of cochain complexes

where the first map is the inclusion of the cyclic cochains. Moreover, this short exact sequence is natural over
$A\in {\mathsf{Alg}^\infty }$
along the induced pullbacks on Hochschild cochains and bimodule maps.
The above shows that the map
$S$
induces an isomorphism between
$\Omega ^{2,{\rm cl}}(A)[1]$
and the quotient complex
$\mathsf{C}^\bullet (A,A_\Delta ^\vee )/\mathsf{C}_\lambda ^\bullet (A)$
. As observed by Kontsevich and Soibelman, the latter complex can be related to the negative cyclic complex via the following short exact sequence.
Proposition 4.13 ([Reference Amorim and TuAT25, Proposition 2.22]). There is a short exact sequence of chain complexes

where the maps are the compositions of the norm operator
$(N\unicode {x03BE})_n = (1 + t + \cdots + t^{n})\unicode {x03BE}_n$
and the operator
${\rm id} - t$
via the identification
The short exact sequence is, moreover, natural in
$A\in {\mathsf{Alg}^\infty }$
via the induced maps.
It is well known that the normalised bar complex
$\mathsf{B} A/\ell$
is acyclic if
$A$
is unital, and that the same is true of its dual. Choosing a contracting homotopy
$s\colon (\mathsf{B} A/\ell )^\vee [1] \to (\mathsf{B} A/\ell )^\vee$
, one obtains a quasi-isomorphism
after composing with the inverse of
$S$
. One can show that this map identifies right CY structures with SHIPs, leading to the following statement for unital
$A_\infty$
-algebras.
Proposition 4.14 ([Reference Amorim and TuAT25, Corollary 2.24]). The map
$\Omega ^{2,{\rm cl}}(A)[2] \xrightarrow {\sim } \mathsf{C}_\lambda ^\bullet (A)$
is a quasi-isomorphism, is natural with respect to
$A_\infty$
-morphisms, and identifies right CY structures with SHIPs.
We now want to show a version of the above for analytic
$A_\infty$
-algebras, involving analytic SHIPs and analytic right Calabi–Yau structures, by which we mean the following.
Definition 4.15. Let
$A\in {\mathsf{Alg}^{\infty ,{\rm an}}}$
. Then a right Calabi–Yau structure
$\unicode {x03D5}$
is analytic if it lies in the subcomplex
$\mathsf{C}_\lambda ^{{\rm an},\bullet }(A) \subset \mathsf{C}_\lambda ^{\bullet }(A)$
.
Example 4.16. Let
$(A,D,{{\left \|\cdot \right \|}})$
be a normed DG algebra and
$\unicode {x03BB} \colon A^n \to {\mathbb{C}}$
a
${\left \|\cdot \right \|}$
-bounded linear functional such that
Then the element
$\unicode {x03D5} \in \mathsf{C}_\lambda ^{-n,{\rm an}}(A)$
defined by
$\unicode {x03D5}_0 = \unicode {x03BB}$
and
$\unicode {x03D5}_n=0$
for
$n\gt 0$
is a cocycle, and it is a right
$n$
-Calabi–Yau structure if the cohomology pairing
$([a_1],[a_2]) \mapsto \unicode {x03BB}([a_1\cdot a_2])$
is nondegenerate.
We will show that the map
$\Omega ^{2,{\rm cl}}(A)[2] \to \mathsf{C}_\lambda ^\bullet (A)$
restricts to a map on analytic elements by showing that the short exact sequences (18) and (19) restrict to the relevant analytic subspaces. The analytic version of Proposition4.12 is as follows.
Lemma 4.17.
Let
$A$
be an analytic
$A_\infty$
-algebra. Then the map
$S$
fits into a short exact sequence

which is, moreover, natural with respect to analytic
$A_\infty$
-morphisms
$f\in {{\rm Hom}}_{{\mathsf{Alg}^\infty }}^{{\rm an}}(A,B)$
.
Proof.
By construction,
$\mathsf{C}^{{\rm an},\bullet }_\lambda (A) = \mathsf{C}^{\bullet }_\lambda (A) \cap \mathsf{C}^{{\rm an},\bullet }(A,A_\Delta ')$
is a subcomplex of
$\mathsf{C}^{{\rm an},\bullet }(A,A_\Delta ')$
, and this subcomplex is the kernel of the restriction of
$S$
to
$\mathsf{C}^{{\rm an},\bullet }(A,A_\Delta ')$
by Proposition4.12. Hence it suffices to show that
$S$
restricts to a surjective map
$S\colon \mathsf{C}^{{\rm an},\bullet }(A,A'_\Delta ) \to \Omega ^{2,{\rm cl},{\rm an}}(A)[1]$
.
Suppose
$\unicode {x03D5} \in \mathsf{C}^{\bullet ,an}(A,A_\Delta ')$
, and pick
$C\gt 0$
such that
${\left \|\unicode {x03D5}_n\right \|} \lt C^n$
for all
$n\geqslant 1$
. Then for any element
$a \in A[1]^{\otimes i}\otimes A[1] \otimes A[1]^{\otimes j}$
and any decomposition
$a=\sum _k {\bf x}_k \otimes \underline v_k \otimes {\bf y}_k$
\begin{align*} \begin{aligned} {\left \|(S\unicode {x03D5})_{i,j}(a)\right \|} &\leqslant \sum _k \sup _{{\left \|w\right \|} = 1} {\left \|(S\unicode {x03D5})_{i,j}({\bf x}_k\otimes \underline v_k \otimes {\bf y}_k)(w)\right \|} \\[5pt] &\leqslant \sum _k \sup _{{\left \|w\right \|}=1} \left ({\left \|\unicode {x03D5}_{i+j+1}({\bf x}_k\otimes \underline v_k \otimes {\bf y}_k)(w)\right \|} + {\left \|\unicode {x03D5}_{i+j+1}({\bf y}_k\otimes \underline w \otimes {\bf x}_k)(v_k)\right \|}\right ) \\[5pt] &\leqslant 2{\left \|\unicode {x03D5}_{i+j+1}\right \|}\cdot \sum _k {\left \|{\bf x}_k\right \|} {\left \|v_k\right \|} {\left \|{\bf y}_k\right \|}. \end{aligned} \end{align*}
Taking the infimum over all decompositions of
$a$
, it follows that
${\left \|(S\unicode {x03D5})_{i,j}(a)\right \|} \leqslant 2{\left \|\unicode {x03D5}_{i+j+1}\right \|} \cdot {\left \|a\right \|}$
, so that
${\left \|(S\unicode {x03D5})_{i,j}\right \|} \leqslant 2{\left \|\unicode {x03D5}_{i+j+1}\right \|} \lt (2C)^{i+j+1}$
. It follows by Lemma3.8 that
$S\unicode {x03D5}$
is analytic.
To show the surjectivity of
$S$
we use the mapFootnote
1
$h\colon \Omega ^{2,{\rm cl}}(A)[1] \to \mathsf{C}^\bullet (A,A^\vee )$
defined in [Reference Amorim and TuAT25, Equation 11], which is defined by the equations
\begin{align} (h\unicode {x03C1})(x_1\otimes \cdots \otimes x_n)(x_0) = \sum _{i=1}^n \frac {(-1)^\#}{n+1}\unicode {x03C1}(x_{i+1},\ldots ,x_n,\underline x_0,\ldots ,x_{i-1})(x_i), \end{align}
and which satisfies
$S \circ h = {\rm id}$
. Now suppose
$\unicode {x03C1}\in \Omega ^{2,{\rm cl},an}(A)$
is an analytic closed 2-form, and let
$C\gt 0$
be a constant such that
${\left \|\unicode {x03C1}_{i,j}\right \|} \lt C^{i+j+1}$
for all
$i,j\in \mathbb{N}$
. Then for any element
$a \in A[1]^{\otimes n}$
and decomposition
$a = \sum _k a_{k,1}\otimes \cdots \otimes a_{k,n}$
there is an inequality
\begin{align*} \begin{aligned} {\left \|(h\unicode {x03C1})_n(a)\right \|} &\leqslant \sup _{{\left \|a_0\right \|}=1} \sum _k {\left \|(h\unicode {x03C1})_n(a_{k,1}\otimes \cdots \otimes a_{k,n})(a_0)\right \|} \\[5pt] &\leqslant \frac {1}{n+1} \cdot \sum _k\sum _{i=1}^n\sup _{{\left \|a_0\right \|}=1} {\left \|\unicode {x03C1}_{n-i,i-1}(a_{k,i+1},\ldots ,a_{k,n},\underline a_0,a_{k,1},\ldots ,a_{k,i-1})(a_{k,i})\right \|} \end{aligned} \end{align*}
\begin{align*} \begin{aligned} &\leqslant \frac {1}{n+1} \cdot \sum _{i=1}^n{\left \|\unicode {x03C1}_{n-i,i-1}\right \|} \cdot \sum _k{\left \|a_{k,1}\right \|} \cdots {\left \|a_{k,n}\right \|} \\[5pt] &\lt C^n \cdot \sum _k{\left \|a_{k,1}\right \|} \cdots {\left \|a_{k,n}\right \|}. \end{aligned} \end{align*}
Taking the infimum over all decompositions of
$a$
, it follows that
${\left \|(h\unicode {x03C1})_n(a)\right \|} \leqslant C^n{\left \|a\right \|}$
, which shows that
$h\unicode {x03C1}$
is analytic. Hence
$h$
defines a map
$\Omega ^{2,{\rm cl},{\rm an}}(A)[1] \to \mathsf{C}^\bullet (A,A_\Delta ')$
which satisfies
$S\circ h = {\rm id}$
, showing that
$S$
is surjective.
Finally, if
$f\in {{\rm Hom}}_{{\mathsf{Alg}^\infty }}^{{\rm an}}(A,B)$
is an analytic morphism, it follows from Lemma3.12 and the subsequent discussion that the pullback morphisms
$f^*$
preserve analytic elements, so naturality follows.
Corollary 4.18.
The map
$S$
induces an isomorphism
$\mathsf{C}^{{\rm an},\bullet }(A,A_\Delta ')/ \mathsf{C}^{{\rm an},\bullet }_\lambda (A) \xrightarrow {\sim } \Omega ^{2,{\rm cl},{\rm an}}(A)[1]$
.
For the analytic analogue of Proposition4.13 we note that
$(\mathsf{B} A/\ell )^\vee \cong \mathcal{M}(A,A^\vee )[-2]$
, and define
as the subspace obtained from
${\mathcal{A}}(A,A')[-2]$
via this identification. The following now holds.
Lemma 4.19.
Let
$A$
be an analytic
$A_\infty$
-algebra. Then there is a short exact sequence

which is natural with respect to analytic
$A_\infty$
-morphisms.
Proof.
The operator
${\rm id}-t$
restricts to
${\mathcal{A}}(A,A')[-1] \subset \mathcal{M}(A,A^\vee )[-1]$
and clearly has the set of cyclic analytic elements as its kernel. Hence, it immediately follows that it defines an injective chain map

To see that the norm operator likewise preserves
${\mathcal{A}}(A,A')$
, note that if
$\unicode {x03D5}$
satisfies
${\left \|\unicode {x03D5}_n\right \|} \lt C^n$
then
so that
$N\unicode {x03D5}$
is again analytic. Therefore it follows that
$N$
defines a chain map

It is, moreover, surjective, as every
$\unicode {x03D5}\in \mathsf{C}_\lambda ^{{\rm an},\bullet }(A)$
is the image of
$\sum _n 1/{n+1} \unicode {x03D5}_n \in {\mathcal{A}}(A,A')[-1]$
. To see that the sequence (21) is exact at the middle term, one can consider the inverse operator
which maps an analytic element with
${\left \|\unicode {x03BE}_n\right \|} \lt C^n$
for
$n\geqslant 1$
to an element
$f\unicode {x03BE}$
satisfying
${\left \|(f\unicode {x03BE})_n\right \|} \leqslant {n^2}/{n+1} {\left \|\unicode {x03BE}_n\right \|} \lt (2C)^n$
, which is therefore again analytic. It follows that (21) is a short exact sequence as required. Naturality again follows from the naturality in (21).
To construct the map
$\Omega ^{2,{\rm cl},{\rm an}}(A)[2] \to \mathsf{C}_\lambda ^\bullet (A)$
, it now suffices to find a contracting homotopy for
$(\mathsf{B} A/\ell )^\vee$
which restricts to a contracting homotopy for
$(\mathsf{B} A/\ell )^{\vee ,{\rm an}}$
. For this one can take, for example, the dual of the degeneracy map in [Reference LodayLod92, Proposition-definition 1.1.12], which is given by the formula
where
$1$
is any choice of unit in
$A$
. The following lemma shows that this restricts to analytic elements.
Lemma 4.20.
Let
$A$
be a unital analytic
$A_\infty$
-algebra. Then the degeneracy map restricts to a contracting homotopy
$s\colon (\mathsf{B} A/\ell )^{\vee ,{\rm an}} \to (\mathsf{B} A/\ell )^{\vee ,{\rm an}}[-1]$
.
Proof.
Let
$f = (f_n)_{n\in \mathbb{N}} \in {\mathcal{A}}(A,A')$
be an analytic sequence, and pick
$C\gt 0$
such that
${\left \|f_n\right \|} \lt C^n$
for all
$n\geqslant 1$
. Then the corresponding element
$g\in (\mathsf{B} A/\ell )^\vee$
is the map defined by
$g_n(a_1,\ldots ,a_n) = f_{n-1}(a_1,\ldots ,a_{n-1})(a_n)$
. Hence
and the element
$sf\in {\mathcal{A}}(A,A')$
corresponding to
$sg$
is given by
$(sf)_n(a) = f_{n+1}(1\otimes a)$
. Clearly this now satisfies the bound
and hence
$sf$
is analytic as claimed.
Corollary 4.21.
For a unital analytic
$A_\infty$
-algebra
$A$
there is a natural quasi-isomorphism
which maps analytic SHIPs to analytic right CY structures.
Example 4.22. Let
$(A,\unicode {x03BC})$
be the analytic
$A_\infty$
-algebra obtained from a normed DG algebra with
$\unicode {x03D5}$
an analytic right CY structure obtained from a bounded linear functional
$\unicode {x03BB} \colon A^n \to {\mathbb{C}}$
as in Example 4.16. Then
$\unicode {x03D5}$
is the image of the analytic SHIP
$\unicode {x03C1} \in \Omega ^{2,{\rm cl},{\rm an}}(A)$
defined by
$\unicode {x03C1}_0(a)(b) = \unicode {x03BB}(\unicode {x03BC}_2(a,b))$
and
$\unicode {x03C1}_n=0$
for
$n\gt 0$
: one has
$\unicode {x03C1} = S(\unicode {x03BE})$
for the analytic cocycle
$\unicode {x03BE} \in \mathsf{C}^{{\rm an},\bullet }(A,A'_\Delta )$
with
$\unicode {x03BE}_1(a)(b) = 1/2 \unicode {x03BB}(a\cdot b)$
and
$\unicode {x03BE}_n=0$
otherwise, and this cocycle maps to the Connes cocycle
$(N\circ s\circ ({\rm id} - t) \unicode {x03BE})$
with
and vanishing higher terms. This example appears in the non-analytic case in [Reference Amorim and TuAT25, Example 2.25].
As a result of the corollary, we find that every analytic SHIP is determined, up to homotopy, by an analytic right Calabi–Yau structure. Using the corollary above, we can restate the analytic Darboux lemma in terms of Calabi–Yau structures, which yields our main theorem.
Theorem 4.23.
Suppose
$A \in {\mathsf{Alg}^{\infty ,{\rm an}}}$
is compact and admits a unital analytic minimal model. Then:
-
(i) every analytic right
$d$
-CY structure
$\unicode {x03D5}$
defines a cyclic analytic minimal model
$({\rm H}(A)^{\unicode {x03D5}},\unicode {x03C3}^{\unicode {x03D5}})$
; -
(ii) if
$\unicode {x03D5},\unicode {x03C8}$
are analytic right
$d$
-CY structures such that
$[\unicode {x03C8}] - [\unicode {x03D5}]$
maps to
$0$
in
${\rm HC}_\lambda ^{-d}(A)$
, then there is a cyclic analytic
$A_\infty$
-isomorphism
\begin{align*} ({\rm H}(A)^{\unicode {x03D5}},\unicode {x03C3}^{\unicode {x03D5}}) \cong _{{\rm an},{\rm cyc}} ({\rm H}(A)^{\unicode {x03C8}},\unicode {x03C3}^{\unicode {x03C8}}); \end{align*}
-
(iii) if
$B \in {\mathsf{Alg}^{\infty ,{\rm an}}}$
is also compact with a unital analytic minimal model, and
$g\colon B \to A$
is an analytic quasi-isomorphism, then there is an induced a cyclic analytic
$A_\infty$
-isomorphism
\begin{align*} ({\rm H}(B)^{g^*\unicode {x03D5}},\unicode {x03C3}^{g^*\unicode {x03D5}}) \cong _{{\rm an},{\rm cyc}} ({\rm H}(A)^{\unicode {x03D5}},\unicode {x03C3}^{\unicode {x03D5}}). \end{align*}
Hence, every nondegenerate class in
${\rm HC}_\lambda ^{{\rm an},-d}(A)$
defines a canonical cyclic analytic minimal model.
Proof.
(i) Let
${\rm H}(A)\in {\mathsf{Alg}^{\infty ,{\rm an}}}$
be a finite dimensional analytic minimal model of
$A$
with analytic morphisms
$I$
and
$P$
as in Definition2.24. Given an analytic right CY structure
$\unicode {x03D5}\in \mathsf{C}_\lambda ^{{\rm an},-d}(A)$
, the induced map
$A\to A^\vee [-d]$
induces an isomorphism
${\rm H}(A) \to {\rm H}(A)^\vee [-d]$
, which coincides with the morphism induced by
$I^*\unicode {x03D5} \in \mathsf{C}_\lambda ^{{\rm an},\bullet }({\rm H}(A))$
. Hence,
$I^*\unicode {x03D5}$
is an analytic right CY structure on
${\rm H}(A)$
.
Because
${\rm H}(A)$
is unital, it follows by Corollary4.21 that there exists an analytic strong homotopy inner product
$\unicode {x03C1}^{\unicode {x03D5}} \in Z^{2-d}\Omega ^{2,{\rm cl},{\rm an}}(A)$
with image in
$\mathsf{C}_\lambda ^{{\rm an},-d}(A)$
homotopic to
$I^*\unicode {x03D5}$
. Therefore Lemma4.10 determines a cyclic
$A_\infty$
-algebra
$({\rm H}(A)^{\unicode {x03D5}},\unicode {x03C3}^{\unicode {x03D5}}) = ({\rm H}(A)^{\unicode {x03C1}^{\unicode {x03D5}}},\unicode {x03C3}^{\unicode {x03C1}^{\unicode {x03D5}}})$
and an analytic
$A_\infty$
-isomorphism
$f\in {{\rm Hom}}_{{\mathsf{Alg}^\infty }}^{{\rm an}}({\rm H}(A)^{\unicode {x03D5}},{\rm H}(A))$
such that
$f^*\unicode {x03C1}^{\unicode {x03D5}} = \unicode {x03C3}^{\unicode {x03D5}}$
. Because
${\rm H}(A)$
is finite dimensional, it follows by Lemma2.25 that the map
$f$
is invertible in
$\mathsf{Alg}^{\infty ,{\rm an}}$
, and we obtain a diagram

which exhibits
$({\rm H}(A)^{\unicode {x03D5}},\unicode {x03C3}^{\unicode {x03D5}})$
as a cyclic analytic minimal model of
$A$
.
(ii) Let
$\unicode {x03C8}$
be a second right CY structure, and pick a lift
$\unicode {x03C1}^{\unicode {x03C8}} \in \Omega ^{2,{\rm cl},{\rm an}}({\rm H}(A))$
for
$I^*\unicode {x03C8}$
, yielding a cyclic minimal model
$({\rm H}(A)^{\unicode {x03C8}},\unicode {x03C3}^{\unicode {x03C8}})$
as above. Suppose
$[\unicode {x03D5}] - [\unicode {x03C8}]$
maps to
$0$
in
${\rm HC}_\lambda ^{-d}(A)$
. Then it follows by naturality that
$[I^*\unicode {x03D5}] - [I^*\unicode {x03C8}]$
maps to
$0$
in
${\rm HC}_\lambda ^{-d}({\rm H}(A))$
. Considering the commutative diagram

it is also clear that
$[\unicode {x03C1}^{\unicode {x03D5}}] - [\unicode {x03C1}^{\unicode {x03C8}}]$
maps to
$0$
in
$\Omega ^{2,{\rm cl}}({\rm H}(A))$
. Hence it follows from Lemma4.10 that there is a cyclic analytic
$A_\infty$
-isomorphism
between the minimal models as claimed.
(iii) Let
$B\in {\mathsf{Alg}^{\infty ,{\rm an}}}$
admit a finite dimensional analytic unital minimal model
${\rm H}(B)$
and suppose
$g\colon B \to A$
is an analytic quasi-isomorphism. Then
$g^*\unicode {x03D5} \in \mathsf{C}^{{\rm an},\bullet }_\lambda (B)$
is again right CY and induces a cyclic minimal model
${\rm H}(B)^{g^*\unicode {x03D5}}$
. The map
$g$
induces an analytic
$A_\infty$
-isomorphism
${\rm H}(g)$
fitting into the following commutative diagram.

This implies that the equality
$[I^*(g^*\unicode {x03D5})] = [{\rm H}(g)^*I^*\unicode {x03D5}]$
holds, and therefore
$[{\rm H}(g)^*\unicode {x03C1}^{\unicode {x03D5}}] = [\unicode {x03C1}^{g^*\unicode {x03D5}}]$
for the associated closed 2-forms. It therefore follows from Lemma4.10 that the cyclic minimal model
$(H^{g^*\unicode {x03D5}},\unicode {x03C3}^{g^*\unicode {x03D5}})$
is cyclic-analytic
$A_\infty$
-isomorphic to the cyclic minimal model corresponding to
${\rm H}(g)^*\unicode {x03C1}^{\unicode {x03D5}}$
. The latter is given by
$({\rm H}(A)^{\unicode {x03D5}},\unicode {x03C3}^{\unicode {x03D5}})$
, as the composition
${\rm H}(g)^{-1} \diamond f$
satisfies
Corollary 4.24.
If
$A\in {\mathsf{Alg}^{\infty ,{\rm an}}}$
is compact with a unital analytic minimal model
${\rm H}^0(A) \cong \ell$
, then any analytic 3-CY structure
$\unicode {x03D5}$
determines an analytic potential
in the analytic tensor algebra over
$V = {\rm H}^1(A)^*$
which only depends on
$[\unicode {x03D5}] \in {\rm HC}_\lambda ^{-3}(A)$
up to a change of coordinates
$\widetilde {\mathsf{T}}_\ell V \to \widetilde {\mathsf{T}}_\ell V$
. Moreover, if
$g\colon B \to A$
is an analytic quasi-isomorphism for
$B$
, another such analytic
$A_\infty$
-algebra, then there is an isomorphism
$h\colon \widetilde {\mathsf{T}}_\ell W \to \widetilde {\mathsf{T}}_\ell V$
from the tensor algebra over
$W = {\rm H}^1(B)$
such that
Proof.
Letting
$({\rm H}(A)^{\unicode {x03D5}},\unicode {x03C3}^{\unicode {x03D5}})$
be the cyclic minimal model from Theorem4.23(i) associated to a 3-CY structure
$\unicode {x03D5}$
, it follows from Proposition4.2 that there is an associated analytic potential
$W_A^{\unicode {x03D5}} \in \widetilde {\mathsf{T}}_\ell V$
for
$V= (({\rm H}(A))^1)^* = {\rm H}^1(A)^*$
. If
$\unicode {x03C8}$
is another 3-CY structure with
$[\unicode {x03C8}] = [\unicode {x03D5}]$
then it follows by Theorem4.23(ii) that there is an isomorphism
$f\in {{\rm Hom}}_{{\mathsf{Alg}^\infty }}^{{\rm an}}({\rm H}(A)^{\unicode {x03D5}},{\rm H}(A)^{\unicode {x03C8}})$
which is cyclic. There is an induced algebra isomorphism
$f^*\colon \widehat {\mathsf{T}}_\ell V \to \widehat {\mathsf{T}}_\ell V$
, and it follows, using [Reference KajiuraKaj07, Proposition 4.16], that
Hence it remains to verify that
$f^*$
restricts to a map
$\widetilde {\mathsf{T}}_\ell V \to \widetilde {\mathsf{T}}_\ell V$
of analytic tensor algebras. As in [Reference Hua and KellerHK19, Lemma 3.12], it suffices to show that
$f^*(v) \in \widetilde {\mathsf{T}}_\ell V$
for each
$v \in V$
. Picking a basis
$v_1,\ldots ,v_m \in V$
and letting
$a_1,\ldots ,a_m \in {\rm H}^1(A)$
denote the dual basis, the element
$f^*(v)$
can be written as the power series
Because
$f$
is analytic, it follows that there exists
$C_0 \gt 0$
such that
${\left \|f_n\right \|} \lt C_0^n$
for all
$n\in \mathbb{N}$
,
${\left \|v\right \|} \lt C_0$
, and
${\left \|a_i\right \|} \lt C_0$
for each
$a_i$
. Then for each
$i_1,\ldots ,i_n$
the coefficient satisfies
which shows that
$f^*(v) \in \widetilde {\mathsf{T}}_\ell V$
. It follows that
$W_A^{\unicode {x03D5}}$
and
$W_A^{\unicode {x03C8}}$
are related by an analytic change of coordinates. A similar argument now shows the second statement.
5. Analytic Calabi–Yau structures in geometry
We will now apply our main theorem to a geometric setting: we will consider
$A_\infty$
-algebras which govern the deformations of sheaves on a smooth projective variety. To set the notation, we will write
$X$
for a smooth projective variety of dimension
$n$
, which we interpret as an analytic space, and we will write
$Y$
for an arbitrary complex manifold.
The
$A_\infty$
-algebras arising in this setting are obtained from normed DG algebras, and the corresponding
$A_\infty$
-structures are therefore obtained as in Example2.2 using the canonical shift map
$s\colon A \to A[1]$
.
5.1 The Dolbeault construction
Recall that the sheaf of holomorphic functions
$\mathcal{O}_Y$
on a complex manifold
$Y$
admits a fine resolution via the Dolbeault complex
where
$\mathscr{A}^{\;\,p,q}_X$
is the sheaf of smooth
$(p,q)$
-forms on
$Y$
. The sheaves
$\mathscr{A}^{\;\,p,q}_X$
are acyclic, and hence can be used to compute the sheaf cohomology of
$\mathcal{O}_Y$
via
${\rm H}^i(U,\mathcal{O}_Y) \cong {\rm H}^i(\Gamma (U,\mathscr{A\;\,}_Y^{0,\bullet }),\overline {\partial })$
on any open
$U\subset Y$
. More generally, one can take any bounded complex of locally free
$\mathcal{O}_Y$
-modules
$\mathcal{E} = (\mathcal{E}^\bullet ,\unicode {x03B4})$
on
$Y$
(that is, a perfect complex), and obtain an acyclic resolution of
$\mathcal{E}$
where the differential is given by
$D = \overline {\partial } + \unicode {x03B4}$
. This complex again computes the hypercohomology
${\bf R}\Gamma ^i(U,\mathcal{E}) \cong {\rm H}^i\Gamma (U,\mathscr{A\;\,}_Y^{0,\bullet }(\mathcal{E}))$
on any open
$U\subset Y$
.
The Dolbeault construction can be used to construct a DG enhancement of the derived category
$\mathsf{D}^{{\rm perf}}(Y)$
: for any perfect complexes
$\mathcal{E},\mathcal{F}$
there is a natural isomorphism
so the complex of global sections for
$\mathscr{A\;\,}_Y^{0,\bullet }(\mathcal{H} om(\mathcal{E},\mathcal{F}))$
is a morphism complex between
$\mathcal{E}$
and
$\mathcal{F}$
. The natural composition on
$\mathsf{D}^{{\rm perf}}(Y)$
is given by a wedge product
$\wedge$
, which can be defined in terms of local sections
$f \otimes \unicode {x03BE} \in (\mathcal{H} om^{i_1}(\mathcal{F},\mathcal{G}) \otimes \mathscr{A\;\,}_Y^{0,q})(U)$
and
$g \otimes \unicode {x03B6} \in (\mathcal{H} om^{i_1}(\mathcal{E},\mathcal{F})\otimes \mathscr{A\;\,}_Y^{0,q_2})$
(U) as
This product satisfies the Leibniz rule with respect to
$D$
, and therefore defines a DG enhancement of
$\mathsf{D}^{{\rm perf}}(Y)$
called the Dolbeault enhancement; see, for example, [Reference ToënToë11, § 2.3, Example 9].
To each perfect complex
$\mathcal{E} \in \mathsf{D}^{{\rm perf}}(Y)$
there is associated an endomorphism DGA: the Dolbeault DG algebra
with cohomology
${\rm Ext}^\bullet (\mathcal{E},\mathcal{E})$
. If
$\mathcal{E}$
admits a direct sum decomposition
$\mathcal{E} = \mathcal{E}_1^{\oplus m_1} \oplus \ldots \oplus \mathcal{E}_k^{\oplus m_k}$
then the Dolbeault DG algebra is naturally defined over the base ring
In what follows we will always assume such a splitting is given, and work over the fixed base
$\ell$
.
5.2 Analytic minimal models in the compact setting
Now let
$X$
be (the analytic space associated to) a smooth projective variety and fix a hermitian metric
$\langle -,-\rangle _X \colon \mathscr{A}^{\;\,0,q}_X \otimes \mathscr{A}^{\;\,0,q}_X \to \mathscr{A}^{\;\,0,0}$
. For a perfect complex
$\mathcal{E} = (\mathcal{E}^\bullet ,\unicode {x03B4})$
one can choose a compatible hermitian metric
for each locally free sheaf
$\mathcal{E}^i$
; we will refer to
$\mathcal{E}$
endowed with such a metric as a hermitian perfect complex. Recall (see e.g. [Reference Griffiths and HarrisGH78, Chapter 0, § 6]) that this data determines an
$L^2$
-norm
${{\left \|\cdot \right \|}}_{L^2} \colon \Gamma (X,\mathscr{A\;\,}_X^{0,\bullet }(\mathcal{E})) \to \mathbb{R}$
, which is defined on pure tensors
$\unicode {x03BE} = f \otimes \omega$
with
$f\in \Gamma (X,\mathscr{A}^{\;\,0,0}_X(\mathcal{E}^i))$
and
$\omega \in \Gamma (X,\mathscr{A}^{\;\,0,q})$
by the formula
where
${\rm d} vol_X \in \Gamma (X,\mathscr{A}^{\;\,0,n}_X(\Omega ^n_X))$
is the canonical real volume form on
$X$
. The Sobolev
$(l,2)$
-norm for
$l\in \mathbb{N}$
is defined in terms of the
$L^2$
-norm as
${\left \|\unicode {x03BE}\right \|}_{l,2} := \sum _{k\leqslant l} {\left \|\nabla ^k\unicode {x03BE}\right \|}_{L^2}$
, where the operator
$\nabla$
acts on each locally free sheaf
$\mathcal{E}^i$
as the canonical metric connection.
Given hermitian perfect complexes
$\mathcal{E}$
,
$\mathcal{F}$
, there is an induced hermitian metric on
$\mathcal{H} om(\mathcal{E},\mathcal{F})$
and hence also induced norms
${{\left \|\cdot \right \|}}_{L^2}$
and
${{\left \|\cdot \right \|}}_{l,2}$
on the global sections of its Dolbeault construction. As remarked by Fukaya [Reference Fukaya, Oh, Ohta and OnoFOO+09, § 8.2.5], the operators
$D$
and
$\wedge$
satisfy a bound
if one chooses a sufficiently large
$l \gt 2\dim _{\mathbb{C}} X$
. In particular, the Dolbeault DG algebra
$\mathfrak{g}_{\mathcal{E}}$
of a hermitian perfect complex is naturally an analytic
$A_\infty$
-algebra. It was shown by Tu [Reference TuTu14] and Toda [Reference TodaTod18] that this admits a strong analytic minimal model.
Theorem 5.1 ([Reference TuTu14, Appendix A], [Reference TodaTod18, Lemma 4.1]). The DG algebra
$\mathfrak{g}_{\mathcal{E}}$
admits a minimal model with diagram

such that the
$A_\infty$
-structure
$\unicode {x03BC}$
on
$\mathcal{H}_{\mathcal{E}}$
and the maps
$I$
,
$P$
, and
$Q$
satisfy the bounds
for all
$k\geqslant 1$
and a fixed constant
$C\gt 0$
independent of
$k$
.
At first order, the minimal model is given by Hodge theory:
$\mathcal{H}_{\mathcal{E}}$
is the space of harmonic forms in
$\mathfrak{g}_{\mathcal{E}}$
, with
$I_1$
and
$P_1$
being the inclusion and projection, and
$Q_1$
is defined via the Green operator associated to
$D$
. The higher compositions are all defined via the standard homotopy transfer formula [Reference KadeishviliKad80], which can be expressed via sums over trees [Reference MarklMar06].
If
$X$
is a Calabi–Yau variety, then Polishchuk [Reference PolishchukPol01] showed that the Serre duality pairing pulls back to a cyclic structure on this analytic minimal model. Using the terminology employed in this paper, this can be phrased as follows.
Theorem 5.2 ([Reference PolishchukPol01, Theorem 1.1]). Suppose
$X$
is a projective Calabi–Yau variety with holomorphic volume form
$\unicode {x03BD} \in {\rm H}^0(X,\Omega ^n_X)$
. Then the Serre pairing
pulls back to a cyclic structure
$\unicode {x03C3} = I^*\unicode {x03C1}$
on
$\mathcal{H}_{\mathcal{E}}$
.
The Serre pairing used in this theorem can be viewed as an analytic strong homotopy inner product
$\unicode {x03C1} \in \Omega ^{2,{\rm cl},{\rm an}}(\mathfrak{g}_{\mathcal{E}})$
, which corresponds to the right Calabi–Yau structure associated to the bounded linear functional
as in Example4.22. In view of the analytic Darboux theorem, one might suspect that there exist other cyclic analytic minimal models for other choices of analytic right Calabi–Yau structure.
In what follows we show how such CY structures can be obtained from a choice of holomorphic volume form on open subsets
$U\subset X$
, using a compactly supported version of the Dolbeault construction.
5.3 The compactly supported setting
Let
$U\subset X$
be an open analytic subvariety of a smooth projective variety
$X$
, viewed as an analytic manifold. Given a bounded complex of locally free
$\mathcal{O}_U$
-modules
$\mathcal{F}$
we let
denote the nonunital DG subalgebra of
$\mathfrak{g}_{\mathcal{F}}$
of compactly supported sections. Henceforth, we will assume that the cohomology of
$\mathcal{F}$
is supported on a compact subset
$Z\subset U$
, which implies that
so that the inclusion
$\mathfrak{g}_{\mathcal{F},c} \hookrightarrow \mathfrak{g}_{\mathcal{F}}$
is a quasi-isomorphism. We also fix a hermitian metric on
$\mathcal{F}$
, which induces a hermitian pairing
The metric data again determines a well-defined
$L^2$
-norm
${{\left \|\cdot \right \|}}_{L^2}\colon \mathfrak{g}_{\mathcal{F},c} \to \mathbb{R}$
which is defined on pure tensors
$\unicode {x03BE} = f \otimes \omega$
with
$f\in \Gamma _c(U,\mathscr{A}^{\;\,0,0}(\mathcal{E} nd(\mathcal{F})))$
and
$\omega \in \Gamma _c(U,\mathscr{A}^{\;\,0,q})$
as
\begin{align*} {\left \|\unicode {x03BE}\right \|}_{L^2} = \left (\int _X \langle f,f\rangle _{\mathcal{E} nd(\mathcal{F})} \cdot \langle \omega ,\omega \rangle _X {\rm d} vol_X \right )^{1/2}, \end{align*}
where we note that the compactly supported function
$\langle f,f\rangle _{\mathcal{E} nd(\mathcal{F})}$
can be viewed as a function on
$X$
via extension by
$0$
, and similarly
$\omega$
extends to a smooth
$(0,q)$
-form on
$X$
. The metric connection then also determines a Sobolev norm
${{\left \|\cdot \right \|}}_{l,2} = \sum _{k\leqslant l} {\left \|\nabla ^k-\right \|}_{L^2}$
, as in the compact setting. A priori, the operators
$D$
and
$\wedge$
are not guaranteed to be bounded, but the reader can check that such a bound exists if
$U$
is chosen to be a sufficiently small neighbourhood of the compact set
$Z$
.
Now suppose that
$U$
admits a nowhere-vanishing holomorphic volume form
$\unicode {x03BD} \in \Gamma (U,\Omega ^n_U)$
. Then, again writing
${\rm tr}\colon \mathscr{A\;\,}_U^{0,n}(\mathcal{E} nd(\mathcal{E})) \to \mathscr{A\;\,}_U^{0,n}$
for the pointwise trace, we obtain a linear functional
We will view
$\unicode {x03C4}_{\unicode {x03BD}}$
as an element of
$\mathfrak{g}_{\mathcal{F},c}^\vee \subset \mathcal{M}(\mathfrak{g}_{\mathcal{F},c},\mathfrak{g}_{\mathcal{F},c}^\vee )[-1]$
in the obvious way, and we claim that this is a negative cyclic cocycle.
Lemma 5.3.
The map
$\unicode {x03C4}_{\unicode {x03BD}}$
defines a right
$n$
-Calabi–Yau structure.
Proof.
Unravelling the definition of the differential on
${\bf C}^\bullet (\mathfrak{g}_{\mathcal{F},c},\mathfrak{g}_{\mathcal{F},c}^\vee ) = (\mathcal{M}(\mathfrak{g}_{\mathcal{F},c},\mathfrak{g}_{\mathcal{F},c}^\vee )[-1],b)$
, we see that
$b(\unicode {x03C4}_{\unicode {x03BD}}) = 0$
if and only if the following two equations hold for all homogeneous
$\unicode {x03B6},\unicode {x03BE}\in \mathfrak{g}_{\mathcal{F},c}$
:
\begin{align*} \begin{aligned} \unicode {x03C4}_{\unicode {x03BD}}(D \unicode {x03B6}) &= 0,\\[5pt] \unicode {x03C4}_{\unicode {x03BD}}(\unicode {x03B6}_1 \wedge \unicode {x03B6}_2) &= (-1)^{|\unicode {x03B6}_1||\unicode {x03B6}_2|} \unicode {x03C4}_v(\unicode {x03B6}_2\wedge \unicode {x03B6}_1). \end{aligned} \end{align*}
To show the first equation, we note that, for a local form
$\unicode {x03B6} = f \otimes \omega$
with
$f$
a local section of
$\mathcal{E} nd^i(\mathcal{F})$
and
$\omega$
a local
$(0,n-i-1)$
-form, we have the local identity
Hence, the same identity also holds for a general compactly supported section
$\unicode {x03B6}$
over
$U$
. Because
$\unicode {x03BD}$
is holomorphic, it then follows by Stokes’ theorem for compactly supported forms that
where we note that
$\partial (\unicode {x03BD}\wedge {\rm tr}(\unicode {x03B6})) = 0$
for degree reasons. For the second equation, we can likewise consider local forms
$\unicode {x03B6}_1 = f_1\otimes \omega _1$
and
$\unicode {x03B6}_2 = f_2\otimes \unicode {x03BE}_2$
with
$f_k$
a local section of
$\mathcal{E} nd^{i_k}(\mathcal{F})$
and
$\omega _k$
a local section of
$\mathscr{A\;\,}_U^{0,q_k}$
. There is an identity
\begin{align*} \begin{aligned} {\rm tr}(\unicode {x03B6}_1\wedge \unicode {x03B6}_2) &= (-1)^{q_1 i_2} {\rm tr}(f_1\circ f_2) \cdot \omega _1 \wedge \omega _2 \\[5pt] &= (-1)^{q_1(q_2+i_2) + i_1i_2} {\rm tr}(f_2\circ f_1) \cdot \omega _2\wedge \omega _1 = (-1)^{|\unicode {x03B6}_1||\unicode {x03B6}_2|}{\rm tr}(\unicode {x03B6}_2\wedge \unicode {x03B6}_1). \end{aligned} \end{align*}
This identity then also holds for any compactly supported section on
$U$
, so integrating against
$\unicode {x03BD}$
yields the section equality. It follows that
$\unicode {x03C4}_{\unicode {x03BD}}$
is a cocycle in
$\mathsf{C}^\bullet (\mathfrak{g}_{\mathcal{F},c},\mathfrak{g}_{\mathcal{F},c}^\vee )$
, and it is immediate that it lies in
$\mathsf{C}^\bullet _\lambda (\mathfrak{g}_{\mathcal{F},c})$
because the cyclic action is trivial on the summand
$\mathfrak{g}_{\mathcal{F},c}^\vee \subset \mathsf{C}^\bullet _\lambda (\mathfrak{g}_{\mathcal{F},c})$
.
It remains to show that the map
$\unicode {x03B6} \mapsto \unicode {x03C4}_{\unicode {x03BD}}(\unicode {x03B6} \wedge -)$
is a quasi-isomorphism, or equivalently that
induces a nondegenerate pairing on cohomology. For this, we note that a holomorphic volume form
$\unicode {x03BD} \in \Gamma (U,\Omega ^n_U)$
represents an isomorphism
$[\unicode {x03BD}] \in {{\rm Hom}}_{\mathsf{D}(U)}(\mathcal{O}_U,\Omega ^n_U)$
in the derived category. Therefore, the wedge product
induces the isomorphisms
${{\rm Hom}}_{\mathsf{D}(U)}(\mathcal{E},\mathcal{E}[i]) \to {{\rm Hom}}_{\mathsf{D}(U)}(\mathcal{E},\mathcal{E}\otimes \Omega ^n_U[i])$
in the derived category. By inspection, (22) is the composition of (23) with the Serre duality pairing
which induces a nondegenerate pairing
${{\rm Hom}}_{\mathsf{D}(U)}(\mathcal{E},\mathcal{E}[n-i]) \otimes {{\rm Hom}}_{\mathsf{D}(U)}(\mathcal{E},\mathcal{E} \otimes \Omega ^n[i]) \to {\mathbb{C}}$
on cohomology. Therefore the pairing induced by (22) on cohomology is also nondegenerate, and it follows that
$\unicode {x03C4}_{\unicode {x03BD}}$
is a right Calabi–Yau structure.
We now want to show that the right Calabi–Yau structure
$\unicode {x03C4}_{\unicode {x03BD}}$
is analytic if
$\mathfrak{g}_{\mathcal{F},c}$
is an analytic
$A_\infty$
-algebra. For this, it suffices to show that
$\unicode {x03C4}_{\unicode {x03BD}}$
is bounded with respect to the Sobolev norm.
Lemma 5.4.
If
$\unicode {x03BD} \in \Gamma (U,\Omega ^n_U)$
is an
$L^2$
-integrable holomorphic volume form, then
$\unicode {x03C4}_{\unicode {x03BD}}$
is bounded.
Proof.
For any
$\unicode {x03B6} \in \Gamma _c(U,\mathscr{A}^{\;\,0,\bullet }(\mathcal{E} nd(\mathcal{F}))$
there is a Cauchy–Schwarz type inequality
with respect to the
$L^2$
-inner product on smooth forms determined by the hermitian metric. It is then easy to check that
${\left \|{\rm tr}(\unicode {x03B6})\right \|}_{L^2} \leqslant {\left \|\unicode {x03B6}\right \|}_{L^2}\leqslant {\left \|\unicode {x03B6}\right \|}_{l,2}$
, so that
${\left \|\unicode {x03C4}_{\unicode {x03BD}}\right \|}_{l,2}$
is bounded by
${\left \|\unicode {x03BD}\right \|}_{L^2}$
.
We again remark that one can ensure that any holomorphic volume form
$\unicode {x03BD}\in \Gamma (U,\Omega ^n_U)$
is bounded in the
$L^2$
-norm by replacing
$U$
with a sufficiently small neighbourhood of
$Z$
. After making this slight modification, we find an analytic right Calabi–Yau structure corresponding to the volume form.
5.4 Comparing the compact and noncompact settings
Let
$\mathcal{E}$
be a hermitian perfect complex on a projective variety
$X$
, with cohomology supported on a subset
$Z$
, and choose an open neighbourhood
$U\supset Z$
with inclusion map
$i\colon U \hookrightarrow X$
. Then the extension by zero yields an injective map
which exhibits
$\mathfrak{g}_{\mathcal{E}|_U,c}$
as a DG ideal of
$\mathfrak{g}_{\mathcal{E}}$
. Equipping
$\mathcal{E}|_U$
with the induced metric, this is an isometry with respect to the Sobolev norm, making
$\mathfrak{g}_{\mathcal{E}|_U,c}$
into an analytic
$A_\infty$
-subalgebra of
$\mathfrak{g}_{\mathcal{E}}$
. The assumption on the support, moreover, guarantees that
$i_!$
is a quasi-isomorphism.
In order to pull back the analytic right CY structures found above from
$\mathfrak{g}_{\mathcal{E}|_U,c}$
to
$\mathfrak{g}_{\mathcal{E}}$
we would like to construct a homotopy inverse for
$i_!$
using Lemma2.28. This requires us first to construct a quasi-isomorphism
$\mathfrak{g}_{\mathcal{E}} \to \mathfrak{g}_{\mathcal{E}|_U,c}$
, for which we use a choice of weak unit.
Lemma 5.5.
There exists a pair
$(u,h) \in \mathfrak{g}_{\mathcal{E}|_U,c}^0 \times \mathfrak{g}_{\mathcal{E}}^{-1}$
such that
$D u=0$
and
In particular, the map
$\unicode {x1D7D9} \colon l \mapsto l\cdot u$
is a weak unit for the analytic
$A_\infty$
-algebra
$\mathfrak{g}_{\mathcal{E}|_U,c}$
.
Proof.
Because
$i_!\colon \mathfrak{g}_{\mathcal{E}|_U,c} \to \mathfrak{g}_{\mathcal{E}}$
is a quasi-isomorphism, it follows that there exists a cocycle
$u$
with
$[i_!u] = [{\rm id}_{\mathcal{E}}]$
, and hence there exists a coboundary
$D h=i_!u-{\rm id}_{\mathcal{E}}$
. If
$\unicode {x03BE} \in \mathfrak{g}_{\mathcal{E}|_U,c}$
is
$D$
-closed then
It follows that
$[u\wedge \unicode {x03BE}] = [\unicode {x03BE}]$
and likewise
$[\unicode {x03BE} \wedge u] = [\unicode {x03BE}]$
hold in
${\rm H}^\bullet \mathfrak{g}_{\mathcal{E}|_U,c}$
. The map
$\unicode {x1D7D9} \colon \ell \to \mathfrak{g}_{\mathcal{E}|_U,c}$
then satisfies
$[\unicode {x1D7D9}(l)\wedge \unicode {x03BE}] = [l\cdot u\wedge \unicode {x03BE}]= [l\cdot \unicode {x03BE}]$
and
$[\unicode {x03BE} \wedge \unicode {x1D7D9}(l)] = [\unicode {x03BE} \cdot l \wedge u] = [\unicode {x03BE}\cdot l]$
, making it a weak unit.
For a unit/coboundary pair
$(u,h)$
as above, the wedge product
$i_!u\wedge \unicode {x03BE}$
with any section
$\unicode {x03BE}\in \mathfrak{g}_{\mathcal{E}}$
has compact support contained in
$U$
. Hence, we obtain a restriction
$i^*(i_!u \wedge -) \colon \mathfrak{g}_{\mathcal{E}} \to \mathfrak{g}_{\mathcal{E}|_U,c}$
which is a chain-level inverse to
$i_!$
. To extend it to an analytic
$A_\infty$
-morphism, we need the following lemma.
Lemma 5.6.
Let
$h\in \mathfrak{g}_{\mathcal{E}}^{-1}$
and
$v = {\rm id}_{\mathcal{E}} + D h$
, then the maps
$K_n \colon \mathfrak{g}_{\mathcal{E}}[1]^{\otimes n} \to \mathfrak{g}_{\mathcal{E}}[1]$
given by
\begin{align*} \begin{aligned} K_1(s\xi _1) &= s(v\wedge \xi _1) \\[5pt] K_n(s\xi _1,\ldots ,s\xi _n) &= s(v\wedge \xi _1\wedge h\wedge \cdots \wedge h\wedge \xi _n) \quad (n\gt 1) \end{aligned} \end{align*}
for
$\xi _i \in \mathfrak{g}_{\mathcal{E}}$
, define an analytic
$A_\infty$
-morphism
$K \in {{\rm Hom}}_{{\mathsf{Alg}^\infty }}^{{\rm an}}(\mathfrak{g}_{\mathcal{E}},\mathfrak{g}_{\mathcal{E}})$
.
Proof.
Since the
$A_\infty$
-algebra structures on
$\mathfrak{g}_{\mathcal{E}}$
and
$\mathfrak{g}_{\mathcal{E}|_U,c}$
come from DG algebra structures, the
$A_\infty$
-morphism conditions can be written as
\begin{equation} \begin{aligned} \mu _1 K_n + \sum _{i=1}^{n-1} \mu _2 (K_i \otimes K_{n-i}) &= \sum _{i=0}^{n-1} K_n ({\rm id}^{\otimes i} \otimes \mu _1 \otimes {\rm id}^{\otimes n-i-1}) \\[5pt] &\quad + \sum _{i=0}^{n-2} K_{n-1} ({\rm id}^{\otimes i} \otimes \mu _2 \otimes {\rm id}^{\otimes n-i-2}). \end{aligned} \end{equation}
Plugging in the definitions
$\mu _1 = -s D s^{-1}$
and
$\mu _2 = -s(-\wedge -)(s^{-1})^{\otimes 2}$
, it follows from the graded Leibniz rule for
$D$
and
$\wedge$
that
\begin{align*} \begin{aligned} \mu _1 K_n(s\xi _1,\ldots ,s\xi _n) &= -sD(v\wedge \unicode {x03BE}_1\wedge h \wedge \cdots \wedge \unicode {x03BE}_n) \\[5pt] &= \sum _{i=0}^{n-1} (-1)^{\epsilon _{i+1}} s(v \wedge \cdots \wedge h \wedge D \unicode {x03BE}_{i+1} \wedge h \wedge \cdots \wedge \unicode {x03BE}_n) \\[5pt] &\quad - \sum _{i=1}^{n-1} (-1)^{\epsilon _{i+1}} s(v \wedge \cdots \wedge h \wedge \unicode {x03BE}_i \wedge v \wedge \unicode {x03BE}_{i+1} \wedge h \wedge \cdots \wedge \unicode {x03BE}_n), \\[5pt] &\quad + \sum _{i=1}^{n-1} (-1)^{\epsilon _{i+1}} s(v \wedge \cdots \wedge h \wedge \unicode {x03BE}_i \wedge \unicode {x03BE}_{i+1} \wedge h \wedge \cdots \wedge \unicode {x03BE}_n), \end{aligned} \end{align*}
where we used the notation
${\epsilon _i} = |\xi _1|+\cdots +|\xi _i|+i$
for the sign. By inspection, each of the terms in these summations is given by one of the terms
\begin{align*} \begin{aligned} \mu _2(K_i \otimes K_{n-i})(s\xi ) &= (-1)^{\epsilon _{i+1}} s(v\wedge \xi _1\wedge \cdots \wedge \xi _i \wedge v\wedge \xi _{i+1}\wedge \cdots \wedge h\wedge \xi _n)\\[5pt] K_n({\rm id}^{\otimes i}\otimes \mu _1 \otimes {\rm id}^{\otimes n-i-1})(s\xi ) &= (-1)^{{\epsilon _{i+1}}} s(v\wedge \xi _1 \wedge \ldots \wedge h\wedge D \xi _{i+1} \wedge h \wedge \cdots \wedge \xi _n)\\[5pt] K_{n-1}({\rm id}^{\otimes i-1}\otimes \mu _2\otimes {\rm id}^{\otimes n-i-1})(s\xi ) &= (-1)^{{\epsilon _{i+1}}} s(v\wedge \xi _1 \wedge \ldots \wedge h\wedge \xi _i \wedge \xi _{i+1} \wedge h \wedge \cdots \wedge \xi _n), \end{aligned} \end{align*}
where we use the abbreviation
$s\xi = s\xi _1 \otimes \cdots \otimes s\xi _n$
. Comparing coefficients, it therefore follows that
$K$
defines an
$A_\infty$
-morphism, and it remains to show it is analytic. For this, let
$C\geqslant 1$
be any constant such that
${\left \|\wedge \right \|}_{l,2} \leqslant C$
,
${\left \|u\right \|}_{l,2} \lt C$
and
${\left \|h\right \|}_{l,2} \lt C$
. Then for any sections
$\unicode {x03BE}_1,\ldots ,\unicode {x03BE}_n$
which implies that
${\left \|K_n\right \|} \lt C^{3n-1} \lt (C^3)^n$
, which shows that
$K$
is indeed analytic.
Given a unit/coboundary pair
$(u,h)$
as above,
${\rm id}_{\mathcal{E}}+D h=i_!u$
has support contained in the open
$U\subset X$
, so for any
$\xi _1,\ldots ,\xi _n \in \mathfrak{g}_{\mathcal{E}}$
there is a well-defined pullback
We therefore obtain a well-defined
$A_\infty$
-morphism
$K_c$
from
$\mathfrak{g}_{\mathcal{E}}$
to
$\mathfrak{g}_{\mathcal{E}|_U,c}$
.
Lemma 5.7.
Let
$(u,h)$
be a unit/coboundary pair as in Lemma
5.5
, and
$K$
the morphism associated to
$h$
. Then
$K_c$
is an analytic homotopy inverse to
$i_!$
.
Proof.
We will construct an analytic homotopy
$K^t + Q^t{\rm d} t \in {{\rm Hom}}^{{\rm an}}_{\mathsf{Alg}^\infty }(\mathfrak{g}_{\mathcal{E}},\Omega ^\bullet _{[0,1]} \otimes \mathfrak{g}_{\mathcal{E}})$
between
${\rm id}_{\mathfrak{g}_{\mathcal{E}}}$
and
$K$
, where the coefficient functions are defined as follows:
\begin{align*} \begin{aligned} K^t_n(s\xi _1,\ldots ,s\xi _n) &= s({\rm id}_{\mathcal{E}} + t\cdot D h) \wedge \xi _1 \wedge (t\cdot h) \wedge \cdots \wedge (t\cdot h) \wedge \xi _n),\\[5pt] Q^t_n(s\xi _1,\ldots ,s\xi _n) &= s(h\wedge \xi _1 \wedge (t\cdot h) \wedge \cdots \wedge (t\cdot h) \wedge \xi _n). \end{aligned} \end{align*}
For each
$t\in [0,1]$
the map
$K^t$
is the
$A_\infty$
-morphism of Lemma5.6 corresponding to the element
$t\cdot h\in \mathfrak{g}_{\mathcal{E}}^{-1}$
, so it suffices to check the condition in (6). The two terms on the right-hand side of (6) are, respectively, given by the sum of the terms
\begin{align*} \begin{aligned} \mu _1Q^t_n(s\xi _1,\ldots ,s\xi _n) &= \sum _{i=1}^n (-1)^{\epsilon _{i-1}} t^{n-1} \cdot s(h\wedge \xi _1 \wedge \cdots \wedge D h \wedge \xi _i \wedge \cdots \wedge h \wedge \xi _n) \\[5pt] &\quad -\sum _{i=1}^n (-1)^{\epsilon _{i-1}} t^{n-1} \cdot s(h\wedge \xi _1 \wedge \cdots \wedge h \wedge D \xi _i \wedge \cdots \wedge h \wedge \xi _n) \\[5pt] \mu _2(K^t_i \otimes Q^t_{n-i})(s\xi _1,\ldots ,s\xi _n) &= (n-1) t^{n-1} \cdot s(D h\wedge \xi _1 \wedge \cdots \wedge h \wedge \xi _n) \\[5pt] &\quad + (n-1) t^{n-2} \cdot s(\xi _1 \wedge h \wedge \cdots \wedge h \wedge \xi _n) \\[5pt] \mu _2(Q^t_i \otimes K^t_{n-i})(s\xi _1,\ldots ,s\xi _n) &= -(-1)^{\epsilon _{i+1} }t^{n-1} \cdot s(h\wedge \xi _1 \wedge \cdots \wedge D h \wedge \xi _{i+1} \wedge \cdots \wedge h \wedge \xi _n) \\[5pt] &\quad -(-1)^{\epsilon _{i+1}} t^{n-2}\cdot s(h\wedge \xi _1 \wedge \cdots \wedge h \wedge \xi _{i} \wedge \xi _{i+1} \wedge h \wedge \cdots \wedge h \wedge \xi _n) \end{aligned} \end{align*}
and the term
\begin{align*} \begin{aligned} (Q^t_{n-1} \widetilde {\unicode {x03BC}})(s\xi _1,\ldots ,s\xi _n) &= \sum _{i=1}^n (-1)^{\epsilon _{i-1}}t^{n-1}\cdot s(h\wedge \xi _1 \wedge \cdots \wedge h \wedge D \xi _i \wedge \cdots \wedge h \wedge \xi _n)\\[5pt] &\quad + \sum _{i=1}^{n-1}(-1)^{\epsilon _{i+1}} t^{n-2} \cdot s(h\wedge \xi _1 \wedge \cdots \wedge h \wedge \xi _i \wedge \xi _{i+1} \wedge h \wedge \cdots \wedge h \wedge \xi _n). \end{aligned} \end{align*}
The sum of all these terms is equal to
which shows that
$K^t+Q^t {\rm d} t$
defines a homotopy from
$K^0 = {\rm id}$
to
$K^1 = K$
on
$\mathfrak{g}_{\mathcal{E}}$
. To see that this homotopy is analytic, we again take a constant
$C\geqslant 1$
such that
${\left \|\wedge \right \|}_{l,2} \leqslant C$
,
${\left \|D \right \|}_{l,2}\lt C$
and
${\left \|h\right \|}_{l,2} \lt C$
. Then the component functions in the homotopy are bounded by
\begin{align*} \begin{aligned} {\left \|K_n^t\right \|}_\infty &\leqslant \int _0^1 t^{n-1} {\left \|\wedge \right \|}_{l,2}^{4n}\cdot {\left \|h\right \|}_{l,2}^{2n-2}\left (1+t {\left \|D \right \|}_{l,2}^2\cdot {\left \|h\right \|}_{l,2}^{2}\right ) {\rm d} t \lt 2 C^{6n+2} , \\[5pt] {\left \|\tfrac {\partial }{\partial t} K_n^t\right \|}_\infty & \leqslant \int _0^1 t^{n-2}{\left \|\wedge \right \|}_{l,2}^{4n} \cdot {\left \|h\right \|}_{l,2}^{2n-2}\left (n t {\left \|D \right \|}_{l,2}^2 \cdot {\left \|h\right \|}_{l,2}^{2} + (n-1)\right ) {\rm d} t \lt 2n C^{6n+2}, \\[5pt] {\left \|Q_n^t\right \|}_\infty &\leqslant \int _0^1 t^{n-1} {\left \|\wedge \right \|}_{l,2}^{4n} \cdot {\left \|h\right \|}_{l,2}^{2n}\,{\rm d} t \lt C^{6n}. \end{aligned} \end{align*}
Clearly, we then have a common bound (e.g.
$C' = 2(C+1)^8$
suffices), and it follows that
$K^t + Q^t{\rm d} t$
is an analytic homotopy, which shows that
$i_! \diamond K_c = K \sim _{{\rm an}} {\rm id}_{\mathfrak{g}_{\mathcal{E}}}$
. The forms
$Q^t_n(s\xi _1,\ldots ,s\xi _n)$
and
$K^t_n(s\xi _1,\ldots ,s\xi _n)$
have compact support on
$U$
whenever at least one of the
$\xi _i$
does. Writing
$K_c^t$
and
$Q_c^t$
to denote the composition with the restriction as before, we obtain an analytic homotopy
between
${\rm id}_{\mathfrak{g}_{\mathcal{E}|_U,c}}$
and
$K_c \diamond i_!$
, which shows the result.
We conclude that
$\mathfrak{g}_{\mathcal{E}|_U,c}$
is analytically homotopy equivalent to
$\mathfrak{g}_{\mathcal{E}}$
, and therefore also analytically homotopy equivalent to the minimal model
$\mathcal{H}_{\mathcal{E}}$
. Lemma2.28 then shows that there exists some automorphism
$T\in {{\rm Hom}}_{\mathsf{Alg}^\infty }^{{\rm an}}(\mathfrak{g}_{\mathcal{E}},\mathfrak{g}_{\mathcal{E}})$
such that the compositions in the diagram

make
$\mathcal{H}_E$
into an analytic minimal model for
$\mathfrak{g}_{\mathcal{E}|_U,c}$
. Hence,
$\mathfrak{g}_{\mathcal{E}|_U,c}$
is again one of the well-behaved analytic
$A_\infty$
-algebras, admitting a compact analytic minimal model.
Finally, we wish to compare the situation where
$\mathcal{E}|_U$
is replaced by an arbitrary hermitian perfect complex on
$U$
. It turns out that we can again compare the corresponding Dolbeault DG algebras via a quasi-isomorphism, as the following lemma shows.
Lemma 5.8.
Suppose that
$\mathcal{F}$
is a hermitian perfect complex, quasi-isomorphic to
$\mathcal{E}|_U$
, such that
$\mathfrak{g}_{\mathcal{F},c}$
is analytic with respect to the Sobolev norm. Then there exists a triple
$(r,r^{-1},h_{rr^{-1}})$
with
degree
$0$
cocycles and
$h_{rr^{-1}} \in \mathfrak{g}_{\mathcal{E}}^{-1}$
satisfying
$D h_{rr^{-1}} = i_!(r\wedge r^{-1}) - {\rm id}_{\mathcal{E}}$
, such that the maps
determine an analytic
$A_\infty$
-quasi-isomorphism
$F\in {{\rm Hom}}_{{\mathsf{Alg}^\infty }}(\mathfrak{g}_{\mathcal{E}|_U,c},\mathfrak{g}_{\mathcal{F},c})$
.
Proof.
Because the cohomologies of
$\mathcal{F}$
and
$\mathcal{E}|_U$
are compactly supported on
$U$
, the morphism spaces between
$\mathcal{E}|_U$
and
$\mathcal{F}$
in the derived category can be computed as
and similarly
${{\rm Hom}}_{\mathsf{D}(U)}(\mathcal{F},\mathcal{E}|_U) \cong {\rm H}^0(\Gamma _c(U,\mathscr{A\;\,}_U^{0,\bullet }(\mathcal{H} om(\mathcal{E}|_U,\mathcal{F})),D)$
. Hence there exist degree
$0$
cocycles
$r^{-1} \in \Gamma _c(U,\mathscr{A\;\,}_U^{0,\bullet }(\mathcal{H} om(\mathcal{E}|_U,\mathcal{F})))$
and
$r \in \Gamma _c(U,\mathscr{A\;\,}_U^{0,\bullet }(\mathcal{H} om(\mathcal{E}|_U,\mathcal{F})))$
which induces the isomorphism between
$\mathcal{F}$
and
$\mathcal{E}|_U$
in the derived category. Because the composition
$r\wedge r^{-1}$
induces the identity on
$\mathcal{E}|_U$
in the derived category, there exists some
$h_{rr^{-1}}\in \mathfrak{g}_{\mathcal{E}}^{-1}$
such that
Hence,
$F$
is well defined and one can check easily that it is an
$A_\infty$
-morphism in an analogous fashion to the proof of Lemma5.6. To see that it is a quasi-isomorphism we note that
$F_1(s\xi ) = s(r^{-1}\wedge \xi \wedge r)$
has a quasi-inverse
$F_1^{-1}(s\xi ) := s(r \wedge \xi \wedge r^{-1})$
. Indeed, we have
\begin{align*} \begin{aligned}{} [i_!(F_1^{-1}(F_1(s\unicode {x03BE})))] &= [s(i_!(r\wedge r^{-1}) \wedge i_!\unicode {x03BE} \wedge i_!(r \wedge r^{-1}))] \\[5pt] &= [s(({\rm id}_{\mathcal{E}} + D h_{rr^{-1}}) \wedge i_!\unicode {x03BE} \wedge ({\rm id}_{\mathcal{E}}+D h_{rr^{-1}}))] \\[5pt] &= [si_!\unicode {x03BE}] \in {\rm H}^0\mathfrak{g}_{\mathcal{E}}, \end{aligned} \end{align*}
which implies that
$F_1^{-1}\circ F_1$
induces the identity on
${\rm H}^\bullet \mathfrak{g}_{\mathcal{E}|_U,c}$
, since
$i_!\colon \mathfrak{g}_{\mathcal{E}|_U,c}\to \mathfrak{g}_{\mathcal{E}}$
is a quasi-isomorphism. To check that
$F$
is analytic let
$C\gt \max \{{\left \|r^{-1}\right \|}_{l,2},{\left \|r\right \|}_{l,2},{\left \|h\right \|}_{l,2},{\left \|\wedge \right \|}_{l,2}\}$
, so that
as in the proof of Lemma5.6. It follows that
$F$
is analytic when
$\mathfrak{g}_{\mathcal{F},c}$
is an analytic
$A_\infty$
-algebra.
If
$\mathcal{F}$
is an arbitrary perfect complex on
$U$
with compactly supported cohomology, then
$\mathcal{F}$
is quasi-isomorphic to
$i^*\mathcal{E} = \mathcal{E}|_U$
, where
$\mathcal{E} \to {\bf R} i_! \mathcal{F}$
is any resolution of the exceptional direct image. With the above lemma, we find maps on analytic negative cyclic cohomology

along which right Calabi–Yau structures can be pulled back. With these comparison maps, we are now ready to prove the main theorems of the paper.
5.5 Cyclic minimal models from local volumes
We now combine all our results to obtain new cyclic minimal models associated to local holomorphic volume forms. It turns out that the cyclic minimal model one obtains does not depend on the neighbourhood chosen, so we can take an agnostic approach: given a closed subset
$Z$
we consider the space of germs along
$Z$
where
$\unicode {x03BD} \sim \unicode {x03BD}'$
for two sections
$\unicode {x03BD} \in \Gamma (V,\Omega ^n_X)$
and
$\unicode {x03BD}' \in \Gamma (V',\Omega ^n_X)$
if there exists
$V'' \subset V\cap V'$
such that
$Z \subset V''$
and
$\unicode {x03BD}|_{V''} = \unicode {x03BD}'|_{V''}$
. We consider germs which locally act as a volume.
Definition 5.9. An element
$\unicode {x03BD} \in (\Omega ^n_X)_Z$
is a volume germ along
$Z$
if there is some open neighbourhood
$V\supset Z$
such that
$\unicode {x03BD}|_V$
is nonzero at every point in
$V$
.
The main result of this section is the following theorem.
Theorem 5.10.
Let
$X$
be a smooth projective variety of dimension
$n$
, and
$\mathcal{E}$
a perfect complex on
$X$
with cohomology supported on
$Z \subset X$
. Then any volume germ
$\unicode {x03BD} \in (\Omega ^n_X)_Z$
determines a canonical class
$[\unicode {x03D5}^{\unicode {x03BD}}]_{{\rm an}} \in {\rm HC}_\lambda ^{\bullet ,{\rm an}}(\mathfrak{g}_{\mathcal{E}})$
of an analytic right Calabi–Yau structure, which determines a corresponding analytic cyclic minimal model of
$\mathfrak{g}_{\mathcal{E}}$
which is well defined up to cyclic analytic
$A_\infty$
-isomorphism.
Proof.
We fix a hermitian structure on
$X$
and
$\mathcal{E}$
as before, so that
$\mathfrak{g}_{\mathcal{E}}$
is an analytic DG algebra which admits a strong analytic minimal model, by Theorem5.1, with underlying space
We claim that every volume germ
$\unicode {x03BD}$
along
$Z$
has a representative which is
$L^2$
-integrable. To construct this, pick any nonvanishing representative
$\unicode {x03BD}^0 \in \Gamma (V,\Omega ^n_X)$
, and note that the pointwise squared-norm is a continuous function
$p \mapsto |\unicode {x03BD}^0(p)|_X^2$
on
$V$
. Because
$Z$
is compact, this function is bounded on
$Z$
, so picking any
$\epsilon \gt 0$
we obtain an open neighbourhood
on which
$|\unicode {x03BD}_p^0|^2$
is bounded. Then
$\unicode {x03BD} = \unicode {x03BD}^0|_U$
is square-integrable, yielding the required representative.
Fixing such a
$\unicode {x03BD} \in \Gamma (U,\Omega ^n_X)$
, the trace
$\unicode {x03C4}_{\unicode {x03BD}} \in \hom _{\ell ^e}^{{\rm cont}}(\ell ,\mathfrak{g}_{\mathcal{E}|_U,c}')$
from Lemma5.3 is an analytic right CY structure on
$\mathfrak{g}_{\mathcal{E}|_U,c}$
by Lemma5.4. Writing
$i\colon U\to X$
for the embedding of
$U$
, it follows by Lemma5.5 that there is a unit/coboundary pair
$(u,h) \in \mathfrak{g}_{\mathcal{E}|_U,c}^0\times \mathfrak{g}_{\mathcal{E}}^{-1}$
, which induces an analytic homotopy equivalence
$K_c\in {{\rm Hom}}_{{\mathsf{Alg}^\infty }}^{{\rm an}}(\mathfrak{g}_{\mathcal{E}},\mathfrak{g}_{\mathcal{E}|_U,c})$
by Lemma5.6. We obtain the analytic right CY structure
Because the minimal model
$\mathcal{H}_{\mathcal{E}}$
is unital, it follows from Theorem4.23(i) that
$\unicode {x03D5}^{\unicode {x03BD}}$
determines an analytic cyclic minimal model
so that
$\unicode {x03D5}^{\unicode {x03BD}}$
pulls back to a class in
$\mathsf{C}_\lambda ^{\bullet ,{\rm an}}(\mathcal{H}_{\mathcal{E}}^{\unicode {x03BD}})$
which is homotopic to the image of
$\unicode {x03C3}^{\unicode {x03BD}}$
along the map in Corollary4.21. It now remains to show that the right CY structure and the cyclic minimal model are independent of the choice of neighbourhood
$U$
or the unit/coboundary pair
$(u,h)$
.
Suppose
$V\subset U$
is another open subset with inclusion
$j\colon V\hookrightarrow U$
, and let
$(u_V,h_V)$
be a choice of unit/coboundary pair such that
$(ij)_!u_V = {\rm id}_{\mathcal{E}} + D h_V$
, and let
$K_{c,V}\in {{\rm Hom}}_{{\mathsf{Alg}^\infty }}^{{\rm an}}(\mathfrak{g}_{\mathcal{E}},\mathfrak{g}_{\mathcal{E}|_V,c})$
be the induced analytic homotopy equivalence. Then
$\unicode {x03BD}|_V \sim \unicode {x03BD}$
is another representative of the germ and induces the analytic right CY structure
$K_{c,V}^*\unicode {x03C4}_{\unicode {x03BD}|_V}$
as before. Since
$j_!$
is a strict morphism from
$\mathfrak{g}_{\mathcal{E}|_V,c}$
to
$\mathfrak{g}_{\mathcal{E}|_U,c}$
, it follows that
Now since
$K_c\diamond i_! \sim _{{\rm an}} {\rm id}_{\mathfrak{g}_{\mathcal{E}|_U,c}}$
and
$i_!\diamond j_!\diamond K_{c,V} \sim _{{\rm an}} {\rm id}_{\mathfrak{g}_{\mathcal{E}}}$
, it follows by Lemma3.14 that
By Theorem4.23(ii) the cyclic minimal model induced by
$K_{c,V}^*\unicode {x03C4}_{\unicode {x03BD}|_V}$
is then cyclic-analytic
$A_\infty$
-isomorphic to
$\mathcal{H}^{\unicode {x03BD}}_{\mathcal{E}}$
.
In the 3-Calabi–Yau case, a potential can be constructed using Corollary4.24.
Corollary 5.11.
Suppose
$X$
is a threefold, then any volume germ
$\unicode {x03BD}$
induces an analytic potential
which is well defined up to an analytic change of coordinates
$\widetilde {\mathsf{T}}_{\kern -1pt\ell } {\rm Ext}^1(\mathcal{E},\mathcal{E})^\vee \xrightarrow {\sim } \widetilde {\mathsf{T}}_{\kern -1pt\ell } {\rm Ext}^1(\mathcal{E},\mathcal{E})^\vee$
.
Remark 5.12. If
$X$
is itself Calabi–Yau, then the global volume form
$\unicode {x03BD} \in \Gamma (X,\Omega ^n_X)$
is
$L^2$
-integrable and
$(u,h) = ({\rm id}_{\mathcal{E}},0)$
is a valid unit/coboundary inducing the identity maps
$K_c = {\rm id}$
on
$\mathfrak{g}_{\mathcal{E},c} = \mathfrak{g}_{\mathcal{E}}$
. The trace
$K_c^*\unicode {x03C4}_{\unicode {x03BD}} = \unicode {x03C4}_{\unicode {x03BD}}$
induces the Serre pairing, and
$(\mathcal{H}^{\unicode {x03BD}},\unicode {x03C3}^{\unicode {x03BD}})$
is simply the cyclic analytic minimal model of [Reference PolishchukPol01, Reference TuTu14, Reference TodaTod18], as given in Theorem 5.2.
The cyclic minimal models obtained from the above theorem express the local geometry on an open subset, but they are always defined with respect to a global choice of projective variety. We claim, however, that the cyclic minimal model really only depends on the local geometry. To substantiate this claim, we will consider diagrams of the form

where
$Y$
is an open analytic subvariety in a smooth projective variety
$X$
, and
$f$
is an open embedding into a second smooth projective variety
$X'$
. We claim that the cyclic minimal model for a perfect complex with support on
$Y$
can be computed equivalently on
$X'$
or
$X$
.
Theorem 5.13.
In the situation of (26), let
$\mathcal{E}' \in \mathsf{D}^{{\rm perf}}(X')$
have support
$f(Z) \subset f(Y)$
for some compact
$Z\subset Y$
, let
$\unicode {x03BD} \in (\Omega ^n_{X'})_Z$
be a volume form germ, and let
$\mathcal{E}\in \mathsf{D}^{{\rm perf}}(X)$
be such that
$\mathcal{E}|_Y \simeq f^*\mathcal{E}'$
. Then there exists an analytic homotopy equivalence
along which
$\unicode {x03D5}^{\unicode {x03BD}}$
pulls back to a an analytic right CY structure analytically homotopic to
$\unicode {x03D5}^{f^*\unicode {x03D5}}$
. In particular, there is an analytic cyclic
$A_\infty$
-isomorphism between the cyclic analytic minimal models:
Proof.
Given a germ in
$(\Omega ^n_{X'})_{f(Z)}$
, we can find a representative
$\unicode {x03BD} \in \Gamma (f(U),\Omega ^n_{X'})$
defined on the image of some open neighbourhood
$U\supset Z$
. As before, this neighbourhood can be chosen so that
$\unicode {x03BD}$
and
$f^*\unicode {x03BD}$
are
$L^2$
-integrable forms on
$f(U)$
and
$U$
respectively, yielding
$\unicode {x03C4}_{\unicode {x03BD}}\in \mathsf{C}_\lambda ^{\bullet ,{\rm an}}(\mathfrak{g}_{\mathcal{E}|_{f(U)},c})$
and
$\unicode {x03C4}_{f^*\unicode {x03BD}}\in \mathsf{C}_\lambda ^{\bullet ,{\rm an}}(\mathfrak{g}_{\mathcal{E}|_U,c})$
. Now for any choice of complexes
$\mathcal{E}$
and
$\mathcal{E}'$
as above, we can consider the chain of quasi-isomorphisms

where
$F\colon \mathfrak{g}_{\mathcal{E}|_U,c} \to \mathfrak{g}_{f^*\mathcal{E}'|_U,c}$
is the map in Lemma5.8 associated to a triple
$(r,r^{-1},h_{rr^{-1}})$
of mutually inverse quasi-isomorphisms
$r^{-1}\colon \mathcal{E}|_U\to f^*\mathcal{E}'|_U$
and
$r^{-1}\colon f^*\mathcal{E}'|_U\to \mathcal{E}|_U$
with coboundary
$h_{rr^{-1}}$
for the composition
$r\wedge r^{-1}$
, and
$(f^*)^{-1}$
denotes the DG algebra morphism given by the inverse of the pullback map
which is a DG algebra isomorphism because
$f$
is a diffeomorphism onto its image. Choosing hermitian metrics on
$\mathcal{E}$
and
$\mathcal{E}'$
, there is an induced hermitian metric on
$f^*\mathcal{E}'$
, and the maps
$K_c$
and
$F$
are analytic. The strict map
$f^*$
is again bounded, provided that
$U$
is chosen sufficiently small, as the ratio between the metric on
$U$
and the metric pulled back from
$f(U)$
is again bounded on a neighbourhood of the compact subset
$Z$
.
Now we observe that the functional
$\unicode {x03C4}_{\unicode {x03BD}}$
pulls back along the quasi-isomorphism
$(f^*)^{-1} \diamond F$
to an analytic negative cyclic cocycle of the form
\begin{align*} \begin{aligned} (((f^*)^{-1} \diamond F)^*\unicode {x03C4}_{\unicode {x03BD}})_n(s\unicode {x03BE}_1,\ldots ,s\unicode {x03BE}_n) &= \int _{f(U)} \unicode {x03BD} \wedge {\rm tr}((f^*)^{-1}(r^{-1} \wedge \unicode {x03BE}_1 \wedge h_{rr^{-1}} \wedge \cdots \wedge \unicode {x03BE}_n \wedge r)) \\[5pt] &= \int _{U} f^*\unicode {x03BD} \wedge {\rm tr}(r^{-1} \wedge \unicode {x03BE}_1 \wedge h_{rr^{-1}} \wedge \cdots \wedge \unicode {x03BE}_n \wedge r) \\[5pt] &= \int _{U} f^*\unicode {x03BD} \wedge {\rm tr}(r\wedge r^{-1} \wedge \unicode {x03BE}_1 \wedge h_{rr^{-1}} \wedge \cdots \wedge \unicode {x03BE}_n) \\[5pt] &= ((K_c\diamond i_!)^*\unicode {x03C4}_{f^*\unicode {x03BD}})_n(s\unicode {x03BE}_1,\ldots ,s\unicode {x03BE}_n), \end{aligned} \end{align*}
where
$K_c$
is the map associated to the unit/coboundary pair
$(u,h) = (r\wedge r^{-1}, h_{rr^{-1}})$
constructed in Lemma5.6. Since
$K_c\diamond i_!\sim _{{\rm an}} {\rm id}_{\mathfrak{g}_{\mathcal{E}|_U,c}}$
it follows that
$((f^*)^{-1}\diamond F)^*\unicode {x03C4}_{\unicode {x03BD}} \sim _{{\rm an}} \unicode {x03C4}_{f^*\unicode {x03BD}}$
. Now let
$j\colon f(U) \hookrightarrow X'$
denote the inclusion of
$f(U)$
, and let
$K_c'$
be the homotopy inverse of
$j_!$
defining the analytic right CY structure
$\unicode {x03D5}^{\unicode {x03BD}} = (K_c')^*\unicode {x03C4}_{\unicode {x03BD}}$
. Then
is an analytic quasi-isomorphism for which the pullback of the cocycle
$\unicode {x03D5}^{\unicode {x03BD}}$
satisfies
\begin{align*} \begin{aligned} (j_! \diamond (f^*)^{-1} \diamond F \diamond K_c)^*\unicode {x03D5}^{\unicode {x03BD}} &= (K_c' \diamond j_! \diamond (f^*)^{-1} \diamond F \diamond K_c)^*\unicode {x03C4}_{\unicode {x03BD}} \\[5pt] &\sim _{{\rm an}} ((f^*)^{-1} \diamond F \diamond K_c)^*\unicode {x03C4}_{\unicode {x03BD}} \\[5pt] &= K_c^*((f^*)^{-1} \diamond F)^*\unicode {x03C4}_{\unicode {x03BD}} \\[5pt] &\sim _{{\rm an}} K_c^*\unicode {x03C4}_{f^*\unicode {x03BD}} = \unicode {x03D5}^{f^*\unicode {x03BD}}. \end{aligned} \end{align*}
It now follows by Theorem4.23(iii) that there is a cyclic analytic
$A_\infty$
-isomorphism between the cyclic analytic minimal models, which finishes the proof.
In the threefold case, the second part of Corollary4.24 now directly implies the following.
Corollary 5.14.
Suppose
$X$
and
$X'$
are threefolds with complexes
$\mathcal{E}$
and
$\mathcal{E}'$
as above. Then for any volume germ
$\unicode {x03BD} \in (\Omega _{X'}^3)_Z$
there is an algebra isomorphism
which relates the two potentials via
$g(W^{\unicode {x03BD}}) = W^{f^*\unicode {x03BD}}$
.
5.6 The example of a point
We will give an explicit computation of the cyclic minimal model associated to the point sheaf of the origin in
${\mathbb{A}}^n$
, which is a quasi-projective Calabi–Yau with standard volume form
$\omega = {\rm d} z_1 \wedge \cdots \wedge {\rm d} z_n$
in standard coordinates.
Let
$\mathbb{P}^n \subset {\mathbb{A}}^n$
be the projective compactification with coordinates
$z_0,z_1,\ldots ,z_n$
, and write
$o \in {\mathbb{A}}^n \subset \mathbb{P}^n$
for the origin. Writing
$V = (T_o{\mathbb{A}}^n)^* \cong {\mathbb{C}}^n$
, the point sheaf
$\mathcal{O}_o$
is resolved by the Koszul complex
where the differential acts as
$v \otimes f \mapsto \sum _{i=1}^n v(\partial _{z_i}) z_i \cdot f$
on
$\mathcal{E}^{-1} = V\otimes _{\mathbb{C}} \mathcal{O}_{\mathbb{P}^n}(-1)$
and acts on the other terms by extension over the wedge product. We endow
$\mathcal{E}$
with a hermitian structure from the Fubini–Study metric on
$\mathbb{P}^n$
, yielding a Dolbeault DG algebra
$\mathfrak{g}_{\mathcal{E}}$
as a model for
${\rm Ext}^\bullet (\mathcal{O}_o,\mathcal{O}_o)$
. It is known (see e.g. [Reference Ricolfi and SavvasRS24, Lemma 3.6] for the threefold case) that the algebra of polyvectors
\begin{align*} \mathfrak{h} := \left (\bigoplus _{i=0}^n (T_o{\mathbb{A}}^n)^{\wedge i}, \wedge \right ) \end{align*}
at
$o$
forms an
$A_\infty$
-minimal model for
$\mathfrak{g}_{\mathcal{E}}$
. Here we include a proof for the analytic setting.
Lemma 5.15.
There is an analytic DG algebra quasi-isomorphism
$I \colon \mathfrak{h} \xrightarrow {\sim } \mathfrak{g}_{\mathcal{E}}$
which makes
$\mathfrak{h}$
into an analytic minimal model for
$\mathfrak{g}_{\mathcal{E}}$
.
Proof.
It suffices to define
$I(\xi )$
for
$\xi \in T_o{\mathbb{A}}^n$
and check that
$I(\xi )\wedge I(\xi ) = 0$
and
$D I(\xi ) = 0$
hold. For a vector
$\xi \in T_o{\mathbb{A}}^n$
the element
$I(\xi )$
is defined as the holomorphic endomorphism acting by
$v\otimes f \mapsto v(\xi )\cdot f \in \mathcal{E}^0$
on
$\mathcal{E}^{-1}$
and extended to maps
$\mathcal{E}^{-k} \mapsto \mathcal{E}^{1-k}$
over the wedge product. A standard computation shows that
$I(\xi ) \wedge I(\xi ) = I(\xi ) \circ I(\xi )$
acts by
\begin{align*} \begin{aligned} (I(\xi )\circ I(\xi ))(v_1 \otimes f_1 \wedge \cdots \wedge v_k \otimes f_k) &= \sum _{i=1}^n (-1)^i v_i(\xi )f_i \cdot I(\xi )(v_1\otimes f_1 \wedge \cdots \widehat {v_i\otimes f_i}\cdots \wedge v_k \otimes f_k)\\[5pt] &= \sum _{i\lt j} ((-1)^{i+j} v_i(\xi )v_j(\xi )f_if_j + (-1)^{i+j-1} v_i(\xi )v_j(\xi )f_if_j) \\[5pt] &\quad \quad \quad \cdot (v_1\otimes f_1 \wedge \cdots \cdots \widehat {v_i\otimes f_i} \cdots \widehat {v_j\otimes f_j}\cdots \wedge v_k \otimes f_k))\\[5pt] &=0, \end{aligned} \end{align*}
where the hats indicate omission. It follows that
$I$
is an algebra morphism, and a similar argument shows that
$D(I(\xi )) = 0$
, making
$I$
into an analytic DG algebra morphism. It is, moreover, a quasi-isomorphism because the dimension of
$\mathfrak{h}$
is
$\dim _{\mathbb{C}} {\rm Ext}^i(\mathcal{O}_o,\mathcal{O}_o) = \dim _{\mathbb{C}} (T_o{\mathbb{A}}^n)^{\wedge i}$
. By Corollary2.27 it follows that
$\mathfrak{h}$
is equivalent to the analytic minimal model
$\mathcal{H}_{\mathcal{E}}$
of
$\mathfrak{g}_{\mathcal{E}}$
.
It follows easily from [Reference Van den BerghVdB15, Lemma 11.2] that
$\mathfrak{h}$
admits a cyclic structure: for every choice of trace
$\unicode {x03BB}\colon \mathfrak{h}^n \to {\mathbb{C}}$
there is a cyclic structure of the form
Viewing
$\unicode {x03BB}$
as a cocycle in
$\mathsf{C}_\lambda ^{\bullet ,{\rm an}}(\mathfrak{h})$
, one checks that it corresponds to
$\unicode {x03C3}$
along the map in Corollary4.21. The following lemma relates
$\unicode {x03BB}$
to an analytic right CY structure on
$\mathfrak{g}_{\mathcal{E}|_U,c}$
induced by the volume
$\omega$
.
Lemma 5.16.
There exists an open
$U\subset {\mathbb{A}}^n$
and unit/coboundary pair
$(u,h)$
for
$\mathfrak{g}_{\mathcal{E}|_U,c} \subset \mathfrak{g}_{\mathcal{E}}$
with associated quasi-isomorphism
$K_c$
, such that
$(K_c\diamond I)^*\unicode {x03C4}_{\omega |_U}$
is analytically homotopic to a trace
$\unicode {x03BB}$
.
Proof.
Let
$p\colon \mathbb{R} \to \mathbb{R}$
be the smooth function with compact support in
$[-1,1]$
defined by
\begin{align*} p(t) = \left\{\begin{array}{l@{\quad}l} e^{\frac {-t^2}{1-t^2}} & \textrm{if} t \in [-1,1],\\[5pt] 0 & {\rm otherwise}. \end{array}\right. \end{align*}
Then
$q(t) = t^{-1}(p(t) - 1)$
is another smooth function
$q\colon \mathbb{R}\to \mathbb{R}$
and we define, for each
$i=1,\ldots ,n$
, the smooth sections
$u_i \in \mathfrak{g}_{\mathcal{E}|_{{\mathbb{A}}^n}}^0$
and
$h_i\in \mathfrak{g}_{\mathcal{E}|_{{\mathbb{A}}^n}}^{-1}$
by the formulas
\begin{align*} \begin{aligned} u_i(z) &= p(|z_i|^2) \cdot {\rm id}_{\mathcal{E}|_{{\mathbb{A}}^n}} - p'(|z_i|^2)(\partial _{z_i}^* \wedge -) \cdot {\rm d} \overline z_i,\\[5pt] h_i(z) &= q(|z_i|^2)\overline z_i (\partial _{z_i}^*\wedge -), \end{aligned} \end{align*}
where
$\partial _{z_i}^* \in (T_o{\mathbb{A}}^n)^* = V$
is the dual of the standard basis vector
$\partial _{z_i}$
. By inspection, we have
\begin{align*} \begin{aligned} D h_i(z) &= q(|z_i|^2)|z_i|^2 \cdot {\rm id}_{\mathcal{E}|_{{\mathbb{A}}^n}} + (q(|z_i|^2) + q'(|z_i|^2)|z_i|^2)(\partial ^*_{z_i}\wedge -) {\rm d} \overline z_i\\[5pt] &= (p(|z_i|^2) - 1) \cdot {\rm id}_{\mathcal{E}|_{{\mathbb{A}}^n}} - p'(|z_i|^2)(\partial ^*_{z_i}\wedge -) {\rm d} \overline z_i\\[5pt] &= u_i(z) - {\rm id}_{\mathcal{E}|_{{\mathbb{A}}^n}}. \end{aligned} \end{align*}
The element
$u = u_1 \wedge \cdots \wedge u_n$
has the closed polydisc
$\{z \mid |z_i| \leqslant 1 \ \forall i\}$
as its support and can therefore be interpreted as an element of
$\mathfrak{g}_{\mathcal{E}|_U,c}$
for a bounded open neighbourhood
$U$
of the said polydisc. Moreover, it satisfies
$u = {\rm id}_{\mathcal{E}|_{{\mathbb{A}}^n}} + D \widetilde h$
with respect to
\begin{align*} \widetilde h = \sum _{k=1}^n h_k + \sum _{i \lt j} h_i \wedge D h_j + \ldots + \sum _{j_1 \lt \cdots \lt j_{n-1}} h_{j_1} \wedge D h_{j_2} \wedge \cdots \wedge D h_{j_n} + h_1 \wedge D h_2 \wedge \cdots \wedge D h_n. \end{align*}
We want to extend
$(u,\widetilde h)$
to a unit/coboundary pair on all of
$\mathbb{P}^n$
, but note that
$\widetilde h$
blows up at infinity. To remedy this, we can pick any smooth bump function
$\phi$
on
${\mathbb{A}}^n$
with
$\phi |_U=1$
. Then
$\phi \cdot \widetilde h$
has compact support, and hence extends to a form
$i_!(\phi \cdot \widetilde h)$
on
$\mathbb{P}^n$
which satisfies
Now the element
$(1-\phi ) {\rm id}_{\mathcal{E}} + i_!(\overline {\partial } \phi \cdot \widetilde h) \in \mathfrak{g}_{\mathcal{E}}^0$
has support in
$\mathbb{P}^n \setminus U$
, and is therefore given by
$D\unicode {x03B2}$
for some
$\unicode {x03B2}\in \mathfrak{g}_{\mathcal{E}}^{-1}$
with compact support in
$\mathbb{P}^n\setminus U$
. Taking
$h = i_!(\phi \cdot \widetilde h) - \unicode {x03B2}$
then yields the required extension, making
$(u,h)$
into a unit/coboundary pair with
$h|_U = \widetilde h$
. Let
$K_c \colon \mathfrak{g}_{\mathcal{E}} \to \mathfrak{g}_{\mathcal{E}|_U,c}$
be the morphism obtained from Lemma5.6, so that
$I^*K_c^*\unicode {x03C4}_{\omega |_U}$
is an analytic negative cyclic cocycle for
$\mathfrak{h}$
. A computation in polar coordinates shows that the zeroth component maps the shift of
$\xi = \partial _{z_1} \wedge \cdots \wedge \partial _{z_n} \in \mathfrak{h}^n$
to
\begin{align*} \begin{aligned} (I^*K_c^*\unicode {x03C4}_{\omega |_U})_0(s\xi ) &= \int _U p'(|z_1|^2)\cdots p'(|z_n|^2) \cdot {\rm d} z_1\cdots {\rm d} z_n {\rm d} \overline z_1\cdots {\rm d} \overline z_n. \\[5pt] &= (-1)^n \int _0^{2\pi }\int _0^1 p'(r_1^2) r_1 {\rm d} r_1{\rm d} \theta _1 \cdots \int _0^{2\pi }\int _0^1 p'(r_n)^2 r_n {\rm d} r_n{\rm d} \theta _n \\[5pt] &= (-1)^n (\pi p(1) - \pi \cdot p(0))^n = \pi ^n. \end{aligned} \end{align*}
A similar computation shows that the higher components of
$I^*K_c^*\unicode {x03C4}_{\omega |_U}$
vanish, since
\begin{align*} \begin{aligned} (I^*K_c^*\unicode {x03C4}_{\omega |_U})_k(s\xi _1,\ldots ,s\xi _k)(\xi _0) &= \int _{{\mathbb{A}}^n} {\rm d} z_1 \cdots {\rm d} z_n {\rm tr}(u \wedge I(\xi _0) \wedge h \wedge \cdots \wedge h \wedge I(\xi _k)) \\[5pt] &= \sum _{\substack {\alpha \in \mathbb{N}^n\\[5pt] |\alpha | = k}} \int _{{\mathbb{A}}^n} F_{\xi ,\alpha }(|z_1|^2,\ldots ,|z_n|^2) \overline z_1^{\alpha _1} \cdots \overline z_n^{\alpha _n} {\rm d} z_1 \cdots {\rm d} z_n {\rm d} \overline z_1 \cdots {\rm d} \overline z_n \\[5pt] &= \sum _{\substack {\alpha \in \mathbb{N}^n\\[5pt] |\alpha |=k}} (-1)^n\int _{[0,1]^n} F_{\xi ,\alpha }(r_1^2,\ldots ,r_n^2)r^{\alpha+1} {\rm d} r \cdot \prod _{j=1}^n \int _0^{2\pi } e^{-\alpha _j \theta _j \cdot i} {\rm d} \theta _j, \end{aligned} \end{align*}
for some smooth functions
$F_{\xi ,\alpha }\colon \mathbb{R}^n \to \mathbb{R}$
supported on
$[-1,1]^n$
which depend on
$\xi$
and a multi-index
$\alpha$
with
$|\alpha | = \alpha _1+ \ldots + \alpha _n = k$
. For
$k\geqslant 1$
there is at least one
$\alpha _j \neq 0$
, contributing a factor
$\int _0^{2\pi } e^{-\alpha _j \theta _j \cdot i} {\rm d}\theta _j=0$
which makes the term in the sum vanish. It follows that
$(I^*K_c^*\unicode {x03C4}_{\omega |_U})_k=0$
for
$k\geqslant 1$
, and therefore
$\unicode {x03BB} = I^*K_c^*\unicode {x03C4}_{\omega |_U} = (I^*K_c^*\unicode {x03C4}_{\omega |_U})_0$
is a linear functional.
Corollary 5.17.
The pair
$(\mathfrak{h},\unicode {x03C3})$
is equivalent to the cyclic analytic minimal model
$(\mathcal{H}_{\mathcal{E}}^{\omega },\unicode {x03C3}^\omega )$
.
Proof.
Letting
$U$
and
$K_c$
be as in Lemma5.16 above, the map
$K_c\diamond I$
makes
$(\mathfrak{h},\unicode {x03C3})$
into the cyclic analytic minimal model of
$\mathfrak{g}_{\mathcal{E}|_U,c}$
corresponding to the analytic right CY structure
$\unicode {x03C4}_{\omega |_U}$
as in Theorem4.23. It follows that
$K_c \in {{\rm Hom}}_{{\mathsf{Alg}^\infty }}^{{\rm an}}(\mathfrak{g}_{\mathcal{E}},\mathfrak{g}_{\mathcal{E}|_U,c})$
is a quasi-isomorphism such that
is the canonical analytic right CY structure of Theorem5.10, but then it follows from Theorem4.23(iii) that there is a cyclic analytic
$A_\infty$
-isomorphism
$(\mathfrak{h},\unicode {x03C3}) \cong _{{\rm cyc},{\rm an}} (\mathcal{H}_{\mathcal{E}}^\omega ,\unicode {x03C3}^\omega )$
.
Because any point of a smooth variety has an analytic neighbourhood biholomorphic to an open analytic subset of
${\mathbb{A}}^n \subset \mathbb{P}^n$
, we now find a similar result for the cyclic analytic minimal models of arbitrary points.
Proposition 5.18.
Let
$p\in X'$
be a closed point in a smooth projective variety
$X'$
of dimension
$n$
, and let
$\mathcal{E}' \to \mathcal{O}_p$
be any resolution by a perfect complex. Then for every holomorphic volume germ
$\unicode {x03BD} \in (\Omega ^d_{X'})_Z$
the cyclic analytic minimal model is cyclic-analytic
$A_\infty$
-isomorphic to
$(\mathfrak{h},\unicode {x03C3})$
.
Proof.
Let
$Y \subset {\mathbb{A}}^n \subset \mathbb{P}^n$
be a sufficiently small neighbourhood of
$o \in {\mathbb{A}}^n$
so that there is an open embedding
$f\colon Y \to X'$
with
$f(o) = p$
. Then along this map
$f^*\mathcal{O}_p \cong \mathcal{O}_o$
and the volume
$\unicode {x03BD}$
pulls back to a form
for some nonvanishing holomorphic function
$g$
on
$Y$
. Let
$G(z_1,\ldots ,z_n)$
be a holomorphic function such that
${\partial G}/{\partial z_1} = g$
and
$G(0,\ldots ,0)=0$
. Then the map
$\varphi \colon Y \to {\mathbb{A}}^n$
given by
has a Jacobian
$J(\varphi ) = {\rm det} {\partial G_i}/{\partial z_j} = g$
which does not vanish on
$Y$
. Shrinking
$Y$
if necessary, we obtain an open embedding
$\varphi \colon Y \to {\mathbb{A}}^n$
such that
$\varphi ^*\mathcal{O}_o \cong \mathcal{O}_o$
and
Applying Theorem5.13 twice then yields cyclic-analytic
$A_\infty$
-isomorphisms
Acknowledgements
The author thanks Ben Davison and Louis Ioos for interesting discussions. The research for this paper was conducted while the author held a postdoctoral position under Sarah Scherotzke at the University of Luxembourg, whom he thanks for their support. He also thanks an anonymous referee for suggesting important improvements.
Conflicts of Interest
Ben Davison was my former PhD supervisor, and is also on the editorial board for the journal Moduli. The other authors have no conflicts of interest.
Journal Information
Moduli is published as a joint venture of the Foundation Compositio Mathematica and the London Mathematical Society. As not-for-profit organisations, the Foundation and Society reinvest
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