Homotopy associative algebra

In mathematics, an algebra such as (\R,+,\cdot) has multiplication \cdot whose associativity is well-defined on the nose. This means for any real numbers a,b,c\in \R we have

:a\cdot(b\cdot c) - (a\cdot b)\cdot c = 0.

But, there are algebras R which are not necessarily associative, meaning if a,b,c\in R then

:a\cdot(b\cdot c) - (a\cdot b)\cdot c \neq 0

in general. There is a notion of algebras, called A_\infty-algebras, which still have a property on the multiplication which still acts like the first relation, meaning associativity holds, but only holds up to a homotopy, which is a way to say after an operation "compressing" the information in the algebra, the multiplication is associative. This means although we get something which looks like the second equation, the one of inequality, we actually get equality after "compressing" the information in the algebra.

The study of A_\infty-algebras is a subset of homotopical algebra, where there is a homotopical notion of associative algebras through a differential graded algebra with a multiplication operation and a series of higher homotopies giving the failure for the multiplication to be associative. Loosely, an A_\infty-algebra{{Cite book |last=Aspinwall |first=Paul |title=Dirichlet branes and mirror symmetry |date=2009 |publisher=American Mathematical Society |isbn=978-0-8218-3848-8 |oclc=939927173}} (A^\bullet, m_i) is a \Z-graded vector space over a field k with a series of operations m_i on the i-th tensor powers of A^\bullet. The m_1 corresponds to a chain complex differential, m_2 is the multiplication map, and the higher m_i are a measure of the failure of associativity of the m_2. When looking at the underlying cohomology algebra H(A^\bullet, m_1), the map m_2 should be an associative map. Then, these higher maps m_3,m_4,\ldots should be interpreted as higher homotopies, where m_3 is the failure of m_2 to be associative, m_4 is the failure for m_3 to be higher associative, and so forth. Their structure was originally discovered by Jim Stasheff{{cite arXiv|last=Stasheff|first=Jim|author-link=Jim Stasheff|date=2018-09-04|title=L and A structures: then and now|class=math.QA|eprint=1809.02526|language=en}}{{Cite journal|last=Stasheff|first=James Dillon|author-link=Jim Stasheff|date=1963|title=Homotopy Associativity of H-Spaces. II|jstor=1993609|journal=Transactions of the American Mathematical Society|volume=108|issue=2|pages=293–312|doi=10.2307/1993609|issn=0002-9947}} while studying A∞-spaces, but this was interpreted as a purely algebraic structure later on. These are spaces equipped with maps that are associative only up to homotopy, and the A∞ structure keeps track of these homotopies, homotopies of homotopies, and so forth.

They are ubiquitous in homological mirror symmetry because of their necessity in defining the structure of the Fukaya category of D-branes on a Calabi–Yau manifold who have only a homotopy associative structure.

Definition

= Definition =

For a fixed field k an A_\infty-algebra{{Citation |last=Lefèvre-Hasegawa |first=Kenji |title=Sur les A-infini catégories |date=2003-10-21 |arxiv=math/0310337 |id=arXiv:math/0310337}} is a \Z-graded vector space

:A = \bigoplus_{p \in \Z}A_p

equipped with morphisms m_i \colon A^{\otimes i} \to A of degree 2 - i for each i \geq 1 satisfying a coherence condition: for all n,

:\sum_{j+k+l=n,\,j+1+l=i} (-1)^{jk+l} m_i(\mathrm{id}^{\otimes j} \otimes m_k \otimes \mathrm{id}^{\otimes l}) = 0.

An A_\infty-morphism of A_\infty-algebras f: A \to B is a family of morphisms f_i: A^{\otimes i} \to B of degree i-1 satisfying a similar coherence condition: for all n,\sum_{j+k+l=n,\,j+1+l=i} (-1)^{jk+l} f_i(\mathrm{id}^{\otimes j} \otimes m_k \otimes \mathrm{id}^{\otimes l}) = \sum_{i_1+\cdots+i_r=n} (-1)^s m_r(f_{i_1} \otimes \cdots \otimes f_{i_r})where s = \sum_{2 \leq u \leq r}((1-i_u)\sum_{i \leq v \leq u} i_v). (In both coherence conditions, the signs in the sums can be bypassed by shifting the grading by one.)

= Understanding the coherence conditions =

The coherence conditions are easy to write down for low degrees.

== n=1 ==

For n = 1 this is the condition that

:m_1(m_1(a_1)) = 0 ,

since j+1+l=1 gives j=l=0 and thus k=1=i. This means that m_1 is a differential on A.

== n=2 ==

The coherence condition for n=2 gives m_1 \circ m_2 (a_1 \otimes a_2) - m_2 \circ (1 \otimes m_1)(a_1 \otimes a_2) - m_2 \circ (m_1 \otimes 1)(a_1 \otimes a_2) = 0,or m_1(m_2(a_1 \otimes a_2)) = m_2(m_1(a_1) \otimes a_2) + (-1)^

a_1
m_2(a_1 \otimes m_1(a_2)). This is the fact that the multiplication m_2 is a chain map with respect to the differential m_1.

== n=3 ==

In this degree the coherence condition reads

:\begin{align}

m_2(m_2(a_1\otimes a_2)\otimes a_3) - m_2(a_1\otimes m_2(a_2\otimes a_3)) =& +m_3(m_1(a_1)\otimes a_2\otimes a_3) \\

&-m_3(a_1\otimes m_1(a_2)\otimes a_3) \\

& + m_3(a_1\otimes a_2\otimes m_1(a_3)) \\

& + m_1(m_3(a_1\otimes a_2 \otimes a_3)).

\end{align}

Notice that the left hand side of the equation is the failure of the multiplication m_2 to make A into an algebra which is associative on the nose. The right hand side is the differential on A applied to the triple product plus the triple product applied to the differential on A \otimes A \otimes A, and says precisely that associativity holds up to a homotopy given by m_3. In particular, we have that the multiplication induced by m_2 on H_*(A,m_1) is strictly associative.

Note if m_3=0 then (A,m_1) is a differential graded algebra with multiplication m_2, as the vanishing of m_3 means that m_2 is associative on the nose.

== n=4 and higher order terms ==

In higher degrees the coherency conditions give many different terms. We can arrange the right hand side to be a chain homotopy given by m_n as we did in the case of n=3:

:\begin{align}

&\pm m_n(m_1(a_1) \otimes \cdots \otimes a_n)) \\ &\pm \cdots \\

&\pm m_n(a_1 \otimes \cdots \otimes m_1(a_n)) \\

&\pm m_1(m_n(a_1 \otimes \cdots \otimes a_n)),

\end{align}

while the terms on the left hand side indicate the failure of lower m_i terms to satisfy a kind of generalized associativity. In essence, this means that an A_\infty algebra may fail to be "higher-associative" in every degree, but at every degree its failure to be so will be parametrized by a chain homotopy given by the higher multiplication in the next degree.

= Diagrammatic interpretation of axioms =

There is a nice diagrammatic formalism of algebras which is described in Algebra+Homotopy=Operad{{cite arXiv|last=Vallette|first=Bruno|date=2012-02-15|title=Algebra+Homotopy=Operad|class=math.AT|eprint=1202.3245}} explaining how to visually think about this higher homotopies. This intuition is encapsulated with the discussion above algebraically, but it is useful to visualize it as well.

= The bar construction; interpretation as a coderivation =

Since the definition of an A_\infty-algebra requires an infinite sequence of higher multiplications, one might hope that there is a way to repackage the definition in terms of a single structure with finitely many operations. This is possible (after a little setup) by reinterpreting the m_i as components of a single map instead.

Given a (graded) vector space V, the reduced tensor coalgebra \overline{T^c}V on V is \bigoplus_{n \geq 1} V^{\otimes n} with the (non-cocommutative) coproduct \Delta_{\overline{T^c}} given by splitting of tensors, i.e., \Delta(v_1 \otimes \cdots \otimes v_n) = \sum_{1 \leq i < n}(v_1 \otimes \cdots \otimes v_i) | (v_{i+1} \otimes \cdots \otimes v_n), where we write the internal tensor product of \overline{T^c}V with the standard tensor product symbol and the external tensor product used in defining a coproduct with the vertical stroke for clarity. Given any coalgebra C, there is a canonical filtration of C defined by F_kC = \ker \Delta^{(k+1)}, where \Delta^{(2)} = \Delta_C, \Delta^{(n)} = (\mathrm{id}^{\otimes (n-2)} \otimes \Delta_C) \circ \Delta^{(n-1)}; C is called cocomplete if C = \bigcup_k F_kC. The reduced tensor coalgebra is the universal cocomplete coalgebra over V, i.e., for any other cocomplete coalgebra C', there is a natural bijection between the coalgebra maps from C' to \overline{T^c}V and the graded vector space maps C' \to V.

A coderivation on a coalgebra C is a k-module map D: C \to C satisfying the "co-Leibniz rule"\Delta_C \circ D = (D \otimes \mathrm{id} + \mathrm{id} \otimes D) \circ \Delta_C. The suspension SV of a graded vector space V is the graded vector space defined by (SV)^i = V^{i+1}.

With this notation, we have the following fact: an A_\infty-algebra structure on a graded vector space A is the same thing as a coderivation D on \overline{T^c}(SA) which is a differential, that is, D^2 = 0. To see this, note that D is determined by its composite with the quotient \overline{T^c}(SA) \to SA since \overline{T^c}V is the cofree cocomplete coalgebra on V. We obtain the m_n by decomposing the composite into b_n: (SA)^{\otimes n} \to SA and unshifting the map to a map from A^{\otimes n} to A. The condition that D be a coderivation yields D = b_1' + b_2' + b_3' + \cdots, with b_i'(v_1\otimes \cdots \otimes v_j) = \sum_{a+i+b=j} v_1 \otimes \cdots \otimes v_a \otimes b_i(v_{a+1} \otimes \cdots \otimes v_{a+i}) \otimes v_{a+i+1} \otimes \cdots \otimes v_j, and the condition that D^2 = 0 yields \sum_{i+j-1=m} b_i'(b_j'(v_1 \otimes \cdots \otimes v_m)) = 0 for all m, or equivalently \sum_{j+k+l=m,j+1+l=i} b_i(\mathrm{id}^{\otimes j} \otimes b_k \otimes \mathrm{id}^{\otimes l}) = 0, which unshifts to the standard (signed) conditions on the m_n due to the sign rule for shifting complexes. The differential graded coalgebra (\overline{T^c}(SA),D) defined in this way is called the bar construction on A and denoted BA.

Many notions are easier to write out by considering A_\infty-algebras via their bar constructions. For instance, a morphism f: A \to A' of A_\infty-algebras is equivalently a morphism of differential graded coalgebras Bf: BA \to BA', a quasiisomorphism of A_\infty-algebras is equivalently a quasiisomorphism of differential graded coalgebras, and a homotopy between A_\infty-algebra morphisms is equivalently a homotopy between differential graded coalgebra morphisms.

Examples

= Associative algebras =

Every associative algebra (A,\cdot) has an A_\infty-infinity structure by defining m_2(a,b) = a\cdot b and m_i = 0 for i \neq 2. Hence A_\infty-algebras generalize associative algebras.

= Differential graded algebras =

Every differential graded algebra (A^\bullet, d) has a canonical structure as an A_\infty-algebra where m_1 = d and m_2 is the multiplication map. All other higher maps m_i are equal to 0. Using the structure theorem for minimal models, there is a canonical A_\infty-structure on the graded cohomology algebra HA^\bullet which preserves the quasi-isomorphism structure of the original differential graded algebra. One common example of such dga's comes from the Koszul algebra arising from a regular sequence. This is an important result because it helps pave the way for the equivalence of homotopy categories

\text{Ho}(\text{dga}) \simeq \text{Ho}(A_\infty\text{-alg})
of differential graded algebras and A_\infty-algebras.

= Cochain algebras of H-spaces =

One of the motivating examples of A_\infty-algebras comes from the study of H-spaces. Whenever a topological space X is an H-space, its associated singular chain complex C_*(X) has a canonical A_\infty-algebra structure from its structure as an H-space.

= Example with infinitely many non-trivial m<sub>i</sub> =

Consider the graded algebra V^\bullet = V_0\oplus V_1 over a field k of characteristic 0 where V_0 is spanned by the degree 0 vectors v_1,v_2 and V_1 is spanned by the degree 1 vector w.{{Cite web|last1=Allocca|first1=Michael|last2=Lada|first2=Thomas|date=|title=A Finite Dimensional A-infinity algebra example|url=https://lada.math.ncsu.edu/FinDimAInfEx-final.pdf|url-status=live|archive-url=https://web.archive.org/web/20200928010418/https://lada.math.ncsu.edu/FinDimAInfEx-final.pdf|archive-date=28 Sep 2020|access-date=|website=}}{{Cite journal|last1=Daily|first1=Marilyn|last2=Lada|first2=Tom|date=2005|title=A finite dimensional $L_\infty$ algebra example in gauge theory|url=https://projecteuclid.org/euclid.hha/1139839375|journal=Homology, Homotopy and Applications|language=EN|volume=7|issue=2|pages=87–93|doi=10.4310/HHA.2005.v7.n2.a4|issn=1532-0073|doi-access=free}} Even in this simple example there is a non-trivial A_\infty-structure which gives differentials in all possible degrees. This is partially due to the fact there is a degree 1 vector, giving a degree k vector space of rank 1 in (V^\bullet)^{\otimes k}. Define the differential m_1 by

:\begin{align}

m_1(v_0) = w \\

m_1(v_1) = w,

\end{align}

and for d \geq 2

:\begin{align}

m_d(v_1\otimes w^{\otimes k}\otimes v_1\otimes w^{\otimes (d-2)-k}) &=(-1)^ks_dv_1 & 0 \leq k \leq d-2 \\

m_d(v_1\otimes w^{\otimes (d-2)}\otimes v_2)&= s_{d+1}v_1 \\

m_d(v_1\otimes w^{\otimes (d-1)}) &= s_{d+1}w,

\end{align}

where m_n = 0 on any map not listed above and s_n = (-1)^{(n-1)(n-2)/2}. In degree d=2, so for the multiplication map, we have

\begin{align}

m_2(v_1,v_1)&= -v_1 \\

m_2(v_1,v_2)&= v_1 \\

m_2(v_1,w)&= w.

\end{align}

And in d=3 the above relations give

:\begin{align}

m_3(v_1,v_1,w) &= v_1 \\

m_3(v_1,w,v_1) &= -v_1 \\

m_3(v_1,w,v_2) &= -v_1 \\

m_3(v_1,w,w) &= -w.

\end{align}

When relating these equations to the failure for associativity, there exist non-zero terms. For example, the coherence conditions for v_1,v_2,w will give a non-trivial example where associativity doesn't hold on the nose. Note that in the cohomology algebra H^*(V^\bullet, [m_2]) we have only the degree 0 terms v_1,v_2 since w is killed by the differential m_1.

Properties

= Transfer of A<small>∞</small> structure =

One of the key properties of A_\infty-algebras is their structure can be transferred to other algebraic objects given the correct hypotheses. An early rendition of this property was the following: Given an A_\infty-algebra A^\bullet and a homotopy equivalence of complexes

:f\colon B^\bullet \to A^\bullet,

then there is an A_\infty-algebra structure on B^\bullet inherited from A^\bullet and f can be extended to a morphism of A_\infty-algebras. There are multiple theorems of this flavor with different hypotheses on B^\bullet and f, some of which have stronger results, such as uniqueness up to homotopy for the structure on B^\bullet and strictness on the map f.{{cite arXiv|last=Burke|first=Jesse|date=2018-01-26|title=Transfer of A-infinity structures to projective resolutions|class=math.KT|eprint=1801.08933}}

Structure

= Minimal models and Kadeishvili's theorem =

One of the important structure theorems for A_\infty-algebras is the existence and uniqueness of minimal models – which are defined as A_\infty-algebras where the differential map m_1 = 0 is zero. Taking the cohomology algebra HA^\bullet of an A_\infty-algebra A^\bullet from the differential m_1, so as a graded algebra,

:HA^\bullet = \frac{\text{ker}(m_1)}{m_1(A^\bullet)},

with multiplication map [m_2]. It turns out this graded algebra can then canonically be equipped with an A_\infty-structure,

:(HA^\bullet, 0, [m_2], m_3,m_4,\ldots),

which is unique up-to quasi-isomorphisms of A_\infty-algebras.{{cite arXiv|last=Kadeishvili|first=Tornike|date=2005-04-21|title=On the homology theory of fibre spaces|eprint=math/0504437}} In fact, the statement is even stronger: there is a canonical A_\infty-morphism

:(HA^\bullet, 0, [m_2], m_3,m_4,\ldots) \to A^\bullet,

which lifts the identity map of A^\bullet. Note these higher products are given by the Massey product.

== Motivation ==

This theorem is very important for the study of differential graded algebras because they were originally introduced to study the homotopy theory of rings. Since the cohomology operation kills the homotopy information, and not every differential graded algebra is quasi-isomorphic to its cohomology algebra, information is lost by taking this operation. But, the minimal models let you recover the quasi-isomorphism class while still forgetting the differential. There is an analogous result for A∞-categories by Maxim Kontsevich and Yan Soibelman, giving an A∞-category structure on the cohomology category H^*(D^b_\infty(X)) of the dg-category consisting of cochain complexes of coherent sheaves on a non-singular variety X over a field k of characteristic 0 and morphisms given by the total complex of the Cech bi-complex of the differential graded sheaf \mathcal{Hom}^\bullet(\mathcal{F}^\bullet,\mathcal{G}^\bullet)pg 586-593. In this was, the degree k morphisms in the category H^*(D^b_\infty(X)) are given by \text{Ext}(\mathcal{F}^\bullet,\mathcal{G}^\bullet).

== Applications ==

There are several applications of this theorem. In particular, given a dg-algebra, such as the de Rham algebra (\Omega^\bullet(X),d,\wedge), or the Hochschild cohomology algebra, they can be equipped with an A_\infty-structure.

= Massey structure from DGA's =

Given a differential graded algebra (A^\bullet, d) its minimal model as an A_\infty-algebra (HA^\bullet, 0, [m_2], m_3,m_4,\ldots) is constructed using the Massey products. That is,

:\begin{align}

m_3(x_3,x_2,x_1) &= \langle x_3,x_2,x_1 \rangle \\

m_4(x_4,x_3,x_2,x_1) &= \langle x_4, x_3,x_2,x_1 \rangle \\

&\cdots &

\end{align}

It turns out that any A_\infty-algebra structure on HA^\bullet is closely related to this construction. Given another A_\infty-structure on HA^\bullet with maps m_i', there is the relation{{cite arXiv|last1=Buijs|first1=Urtzi|last2=Moreno-Fernández|first2=José Manuel|last3=Murillo|first3=Aniceto|date=2019-02-19|title=A-infinity structures and Massey products|class=math.AT|eprint=1801.03408}}

:m_n(x_1,\ldots,x_n) = \langle x_1,\ldots, x_n\rangle + \Gamma,

where

:\Gamma \in \sum_{j=1}^{n-1} \text{Im}(m_j).

Hence all such A_\infty-enrichments on the cohomology algebra are related to one another.

= Graded algebras from its ext algebra =

Another structure theorem is the reconstruction of an algebra from its ext algebra. Given a connected graded algebra

:A = k_A \oplus A_1 \oplus A_2 \oplus \cdots,

it is canonically an associative algebra. There is an associated algebra, called its Ext algebra, defined as

:\operatorname{Ext}_A^\bullet(k_A,k_A),

where multiplication is given by the Yoneda product. Then, there is an A_\infty-quasi-isomorphism between (A,0,m_2,0,\ldots) and \operatorname{Ext}_A^\bullet(k_A,k_A). This identification is important because it gives a way to show that all derived categories are derived affine, meaning they are isomorphic to the derived category of some algebra.

See also

References

{{refbegin}}

  • {{cite arXiv |eprint=1202.3245 |title=Algebra+Homotopy=Operad |last1 = Vallette|first1 = Bruno|year = 2012|class = math.AT}}
  • {{cite arXiv |eprint=hep-th/9408064|title=A-infinity Algebras and the Cohomology of Moduli Spaces |last1=Penkava |first1=Michael |last2=Schwarz |first2=Albert |year=1994 }}
  • {{cite journal |arxiv=0909.3222|title=Uniqueness of A-infinity-structures and Hochschild cohomology |year=2011 |doi=10.2140/agt.2011.11.107 |last1=Roitzheim |first1=Constanze |last2=Whitehouse |first2=Sarah |journal=Algebraic & Geometric Topology |volume=11 |pages=107–143 |s2cid=115160163 }}
  • {{cite arXiv |eprint=alg-geom/9411018|title=Homological Algebra of Mirror Symmetry|last1=Kontsevich|first1=Maxim|year=1994}} — Original paper linking A_\infty structures to Mirror symmetry
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  • {{cite arXiv |eprint=math/0604379|title=Constructible Sheaves and the Fukaya Category |last1=Nadler |first1=David |last2=Zaslow |first2=Eric |year=2006 }}
  • {{cite arXiv |eprint=math/0310414|title=Homological mirror symmetry for the quartic surface |last1=Seidel |first1=Paul |year=2003 }}
  • {{cite thesis |last=Zhou |first=Jiawei |type=PhD |url=https://escholarship.org/uc/item/7v313232 |title=On the Construction of Minimal Model for Some A-infinity Algebras |year=2019 |publisher=UC Irvine |id=7v313232}}
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{{refend}}

Category:Homotopical algebra

Category:Homological algebra

Category:Algebraic geometry

Category:Homotopy theory