Open Access
Issue
Emergent Scientist
Volume 3, 2019
Article Number 4
Number of page(s) 17
Section Mathematics
DOI https://doi.org/10.1051/emsci/2019003
Published online 04 June 2019

© B. Reinhold, published by EDP Sciences, 2019

Licence Creative CommonsThis is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

1 Introduction

L-algebras (also called strongly homotopy Lie algebras) were first introduced in [1] and [2] and are a generalisation of graded Lie algebras in which a system of antisymmetric n-ary brackets satisfies a generalised Jacobi identity. The first part of this article serves as a self-contained introduction to L-algebras, in which we discuss different characterisations of L-algebras and their representations (up to homotopy), closely following [3].

The L-algebra cohomology with values in the adjoint representation was introduced in [4] using a Lie bracket on the space of cochains. We extend this approach to arbitrary representations, which leads to a characterisation of certain L-algebras as abelian extensions of L-algebras by 2-cocycles. This generalises a theorem from [5] that characterises certain L-algebras in terms of Lie algebra cohomology.

This article is largely based on my same-titled Bachelor’s thesis, which I wrote under the supervision of Chenchang Zhu at the University of Göttingen in 2018.

2 Mathematical background

In this section, we discuss exterior and symmetric powers, algebras and coalgebras in the graded framework. In particular, we show that antisymmetric and symmetric maps are related by a shift in degree and that coderivations of the symmetric coalgebra are in one-to-one correspondence with their weight one components. These results are later key to the characterisations of L-structures in terms of symmetric brackets and codifferentials. The main references for this section are [3,4,6,7].

2.1 Graded vector spaces

A graded vector space is a vector space V together with a decomposition V p V p $V \cong \bigoplus_{p \in\Z}V_p$ for a family of vector spaces { V p } p $\{V_p\}_{p\in\Z}$. An element vV p is then called homogeneous of degree p and we write |v| = p.

Here and subsequently, we assume all vector spaces to be over a fixed ground field k ${\mathbb k}$ of characteristic zero. We always denote by V and W graded vector spaces and by v1, …, vnV arbitrary homogeneous elements.

A linear map f : VW is called homogeneous (of degree p) if there is p $p\in \Z$ such that f(V n) ⊂ Wn+p for all n $n \in \Z$. We denote by Hom p(V, W) the vector space of all homogeneous linear maps VW of degree p and by Hom (V, W) the graded vector space p Hom p (V,W) $\bigoplus_{p\in \Z}\Hom_p(V,W)$. Elements in Hom0(V, W) are also called degree preserving.

Note that we can identify ungraded vector spaces with graded ones that are concentrated in degree zero, that is V k = 0 for k≠ 0.

There is a canonical grading on the direct sum of V and W given by (VW) p = V p W p $(V\oplus W)_p=V_p\oplus W_p$. The isomorphism VW p i+j=p ( V i W j ) \[ V\otimes W \cong \bigoplus_{p \in \Z} \bigoplus_{i+j=p}\left(V_i\otimes W_j\right) \]

allows us to define a grading on VW by ( VW ) p = i+j=p ( V i W j ). \[\left(V\otimes W\right)_p = \bigoplus_{i+j=p}\left(V_i\otimes W_j\right). \]

This extends to a grading on V n i=1 n V ${V^{\otimes n}} \vcentcolon=\bigotimes_{i=1}^nV$ given by ( V n ) p = i 1 ++ i n =p V i 1 V i n . \[({V^{\otimes n}})_p=\bigoplus_{i_1+\dotsc +i_n=p}V_{i_1}\otimes \dotsc \otimes V_{i_n}. \]

We denote by τV,W the linear degree preserving map τ V,W :VWWV,vw (1) |v||w| wv. \[ \tau_{V,W}\colon V\otimes W\to W\otimes V,\quad v\otimes w\mapsto (-1)^{|v||w|}w\otimes v. \]

If f ∈ Hom(V, W) and g ∈ Hom(V ′, W′) are homogeneous for graded vector spaces V ′ and W′, we define the linear map fg: VV ′→ WW′ by (fg)(v v )= (1) |v||g| f(v)g( v ) \begin{equation*}(f\otimes g) (v\otimes v')= (-1)^{|v| |g|}f(v)\otimes g(v') \end{equation*}(1)

for vV , v′ ∈ V ′ homogeneous. Note that |fg| = |f| + |g|. This generalises to tensor products of three or more vector spaces in the obvious way and we abbreviate f ⊗ … ⊗ f : V nWn to fn .

For the composition of such functions, (1) implies ( f g )(fg)= (1) | g ||f| ( f f)( g g), \begin{equation*}(f' \otimes g')\circ (f\otimes g)= (-1)^{|g'||f|}(f'\circ f)\otimes (g'\circ g), \end{equation*}(2)

when f′ and g′ are homogeneous linear maps with domains W and W′, respectively.

When working in the framework of graded vector spaces, the general rule of thumb for the signs is that whenever two “graded symbols” of degree p and q, respectively, change their order in an equation, there should be the sign (1) |p||q| $(-1)^{|p||q|}$. This is called the Koszul sign convention.

We denote by 𝔖n the symmetric group, the group of all permutations of the set {1, …, n}, and by si𝔖n for 1 ≤ in − 1 the transposition with si(i) = i + 1 and si (i + 1) = i. There are two canonical linear right actions of 𝔖n on V n. These are given on the generating subset {s1, …sn−1}⊂ 𝔖n by ε ^ ( s i )( v 1 v n ) = (1) | v i || v i+1 | v 1 v i1 v i+1 v i v i+2 v n , χ ^ ( s i )( v 1 v n ) = (1) | v i || v i+1 | v 1 v i1 v i+1 v i v i+2 v n . \begin{align*} \hat{\varepsilon}(s_i)(v_1\otimes\dotsc\otimes v_n) &=(-1)^{|v_i||v_{i+1}|}v_1\otimes \dotsc \otimes v_{i-1}\\ &\quad\otimes v_{i+1} \otimes v_i \otimes v_{i+2}\otimes \dotsc \otimes v_n,\\ \hat{\chi}( s_i)(v_1\otimes\dotsc\otimes v_n) &= -(-1)^{|v_i||v_{i+1}|}v_1\otimes \dotsc \otimes v_{i-1}\\ &\quad\otimes v_{i+1} \otimes v_i \otimes v_{i+2}\otimes \dotsc \otimes v_n. \end{align*}

We call ε ^ $\hatsilon$ and χ ^ $\hat\chi$ the (graded) symmetric and (graded) antisymmetric action of 𝔖n on V n, respectively. Note that ε ^ (σ) $\hatsilon(\sigma)$ is degree preserving for all σ𝔖n as ε ^ (σ)( v 1 v n )=± v σ(1) v σ(n) . \begin{equation*}\hat\varepsilon(\sigma)(v_1\otimes\dotsc\otimes v_n)=\pm v_{\sigma(1)}\otimes\dotsc\otimes v_{\sigma(n)}. \end{equation*}(3)

We then denote the sign in (3) by ε(σ;v1, …, vn) and similarly by χ(σ;v1, …, vn) the sign such that χ ^ (σ)( v 1 v n )=χ(σ; v 1 ,, v n ) v σ(1) v σ(n) . \[\hat\chi(\sigma)(v_1\otimes\dotsc\otimes v_n)=\chi(\sigma;v_1,\dots,v_n)v_{\sigma(1)}\otimes\dotsc\otimes v_{\sigma(n)}.\]

We abbreviate ε(σ;v1, …, vn) and χ(σ;v1, …, vn) to ε(σ) and χ(σ), when no confusion can arise.

Let USV n be the graded subspace spanned by all elements of the form v 1 v n ε ^ (σ)( v 1 v n ) \[ v_1\otimes\dotsc\otimes v_n-\hatsilon(\sigma)(v_1\otimes\dotsc\otimes v_n) \]

for σ𝔖n. The space S n (V) V n / U S $\Sy^n(V)\vcentcolon= {V^{\otimes n}}/U_S$ is called the nth symmetric power of V . Similarly, the nth exterior power of V is defined as the quotient of V n by the graded subspace spanned by all elements of the form v 1 v n χ ^ (σ)( v 1 v n ) \[ v_1\otimes\dotsc\otimes v_n-\hat\chi(\sigma)(v_1\otimes\dotsc\otimes v_n) \]

for σ𝔖n and is denoted by ∧nV.

An n-linear map f : V nW is called (graded) symmetric iffor all σ𝔖n f( v 1 ,, v n )=ε(σ)f( v σ(1) ,, v (n) ) \[ f(v_1,\dotsc,v_n)=\varepsilon(\sigma)f(v_{\sigma(1)},\dotsc, v_{(n)}) \]

holds. We can write this conveniently as f ε ^ (σ)=f $f\circ \hatsilon(\sigma)=f$. Similarly, f is called (graded) antisymmetric if f χ ^ (σ)=f $f\circ \hat\chi(\sigma)=f$ for all σ𝔖n.

Proposition 1. Let f : V nW be a symmetric linear map. There is a unique linear map φ: S n (V)W $\varphi\colon\Sy^n(V)\to W$ such that the following diagram commutes: where π S : V n S n (V) $\pi_S\colon {V^{\otimes n}} \to \Sy^n(V)$ is the canonical projection.

Proof. As f is symmetric, it vanishes on the generators of US and factors through πS to a linear map φ: S n (V)W $\varphi\colon \Sy^n(V)\to W$ such that the diagram above commutes. This map is unique as πS is surjective.

Remark 2. As the symmetric 𝔖n-action on Vn is degree preserving, S n (V) $\Sy^n(V)$ inherits a canonical grading from V n such that πS is degree preserving. It is then immediate that if f is homogeneous in Proposition 1, so is the map φ and |φ| = |f|. As πS is symmetricby construction of S n (V) $\Sy^n(V)$, Proposition 1 yields an isomorphism between the subspace of Hom(V n, W) consisting of all symmetric maps and Hom( S n (V),W) $\Hom(\Sy^n(V),W)$. An analogue of Proposition 1 holds for ∧ nV and induces an isomorphism between the subspace Hom(V n, W) of all anti-symmetric maps and Hom(∧ nV, W).

An element in V n is called symmetric if it is invariant under the symmetric 𝔖n-action on V n. We claim that S n (V) $\Sy^n(V)$ is isomorphic to the subspace of V n of all symmetric elements. Indeed, letting v1 ∨… ∨ vn denote the image of v1 ⊗… ⊗ vn under πS, the linear map φ: S n (V) V n , x 1 x n 1 n! σ S n ε(σ) x σ(1) x σ(n) \[ \begin{array}{l} \varphi\colon \Sy^n(V)\to {V^{\otimes n}}, \\ x_1\vee\dotsc\vee x_n\mapsto \frac{1}{n!}\sum_{\sigma\in \mathfrak S_n}\varepsilon(\sigma)x_{\sigma(1)}\otimes\dotsc\otimes x_{\sigma(n)} \end{array} \]

is well-defined and satisfies π S φ= id S n (V) $\pi_S\circ \varphi=\id_{\Sy^n(V)}$ and φ π S = 1 n! σ S n ε ^ (σ) $\varphi\circ \pi_S=\frac{1}{n!}\sum_{\sigma\in\mathfrak S_n}\hatsilon(\sigma)$. As the latter is a projection of V n onto said subspace, the claim follows. A similar statement clearly holds for ∧nV .

For n $n\in\Z$, we defProposition2 ine the graded vector space V [n] to be the vector space V with the grading defined by V [n] p = V p+n $V[n]_p= V_{p+n}$. We denote by n: VV [n] the identity map on V , which becomes a linear isomorphism of degree − n, and by n its inverse. We abbreviate 1 and 1 to and , respectively. Note that ( k ) 1 = (1) k(k1) 2 k $(\downarrow^{\otimes k})^{-1}=(-1)^{\frac{k(k-1)}{2}}\uparrow^{\otimes k}$ as a consequence of (2).

Proposition 3 (The décalage isomorphism). For σ𝔖n,

ε ^ (σ) n = n χ ^ (σ). \begin{equation*}\hat\varepsilon(\sigma)\circ \downarrow^{\otimes n} = \downarrow^{\otimes n} \circ \hat\chi(\sigma). \end{equation*}(4)

There is then a degree preserving isomorphism S n (V[1])( \Asy n V )[n]. \begin{equation*}\Sy^n(V[1])\cong\left(\Asy^n V\right)[n]. \end{equation*}(5)

Proof. Note that for the first part, we only have to check (4) on the generating subset {s1 , …, sn−1}⊂ 𝔖n. This is an easy computation left to the reader. Let πA: V n →∧nV be the canonical projection. The linear maps \begin{array}{@{}c@{}c@{}l@{}}nn& π S &^n: V n S(V[1]), (1) n(n1) 2 & π A &^n: (V[1]) n  \Asy n Vnn\end{array} \[ \begin{array}{@{}c@{}c@{}l@{}} &\pi_S\circ \downarrow&^{\otimes n}\colon {V^{\otimes n}} \to \Sy(V[1]),\\ (-1)^{\frac{n(n-1)}{2}}&\pi_A\circ\uparrow&^{\otimes n}\colon (V[1])^{\otimes n}\to \Asy^n V \end{array} \]

are then antisymmetric and symmetric, respectively. The induced linear maps between S(V[1]) $\Sy(V[1])$ and ∧nV are then easily seen to be inverse to each other. As these maps are of degree − n and n, respectively, we obtain a degree preserving isomorphism S(V[1])( \Asy n V)[n] $\Sy(V[1])\cong \big(\Asy^n V\big)[n]$.

Corollary 1. There is for each p $p\in\Z$ a one-to-one correspondence between symmetric linear maps λ: (V[1]) n V[1] $\lambda\colon (V[1])^{\otimes n}\to V[1]$ of degree p and antisymmetric linear maps l: V nV of degree p + 1 − n given by

l =λ n , λ = (1) n(n1) 2 l n . \[ \begin{array}{@{}l@{}l@{}} l&=\uparrow\circ\lambda \circ \downarrow^{\otimes n},\\ \lambda&=(-1)^{\frac{n(n-1)}{2}}\downarrow\circ l\circ \uparrow^{\otimes n}. \end{array} \]

A differential on the graded vector space V is a linear map d: VV of degree one such that d2 = 0. We then callthe pair (V, d) a differential graded vector space (DG vector space for short). A homomorphism between DG vector spaces (V, d) and (W, d′) is a degree preserving linear map f : VW such that d′ ○ f = fd.

DG vector spaces are sometimes called cochain complexes. Given a cochain complex (V, d), one then calls an element vV n an n-cocycle if d(v) = 0 and an n-coboundary if v = d(w) for some wV n−1. The graded vector space H(V ) = ker(d)∕im(d) measures the non-exactness of the sequence d V n1 d V n d V n+1 d \[\cdots\xrightarrow{d} V_{n-1} \xrightarrow{d} V_n \xrightarrow{d}V_{n+1} \xrightarrow{d}\cdots\]

and is called the cohomology of (V, d). We then call H n (V)= \frac{{ $H_n(V)= \frac{\text{$ the nth cohomology group.

2.2 Graded algebras

By an algebra we mean a vector space A together with a linear map μ: AAA; the multiplication μ is in generalnot assumed to be associative.

A graded algebra A is an algebra that is also a graded vector space in which the multiplication is degree preserving. If also ab= (1) |a||b| ba $a b=(-1)^{|a||b|}b a$ for all a, bA, we call A (graded) commutative. A homomorphism of graded algebras is a degree preserving algebra homomorphism.

A (two-sided) ideal I in A is called homogeneous if IA is a graded subspace. Note that an ideal is homogeneous if and only if it is spanned by homogeneous elements.

Remark 5. If IA is a homogeneous ideal, the canonical isomorphism A/I n A n / I n $A/I\cong \bigoplus_{n\in \Z} A_n/I_n$ makes AI into a graded algebra such that the canonical projection AAI is a homomorphism of graded algebras.

Remark 6. Let A and B be two graded associative algebras. The multiplication defined by (ab)( a b )= (1) |b|| a | a a b b . \begin{equation*}(a\otimes b)(a'\otimes b')= (-1)^{|b||a'|}a a'\otimes b b'. \end{equation*}(6) for a, a′∈ A, b, b′ ∈ B homogeneous makes AB into a graded associative algebra. If A and B are both unital/commutative, then so is AB.

Example 7 (The tensor algebra). We denote by T(V ) := ⊕ n≥0V n the tensor algebra of V . It carries the multiplication induced by the canonical isomorphism V rV sV ⊗(r+s), making it into a unital associative algebra. The grading on T(V ) induced by the grading on V n is given by T (V) p = i 1 ++ i n =p V i 1 V i n \[ T(V)_p= \bigoplus_{i_1+\dotsc+i_n=p} V_{i_1}\otimes\dotsc\otimes V_{i_n} \] and is calledthe interior grading. On the other hand, T(V ) carries the grading given by T(V ) = ⊕ n≥0V n, which is called the exterior grading or grading by weight. If not specified otherwise, we always understand T(V ) to carry its interior grading. Note that both gradings make T(V ) into a graded algebra.

Example 8 (The symmetric and exterior algebra). Let IST(V ) be the two-sided homogeneous ideal generated by elements of the form v 1 v 2 (1) | v 1 || v 2 | v 2 v 1 $v_1\otimes v_2 - (-1)^{|v_1||v_2|}v_2\otimes v_1$. We call S(V)T(V)/ I S $\Sy(V)\vcentcolon= T(V)/I_S$ the symmetric algebra of V . Similarly, the exterior algebra of V , denoted by ∧ V , is defined as the quotient of T(V ) by the two-sided homogeneous ideal generated by elements of the form v 1 v 2 + (1) | v 1 || v 2 | v 2 v 1 $v_1\otimes v_2 + (-1)^{|v_1||v_2|}v_2\otimes v_1$. We denote the multiplication in S(V) $\Sy(V)$ and ∧ V by ∨ and ∧, respectively. Note that S(V) $\Sy(V)$ and ∧ V also admit an exterior grading or grading by weight: as V nIS = US, we have S(V)= n0 S n (V) $\Sy(V)=\bigoplus_{n\geq 0}\Sy^n(V)$ and similarly ∧ V = ⊕ n≥0nV.

It is easy to see that if A is a graded unital associative algebra, there is for each linear degree preserving map f : VA a unique homomorphism of unital graded algebras φ: T(V ) → A that agrees on V with f (see for example [6], Proposition 1.1.1). It is then immediate that if A is commutative, φ factors to a unique homomorphism of unital graded algebras S(V)A $\Sy(V)\to A$. Applying this to the linear map VWS(V)S(W),(v,w)v1+1w \[V\oplus W\to \Sy(V)\otimes \Sy(W), \quad (v,w)\mapsto v\otimes 1 + 1\otimes w\] yields a homomorphism of graded unital algebras S(VW)S(V)S(W) $\Sy(V\oplus W)\to \Sy(V)\otimes \Sy(W)$ that is easilyseen to be an isomorphism with inverse S(V)S(W)S(VW) $\Sy(V)\otimes \Sy(W)\to \Sy(V\oplus W)$, vwvw. With a slight modification of the sign in (6), similar arguments show that ∧ (VW)≅∧ V ⊗∧ W. In particular, we have nn\Sy n (VW) p+q=n S p (V) S q (W), \begin{equation*} \Sy^n(V\oplus W)\cong \bigoplus_{p+q=n}\Sy^p(V)\otimes \Sy^q(W),\end{equation*}(7) nn\Asy n (VW) p+q=n \Asy p V  \Asy q W. \begin{equation*} \Asy^n(V\oplus W)\cong \bigoplus_{p+q=n}\Asy^p V \otimes \Asy^q W. \end{equation*}(8)

For a graded algebra A, a derivation of A of degree p is a linear map d: AA of degree p satisfying d(ab)=d(a)b+ (1) p|a| ad(b) \[ d(ab)=d(a)b+(-1)^{p|a|}ad(b) \]

for all a, bA homogeneous. We denote by Derp(A) the vector space of all derivations of A of degree p and by Der (A) the graded vector space p \Der p (A) $\bigoplus_{p\in\Z}\Der_p(A)$. A differential on the graded algebra A is an element d ∈Der(A) of degree one such that d2 = 0. The pair (A, d) is then called a differential graded algebra (DG algebra for short). A homomorphism of DG algebras is a homomorphism of graded algebras that is also a homomorphism of DG vector spaces.

2.3 Graded Lie algebras and unshuffle permutations

Definition 9. A graded Lie algebra is a graded vector space L together with a (graded) antisymmetric degree preserving linear map [⋅, ⋅]: LLL called the Lie bracket satisfying the (graded) Jacobi identity [x,[y,z]]=[[x,y],z]+ (1) |x||y| [y,[x,z]]=0 \begin{equation*}[x,[y,z]]=[[x,y],z]+(-1)^{|x||y|}[y,[x,z]]=0 \end{equation*}(9)

for all x, y, zL homogeneous.

If L is ungraded, we recover the usual definition of a Lie algebra. Note that (9) is nothing else than [x, ⋅ ] being a derivation of the graded algebra (L, [⋅, ⋅]).

Example 10. For a graded associative algebra A, we define the graded commutator [⋅, ⋅]: AAA by [a,b]=ab (1) |a||b| ba $[a,b]= ab-(-1)^{|a||b|}ba$ for a, bA homogeneous. This makes A into a graded Lie algebra. In particular, 𝔤𝔩(V ) := Hom(V, V ) becomes a graded Lie algebra. If V is itself a graded algebra, one can check that Der(V ) ⊂ 𝔤𝔩(V ) is a Lie subalgebra.

Definition 11. A differential graded Lie algebra (DGLA for short) is a DG algebra in which the underlying algebra is a graded Lie algebra.

Example 12. Let L be a graded Lie algebra and xL a degree one element such that 1 2 [x,x]=0 $\frac{1}{2}[x,x]=0$. Then d := [x, ⋅ ] satisfies d2 = 0 by the Jacobi identity (9) and (L, [⋅, ⋅], d) is a DGLA. In particular, for (V, ) a DG vector space, this makes (𝔤𝔩(V ), [⋅, ⋅], [, ⋅ ]) canonically into a DGLA as 1 2 [,]= 2 =0 $\frac{1}{2}[\partial,\partial]=\partial^2=0$.

Definition 13. For a DGLA (L, [⋅, ⋅], d), a Maurer–Cartan element is an element xL of degree one such that d(x)+ 1 2 [x,x]=0. \begin{equation*}d(x)+\frac{1}{2}[x,x]=0. \end{equation*}(10)

The equation (10) is called the Maurer–Cartan equation.

Example 14. Let (L, [⋅, ⋅], d = [x, ⋅ ]) be as in Example 12. For yL of degree one, we then have 1 2 [x+y,x+y]=0 $\frac{1}{2}[x+y,x+y]=0$ if and only if y satisfies the Maurer–Cartan equation.

For 0 ≤ in, an (i, ni)-unshuffle is a permutation σ𝔖n satisfying σ(1) < … < σ(i) and σ(i + 1) < … < σ(n). Following the notation in [3], we denote the set of all (i, ni)-unshuffles by \Sh i,ni 1 S n ${\Sh^{-1}_{{i,n-i}}}\subset\mathfrak S_n$. Using the antisymmetry of the Lie bracket, one can rewrite (9) as σ \Sh 2,1 1 χ(σ)[[ x σ(1) , x σ(2) ], x σ(3) ]=0 \begin{equation*}\sum_{\sigma\in\Sh^{-1}_{2,1}}\chi(\sigma)[[x_{\sigma(1)},x_{\sigma(2)}],x_{\sigma(3)}]=0 \end{equation*}(11)

for all x1, x2, x3L homogeneous.

Lemma 15. Each element σ𝔖n has for each i ∈{0, …, n} a unique decomposition σ = τ(α, β), where τ  \Sh i,ni 1 $\tau\in \Sh^{-1}_{i,n-i}$ and (α, β) ∈ 𝔖i × 𝔖ni. Here, 𝔖i × 𝔖ni is considered as a subgroup of 𝔖n in the obvious way.

Proof. Clearly, τ has to be the unique (i, ni)-unshuffle such that {τ(1), …, τ(i)} = {σ(1), …, σ(i)} and {τ(i + 1), …, τ(n)} = {σ(i + 1), …, σ(n)}. We then have τ−1σ𝔖i × 𝔖ni.

2.4 Graded coalgebras

A (graded) coalgebra (C, Δ) is a graded vector space C together with a degree preserving linear map Δ: CCC called the coproduct. If the diagram

commutes, C is called coassociative. We call C counital if there is a degree preserving linear map ε:Ck $\varepsilon\colon C\to {\mathbb k}$ such that the diagram

commutes. The map ε is then called the counit of C. If τC,C○Δ = Δ, then C is called cocommutative. A linear degree preserving map f : CD between coalgebras (C, ΔC) and (D, ΔD) is called a homomorphism of coalgebras if (ff) Δ C = Δ D f. \begin{equation*}(f\otimes f)\Delta_C=\Delta_D\circ f. \end{equation*}(14)

If C and D are counital with counits ε and η, respectively, and if f also satisfies ηf = ε, we call f a homomorphism of counital coalgebras.

For a coassociative coalgebra (C, Δ) and n $n\in \N$, we define the iterated coproduct Δn: CC⊗(n+1) by Δ0 = idC and Δn = (Δ ⊗idC ⊗… ⊗idCn−1 for n ≥ 1. It is convenient to then use Sweedler notation and to write Δn(x) ∈ C⊗(n+1) for xC as Δ n (x)= x (1) x (n+1) . \[\Delta^n(x)=\sum x_{(1)}\otimes\dotsc\otimes x_{(n+1)}.\]

In this notation, for example, the condition for C to be cocommutative becomes x (1) x (2) = (1) | x (1) || x (2) | x (2) x (1) $\sum x_{(1)}\otimes x_{(2)}=\sum (-1)^{|x_{(1)}||x_{(2)}|} x_{(2)}\otimes x_{(1)}$ for all xC.

Lemma 16. Let (C, ΔC) be a coassociative coalgebra. Then for all p,q $p,q\in \N$, ( Δ C p Δ C q ) Δ C = Δ C p+q+1 . \begin{equation*}(\Delta_C^p\otimes \Delta_C^q)\Delta_C=\Delta_C^{p+q+1}. \end{equation*}(15)

If (D, ΔD) is another coassociative coalgebra and if f : CD is a coalgebra homomorphism, f (n+1) Δ C n = Δ D n f \begin{equation*}f^{\otimes (n+1)}\circ \Delta_C^n=\Delta_D^n\circ f \end{equation*}(16) holds for all n $n\in\N$.

Proof. One obtains (15) and (16) by iterating (12) and (14); the details are left to the reader or can be found in ([7, Lemma-Definition VIII.10).

2.4.1 Coaugmented coalgebras

A coaugmented coalgebra (C, Δ, ε, u) is a counital coassociative coalgebra (C, Δ, ε) together with a homomorphism of counital coalgebras u:kC $u\colon{\mathbb k}\to C$. The coproduct on k ${\mathbb k}$ is given by 1 k 1 k 1 k $1_{\mathbb k}\mapsto 1_{\mathbb k}\otimes 1_{\mathbb k}$ and its counit is the identity on k ${\mathbb k}$. Denoting u( 1 k )C $u(1_{\mathbb k})\in C$ as 1, the conditions for u to be a homomorphism of counital coalgebras become Δ(1) = 1 ⊗ 1 and εu= id k $\varepsilon\circ u=\id_{\mathbb k}$. A homomorphism between coaugmented coalgebras C and D is a homomorphism of counital coalgebras f : CD such that f(1) = 1.

Given a coaugmented coalgebra (C, Δ, ε, u), set \olCker(ε) $\ol C\vcentcolon =\ker(\varepsilon)$. We claim that C \olCk $C\cong \ol C \oplus {\mathbb k}$. Indeed, as εu= id k $\varepsilon\circ u=\id_{\mathbb k}$, the short exact sequence of graded vector spaces 0ker(ε)C ε k0 \[0\to \ker(\varepsilon)\hookrightarrow C\xrightarrow{\varepsilon} {\mathbb k} \to 0\]

splits. For x \olC $x\in \ol C$, we then define \olΔ(x)Δ(x)x11x $\ol \Delta(x)\vcentcolon= \Delta(x)- x\otimes 1 -1 \otimes x$. Using (13) and ε(x) = 0, one easily sees that \olΔ(x)ker(ε  \id C )ker( id C ε)= \olC \olC; \[ \ol\Delta(x)\in \ker(\varepsilon\otimes \id_C)\cap \ker(\id_C\otimes \varepsilon)= \ol C\otimes \ol C; \]

for the last equality, note that CC(\olC \olC)(\olCk)(k \olC)(kk). $C\otimes C\cong (\ol C\otimes \ol C) \oplus (\ol C\otimes {\mathbb k})\oplus ({\mathbb k}\otimes \ol C)\oplus ({\mathbb k}\otimes {\mathbb k}).$ We call \olΔ: \olC \olC \olC $\ol \Delta\colon \ol C\to \ol C\otimes \ol C$ the reduced coproduct on \olC $\ol C$. It is straightforward to check that (\olC,\olΔ) $(\ol C,\ol\Delta)$ is a coassociative coalgebra.

Conversely, given a coassociative coalgebra (\olC, \olΔ) $(\ol C, \ol \Delta)$, we define a coproduct on C \olCk $C\vcentcolon= \ol C\oplus {\mathbb k}$ by Δ(1) = 1 ⊗ 1 and Δ(x)=\olΔ(x)+x1+1x $\Delta(x)=\ol \Delta(x) + x\otimes 1+1\otimes x$ for x \olC $x\in \ol C$. This makes C into a coaugmented coalgebra; the counit and coaugmentation map are given by the projection Ck $C\to {\mathbb k}$ and the inclusion kC ${\mathbb k} \hookrightarrow C$, respectively.These constructions are clearly inverse to each other (up to isomorphism).

Let C and D be coaugmented coalgebras with counitsε and η, respectively. A linear degree preserving map f : CD satisfying ηf = ε and f(1) = 1 decomposes as f=\olf  \id k : \olCk \olDk \[f=\ol f\oplus \id_{\mathbb k}\colon \ol C \oplus {\mathbb k}\to \ol D \oplus {\mathbb k}\]

for a unique degree preserving linear map \olf: \olC \olD $\ol f\colon \ol C\to \ol D$. It is then easy to see that f is a homomorphism of coaugmented coalgebras if and only if \olf $\ol f$ is a homomorphism of coalgebras. This yields a one-to-one correspondence between coalgebra homomorphisms \olC \olD $\ol C\to \ol D$ and homomorphisms of coaugmented coalgebras CD.

Loosely speaking, this let us choose if we want to work with coaugmented coalgebras or non-coaugmented ones. In more technical terms, we have an equivalence between the category of coaugmented coalgebras and the category of coassociative coalgebras.

We call a coaugmented coalgebra (C, Δ) conilpotent if for all x \olC $x\in \ol C$ there is an n $n\in \N$ such that \ol Δ n (x)=0 $\ol\Delta^n (x)=0$.

2.4.2 Examples of coalgebras

There is a coproduct \ol Δ A $\ol\Delta_A$ on \rten(V) n1 V n $\rten(V)\vcentcolon= \bigoplus_{n\geq 1}{V^{\otimes n}}$ given by \ol Δ A ( v 1 v n )= i=1 n1 ( v 1 v i )( v i+1 v n ), \[ \ol\Delta_A(v_1\dots v_n) = \sum_{i=1}^{n-1}(v_1\dots v_i)\otimes (v_{i+1}\dotsc v_n), \]

where we now denote the multiplication in T(V ) by concatenation to avoid ambiguities. This makes \rten(V) $\rten(V)$ into a coassociative graded coalgebra. The induced coaugmented coalgebra (T(V ), ΔA) is called the tensor coalgebra. Inductively, one finds \ol Δ A m ( v 1 v n ) = 1 i 1 << i m <n ( v 1 v i 1 )( v i m +1 v n ), \begin{eqnarray*}&&\hskip-6pt\ol\Delta_A^m(v_1\dots v_n)\nonumber\\ &&\quad=\sum_{1\leq i_1 <\dotsc<i_m<n}(v_1\dots v_{i_1})\otimes\dotsc\otimes (v_{i_m+1}\dotsc v_n),\nonumber\\ \end{eqnarray*}(17) which shows that T(V ) is conilpotent.

Proposition 17. Let (C, Δ) be a conilpotent coalgebra and f: \olCV $f\colon \ol C\to V$ a linear degree preserving map. There is a unique homomorphism of coaugmented coalgebras f ˜ :CT(V) $\tilde f\colon C \to T(V)$ such that f=  \pr V f ˜ , $ f = \pr_V \circ\tilde f, $ where here and subsequently, pr( ⋅) denotes the projection onto a subspace under a given decomposition.

Proof. It clearly suffices to show that there is a unique homomorphism of coalgebras f ˜ : \olC \rten(V) $\tilde f\colon \ol C\to \rten(V)$ satifying \pr V f ˜ =f $\pr_V\circ \tilde f= f$. For the uniqueness, assume that there is such f ˜ $\tilde f$. By Lemma 16, we have f ˜ (n+1)  \ol Δ n =\ol Δ A n f ˜ \[ \tilde f^{\otimes(n+1)}\circ \ol\Delta^n=\ol\Delta_A^n \circ\tilde f \]

for all n $n\in\N$. Composing both sides with \pr V (n+1) $\pr_V^{\otimes(n+1)}$ and noting that \pr V (n+1) \ol Δ A n =  \pr V (n+1) $\pr_V^{\otimes(n+1)}\circ\ol\Delta_A^n= \pr_{V^{\otimes(n+1)}}$ then yields \pr V (n+1) f ˜ = \pr V (n+1) f ˜ (n+1) \ol Δ n = f (n+1) \ol Δ n . \[ \pr_{V^{\otimes(n+1)}} \circ\tilde f=\pr_V^{\otimes(n+1)}\circ\tilde f^{\otimes(n+1)}\circ\ol\Delta^n= f^{\otimes(n+1)} \circ\ol\Delta^n. \]

This shows that f ˜ $\tilde f$ is completely determined by f and therefore unique. For the existence, consider the linear map n=0  \ol Δ n : \olC \rten(\olC). $\sum_{n=0}^{\infty} \ol\Delta^n \colon \ol C \to \rten(\ol C).$ This is well-defined as C is conilpotent. A straightforward computation using Lemma 16 and \ol Δ A | V =0 $\left.\ol\Delta_A\right|_{V}=0$ shows that ( n=0  \ol Δ n n=0  \ol Δ n )\olΔ=\ol Δ A n=0  \ol Δ n , \[ \left(\sum_{n=0}^{\infty} \ol\Delta^n \otimes \sum_{n=0}^{\infty} \ol\Delta^n \right)\ol\Delta =\ol\Delta_A \circ\sum_{n=0}^{\infty} \ol\Delta^{n}, \]

so that n=0  \ol Δ n $\sum_{n=0}^{\infty} \ol\Delta^n$ is a coalgebra homomorphism. As \rten(f)= n1 f n : \rten(\olC) \rten(V) $\rten(f)=\bigoplus_{n\geq 1}f^{\otimes n}\colon \rten(\ol C)\to \rten(V)$ is easily seen to be also a coalgebra homomorphism, f ˜  \rten(f) n=0  \ol Δ n :C \rten(V) $\tilde f \vcentcolon = \rten(f) \circ\sum_{n=0}^{\infty} \ol\Delta^n \colon C \to \rten(V)$ is a homomorphism of coalgebras with \pr V f ˜ =f $\pr_V\circ \tilde f= f$.

Let \rsym(V) n1 S n (V) $\rsym(V)\vcentcolon= \bigoplus_{n\geq 1}\Sy^n(V)$. Consider the linear maps π: \rten(V) \rsym(V), v 1 v n 1 n! v 1 v n , N: \rsym(V) \rten(V), v 1 v n σ S n ε(σ) v σ(1) v σ(n) . \[ \begin{array}{l} \displaystyle\pi\colon \rten(V)\to \rsym(V), \quad v_1\otimes\dotsc\otimes v_n\mapsto \frac{1}{n!} v_1\vee\dotsc\vee v_n,\\[5pt] \displaystyle N\colon \rsym(V)\to \rten(V),\nonumber\\[5pt] \displaystyle v_1 \vee \dotsc\vee v_n\mapsto \sum_{\sigma\in \mathfrak S_n}\varepsilon(\sigma)v_{\sigma(1)}\otimes\dotsc\otimes v_{\sigma(n)}. \end{array} \]

It is immediate that πN = idS, where here and subsequently, we abbreviate \rsym(V) $\rsym(V)$ and S(V) $\Sy(V)$ to S in subscripts. Using Lemma 15, we compute \ol Δ A (N( v 1 v n )) = i=1 n1 σ S n ε(σ)( v σ(1) v σ(i) )( v σ(i+1) v σ(n) ) = i=1 n1 τ \Sh i,ni 1 (α,β) S i × S ni ε(τ(α,β))( v (τ(α,β))(1) v (τ(α,β))(i) )( v (τ(α,β))(i+1) v (τ(α,β))(n) ) = i=1 n1 τ \Sh i,ni 1 ε(τ) (α,β) S i × S ni ε ^ (α)( v τ(1) v τ(i) ) ε ^ (β)( v τ(i+1) v τ)(n) ) = i=1 n1 τ \Sh i,ni 1 ε(τ)N( v 1 v i )N( v i+1 v n ). \[ \begin{array}{ll}\displaystyle &\displaystyle\ol\Delta_A(N(v_1\vee\dots\vee v_n)) \\ &\displaystyle=\sum_{i=1}^{n-1} \sum_{\sigma\in \mathfrak S_n}\varepsilon(\sigma)(v_{\sigma(1)}\dotsc v_{\sigma(i)})\otimes(v_{\sigma(i+1)}\dotsc v_{\sigma(n)})\\ &\displaystyle=\sum_{i=1}^{n-1}\sum_{\tau\in\Sh^{-1}_{i,n-i}}\sum_{(\alpha,\beta)\in\mathfrak S_i \times \mathfrak S_{n-i}}\varepsilon(\tau(\alpha,\beta)) (v_{(\tau(\alpha,\beta))(1)}\dotsc v_{(\tau(\alpha,\beta))(i)})\otimes (v_{(\tau(\alpha,\beta))(i+1)}\dotsc v_{(\tau(\alpha,\beta))(n)})\\ &\displaystyle=\sum_{i=1}^{n-1}\sum_{\tau\in\Sh^{-1}_{i,n-i}}\varepsilon(\tau)\sum_{(\alpha,\beta)\in\mathfrak S_i \times \mathfrak S_{n-i}}\hat\varepsilon(\alpha)(v_{\tau(1)}\dotsc v_{\tau(i)})\otimes \hat\varepsilon(\beta)(v_{\tau(i+1)}\dotsc v_{\tau)(n)})\\ &\displaystyle= \sum_{i=1}^{n-1}\sum_{\tau\in\Sh^{-1}_{i,n-i}}\varepsilon(\tau)N(v_1\vee\dotsc\vee v_i)\otimes N(v_{i+1}\vee\dotsc\vee v_n). \end{array} \]

This shows that \ima(N) \rten(V) $\ima(N)\subset \rten(V)$ is a subcoalgebra and induces a coproduct on \rsym(V) \ima(N) $\rsym(V)\cong \ima(N)$. As a subcoalgebra of a coassociative coalgebra is clearly coassociative itself, S(V) $\Sy(V)$ becomes a coaugmented coalgebra with the coproduct Δ S :S(V)S(V)S(V) $\Delta_S\colon \Sy(V)\to \Sy(V)\otimes \Sy(V)$ given by Δ S ( v 1 v n ) = i=0 n τ \Sh i,ni 1 ε(τ)( v τ(1) v τ(i) ) ( v τ(i+1) v τ(n) ). \begin{eqnarray*}\Delta_S(v_1\vee\dotsc\vee v_n)&=&\sum_{i=0}^{n}\sum_{\tau\in\Sh^{-1}_{i,n-i}}\varepsilon(\tau)(v_{\tau(1)}\vee\dotsc \vee v_{\tau(i)})\nonumber\\ &&\otimes\,(v_{\tau(i+1)}\vee\dotsc\vee v_{\tau(n)}). \end{eqnarray*}(18)

It is immediate that S(V) $\Sy(V)$ is conilpotent, as it is a subcoalgebra of T(V ). We claim that S(V) $\Sy(V)$ is even cocommutative. Indeed, let σi𝔖n be for 0 ≤ in the permutation given by (σi(1), …, σi(n)) = (i + 1, …, n, 1, …, i). We then have \Sh i,ni 1 σ i = \Sh ni,i 1 $\Sh^{-1}_{i,n-i}\sigma_i=\Sh^{-1}_{n-i,i}$ and therefore τ S,S Δ S ( v 1 v n ) = i=0 n τ \Sh i,ni 1 ε(τ σ i )( v (τ σ i )(1) v (τ σ i )(ni) ) ( v (τ σ i )(ni+1) v (τ σ i )(n) ) = i=0 n τ \Sh ni,i 1 ε(τ)( v τ(1) v τ(i) ) ( v τ(i+1) v τ(n) ) = Δ S ( v 1 v n ). \[ \begin{array}{ll} &\displaystyle\tau_{S,S}\circ\Delta_S(v_1\vee\dotsc\vee v_n)\\&\displaystyle=\sum_{i=0}^{n}\sum_{\tau\in\Sh^{-1}_{i,n-i}}\varepsilon(\tau\sigma_i)(v_{(\tau\sigma_i)(1)}\vee\dotsc \vee v_{(\tau\sigma_i)(n-i)})\\ &\displaystyle\quad\otimes(v_{(\tau\sigma_i)(n-i+1)}\vee\dotsc\vee v_{(\tau\sigma_i)(n)})\\ &\displaystyle=\sum_{i=0}^{n}\sum_{\tau\in\Sh^{-1}_{n-i,i}}\varepsilon(\tau)(v_{\tau(1)}\vee\dotsc \vee v_{\tau(i)})\\ &\displaystyle\quad \otimes(v_{\tau(i+1)}\vee\dotsc\vee v_{\tau(n)})\\ &\displaystyle=\Delta_S(v_1\vee\dotsc\vee v_n). \end{array} \]

Proposition 18. Let (C, Δ) be a cocommutative conilpotent coalgebra and f: \olCV $f\colon \ol C\to V$ a degree preserving linear map. There is a unique homomorphism of coaugmented coalgebras f ˜ :CS(V) $\tilde f\colon C \to \Sy(V)$ such that f=  \pr V f ˜ . $ f = \pr_V \circ\tilde f. $

Proof. As in the proof of Proposition 17, it suffices to show that there is a unique homomorphism of coalgebras f ˜ : \olC \rsym(V) $\tilde f\colon \ol C\to \rsym(V)$ satisfying \pr V f ˜ =f $\pr_V\circ \tilde f=f$. Recall that \olT(f) n  \ol Δ n $\ol T(f)\circ \sum_n \ol\Delta^n$ is the unique coalgebra homomorphism \olC \olT(V) $\ol C\to \ol T(V)$ extending f. For 0 ≤ in − 1, we have ( id V i τ C,C  \id V (ni1) )\rten(f)\ol Δ n =\rten(f)( id C i τ C,C  \id C (ni1) )\ol Δ n = \rten(f)( id C i ( τ C,C \olΔ)  \id C (ni1) )\ol Δ n1 = \rten(f)( id C i  \olΔ  \id C (ni1) )\ol Δ n1 = \rten(f)\ol Δ n \[\begin{array}{ll} &\displaystyle(\id_V^{\otimes i}\otimes \tau_{C,C}\otimes \id_V^{\otimes(n-i-1)})\rten(f)\circ\ol\Delta^n\\[4pt] &\displaystyle\quad=\rten(f)(\id_C^{\otimes i}\otimes \tau_{C,C}\otimes \id_C^{\otimes(n-i-1)})\ol\Delta^n\\[4pt] &\displaystyle\quad= \rten(f)(\id_C^{\otimes i}\otimes (\tau_{C,C}\circ\ol\Delta) \otimes \id_C^{\otimes(n-i-1)})\ol\Delta^{n-1}\\[4pt] &\displaystyle\quad= \rten(f)(\id_C^{\otimes i}\otimes \ol\Delta \otimes \id_C^{\otimes(n-i-1)})\ol\Delta^{n-1}\\[4pt] &\displaystyle\quad= \rten(f)\circ\ol\Delta^{n} \end{array} \]

since C is cocommutative. As ( id V i τ C,C  \id V (ni1) )= ε ^ ( s i ), $(\id_V^{\otimes i}\otimes \tau_{C,C}\otimes \id_V^{\otimes(n-i-1)})= \hat\varepsilon(s_{i}),$ the image of \rten(f) n \ol Δ n $\rten(f)\circ \sum_n\ol\Delta^n$ is contained in the subspace of \rten(V) $\rten(V)$ of all symmetric elements, which is im(N). We obtain an induced homomorphism of coalgebras f ˜ =π \olT(f) n=0 \ol Δ n : \olC  \rsym(V), x n=1 1 n! f ( x (1) )f( x (n) ) \begin{equation*}\begin{array}{l} \displaystyle\tilde f=\pi\circ \ol T(f)\circ \sum_{n=0}^{\infty}\ol\Delta^n \colon \ol C\to \rsym(V),\\[4pt] \displaystyle x\mapsto \sum_{n=1}^{\infty} \frac{1}{n!}\sum f(x_{(1)})\vee\dotsc\vee f(x_{(n)}) \end{array} \end{equation*}(19)

with \pr V f ˜ =f $\pr_V \circ\tilde f= f$. Similarly, a coalgebra homomorphism f ˜ : \olC \rsym(V) $\tilde f\colon \ol C \to \rsym(V)$ gives rise to a coalgebra homomorphism N f ˜ : \olC \rten(V) $N \circ \tilde f \colon \ol C\to \rten(V)$ that is uniquely determined by \pr V N f ˜ = \pr V f ˜ $\pr_V \circ N\circ\tilde f=\pr_V\circ \tilde f$ by Proposition 17. As N is injective, this shows uniqueness of f ˜ $\tilde f$.

Example 19. A linear degree preserving map f : VW can be extended by zero to a linear map \rsym(V)W $\rsym(V)\to W$. The induced homomorphism of coaugmented coalgebras S(V)S(W) $\Sy(V)\to \Sy(W)$ is denoted by S(f) $\Sy(f)$ and is given by S(f)( v 1 v n )=f( v 1 )f( v n ). $ \Sy(f)(v_1\vee\dotsc\vee v_n)=f(v_1)\vee\dotsc\vee f(v_n). $

2.4.3 Comodules and coderivations

Let (C, Δ) be a coassociative coalgebra. A left comodule over C is a graded vector space M together with a degree preserving linear map Δl: MCM satisfying (Δ  \id M ) Δ l =( id C Δ l ) Δ l . \begin{equation*}(\Delta \otimes \id_M)\Delta_l = (\id_C \otimes \Delta_l)\Delta_l. \end{equation*}(20)

Similarly, a right comodule over C is a graded vector space M together with a degree preserving linear map Δr: MMC such that ( id M Δ) Δ r =( Δ r  \id C ) Δ r . \begin{equation*}(\id_M \otimes \Delta)\Delta_r = (\Delta_r\otimes \id_C)\Delta_r. \end{equation*}(21)

If M is both a left and a right comodule over C and if the compatibility relation ( Δ l  \id C ) Δ r =( id C Δ r ) Δ l \begin{equation*}(\Delta_l \otimes \id_C)\Delta_r = (\id_C \otimes \Delta_r)\Delta_l \end{equation*}(22)

is satisfied, M is called a (bi)comodule over C. Given such M, we define a coderivation of degree p to be a homogeneous linear map d: MC of degree p such that Δd=(d  \id C ) Δ r +( id C d) Δ l . \begin{equation*}\Delta \circ d= (d\otimes \id_C)\Delta_r + (\id_C\otimes d)\Delta_l. \end{equation*}(23)

We denote the vector space of all these maps by Coderp(M, C) and by Coder(M, C) the graded vector space p  \Coder p (M,C) $\bigoplus_{p\in \Z} \Coder_p(M,C)$.

Let (C, ΔC) and (D, ΔD) be coassociative coalgebras and f : DC a coalgebra homomorphism. Then Δr := (idDfD and Δl := (f ⊗idDD make D into a comodule over C. In particular, C is a comodule over itself and we abbreviate Coder(C, C) to Coder(C). If C and D are coaugmented and if f is a homomorphism of coaugmented coalgebras, the comodule structure is compatible with the counit in the sense that the diagram

commutes, where ε is the counit on C. Observe that \olf: \olD \olC $\ol f\colon \ol D \to \ol C$ then makes \olD $\ol D$ into a comodule over \olC $\ol C$. The following proposition relates elements in \Coder(\olD,\olC) $\Coder(\ol D,\ol C)$ to coderivations d: DC that satisfy d(1) = 0; the latter is called a coderivation of coaugmented coalgebras.

Proposition 20. Let f : DC be a homomorphism of coaugmented coalgebras. There is a one-to-one correspondence between coderivations d: DC satisfying d(1) = 0 and coderivations \old: \olD \olC $\ol d\colon \ol D\to \ol C$ given by d=\old0: \olDk \olCk $d=\ol d\oplus 0\colon \ol D\oplus {\mathbb k} \to \ol C\oplus {\mathbb k}$.

Proof. Given a linear map \oldHom(\olD,\olC) $\ol d\in\Hom(\ol D,\ol C)$, one easily checksthat \old $\ol d$ is a coderivation if and only if \old0: \olDk \olCk $\ol d\oplus 0\colon \ol D\oplus {\mathbb k} \to \ol C\oplus {\mathbb k}$ is. It then suffices to show thateach coderivation d: DC with d(1) = 0 is of this form. Let ε be the counit of C and μ k :kkk $\mu_{\mathbb k}\colon {\mathbb k}\otimes {\mathbb k}\to {\mathbb k}$ the multiplication on k ${\mathbb k}$. From (13), (23) and the compatibility with the counit (24) it then follows that εd = μ k (εε) Δ C d = μ k (ε(εd)) Δ l + μ k ((εd)ε) Δ r =2(εd), \begin{align*} \varepsilon\circ d&=\mu_{\mathbb k} (\varepsilon\otimes\varepsilon)\Delta_C\circ d\\ &=\mu_{\mathbb k} (\varepsilon\otimes (\varepsilon\circ d))\Delta_l+\mu_{\mathbb k} ((\varepsilon\circ d)\otimes\varepsilon)\Delta_r\\ &= 2(\varepsilon\circ d), \end{align*}

which shows that d(D) \olC $d(D)\subset \ol C$. Hence, d decomposes as \old0: \olDk \olCk $\ol d\oplus 0\colon \ol D\oplus {\mathbb k}\to \ol C\oplus {\mathbb k}$.

For a coassociative coalgebra C, we call an element d ∈ Coder(C) of degree one with d2 = 0 a codifferential on C. We then call the pair (C, d) a differential graded coassociative coalgebra (DGC for short). If C is coaugmented and d(1) = 0, we call (C, d) a coaugmented DGC. A homomorphism of DGCs is then a coalgebra homomorphism that is also a homomorphism of DG vector spaces; homomorphisms of coaugmented DGCs are defined accordingly. From Proposition 20 and Section 2.4.1, we then obtain an equivalence between the categories of DGCs and coaugmented DGCs.

Proposition 21. Let C be a coassociative coalgebra. Then Coder(C) ⊂ 𝔤𝔩(C) is closed under the graded commutator. Also, if f : DC is a homomorphism of coassociative coalgebras, d ∈ Coder(C) and d′∈ Coder(D), then fd′, df ∈ Coder(D, C).

Proof. Both parts of the proposition are straightforward computations which are left to the reader.

Theorem 22. Let D be a cocommutative coaugmented coalgebra and f:DS(V) $f\colon D\to \Sy(V)$ a homomorphism of coaugmented coalgebras. The linear map \Coder(D,S(V)) \Hom(D,V),d  \pr V d \[\Coder(D,\Sy(V))\to \Hom(D,V), \quad d\mapsto \pr_V\circ d \] is then an isomorphism. Its inverse is given by Hom(D,V) \Coder(D,S(V)),λ μ S (λf) Δ D , \[ \Hom(D,V) \to \Coder(D,\Sy(V)), \quad \lambda \mapsto \mu_S(\lambda\otimes f)\Delta_D, \] where μ S :S(V)S(V)S(V) $\mu_S\colon \Sy(V)\otimes \Sy(V)\to \Sy(V)$ denotes the multiplication on S(V) $\Sy(V)$ and ΔD the coproduct on D.

It is immediate that d(1) = 0 if and only if λ = prVd vanishes on k ${\mathbb k}$. Together with Proposition 20, this shows \Coder(\olD,\rsym(V)) \Hom(\olD,V) $\Coder(\ol D,\rsym(V))\cong \Hom(\ol D,V)$.

The first part of Theorem 22 actually holds for a broader class of comodules over S(V) $\Sy(V)$ (see for example [8], Lemma 2.4); the inverse formula d = μS(λ ⊗idMr then continues to hold for comodules M in which τM,S▼Δr = Δl.

Remark 23. For 1 ≤ in − 1 and τ \Sh i,ni 1 $\tau\in\Sh^{-1}_{i,n-i}$ either τ(i) = n or τ(n) = n. In the first case, there is a unique σ \Sh i1,ni 1 $\sigma\in\Sh^{-1}_{i-1,n-i}$ such that (τ(1), …, τ(n)) = (σ(1), …, σ(i − 1), n, σ(i), …, σ(n − 1)), while in the second case (τ(1), …, τ(n)) = (σ(1), …, σ(n − 1), n) for a unique σ \Sh i,ni1 1 $\sigma\in\Sh^{-1}_{i,n-i-1}$. This yields abijection \Sh i,ni 1 \Sh i1,ni 1  \Sh i,ni1 1 $\Sh^{-1}_{i,n-i}\cong\Sh^{-1}_{i-1,n-i}\sqcup \Sh^{-1}_{i,n-i-1}$. By setting \Sh 1,n 1 , \Sh n,1 1 = $\Sh^{-1}_{-1,n},\Sh^{-1}_{n,-1}=\emptyset$, this also holds for i = 0, n.

Lemma 24. The map Δ S :S(V)S(V)S(V) $\Delta_S\colon \Sy(V)\to \Sy(V)\otimes \Sy(V)$ is a homomorphism of graded algebras.

Proof. We show by induction over n $n\in\N$ that Δ S ( v 1 v n )= Δ S ( v 1 ) Δ S ( v n ). \begin{equation*}\Delta_S(v_1 \vee\dotsc \vee v_n)=\Delta_S(v_1)\dotsc \Delta_S(v_n). \end{equation*}(25)

For n = 1 there is nothing to do. Assume that (25) holds for n ≥ 1. We compute Δ S ( v 1 ) Δ S ( v n+1 ) = Δ S ( v 1 v n ) Δ S ( v n+1 ) = i=0 n τ \Sh i,ni 1 ( ε(τ)( v τ(1) v τ(i) )( v τ(i+1) v τ(n) ) )( v n+1 1+1 v n+1 ) = i=0 n σ \Sh i,ni 1 (1) | v n+1 | k=i+1 n | v σ(k) | ε(σ)( v σ(1) v σ(i) v n+1 )( v σ(i+1) v σ(n) ) + i=0 n σ \Sh i,ni 1 ε(σ)( v σ(1) v σ(i) )( v σ(i+1) v σ(n) v n+1 ) = i=0 n+1 σ \Sh i,n+1i 1 ε(σ)( v σ(1) v σ(i) )( v σ(i+1) v σ(n+1) ) = Δ S ( v 1 v n+1 ). \[\begin{array}{ll} &\displaystyle\Delta_S(v_1)\dotsc \Delta_S(v_{n+1})\\ &\displaystyle=\Delta_S(v_1\vee\dotsc\vee v_n)\Delta_S(v_{n+1})\\ &\displaystyle=\sum_{i=0}^{n}\sum_{\tau\in\Sh^{-1}_{i,n-i}}\left(\varepsilon(\tau)(v_{\tau(1)}\vee\dotsc \vee v_{\tau(i)})\otimes(v_{\tau(i+1)}\vee\dotsc\vee v_{\tau(n)})\right)(v_{n+1}\otimes 1+1\otimes v_{n+1})\\ &\displaystyle=\sum_{i=0}^{n}\sum_{\sigma\in\Sh^{-1}_{i,n-i}}(-1)^{|v_{n+1}|\sum_{k=i+1}^n|v_{\sigma(k)}|}\varepsilon(\sigma) (v_{\sigma(1)}\vee\dotsc\vee v_{\sigma(i)}\vee v_{n+1})\otimes (v_{\sigma(i+1)}\vee\dotsc\vee v_{\sigma(n)})\\ &\displaystyle\quad+\sum_{i=0}^n\sum_{\sigma\in\Sh^{-1}_{i,n-i}}\varepsilon(\sigma)(v_{\sigma(1)}\vee\dotsc\vee v_{\sigma(i)})\otimes (v_{\sigma(i+1)}\vee\dotsc\vee v_{\sigma(n)}\vee v_{n+1})\\ &\displaystyle=\sum_{i=0}^{n+1}\sum_{\sigma\in\Sh^{-1}_{i,n+1-i}}\varepsilon(\sigma)(v_{\sigma(1)}\vee\dotsc\vee v_{\sigma(i)})\otimes (v_{\sigma(i+1)}\vee\dotsc\vee v_{\sigma(n+1)})\\ &\displaystyle=\Delta_S(v_1\vee\dotsc \vee v_{n+1}). \end{array}\]

In the fourth equality, we shifted the summation index of the first sum and used Remark 23.

Proof of Theorem 22. Let d:DS(V) $d\colon D\to \Sy(V)$ be a coderivation, that is Δ S d=(df+fd) Δ D . \[ \Delta_S\circ d = (d\otimes f + f\otimes d)\Delta_D. \]

Inductively,we then get Δ S n d= k=0 n ( f k d f (nk) ) Δ D n . \[ \Delta_S^n\circ d=\sum_{k=0}^n (f^{\otimes k}\otimes d\otimes f^{\otimes(n-k)})\Delta_D^n. \]

For n $n\in\N$, let π n : T n (V) S n (V) $\pi_n\colon T^n(V)\to \Sy^n(V)$ be the linear map defined by π n ( v 1 v n )= 1 n! v 1 v n . \[\pi_n(v_1\otimes\dotsc\otimes v_n)=\frac{1}{n!}v_1\vee\dotsc\vee v_n.\]

From S(V) $\Sy(V)$ being a subcoalgebra of T(V ) and (17), it follows that π n+1  \pr V (n+1) Δ S n = \pr S n+1 (V) $\pi_{n+1}\circ \pr_V^{\otimes (n+1)}\circ \Delta_S^{n}=\pr_{\Sy^{n+1}(V)}$. We then have \pr S n+1 (V) d = π n+1  \pr V (n+1) k=0 n ( f k d f (nk) ) Δ D n = π n+1 k=0 n ( ( \pr V f) k ( \pr V d) ( \pr V f) (nk) ) Δ D n . \[ \begin{array}{ll} \displaystyle\pr_{\Sy^{n+1}(V)}\circ d &\displaystyle=\pi_{n+1}\circ \pr_V^{\otimes (n+1)}\\ &\displaystyle\quad\circ\sum_{k=0}^n (f^{\otimes k}\otimes d\otimes f^{\otimes(n-k)})\Delta_D^n\\ &\displaystyle=\pi_{n+1}\circ \sum_{k=0}^n ((\pr_V\circ f)^{\otimes k}\otimes (\pr_V\circ d)\\ &\displaystyle\quad\otimes (\pr_V\circ f)^{\otimes(n-k)})\Delta_D^n. \end{array} \]

As this holds for all n $n\in \N$ and as \pr k d=0 $\pr_{\mathbb k}\circ d=0$ by the same computation as in the proof of Proposition 20, d is completely determined by prVd.

What is left is to show that given λ ∈ Hom(D, V ) homogeneous, d := μS(λfD is a coderivation with prVd = λ. While the latter holds by construction, we compute for xD homogeneous ( Δ S d)(x) = Δ S (λ( x (1) )) Δ S (f( x (2) )) = ( λ( x (1) )1+1λ( x (1) ))(ff)( Δ D ( x (2) )) = ( λ( x (1) )1+1λ( x (1) ))(f( x (2) )f( x (3) )) = ( λ( x (1) )f( x (2) ))f( x (3) )+ (1) (|λ|+| x (1) |)| x (2) | f( x (2) )(λ( x (1) )f( x (3) )) = ( μ S (λf)f+f μ S (λf))( x (1) x (2) x (3) ) =( μ S (λf) Δ D f+f μ S (λf) Δ D )( Δ D (x)), \[ \begin{array}{ll} \displaystyle(\Delta_S\circ d)(x)&\displaystyle=\sum \Delta_S(\lambda(x_{(1)}))\vee \Delta_S(f(x_{(2)}))\\[6pt] &\displaystyle=\sum \big(\lambda(x_{(1)})\otimes 1+ 1\otimes \lambda(x_{(1)})\big)\vee (f\otimes f)(\Delta_D(x_{(2)}))\\[6pt] &\displaystyle=\sum\big(\lambda(x_{(1)})\otimes 1+1\otimes \lambda(x_{(1)})\big) (f(x_{(2)})\otimes f(x_{(3)}))\\[6pt] &\displaystyle=\sum\big(\lambda(x_{(1)})\vee f( x_{(2)})\big)\otimes f(x_{(3)}) + (-1)^{(|\lambda|+|x_{(1)}|)|x_{(2)}|}f(x_{(2)})\otimes \big(\lambda(x_{(1)})\vee f(x_{(3)})\big)\\[6pt] \displaystyle&\displaystyle=\sum\big(\mu_S (\lambda\otimes f)\otimes f + f\otimes \mu_S(\lambda\otimes f)\big)(x_{(1)}\otimes x_{(2)}\otimes x_{(3)})\\[6pt] &\displaystyle=\big(\mu_S (\lambda\otimes f) \Delta_D\otimes f + f\otimes \mu_S(\lambda\otimes f)\Delta_D\big)(\Delta_D(x)), \end{array} \]

where we used Lemma 24 in the first and cocommutativity of D in the fifth equality.

2.5 Dual spaces

The graded vector space V * Hom(V,k) $V^*\vcentcolon=\Hom(V,{\mathbb k})$ is called the dual space of V. By degree reasons, ( V * ) k = Hom k (V,k)=Hom( V k ,k)= ( V k ) * $(V^*)_k=\Hom_k(V,{\mathbb k})=\Hom(V_{-k},{\mathbb k})=(V_{-k})^*$. For f ∈ Homp(V, W), the linear map f*∈ Homp(W*, V *) is defined by f * (φ)= (1) |φ||f| φf $f^*(\varphi)=(-1)^{|\varphi||f|}\varphi\circ f$ for φW* homogeneous. Note that id V * =  \id V * $\id_V^*= \id_{V^*}$ and if g is a homogeneous linear map with domain W, we have (gf) * = (1) |f||g| f * g * $(g\circ f)^*=(-1)^{|f||g|}f^*\circ g^*$.

We say that V is of finite type if V k is finite-dimensional for all k $k\in\Z$. Note that if V is of finite type, the canonical inclusion VV ** is an isomorphism.

If V k = 0 for k > 0, then V is called 0 $\Z_{\leq 0}$-graded. Notions as <0 $\Z_{<0}$-graded or 0 $\Z_{\geq 0}$-graded are defined accordingly. In the following, we denote V n as Tn(V ) for better readability.

Proposition 25. If V is of finite type and if for all k $k\in\Z$ the decomposition T n (V) k = i 1 ++ i n =k ( V i 1 V i n ) \[T^n(V)_{k}=\bigoplus_{i_1+\dotsc+ i_n=k} (V_{i_1}\otimes\dotsc\otimes V_{i_n})\] has only finitely many non-trivial summands, then the canonical inclusion T n ( V * ) T n (V) * $T^n(V^*)\hookrightarrow T^n(V)^*$ is an isomorphism.

Proof. It is well-known that for finite-dimensional (ungraded) vector spaces V 1 , …, V n, the canonical inclusion V 1 * V n * ( V 1 V n ) * $V_1^*\otimes\dotsc\otimes V_n^*\hookrightarrow (V_1\otimes\dotsc\otimes V_n)^*$ is an isomorphism. We then have ( T n (V) k ) * = i 1 ++ i n =k ( V i 1 V i n ) * i 1 ++ i n =k ( V * ) i 1 ( V * ) i n = T n ( V * ) k . \begin{eqnarray*} (T^n(V)_{-k})^*&=&\bigoplus_{i_1+\dotsc+i_n=k}(V_{-i_1}\otimes\dotsc\otimes V_{-i_n})^*\nonumber\\ &\cong&\bigoplus_{i_1+\dotsc+i_n=k}(V^*)_{i_1}\otimes\dotsc\otimes (V^*)_{i_n}\nonumber\\ &=& T^n(V^*)_k. \nonumber \end{eqnarray*}

Remark 26. If V is of finite type and 0 $\Z_{\leq 0}$-graded, V * is also of finite type and 0 $\Z_{\geq 0}$-graded and they both satisfy the hypothesis of Proposition 25. It is then easy to see that Δ: VVV makes V into a graded coassociative/cocommutative coalgebra if and only if Δ * : V * V * (VV) * V * $\Delta^*\colon V^*\otimes V^*\cong (V\otimes V)^*\to V^*$ makes V * into an associative/commutative algebra. A linear map d: VV is then a coderivation of (V, Δ) if and only if − d* is a derivation of (V *, Δ*). The map 𝔤𝔩(V ) → 𝔤𝔩(V *), f↦ − f* preserves the graded commutator and therefore restricts to an isomorphism of graded Lie algebras Coder(V )≅Der(V *).

Corollary 27. If V is of finite type and <0 $\Z_{< 0}$-graded, the canonical inclusion T( V * )T (V) * $T(V^*)\hookrightarrow T(V)^*$ is an isomorphism.

Proof. Note that for all k $k\in\Z$ and n > k, we have T n ( V * ) k =0 $T^n(V^*)_{-k}=0$. Then (T (V) k ) * n0 ( T n (V) k ) * = n0 ( T n (V) * ) k n0 T n ( V * ) k =T ( V * ) k . \begin{eqnarray*} (T (V)_{-k})^*&\cong& \bigoplus_{n\geq 0} (T^n(V)_{-k})^*=\bigoplus_{n\geq 0} (T^n(V)^*)_k \nonumber\\ &\cong& \bigoplus_{n\geq 0} T^n(V^*)_k= T(V^*)_k. \nonumber \end{eqnarray*}

Lemma 28. Let ξ T n ( V * ) T n (V) * $\xi\in T^n(V^*)\subset T^n(V)^*$ and σ𝔖n. Then nn\hatsilon(σ)ξ=ξ ε ^ ( σ 1 ). \begin{equation*} \hatsilon(\sigma)\xi=\xi\circ\hatsilon(\sigma^{-1}). \end{equation*}(26)

Proof. It suffices to show this for σ = s1, …, sn−1, in which case it is an easy computation.

Proposition 29. If V is of finite type and <0 $\Z_{<0}$-graded, S (V) * S( V * ) $\Sy(V)^*\cong \Sy(V^*)$. Under this identification, Δ S * $\Delta_S^*$ is the usual multiplication on S( V * ) $\Sy(V^*)$.

Proof. Fix n ≥ 0. By Lemma 28, the isomorphism T n ( V * ) T n (V) * $T^n(V^*)\cong T^n(V)^*$ maps the subspace of symmetric elements in Tn(V *) onto the space of symmetric linear maps V n k ${V^{\otimes n}}\to {\mathbb k}$. While the latter is isomorphic to Hom( S n (V),k) S n (V) * $\Hom(\Sy^n(V),{\mathbb k})\cong \Sy^n(V)^*$ by Remark 2, the former is isomorphic to S n ( V * ) $\Sy^n(V^*)$ via the linear map S n ( V * ) T n ( V * ), v 1 v n σ S n ε(σ) v σ(1) v σ(n) . \begin{eqnarray*} &&\Sy^n(V^*)\to T^n(V^*),\nonumber\\ && v_1\vee\dotsc\vee v_n\mapsto \sum_{\sigma\in\mathfrak S_n}\varepsilon(\sigma)v_{\sigma(1)}\otimes\dotsc\otimes v_{\sigma(n)}.\nonumber \end{eqnarray*}

This yields an isomorphism S n ( V * ) S n (V) * $\Sy^n(V^*)\cong \Sy^n(V)^*$. With a similar reasoning as in the proof of Corollary 27, one obtains S( V * )S (V) * $\Sy(V^*)\cong\Sy(V)^*$. It is then a straightforward computation to show that Δ S * $\Delta_S^*$ is indeed the usual multiplication on S( V * ) $\Sy(V^*)$.

3 L-algebras

We start this section with a theorem from [5] that characterises certain L -algebras using Lie algebra cohomology; later, we seek to generalise it in the context of L -algebra cohomology. After that, we discuss different characterisations of L-structures using the key results of Section 2. Different points of view naturally lead to different notions of homomorphisms between L -algebras; we will finish the section with a comparison of those. For this, we will mostly follow [3], although the original references for Section 3.2 are [1] and [8].

Definition 30. An L-algebra is a graded vector space L together with antisymmetric linear maps lk: LkL called (higher) brackets of degree |lk| = 2 − k for 1 ≤ k < such that the generalized Jacobi identity i+j=n+1 σ \Sh i,ni 1 (1) i(j1) χ(σ) l j ( l i ( x 1 ,, x i ), x i+1 ,, x n )=0 \begin{eqnarray*}&&\sum_{i+j=n+1}\sum_{\sigma\in\Sh^{-1}_{i,n-i}}(-1)^{i(j-1)}\chi(\sigma) \nonumber\\ &&\quad\cdot l_j(l_i(x_1,\dotsc,x_i),x_{i+1},\dotsc,x_n)=0 \end{eqnarray*}(27)

holds for all n ≥ 1 and x1, …, xnL homogeneous. We then callthe set {lk∣1 ≤ k < } an L-structure on L.

Writing out (27) for n = 1, 2, 3 yields l 1 ( l 1 ( x 1 )) = 0, l 1 ( l 2 ( x 1 , x 2 )) = l 2 ( l 1 ( x 1 ), x 2 )+ (1) | x 1 | l 2 ( x 1 , l 1 ( x 2 )), 0 = σ \Sh 2,1 1 χ(σ) l 2 ( l 2 ( x σ(1) , x σ(2) ), x σ(3) )+ l 1 ( l 3 ( x 1 , x 2 , x 3 ))+ l 3 ( l 1 ( x 1 ), x 2 , x 3 ) [12pt] + (1) | x 1 | l 3 ( x 1 , l 1 ( x 2 ), x 3 )+ (1) | x 1 |+| x 2 | l 3 ( x 1 , x 2 , l 1 ( x 3 )) \begin{eqnarray*} l_1(l_1(x_1)) &=&0,\nonumber\\ l_1(l_2(x_1,x_2))&=& l_2(l_1(x_1),x_2)+(-1)^{|x_1|}l_2(x_1,l_1(x_2)),\nonumber\\ 0&=&\sum_{\sigma\in\Sh^{-1}_{2,1}}\chi(\sigma)l_2(l_2(x_{\sigma(1)},x_{\sigma(2)}),x_{\sigma(3)})+ l_1(l_3(x_1,x_2,x_3))+ l_3(l_1(x_1),x_2,x_3) \nonumber\\[-12pt] &&\hspace*{65pt}+ (-1)^{|x_1|}l_3(x_1,l_1(x_2),x_3)+ (-1)^{|x_1|+|x_2|}l_3(x_1,x_2,l_1(x_3))\nonumber \end{eqnarray*}

for all x1, x2, x3L homogeneous. While the first two equations may be summarized by saying that l1 is a differential on the (non-associative) graded algebra (L, l2), a comparison with (11) shows that the third one describes the defect of the Jacobi identity in (L, l2). In particular, an L-algebra with lk = 0 for k ≥ 3 is nothing else than a DGLA.

If L is concentrated in degree zero, lk = 0 for k≠2 by degree reasons and (L, l2) is an (ungraded) Lie algebra.

Definition 31. Let L and L′ be L -algebras with L -structures { l k } k $\{l_k\}_{k\in\N}$ and { l k } k $\{l_k&#x0027;\}_{k\in\N}$, respectively. A strict L∞ -algebra homomorphism is a degree preserving linear map f : LL′ satisfying f l k = l l f k \begin{equation*} f\circ l_k = l_l&#x0027;\circ f^{\otimes k} \end{equation*}(28)

for all 1 ≤ k < .

These homomorphisms are strict in the sense that they strictly preserve all brackets. A different characterisation of L -algebras will later lead to a more general notion of L-algebra homomorphisms.

3.1 Characterisation via Lie algebra cohomology

For an (ungraded) Lie algebra (𝔤, [⋅, ⋅]), a representation of 𝔤 on an (ungraded) vector space V is a homomorphism of Lie algebras ρ: 𝔤 → 𝔤𝔩(V ). Given such a ρ, the Lie algebra cohomology with values in V is the cohomology of the Chevalley–Eilenberg (cochain) complex ( n0 Hom( \Asy n g,V),δ) $\big(\bigoplus_{n\geq 0}\Hom(\Asy^n \mathfrak g, V), \delta\big)$, where for an antisymmetric linear map ω: 𝔤nV , we define δω by δω( x 1 ,, x n+1 ) = i=1 n+1 (1) i+1 ρ( x i )(ω( x 1 ,, x ^ i ,, x n+1 )) + 1j<kn+1 (1) j+k ω([ x j , x k ], x 1 ,, x ^ j ,, x ^ k ,, x n+1 ), \begin{eqnarray*} &&\displaystyle\delta\omega(x_1,\dotsc, x_{n+1})\nonumber\\ &&\displaystyle\quad=\begin{array}{ll}&\displaystyle\sum_{i=1}^{n+1}(-1)^{i+1} \rho(x_i)(\omega(x_1,\dotsc,\hat x_i,\dotsc,x_{n+1})) \nonumber\\ &\displaystyle+\sum_{1\leq j<k\leq n+1}(-1)^{j+k}\nonumber\\ &\displaystyle\cdot\omega([x_j,x_k],x_1,\dotsc,\hat x_j,\dotsc,\hat x_k,\dotsc,x_{n+1}),\end{array}\nonumber \end{eqnarray*}

for x1, …, xn+1𝔤. In the sums above, elements with ̂ are to be omitted.

Theorem 32 ([5], Theorem 55). There is for each n ≥ 1 a one-to-one correspondence between L-algebras L such that Lk = 0 for k≠ − n, 0 and l1 = 0 and quadruples (𝔤, V, ρ, ln+2) consisting of a Lie algebra 𝔤, a representation ρ of 𝔤 on a vector space V and an (n + 2)-cocycle ln+2.

Sketch of proof. For an L-algebra L = L0Ln with l1 = 0, all brackets exept for l2 and ln+2 have to vanish by degree reasons. Also, l2 has to vanish on ∧2Ln and ln+2 can only be non-trivial on ∧n+2L0 with image in Ln. Using (7), we can decompose l2 into linear maps [⋅, ⋅]: ∧2L0L0 and ρ: L0LnLn. It is then a matter of computation to show that l2 and ln+2 satisfying (27) amounts to (L0, [⋅, ⋅]) being a Lie algebra, ρ being a representation of L0 on Ln and ln+2 being a cocycle.

3.2 Symmetric brackets and codifferentials

Recall that by Corollary 4, an antisymmetric map lk : LkL of degree 2 − k is equivalent to a symmetric degree one map λ k : S k (L[1])L[1] $\lambda_k\colon \Sy^k(L[1])\to L[1]$ such that l k = λ k k . \[ l_k = {\uparrow}\circ \lambda_k \circ {\downarrow^{\otimes k}}. \]

If we now rewrite (27) in terms of the maps λk , we obtain a characterisation of L-structures on L in terms of symmetric brackets. Note that for fixed n, we can write (27) as i+j=n+1 σ  \Sh i,ni 1 (1) (j1)i l j ( l i  \id L (j1) ) χ ^ (σ)=0 \[ \sum_{i+j=n+1} \sum_{\sigma \in \Sh^{-1}_{i,n-i}}(-1)^{(j-1)i} l_j( l_i \otimes \id_L^{\otimes(j-1)}) \hat\chi(\sigma)=0 \]

As and n are isomorphisms, this is equivalent to 0 = (1) n(n1) 2 i+j=n+1 σ  \Sh i,ni 1 (1) (j1)i l j ( l i  \id L (j1) ) χ ^ (σ) n = (1) n(n1) 2 i+j=n+1 σ  \Sh i,ni 1 (1) (j1)i λ j j ( l i  \id L (j1) ) n ε ^ (σ) = (1) n(n1) 2 i+j=n+1 σ  \Sh i,ni 1 λ j (( l i ) (j1) ) n ε ^ (σ) = i+j=n+1 σ  \Sh i,ni 1 λ j ( λ i  \id L[1] (j1) ) ε ^ (σ), \[\begin{array}{@{}l@{}l@{}} 0&\displaystyle=(-1)^{\frac{n(n-1)}{2}}\sum_{i+j=n+1} \sum_{\sigma \in \Sh^{-1}_{i,n-i}}(-1)^{(j-1)i}{\downarrow}\circ l_j( l_i \otimes \id_L^{\otimes(j-1)}) \hat\chi(\sigma)\circ{\uparrow^{\otimes n}}\\ &\displaystyle=(-1)^{\frac{n(n-1)}{2}}\sum_{i+j=n+1} \sum_{\sigma \in \Sh^{-1}_{i,n-i}}(-1)^{(j-1)i}\lambda_j\circ {\downarrow^{\otimes j}}( l_i \otimes \id_L^{\otimes(j-1)}){\uparrow^{\otimes n}}\circ \hatsilon(\sigma)\\ &\displaystyle=(-1)^{\frac{n(n-1)}{2}}\sum_{i+j=n+1} \sum_{\sigma \in \Sh^{-1}_{i,n-i}}\lambda_j( ({\downarrow}\circ l_i) \otimes {\downarrow^{\otimes(j-1)}}){\uparrow^{\otimes n}}\circ \hatsilon(\sigma)\\ &\displaystyle=\sum_{i+j=n+1} \sum_{\sigma \in \Sh^{-1}_{i,n-i}}\lambda_j( \lambda_i \otimes \id_{L[1]}^{\otimes(j-1)})\hatsilon(\sigma), \end{array} \]

where we used (2) and (4). We have proved the following.

Proposition 33. An L-structure {lk ∣1 ≤ k < } on the graded vector space L is equivalent to a system of linear maps λ k : S k (L[1])L[1] $\lambda_k \colon \Sy^k(L[1])\to L[1]$ for 1 ≤ k < , all of degree one, such that i+j=n+1 σ  \Sh i,ni 1 ε(σ) λ j ( λ i ( x σ(1) ,, x σ(i) ), x σ(i+1) ,, x σ(n) )=0 \begin{eqnarray*}&&\sum_{i+j=n+1} \sum_{\sigma \in \Sh^{-1}_{i,n-i}}\varepsilon(\sigma)\nonumber\\ &&\quad\cdot\lambda_j(\lambda_i(x_{\sigma(1)},\dotsc,x_{\sigma(i)}),x_{\sigma(i+1)},\dotsc,x_{\sigma(n)})=0\nonumber\\ \end{eqnarray*}(29) holds for all for all n ≥ 1 and x1, …, xnL[1] homogeneous.

Corollary 34. An L-structure on the graded vector space L is equivalent to a linear degree one map λ:\rsym(L[1])L[1] $\lambda \colon\rsym (L[1])\to L[1]$ such that λ μ S (λ  \id S ) Δ S =0. \begin{equation*}\lambda\circ \mu_S(\lambda\otimes \id_S)\Delta_S=0. \end{equation*}(30)

Proof. Combine the brackets in Proposition 33 to a single element λ= k λ k Hom(\rsym(L[1]),L[1]) $\lambda=\sum_k \lambda_k\in\Hom(\rsym(L[1]),L[1])$ of degree one and compare with (18).

By abuse of notation, we then also refer to the pair (L[1], λ) as an L-algebra. Strict homomorphisms of L-algebras can then be described as degree preserving linear maps that preserve the symmetric brackets.

Proposition 35. Let (L[1], λ) and (L′[1], λ′) be L-algebras. There is a one-to-one correspondence between strict L-algebra homomorphisms f : LLand linear degree preserving maps g =f: L[1] → L′[1] satisfying g λ k = λ k g k \begin{equation*}g\circ \lambda_k = \lambda_k&#x0027;\circ g^{\otimes k} \end{equation*}(31) for all k ≥ 1.

The equation (31) can be written more conveniently as gλ= λ S(g). \begin{equation*}g\circ \lambda = \lambda&#x0027;\circ \Sy(g). \end{equation*}(32)

We then also refer to g as a strict L-algebra homomorphism.

Theorem 36. An L-structure on the graded vector space L is equivalent to a codifferential d\Coder(S(L[1])) $d\in\Coder(\Sy(L[1]))$ with d(1) = 0.

In this case, we also refer to the pair (S(L[1]),d) $(\Sy(L[1]),d)$ as an L-algebra.

Proof. Let λ:\rsym(L[1])L[1] $\lambda \colon\rsym(L[1])\to L[1]$ be of degree one and d = μS(λ ⊗idSS be the unique coderivation extending λ in the sense of Theorem 22. As d 2 = 1 2 [d,d] $d^2=\frac{1}{2}[d,d]$ is a coderivation of S(L[1]) $\Sy(L[1])$ by Proposition 21, we have by Theorem 22 that d2 = 0 if and only if 0= \pr L[1] d 2 =λ μ S (λ  \id S ) Δ S . \[ 0=\pr_{L[1]}\circ d^2= \lambda \circ \mu_S(\lambda\otimes \id_S)\Delta_S. \]

Corollary 37. If L is of finite type and 0 $\Z_{\leq 0}$-graded, an L-structure on L is equivalent to a differential on the graded algebra S(L [1] * ) $\Sy(L[1]^*)$. Explicitly, consider dCE = −d* for d as in Theorem 36.

Proof. See Remark 26 and note that as L is 0 $\Z_{\leq 0}$-graded, each d\Coder(S(L[1])) $d\in\Coder(\Sy(L[1]))$ of degree one vanishes on k ${\mathbb k}$ by degree reasons.

3.3 Weak homomorphisms

Let (S(L[1]),d) $(\Sy(L[1]),d)$ and (S( L [1]), d ) $(\Sy(L&#x0027;[1]),d&#x0027;)$ be L -algebras, λ = prL[1]d and λ = \pr L [1] d $\lambda&#x0027;=\pr_{L&#x0027;[1]}\circ d&#x0027;$. The characterisation of L-structures as codifferentials on the symmetric coalgebra leads to another notion of homomorphisms of L -algebras, namely as homomorphisms of (coaugmented) DGCs.

Definition 38. A (weak) homomorphism of L∞-algebras between L and L′ is a homomorphism of coaugmented DGCs f:S(L[1])S( L [1]) $f\colon \Sy(L[1])\to \Sy(L&#x0027;[1])$.

Remark 39. By Proposition 21 and Theorem 22, a homomorphism of coaugmented coalgebras f:S(L[1])S( L [1]) $f\colon \Sy(L[1])\to \Sy(L&#x0027;[1])$ is a homomorphism of L-algebras if and only if ( \pr L [1] f)d= λ f. \[(\pr_{L&#x0027;[1]}\circ f)\circ d=\lambda&#x0027;\circ f.\]

Note that by Proposition 20, it makes sense to also refer to DGC homomorphisms \rsym(L[1]) \rsym( L [1]) $\rsym(L[1])\to \rsym(L&#x0027;[1])$ as homomorphisms of L-algebras.

From the dualised standpoint, we immediately get the following.

Proposition 40. Assume that L and Lare 0 $\Z_{\leq 0}$-graded and of finite type. Then f:S(L[1])S( L [1]) $f\colon \Sy(L[1])\to \Sy(L&#x0027;[1])$ is a homomorphism of L-algebras if and only if f * :S( L [1] * )S(L [1] * ) $f^*\colon \Sy(L&#x0027;[1]^*)\to \Sy(L[1]^*)$ is a homomorphism of unital DG algebras.

With now two different notions of L-algebra homomorphisms at hand, it is reasonable to ask if there is a connection between them. As commented in ([8], Remark 5.3), strict homomorphisms are essentially the weak homomorphisms that preserve the exterior degree.

Lemma 41. Let g: L[1] → L′[1] be a linear degree preserving map. Then g is a strict L-algebra homomorphism if and only if S(g) $\Sy(g)$ is a weak one.

Proof. Observe that \pr L [1] S(g)d=g  \pr L[1] d=gλ $\pr_{L&#x0027;[1]}\circ \Sy(g)\circ d = g\circ \pr_{L[1]}\circ d= g\circ \lambda$.

Lemma 42. A homomorphism of coalgebras f:S(L[1])S( L [1]) $f\colon \Sy(L[1])\to \Sy(L&#x0027;[1])$ preserves the exterior degree if and only if f=S(g) $f=\Sy(g)$ for a linear degree preserving map g: L[1] → L′[1].

Proof. Assume that f:S(L[1])S( L [1]) $f\colon \Sy(L[1])\to \Sy(L&#x0027;[1])$ is a homomorphism of coalgebras such that f( S n (L[1])) S n ( L [1]) $f(\Sy^n(L[1]))\subset \Sy^n(L&#x0027;[1])$ for all n and let g  \pr L [1] f| L[1] $g\vcentcolon = \pr_{L&#x0027;[1]}\circ \left. f \right|_{L[1]}$. Then \pr L [1] f=g  \pr L[1] = \pr L [1] S(g) $\pr_{L&#x0027;[1]}\circ f=g\circ \pr_{L[1]}=\pr_{L&#x0027;[1]}\circ \Sy(g)$. Hence, f=S(g) $f=\Sy(g)$ by Proposition 18.

Proposition 43. Let f:S(L[1])S( L [1]) $f\colon \Sy(L[1])\to \Sy(L&#x0027;[1])$ be a (weak) L-algebra homomorphism. Then f preserves the exterior degree if and only if f=S(g) $f=\Sy(g)$ for a strict L-algebra homomorphism g.

Proof. Combine Lemma 41 and Lemma 42.

From this it follows for example that all (weak) L -algebra homomorphisms between Lie algebras are induced by Lie algebra homomorphisms.

4 Representations (up to homotopy)

While representations (up to homotopy) of L-algebras are often defined in terms of antisymmetric maps, we start with a definition that keeps the symmetric point of view of the last section. While it is a straightforward computation to show equivalence between these definitions, it is convenient to save this for Section 5.1. We then show that representations (up to homotopy) are nothing else than weak L -algebra homomorphisms into 𝔤𝔩(V ) for a DG vector space V , a characterisation due to Lada and Markl [8]. In [3], representations (up to homotopy) were described (under some finiteness assumptions) as differentials on S(L [1] * )V $\Sy(L[1]^*)\otimes V$. We discuss this point of view in the second half of this section, which also leads us to L -algebra cohomology.

From now on, L denotes an L-algebra with L-structure {lk ∣ 1 ≤ k < } and λ and d are as in Corollary 34 and Theorem 36, respectively.

Definition 44. A representation (up to homotopy) of L on V is a linear map ρ:S(L[1])VV ${\rho\colon \Sy(L[1])\otimes V\to V}$ of degree one that satisfies ρ(d  \id V )+ρ( id S ρ)( Δ S  \id V )=0. \begin{equation*}\rho(d\otimes \id_V)+\rho(\id_S\otimes \rho)(\Delta_S\otimes \id_V)=0. \end{equation*}(33)

4.1 Representations as (weak) homomorphisms

We prove the following version of ([8], Theorem 5.2).

Theorem 45. There is a one-to-one correspondence between representations of L on V and pairs (, f ˜ ) $(\partial,\tilde f)$, where ∂ is a differential on V and f ˜ :S(L[1])S(gl(V)[1]) $\tilde f\colon \Sy(L[1])\to \Sy(\mathfrak{gl}(V)[1])$ a homomorphism of L-algebras. Here, 𝔤𝔩(V ) carries the DGLA structure induced by ∂, see Example 12.

One should therefore really think of L being representated on a DG vector space. The following lemma characterises L -algebra homomorphisms into DGLAs and is a symmetric version of ([8], Definition 5.2).

Lemma 46. Let ( L , l 2 , l 1 ) $(L&#x0027;,l&#x0027;_2,l&#x0027;_1)$ be a DGLA and λ = λ 1 + λ 2 $\lambda&#x0027;=\lambda&#x0027;_1+\lambda&#x0027;_2$ be the corresponding linear degree one map \rsym( L [1]) L [1] $\rsym(L&#x0027;[1])\to L&#x0027;[1]$. For f: \ol\Sy(L[1]) L [1] $f\colon \ol\Sy(L[1])\to L&#x0027;[1]$ a linear degree preserving map, the induced homomorphism of coalgebras f ˜ : \rsym(L[1]) \rsym( L [1]) $\tilde f\colon \rsym(L[1])\to \rsym(L&#x0027;[1])$ is a homomorphism of L-algebras if and only if f \old= λ 1 f+ 1 2 λ 2 (ff)\ol Δ S . \begin{equation*}f\circ \ol d= \lambda_1&#x0027;\circ f + \frac{1}{2}\lambda_2&#x0027;(f\otimes f)\ol\Delta_S. \end{equation*}(34)

This is the case if and only if the linear degree one map ρ: \rsym(L[1]) L $\rho\colon \rsym(L[1])\to L&#x0027;$ defined by f(x)= (1) |x|+1 ρ(x) $f(x)=(-1)^{|x|+1}\downarrow \rho(x)$ satisfies ρ \old+ l 1 ρ+ 1 2 l 2 (ρρ)\ol Δ S =0. \begin{equation*}\rho\circ \ol d +l&#x0027;_1\circ \rho +\frac{1}{2} l&#x0027;_2(\rho\otimes \rho)\ol \Delta_S=0. \end{equation*}(35)

Proof. The first part follows immediately from Remark 39 and the explicit construction of f ˜ $\tilde f$ (see Proposition 18). It is straightforward to check that for x \rsym(L[1]) $x\in \rsym(L[1])$ homogeneous, f(d(x)) = (1) |x| ρ(d(x)), λ 1 (f(x)) = (1) |x|+1 l 1 (ρ(x)), ( λ 2 (ff)\ol Δ S )(x) = (1) |x|+1 ( l 2 (ρρ)\ol Δ S )(x), \begin{eqnarray*} f(d(x))&=&(-1)^{|x|}\downarrow\rho(d(x)),\nonumber\\ \lambda&#x0027;_1(f(x))&=&(-1)^{|x|+1}\downarrow l_1&#x0027;(\rho(x)),\nonumber\\ \big(\lambda&#x0027;_2(f\otimes f)\ol\Delta_S\big)(x)&=&(-1)^{|x|+1}\downarrow \big(l&#x0027;_2(\rho\otimes\rho)\ol\Delta_S\big)(x),\nonumber \end{eqnarray*}

from which the second part then follows.

Proof of Theorem 45: As Hom(S(L[1])V,V) \Hom(S(L[1]),\gl(V)) $\Hom(\Sy(L[1])\otimes V,V)\cong \Hom(\Sy(L[1]),\gl(V))$, a linear degree one map ρ:S(L[1])VV $\rho\colon \Sy(L[1])\otimes V \to V$ can be decomposed into linear degree one maps ρ ˜ : \ol\Sy(L[1]) \gl(V) $\tilde\rho\colon \ol\Sy(L[1])\to \gl(V)$ and ρ 0 :k \gl(V) $\rho_0\colon {\mathbb k} \to \gl(V)$; the latter being equivalent to the choice of a degree one element = ρ 0 ( 1 k ) \gl(V) $\partial=\rho_0(1_{\mathbb k})\in \gl(V)$. If we show that under this identification ρ satisfying (33) is equivalent to 2 = 0 and ρ ˜ $\tilde \rho$ satisfying (35), the assertion follows by Lemma 46. For x \rsym(L[1]) $x\in \rsym(L[1])$ homogeneous, 1 2 (\bracket( ρ ˜ ρ ˜ ) \ol Δ S )(x) = 1 2 (1) | x (1) | [ ρ ˜ ( x (1) ), ρ ˜ ( x (2) )] = 1 2 (1) | x (1) | ρ ˜ ( x (1) ) ρ ˜ ( x (2) )   + (1) | x (1) || x (2) |+| x (2) | ρ ˜ ( x (2) ) ρ ˜ ( x (1) ) = 1 2 ρ ( id S ρ)( x (1) x (2)   + (1) | x (1) || x (2) | x (2) x (1) ,\ea) =ρ( id S ρ)(\ol Δ S (x),\ea) \[\begin{array}{ll} &\displaystyle\frac{1}{2}\big(\bracket(\tilde\rho\otimes \tilde\rho) \ol\Delta_{S}\big)(x)\\[6pt] &\displaystyle\quad=\frac{1}{2}\sum (-1)^{|x_{(1)}|}[\tilde\rho(x_{(1)}),\tilde\rho(x_{(2)})]\\[6pt] &\displaystyle\quad=\frac{1}{2}\sum (-1)^{|x_{(1)}|}\tilde\rho(x_{(1)})\circ \tilde\rho(x_{(2)})\\[6pt] &\displaystyle\qquad+(-1)^{|x_{(1)}||x_{(2)}|+|x_{(2)}|}\tilde\rho(x_{(2)})\circ\tilde\rho(x_{(1)})\\[6pt] &\displaystyle\quad=\frac{1}{2}\sum \rho(\id_{S}\otimes \rho)(x_{(1)}\otimes x_{(2)}\\[6pt] &\displaystyle\qquad+(-1)^{|x_{(1)}||x_{(2)}|}x_{(2)}\otimes x_{(1)},\ea)\\[6pt] &\displaystyle\quad=\rho(\id_{S}\otimes \rho)(\ol\Delta_{S}(x),\ea) \end{array}\]

by cocommutativity of \rsym(L[1]) $\rsym(L[1])$ and [, ρ ˜ (x)] = ρ ˜ (x) (1) | ρ ˜ (x)| ρ ˜ (x) = ρ 0 (1) ρ ˜ (x)+ (1) |x| ρ ˜ (x) ρ 0 (1) = ρ( id S ρ)(1x+x1,\ea). \begin{eqnarray*} [\partial,\tilde\rho(x)]&=& \partial\circ \tilde\rho(x) -(-1)^{|\tilde\rho(x)|}\tilde\rho(x)\circ\partial\nonumber\\ &=& \rho_0 (1)\circ \tilde\rho (x) + (-1)^{|x|}\tilde\rho (x)\circ \rho_0(1)\nonumber\\ &=& \rho(\id_S\otimes \rho)(1\otimes x + x\otimes 1,\ea).\nonumber \end{eqnarray*}

As ( ρ ˜ d)(x)=ρ(d  \id V )(x,\ea) $(\tilde\rho\circ d)(x) = \rho(d\otimes \id_V)(x,\ea)$, ρ ˜ $\tilde\rho$ satisfying (35) is equivalent to (33) holding on \rsym(L[1])V $\rsym(L[1])\otimes V$. We also have (ρ(d  \id V )+ρ( id S ρ)( Δ S  \id V ))(1,) =ρ(1,ρ(1,))= 2 , \[ \begin{array}{lll} &&\big(\rho(d\otimes \id_V)+\rho(\id_S\otimes \rho)(\Delta_S\otimes \id_V)\big)(1,\,\cdot\,)\\ &&\quad=\rho(1,\rho(1,\,\cdot\,))=\partial^2,\\ \end{array} \]

which completes the proof as S(L[1])=k \rsym(L[1]) $\Sy(L[1])={\mathbb k}\oplus \rsym(L[1])$.

Example 47 (The trivial representation on a DG vector space). Let (V, ) be a DG vector space. There is a trivial strict homomorphism of L-algebras 0: L → 𝔤𝔩(V ). The induced representation S(L[1])VV $\Sy(L[1])\otimes V\to V$ is on kVV ${\mathbb k} \otimes V\cong V$ given by and zero elsewhere and is called the trivial representation of L on V . In particular, there is a trivial representation of L on k ${\mathbb k}$.

Remark 48. Let ρ be a representation of L on V and (, f ˜ ) $(\partial, \tilde f)$ as in Theorem 45.

  • (1)

    Then − * is a differential on V * and the map 𝔤𝔩(V ) → 𝔤𝔩(V *), g↦ − g* is a homomorphism of DGLAs. By composing the corresponding weak homomorphism with f ˜ $\tilde f$, we obtain an L-algebra homomorphism S(L[1])S(\gl( V * )[1]) $\Sy(L[1])\to \Sy(\gl(V^*)[1])$. The induced representation is given by ρ :S(L[1]) V * V * ,xξρ (x,\ea) * ξ \[ \rho^{\vee} \colon \Sy(L[1])\otimes V^* \to V^*, \quad x\otimes \xi \mapsto -\rho(x,\ea)^*\xi \] and is called the representation dual to ρ.

  • (2)

    Fix n $n\in\Z$. Then (1) n n n $(-1)^n\downarrow^n\circ \partial \circ \uparrow^n$ is a differential on V [n] and \gl(V)\gl(V[n]),g (1) n|g| n g n \[\gl(V)\to\gl(V[n]),\quad g\mapsto (-1)^{n|g|}\downarrow^n\circ g\circ \uparrow^n\] is a DGLA homomorphism. The induced representation of L on V [n] is given by S(L[1])V[n]V[n], x n v (1) n+n|x| n ρ(x,v). \[ \begin{array}{lll} &&\Sy(L[1])\otimes V[n]\to V[n], \\ && x\otimes {\downarrow^n}v\mapsto (-1)^{n+n|x|}{\downarrow^n}\rho(x,v). \end{array} \]

4.2 Representations as coderivations

Observe that the map Δ V Δ S  \id V :S(L[1])VS(L[1])(S(L[1])V) $\Delta_V\vcentcolon= \Delta_S\otimes \id_V\colon \Sy(L[1])\otimes V \to \Sy(L[1])\otimes (\Sy(L[1])\otimes V)$ satisfies ( Δ S  \id SV ) Δ V =( id S Δ V ) Δ V , \begin{equation*}(\Delta_S\otimes \id_{S\otimes V})\Delta_V= (\id_S\otimes \Delta_V)\Delta_V, \end{equation*}(36)

which makes S(L[1])V $\Sy(L[1])\otimes V$ into a left S(L[1]) $\Sy(L[1])$-comodule.

Definition 49. Let d  \Coder(S(L[1])) $d&#x0027;\in \Coder(\Sy(L[1]))$ be of degree p. A coderivation of S(L[1])V $\Sy(L[1])\otimes V$ extending d′ is a linear map D:S(L[1])VS(L[1])V $D\colon \Sy(L[1])\otimes V \to \Sy(L[1])\otimes V$ of degree p such that Δ V D=( d  \id SV +  \id S D) Δ V . \begin{equation*}\Delta_V\circ D= (d&#x0027; \otimes \id_{S\otimes V} + \id_S\otimes D) \Delta_V. \end{equation*}(37)

Proposition 50 ([6], Proposition 1.5.3, p. 31). Let d \Coder(S(L[1])) $d&#x0027;\in\Coder(\Sy(L[1]))$ be of degree p. There is a one-to-one correspondence between coderivations D of S(L[1])V $\Sy(L[1])\otimes V$ extending dand linear maps ρ:S(L[1])VV $\rho\colon\Sy(L[1])\otimes V\to V$ of degree p given by D = d  \id V +( id S ρ) Δ V , ρ = \pr V D, \begin{eqnarray*}D&=&d&#x0027;\otimes \id_V + (\id_S\otimes \rho)\Delta_V,\nonumber\\ \rho&=&\pr_V\circ D,\nonumber \end{eqnarray*} where \pr V :S(L[1])VV $\pr_V\colon \Sy(L[1])\otimes V\to V$ is the projection of S(L[1])V $\Sy(L[1]) \otimes V$ onto kVV ${\mathbb k} \otimes V \cong V$.

Proof. Let D be a coderivationof S(L[1])V $\Sy(L[1])\otimes V$ extending d′. As (idS ⊗prV)(ΔS ⊗idV) = idS ⊗idV, we obtain from (37) that D = ( id S  \pr V ) Δ V D = ( id S  \pr V )( d  \id S  \id V +  \id S D) Δ V = ( d  \id V )( id S  \pr V ) Δ V +( id S ( \pr V D)) Δ V = d  \id V +( id S ( \pr V D)) Δ V . \begin{eqnarray*} D&=& (\id_S\otimes \pr_V) \Delta_V \circ D\nonumber\\ &=& (\id_S\otimes \pr_V) (d&#x0027;\otimes \id_S\otimes \id_V + \id_S\otimes D) \Delta_V\nonumber\\ &=&(d&#x0027;\otimes \id_V)(\id_S\otimes \pr_V)\Delta_V + (\id_S\otimes (\pr_V\circ D)) \Delta_V\nonumber\\ &=&d&#x0027;\otimes \id_V + (\id_S\otimes (\pr_V\circ D)) \Delta_V.\nonumber \end{eqnarray*}

This shows that D is completely determined by prVD.

Let conversely ρ \Hom(S(L[1])V,V) $\rho\in \Hom(\Sy(L[1])\otimes V,V)$ be of degree p. Using (36) and that d′ is a coderivation, we compute Δ V ( id S ρ) Δ V = ( Δ S ρ) Δ V = ( id SS ρ)( id S Δ V ) Δ V = ( id S ( id S ρ) Δ V ) Δ V , Δ V ( d  \id V ) = (( d  \id S + id S d ) Δ S )  \id V = ( d  \id SV +  \id S d  \id V ) Δ V , \begin{eqnarray*} \Delta_V\circ (\id_S\otimes \rho)\Delta_V&=&(\Delta_S\otimes \rho)\Delta_V\nonumber\\ &=&(\id_{S\otimes S}\otimes \rho)(\id_S\otimes \Delta_V)\Delta_V\nonumber\\ &=&(\id_S\otimes (\id_S\otimes \rho)\Delta_V)\Delta_V,\nonumber\\ \Delta_V\circ (d&#x0027;\otimes \id_V)&=& ((d&#x0027;\otimes \id_S+\id_S\otimes d&#x0027;)\Delta_S)\otimes \id_V\nonumber\\ &=& (d&#x0027;\otimes \id_{S\otimes V}+ \id_S \otimes d&#x0027; \otimes \id_V)\Delta_V,\nonumber \end{eqnarray*}

which, combined, show that D := d ⊗idV + (idSρV is a coderivation of S(L[1])V $\Sy(L[1])\otimes V$ extending d. It is easy to see that then prVD = ρ, which completes the proof.

Corollary 51. There is a one-to-one correspondence between representations (up to homotopy) of L on V and coderivations D:S(L[1])VS(L[1])V $D\colon \Sy(L[1])\otimes V\to \Sy(L[1])\otimes V$ extending d such that D2 = 0.

Proof. It is a straightforward computation to check that D 2 = 1 2 [D,D] $D^2=\frac{1}{2}[D,D]$ is a coderivation of S(L[1])V $\Sy(L[1])\otimes V$ extending 1 2 [d,d]= d 2 =0 $\frac{1}{2}[d,d]=d^2=0$. By Proposition 50, D2 = 0 if and only if ρ = prVD satisfies 0= \pr V D 2 =ρ(d  \id V )+ρ( id S ρ)( Δ S  \id V ). \[ 0=\pr_V\circ D^2=\rho(d\otimes \id_V) + \rho(\id_S\otimes \rho)(\Delta_S\otimes \id_V). \]

4.3 A first approach to L-algebra cohomology

Assume now that the L-algebra L is 0 $\Z_{\leq 0}$-graded and of finite type and that V is either finite-dimensional or of finite type and trivial in the negative degrees. We then have S (L[1]) * S(L [1] * ) $\Sy(L[1])^*\cong \Sy(L[1]^*)$, VV ** and (S(L[1]) V * ) * S(L [1] * )V $(\Sy(L[1])\otimes V^*)^*\cong\Sy(L[1]^*)\otimes V$. Let dCE = −d* denote the differential on S(L [1] * ) $\Sy(L[1]^*)$. The map S(L [1] * )(S(L [1] * )V)S(L [1] * )V, (ξ(ηv))(ξη)v \[ \begin{array}{lll} &&\Sy(L[1]^*)\otimes (\Sy(L[1]^*)\otimes V)\to \Sy(L[1]^*)\otimes V,\\ &&\quad(\xi\otimes(\eta\otimes v))\mapsto (\xi\vee \eta)\otimes v \end{array} \]

makes S(L [1] * )V $\Sy(L[1]^*)\otimes V$ into a left S(L [1] * ) $\Sy(L[1]^*)$-module. Similarly to Definition 49, we call a linear map D CE :S(L [1] * )VS(L [1] * )V $D_{CE}\colon \Sy(L[1]^*)\otimes V\to \Sy(L[1]^*)\otimes V$ of degree one a derivation of S(L [1] * )V $\Sy(L[1]^*)\otimes V$ extending dCE if D CE (ξ(ηv))= d CE ξ(ηv)+ (1) |ξ| ξ D CE (ηv) \[ D_{CE}(\xi\vee (\eta\otimes v))=d_{CE}\xi\vee (\eta\otimes v) +(-1)^{|\xi|}\xi\vee D_{CE}(\eta\otimes v) \]

holds for all ξ,ηS(L [1] * ) $\xi,\eta\in \Sy(L[1]^*)$, vV homogeneous.

Note that a representation of L on V is equivalent to a representation on V * by Remark 48 and VV **. As the notion of a derivation extending dCE is dual to the one of a coderivation extending d, we get the following dualized version of Corollary 51.

Proposition 52. A representation ρ of L on V is equivalent to a derivation D CE :S(L [1] * )VS(L [1] * )V $D_{CE}\colon \Sy(L[1]^*)\otimes V\to \Sy(L[1]^*)\otimes V$ extending dCE with D CE 2 =0 $D_{CE}^2=0$. Explicitly, we have DCE = −D*, where D is the coderivation extending d induced by the dual representation ρ.

For a fixed representation ρ of L on V , we can then see S(L [1] * )V $\Sy(L[1]^*)\otimes V$ as our generalized Chevalley–Eilenberg complex with coboundary operator DCE.

4.4 A dead-end

This not only provides us with an explicit construction of the coboundary operator from a given representation, but also gives it the additional structure of a derivation extending dCE . Unfortunately, this came at the cost of the finiteness assumptions we imposed on L on V at the beginning of Section 4.3. As our goal is to establish a generalisation of Theorem 32 – which does not need such assumptions – in terms of L-algebra cohomology, this is not the appropriate framework for our purposes. We can, however, make the following observation.

Remark 53. With our finiteness assumptions on L and V , we have S(L [1] * )VHom(S(L[1]),V), $ \Sy(L[1]^*)\otimes V\cong\Hom(\Sy(L[1]),V), $ where ξvS(L [1] * )V $\xi\otimes v\in \Sy(L[1]^*)\otimes V$ is identified with the linear map S(L[1])V $\Sy(L[1])\to V$, x (1) |x||v| ξ(x)v $x\mapsto (-1)^{|x||v|}\xi(x) \cdot v$. For f \Hom(S(L[1]),V) $f\in \Hom(\Sy(L[1]),V)$ homogeneous, one finds that DCE f is then given by D CE f=ρ( id S f) Δ S (1) |f| fd. \begin{equation*}D_{CE}f= \rho(\id_S\otimes f)\Delta_S-(-1)^{|f|}f\circ d. \end{equation*}(38)

One could then simply define D CE : \Hom(S(L[1]),V) \Hom(S(L[1]),V) $D_{CE}\colon \Hom(\Sy(L[1]),V)\to \Hom(\Sy(L[1]),V)$ by (38), even if L and V do not meet our finiteness assumptions. Although there is a priori no reason for D CE 2 =0 $D_{CE}^2=0$ to hold in the general case, a straightforward computation shows that it actually does. While this leaves us with nothing but the formula (38) to work with, it also suggests that there should be another approach to L -algebra cohomolgy that gets by without the need of finiteness assumptions.

In [4], the L-algebra cohomology with values in the adjoint representation was introduced in terms of the commutator bracket of coderivations and the isomorphism \Coder(\rsym(L[1]),\rsym(L[1])) \Hom(\rsym(L[1]),L[1]) $\Coder(\rsym(L[1]),\rsym(L[1]))\cong \Hom(\rsym(L[1]),L[1])$. In the next section, we extend this approach to arbitrary representations, which leads to a generalisation of Theorem 32 in a rather natural way.

5 L-algebra cohomology

5.1 The Lie bracket on Hom(\rsym(L[1]V),L[1]V) $\Hom(\rsym(L[1]\oplus V),L[1]\oplus V)$

Recall from Proposition 21 that \Coder(S(L[1])) $\Coder(\Sy(L[1]))$ is closed under the graded commutator. Together with Theorem 22, this induces a Lie bracket on Hom(S(L[1]),L[1]) $\Hom(\Sy(L[1] ),L[1] )$. Its explicit formula is [f,g]=f μ S (g id S ) Δ S (1) |f||g| g μ S (f  \id S ) Δ S \begin{equation*}[f,g]=f\circ \mu_S(g\otimes\id_S)\Delta_S-(-1)^{|f||g|}g\circ \mu_S(f\otimes \id_S)\Delta_S \end{equation*}(39)

for f,gHom(S(L[1]),L[1]) $f,g\in\Hom(\Sy(L[1] ),L[1] )$ homogeneous.

As L-structures correspond to codifferentials with d(1) = 0 and elements in Hom(\rsym(L[1]),L[1]) $\Hom(\rsym(L[1]),L[1])$, it is only natural to restrict ourselves to the Lie subalgebra Hom(\rsym(L[1]),L[1]) $\Hom(\rsym(L[1]),L[1])$. Keeping the Hom(k,L[1]) $\Hom({\mathbb k}, L[1])$ part corresponds to the framework of curved L∞-algebras, which are L-algebras that also allow for a 0-ary bracket kL[1] ${\mathbb k}\to L[1]$.

Remark 54. The same construction also makes Hom(\rsym(L[1]V),L[1]V) $\Hom(\rsym(L[1]\oplus V),L[1]\oplus V)$ into a graded Lie algebra. The decomposition S(L[1]V)S(L[1])S(V) $\Sy(L[1]\oplus V)\cong \Sy (L[1]) \otimes \Sy (V)$ implies that \rsym(L[1]V) \rsym(L[1]) \rsym(V) \rsym(L[1]) \rsym(V). \begin{equation*}\rsym(L[1]\oplus V)\cong \rsym(L[1])\otimes \rsym(V)\oplus \rsym(L[1])\oplus \rsym(V). \end{equation*}(40)

We can then consider spaces like Hom(\rsym(L[1]),L[1]) $\Hom(\rsym(L[1]),L[1])$ and Hom(\rsym(L[1])V,V) $\Hom(\rsym (L[1])\otimes V, V)$ as subspaces of Hom(\rsym(L[1]V),L[1]V) $\Hom(\rsym (L[1] \oplus V),\ L[1]\oplus V)$ in the obvious way. The inclusion of Hom(\rsym(L[1]),L[1]) $\Hom(\rsym(L[1]),L[1])$ into Hom(\rsym(L[1]V),L[1]V) $\Hom(\rsym(L[1]\oplus V),L[1]\oplus V)$ is then easily seen to preserve the Lie bracket.

Remark 55. In terms of the Lie bracket on Hom(\rsym(L[1]),L[1]) $\Hom(\rsym(L[1]),L[1])$, the condition (30) for a linear map λ: \rsym(L[1])L[1] $\lambda\colon \rsym(L[1])\to L[1]$ of degree one to define an L-algebra structure on L[1] becomes 1 2 [λ,λ]=0. \begin{equation*} \frac{1}{2}[\lambda,\lambda]=0. \end{equation*}(41)

By Example 12 and Remark 54, this makes Hom(\rsym(L[1]V),L[1]V) $\Hom(\rsym(L[1]\oplus V),L[1]\oplus V)$ into a DGLA. Solutions of the Maurer–Cartan equation then induce new L -structures on L[1] ⊕ V by Example 14.

By abuse of notation, we now denote the (co)products on S(L[1]) $\Sy(L[1])$ and S(L[1]V) $\Sy(L[1]\oplus V)$ both by μS and ΔS . This is justified, as they coincide on S(L[1])S(L[1]V) $\Sy(L[1])\subset \Sy(L[1]\oplus V)$.

In (38), d = μS(λ ⊗idSS and μS(idSfS = μS(f ⊗idSS due to S(L[1]) $\Sy(L[1])$ being (co)commutative. The similarity between (38) and (39) suggests to approach L -algebra cohomology using the Lie bracket on Hom(\rsym(L[1]V),L[1]V) $\Hom(\rsym(L[1]\oplus V),L[1]\oplus V)$.

Proposition 56. Let ρHom(S(L[1])V,V) $\rho\in\Hom(\Sy(L[1])\otimes V,V)$ be of degree one. Then ρ is a representation of L on V if and only if ρ μ S (ρ  \id S ) Δ S +ρ μ S (λ  \id S ) Δ S =0, \begin{equation*}\rho\circ\mu_S(\rho\otimes \id_S)\Delta_S + \rho\circ\mu_S(\lambda\otimes \id_S)\Delta_S=0, \end{equation*}(42) where λ and ρ are considered as elements of Hom(\rsym(L[1]V),L[1]V) $\Hom(\rsym(L[1]\oplus V),L[1]\oplus V)$.

Proof. Note that ρμS(ρ ⊗idSS and ρμS(ρ ⊗idSS are only possibly nonzero on S(L[1])V $\Sy(L[1])\otimes V$. For x1, …, xn−1L[1] and xnV , a routine computation using Lemma 24 shows that (ρ μ S (λ  \id S ) Δ S )( x 1 x n ) =ρ(d( x 1 x n1 ), x n ), (ρ μ S ( id S ρ) Δ S )( x 1 x n ) =ρ( id S ρ)( Δ S ( x 1 x n1 ), x n ). \[\begin{array}{ll} &(\rho\circ\mu_S(\lambda\otimes \id_S)\Delta_S)(x_1\vee\dotsc \vee x_n)\\ &\quad= \rho(d(x_1\vee\dotsc\vee x_{n-1}),x_n),\\ &(\rho\circ\mu_S(\id_S\otimes \rho)\Delta_S)(x_1\vee\dotsc \vee x_n)\\ &\quad=\rho(\id_S\otimes \rho)(\Delta_S(x_1\vee\dotsc\vee x_{n-1}),x_n). \end{array} \]

As again μS(ρ ⊗idSS = μS(idSρS by (co)commutativity of \rsym(L[1]V) $\rsym(L[1]\oplus V)$, ρ satisfies (33) if and only if it satisfies (42).

Corollary 57. An element ρHom(S(L[1])V,V) $\rho\in\Hom(\Sy(L[1])\otimes V,V)$ of degree one is representation of L on V if and only if (L[1] ⊕ V, λ + ρ) is an L-algebra.

Proof. We have 1 2 [λ+ρ,λ+ρ] = 1 2 [λ,λ]+[λ,ρ]+ 1 2 [ρ,ρ] = ρ μ S (λ  \id S ) Δ S +ρ μ S (ρ  \id S ) Δ S . \begin{eqnarray*} \frac{1}{2}[\lambda+\rho,\lambda+\rho]&{=}&\frac{1}{2}[\lambda,\lambda]+[\lambda,\rho]+\frac{1}{2}[\rho,\rho]\nonumber\\ &{=}&\rho\circ\mu_S(\lambda\otimes \id_S)\Delta_S{+} \rho\circ\mu_S(\rho\otimes \id_S)\Delta_S.\nonumber \end{eqnarray*}

Corollary 58. The subspace Hom(S(L[1])V,V) $\Hom(\Sy(L[1])\otimes V,V)$ is invariant under the Lie bracket [⋅, ⋅] and the differential [λ, ⋅ ]. Representations (up to homotopy) of L on V are then exactly the Maurer–Cartan elements in Hom(S(L[1])V,V) $\Hom(\Sy(L[1])\otimes V,V)$.

By applying Proposition 33 to Corollary 57 and using that a representation on V is equivalent to one on V [1] by Remark 48, we obtain the following.

Proposition 59. A representation of L on V is equivalent to a system of linear maps ρk: ∧k−1LVV of degree 2 − k for k ≥ 1 such that {lk + ρk: ∧k(LV ) → LV ∣1 ≤ k < } is an L-structure on LV .

Remark 60. It is easy to see that the generalized Jacobi identity (27) for {lk + ρk∣1 ≤ k < } has only to be checked on ∧ Ln−1V for each n ≥ 1. Representations of L-algebras are often defined in terms of these equations, see for example ([8], Definition 5.1) and ([3], Definition 18). Similarly, equation (42) on S(L[1])V $\Sy(L[1])\otimes V$ is easily seen to be the condition imposed on ρ in ([3], Definition 19).

For a fixed representation ρ of L on V , [λ +ρ, ⋅ ] makes Hom(\rsym(L[1]V),L[1]V) $\Hom(\rsym(L[1]\oplus V),L[1]\oplus V)$ into a DGLA. The space Hom(\rsym(L[1]),V) $\Hom(\rsym(L[1]),V)$ is then an abelian Lie subalgebra that is invariant under [λ + ρ, ⋅ ]. Explicitly, we have for f \Hom(\rsym(L[1]),V) $f\in \Hom(\rsym(L[1]),V)$ homogeneous [λ+ρ,f]=ρ( id S f) Δ S (1) |f| fd. \begin{equation*}[\lambda+\rho, f]=\rho(\id_S\otimes f)\Delta_S-(-1)^{|f|}f\circ d. \end{equation*}(43)

Definition 61. The map δ[λ+ρ,\ea]: \Hom(\rsym(L[1]),V) \Hom(\rsym(L[1]),V) $\delta\vcentcolon=[\lambda+\rho,\ea]\colon \Hom (\rsym(L[1]),V)\to \Hom(\rsym(L[1]),V)$ is called the L∞-coboundary operator. The cohomology of the cochain complex (Hom(\rsym(L[1]),V),δ) $(\Hom(\rsym(L[1]),V),\delta)$ is called the L∞-algebra cohomology with values in V.

Remark 62. For L and V as in Section 4.3, we clearly have δ = DCE. If L = 𝔤 and V are concentrated in degree zero, the décalage isomorphism (5) implies that nn\Hom p (\rsym(g[1]),V) n1 Hom pn ( \Asy n g,V)  \Hom( \Asy p g,V) \begin{eqnarray*} \Hom_p(\rsym(\mathfrak g[1]),V)&\cong& \prod_{n\geq 1}\Hom_{p-n}(\Asy^n \mathfrak g,V)\nonumber\\ &\cong& \Hom(\Asy^p\mathfrak g,V)\nonumber \end{eqnarray*}

for all p ≥ 1. This way, we recover the usual Lie algebra cohomology.

Example 63 (The adjoint representation). The adjoint representation of L on L[1] is given by S(L[1])L[1]L[1] $\Sy(L[1])\otimes L[1]\to L[1]$, xyλ(xy). While there are now two distinct copies of L[1] involved, it is evident by (43) that δ = [λ, ⋅ ], the bracket being the one on Hom(\rsym(L[1]),L[1]) $\Hom(\rsym(L[1]),L[1])$. This is the case discussed in [4].

5.2 L-structures induced by 2-cocycles

The description of L-structures, representations (up to homotopy) and the L-coboundary operator all by the same Lie bracket yields the following generalisation of Theorem 32.

Theorem 64. Let L and V be graded vector spaces and λHom(\rsym(L[1]),L[1]) ${\lambda\in\Hom(\rsym(L[1]),L[1])}$, ρ \Hom(S(L[1])V,V) $\rho\in \Hom(\Sy(L[1])\otimes V,V)$ and ω \Hom(\rsym(L[1]),V) $\omega\in \Hom(\rsym(L[1]),V)$ be all of degree one. Then (L[1] ⊕ V, λ + ρ + ω) is an L-algebra if and only if (L[1], λ) is an L-algebra, ρ is a representation of L on V and ω is a V-valued cocycle.

Proof. The map 1 2 [λ+ρ+ω,λ+ρ+ω]= 1 2 [λ,λ]+[λ,ρ]+ 1 2 [ρ,ρ]+[λ+ρ,ω] $ \frac{1}{2}[\lambda+\rho+\omega,\lambda+\rho+\omega]=\frac{1}{2}[\lambda,\lambda]+[\lambda,\rho]+\frac{1}{2}[\rho,\rho]+[\lambda+\rho,\omega] $ decomposes itself into linear maps 1 2 [λ,λ] : S(L[1])L[1], [λ,ρ]+ 1 2 [ρ,ρ] : S(L[1])VV, [λ+ρ,ω] : S(L[1])V. \begin{eqnarray*} \frac{1}{2}[\lambda,\lambda]&\colon& \Sy(L[1])\to L[1],\nonumber\\ {}[\lambda,\rho]+\frac{1}{2}[\rho,\rho]&\colon& \Sy(L[1])\otimes V\to V,\nonumber\\ {}[\lambda+\rho,\omega]&\colon& \Sy(L[1])\to V.\nonumber \end{eqnarray*}

The assertion then follows from Remark 55, Corollary 58 and the definition of δ.

In terms of antisymmetric brackets, Theorem 64 characterises L-structures on LV in which for each n $n\in \N$, the n-ary bracket decomposes into linear maps nn\Asy n L L,  nn\Asy n1 LV V,  \Asy n L V. \begin{eqnarray*} \Asy^n L&\to& L,\nonumber\\ \Asy^{n-1}L\otimes V&\to& V,\nonumber\\ \quad \Asy^n L &\to& V.\nonumber \end{eqnarray*}

These then correspond to cocycles in Hom 1 (S(L[1]),V[1])  \Hom 2 (S(L[1]),V) $\Hom_1(\Sy(L[1]),V[1])\cong \Hom_2(\Sy(L[1]),V)$. So, it is the 2-cocycles that characterise these L-structures, as in the Lie algebra case (cf. [9], Proposition 7.5.18, p. 202). [ λ 2 , λ m ](xy) = ( λ 2 μ S ( λ m  \id S ) Δ S )(xy)+ (1) |x| λ m (x d 2 (y)) = λ 2 μ S (δ(x)  \id S ) Δ S (y)+ (1) |x| δ(x)( d 2 (y)) = [ λ 2 ,δ(x)](y), 1 2 [ λ m , λ m ](xy) = (1) | x (2) || y (1) | λ m ( λ m ( x (1) y (1) ) x (2) y (2) ) = (1) | x (2) |+| x (1) || x (2) | δ( x (2) )(δ( x (1) y (1) ) y (2) ) = 1 2 (1) x (1) δ( x (1) )(δ( x (2) y (1) ) y (2) ) + (1) | x (2) |+| x (1) || x (2) | δ( x (2) )(δ( x (1) y (1) ) y (2) ) = ( 1 2 \bracket(δδ) Δ S )(x)(y), \begin{eqnarray*} [\lambda_2, \lambda_m](x\vee y)&=&\big(\lambda_2 \circ \mu_S(\lambda_m\otimes \id_S)\Delta_S\big)(x\vee y) + (-1)^{|x|} \lambda_m (x\vee d_2(y))\nonumber\\ &=&\lambda_2\circ \mu_S(\delta(x)\otimes \id_S)\Delta_S(y) + (-1)^{|x|}\delta(x)(d_2(y))\nonumber\\ &=&[\lambda_2,\delta(x)](y),\nonumber\\ \frac{1}{2}[\lambda_m,\lambda_m](x\vee y)&=& \sum (-1)^{|x_{(2)}||y_{(1)}|} \lambda_m(\lambda_m (x_{(1)}\vee y_{(1)})\vee x_{(2)}\vee y_{(2)})\nonumber\\ &=& \sum (-1)^{|x_{(2)}|+|x_{(1)}||x_{(2)}|}\delta(x_{(2)})(\delta(x_{(1)}\vee y_{(1)})\vee y_{(2)})\nonumber\\ &=&\frac{1}{2}\sum (-1)^{x_{(1)}}\delta(x_{(1)})(\delta(x_{(2)}\vee y_{(1)})\vee y_{(2)})\nonumber\\ && +(-1)^{|x_{(2)}|+|x_{(1)}||x_{(2)}|}\delta(x_{(2)})(\delta(x_{(1)}\vee y_{(1)})\vee y_{(2)})\nonumber\\ &=&\left(\frac{1}{2}\bracket\circ (\delta\otimes \delta) \Delta_S\right)(x)(y),\nonumber \end{eqnarray*}

5.3 Extensions of L-algebras

We conclude with a brief discussion of extensions of L-algebras. This puts some constructions we discussed in context. The notions are completely analog to the Lie algebra case, see for example ([9], Sections 5.1.3 and 7.5.2).

A graded subspace IL of an L-algebra (L[1], λ) is called an ideal if λ(xy) ∈ I[1] for all xI[1] and yS(L[1]) $y\in \Sy(L[1])$. Then LI carries a canonical L-structure such that the projection LLI is a strict homomorphism of L-algebras. An ideal IL is always an L-subalgebra as in particular λ(x) ∈ I[1] for all x\rsym(I[1]) $x\in\rsym(I[1])$.

Definition 65. An extension of an L-algebra (L1[1], λ1) by another L-algebra (L2[1], λ2) is an exact sequence of L-algebras and strict homomorphisms 0 L 2 ι L p L 1 0. \begin{equation*}0\to L_2\xrightarrow{\iota} L \xrightarrow{p} L_1 \to 0. \end{equation*}(44)

Given such an exact sequence (44), the graded subspace L2 ≅ker(p) ⊂ L is an ideal and p induces a strict isomorphism LL2L1 of L-algebras.

We then always have LL1L2 (non-canonically) as graded vector spaces, so we are essentially concerned with L-structures on L1L2 such that the canonical maps L2L1L2 and L1L2L1 are strict L-algebra homomorphisms. With the decomposition (40), we can decompose such an L-structure λ: \rsym(( L 1 L 2 )[1])( L 1 L 2 )[1] $\lambda\colon \rsym((L_1\oplus L_2)[1])\to (L_1\oplus L_2)[1]$ into linear degree one maps λ 1 :  \rsym( L 1 [1]) L 1 [1],ω: \rsym( L 1 [1]) L 2 [1], 0 : \rsym( L 2 [1]) L 1 [1], λ 2 : \rsym( L 2 [1]) L 2 [1], 0 :  \rsym( L 1 [1]) \rsym( L 2 [1]) L 1 [1], λ m :  \rsym( L 1 [1]) \rsym( L 2 [1]) L 2 [1]. \begin{eqnarray*} \lambda_1&\colon& \rsym(L_1[1])\to L_1[1],\quad\omega\colon \rsym(L_1[1])\to L_2[1],\nonumber\\ 0&\colon&\rsym(L_2[1])\to L_1[1],\quad \lambda_2\colon \rsym(L_2[1])\to L_2[1],\nonumber\\ 0&\colon& \rsym(L_1[1])\otimes \rsym(L_2[1])\to L_1[1],\nonumber\\ \lambda_m&\colon& \rsym(L_1[1])\otimes \rsym(L_2[1])\to L_2[1].\nonumber \end{eqnarray*}

5.3.1 Abelian and central extensions

An L-algebra L is called abelian if only its 1-ary bracket is nontrivial.An abelian L-algebra is then nothing else than a DG vector space.

An L-algebra extension L2LL1 is called abelian if L2 is abelian. The L-structures constructed in Theorem 64 are examples of abelian extensions of L by V.

Similarly, an extension L2LL1 is called central if λ(xy) = 0 for xL2[1], y \rsym(L[1]) $y\in \rsym(L[1])$. It is immediate that this is the case if and only if L2 is abelian and λm = 0. For abelian L2 , the central extensions L2L1L2L1 are by Theorem 64 characterised by 2-cocycles of L1 with values in the trivial representation of L1 on L2.

5.3.2 Semidirect sums

An L-algebra ((L1L2)[1], λ) is said to be a semidirect sum of the L-algebras (L1[1], λ1) and (L2[1], λ2) if the canonical sequence L2L1L2L1 is an L-algebra extension and if the canonical map L1L1L2 is a strict homomorphism of L-algebras. This is clearly the case if and only if ω = 0 in the decomposition above. A semidirect sum of L1 and L2 is therefore characterised by λm. Note that L1L1L2 is an ideal if and only if λm = 0. In this case, L1L2 carries the L-structure λ1 + λ2 and is called the direct sum of L1 and L2.

For an arbitrary λ m  \Hom 1 (\rsym( L 1 [1]) \rsym( L 2 [1]), L 2 [1]) $\lambda_m\in \Hom_1(\rsym(L_1[1])\otimes \rsym(L_2[1]),L_2[1])$, the condition for λ1 + λ2 + λm to define an L-structure on L1L2 becomes [ λ 1 + λ 2 , λ m ]+ 1 2 [ λ m , λ m ]=0. \begin{equation*}[\lambda_1+\lambda_2,\lambda_m]+\frac{1}{2}[\lambda_m,\lambda_m]=0. \end{equation*}(45)

The isomorphism Hom(\rsym( L 1 [1]) \rsym( L 2 [1]), L 2 [1]) \Hom(\rsym( L 1 [1]),Hom(\rsym( L 2 [1]), L 2 [1])) $\Hom(\rsym(L_1[1])\otimes \rsym(L_2[1]),L_2[1])\cong \Hom(\rsym(L_1[1]),\Hom(\rsym(L_2[1]),L_2[1]))$ allows for the following characterisation of semidirect sums.

Theorem 66. Let λ m  \Hom( \rsym( L 1 [1]) \rsym( L 2 [1]), L 2 [1]) $\lambda_m\in \Hom( \rsym(L_1[1])\otimes \rsym(L_2[1]),L_2[1])$ be of degree one. Then λm satisfies (45) if and only if the corresponding linear degree one map δ: \rsym( L 1 [1]) \Hom(\rsym( L 2 [1]), L 2 [1]) $\delta\colon \rsym(L_1[1])\to \Hom(\rsym(L_2[1]),L_2[1])$ is a weak homomorphism of L-algebras in the sense that it satisfies (35).

Proof. Note that Hom( \rsym( L 1 [1]) \rsym( L 2 [1]), L 2 [1]) $\Hom( \rsym(L_1[1])\otimes \rsym(L_2[1]),L_2[1])$ is closed under [⋅, ⋅] and [λ1 + λ2, ⋅ ]. Therefore, (45) has only to be checked on \rsym( L 1 [1]) \rsym( L 2 [1]) $\rsym(L_1[1])\otimes \rsym(L_2[1])$. Let d1 and d2 denote the codifferentials on S( L 1 [1]) $\Sy(L_1[1])$ and S( L 2 [1]) $\Sy(L_2[1])$, respectively. For x\rsym( L 1 [1]) $x\in\rsym(L_1[1])$ and y\rsym( L 2 [1]) $y\in\rsym(L_2[1])$, we then compute

and [λ1, λm](xy) = λm(d1(x) ∨ y) = (δd1)(x)(y).

Example 67. The L-structure on LV induced by arepresentation of L on V is a semidirect sum. For compliance with Theorem 66, note that \gl( L 2 [1]) \Hom(\rsym( L 2 [1]), L 2 [1]) $\gl(L_2[1])\subset \Hom(\rsym(L_2[1]),L_2[1])$ is a Lie subalgebra.

References

  1. T. Lada, J. Stasheff, Introduction to SH Lie algebras for physicists, Int. J. Theor. Phys. 32, 1087–1104 (1993) [CrossRef] [Google Scholar]
  2. J. Stasheff, Differential graded Lie algebras, quasi-Hopf algebras and higher homotopy algebras, in: Quantum groups (Leningrad, 1990), Lecture Notes in Mathematics, Springer, Berlin, 1992, Vol. 1510, pp. 120–137 [CrossRef] [Google Scholar]
  3. M. Dehling, Shifted L bialgebras, Master’s thesis, Göttingen University, 2011. http://www.uni-math.gwdg.de/mdehling/publ/ma.pdf [Google Scholar]
  4. P. Michael, L-infinity algebras and their cohomology (Escholarship, University of California, 1995) [Google Scholar]
  5. J.C. Baez, A.S. Crans, Higher-dimensional algebra. VI. Lie 2-algebras, Theory Appl. Categ. 12, 492–538 (2004) [Google Scholar]
  6. J.-L. Loday, B. Vallette, Algebraic operads, in: Grundlehren der Mathematischen Wissenschaften [Fundamental Principles of Mathematical Sciences], Springer, Heidelberg, 2012, Vol. 346 [CrossRef] [Google Scholar]
  7. Marco Manetti. Lectures on deformations of complex manifolds (deformations from differential graded viewpoint). Rend. Mat. Appl., 24, 1–183 (2004). [Google Scholar]
  8. T. Lada, M. Markl, Strongly homotopy Lie algebras, Commun. Algebra 23, 2147–2161 (1995) [CrossRef] [Google Scholar]
  9. J. Hilgert, K.-H. Neeb, Structure and geometry of Lie groups, Springer Monographs in Mathematics, Springer, New York, 2012 [CrossRef] [Google Scholar]

Cite this article as: Ben Reinhold. L-algebras and their cohomology, Emergent Scientist 3, 4 (2019)

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