Math 2.0

Nonassociative rings and algebras Definition

L-infinity algebra

Builds on FieldVector spaceSymmetric groupDifferential graded Lie algebra

Definition

Let FF be a field of characteristic 00. Let L=⨁i∈ℤLiL = \bigoplus_{i \in \Z} L^i be a ℤ\Z-graded vector space over FF, and write ∣x∣=i\abs{x} = i for x∈Lix \in L^i. For homogeneous x1,…,xnx_1, \ldots, x_n and a permutation σ\sigma in the symmetric group SnS_n, let χ(σ)=χ(σ;x1,…,xn)\chi(\sigma) = \chi(\sigma; x_1, \ldots, x_n) be the sign defined by two rules. The sign of a transposition of neighbours xk,xk+1x_k, x_{k+1} is −(−1)∣xk∣∣xk+1∣-(-1)^{\abs{x_k}\abs{x_{k+1}}}, and χ\chi is multiplicative along products of such transpositions. An (i,n−i)(i, n - i)-unshuffle is a permutation σ∈Sn\sigma \in S_n with σ(1)<⋯<σ(i)\sigma(1) < \cdots < \sigma(i) and σ(i+1)<⋯<σ(n)\sigma(i + 1) < \cdots < \sigma(n).

An L∞L_\infty-algebra structure on LL is a family of multilinear maps lk ⁣:L⊗k→Ll_k \colon L^{\otimes k} \to L, for k≥1k \ge 1, such that:

  1. lkl_k has degree 2−k2 - k, that is, it maps Li1⊗⋯⊗LikL^{i_1} \otimes \cdots \otimes L^{i_k} into Li1+⋯+ik+2−kL^{i_1 + \cdots + i_k + 2 - k};
  2. lk(xσ(1),…,xσ(k))=χ(σ) lk(x1,…,xk)l_k(x_{\sigma(1)}, \ldots, x_{\sigma(k)}) = \chi(\sigma)\, l_k(x_1, \ldots, x_k) for all homogeneous xjx_j and all σ∈Sk\sigma \in S_k;
  3. for each n≥1n \ge 1 and all homogeneous x1,…,xnx_1, \ldots, x_n, ∑i+j=n+1∑σχ(σ)(−1)i(j−1) lj(li(xσ(1),…,xσ(i)),xσ(i+1),…,xσ(n))=0,\sum_{i + j = n + 1} \sum_{\sigma} \chi(\sigma) (-1)^{i(j - 1)}\, l_j\big(l_i(x_{\sigma(1)}, \ldots, x_{\sigma(i)}), x_{\sigma(i + 1)}, \ldots, x_{\sigma(n)}\big) = 0, where i,j≥1i, j \ge 1 and σ\sigma runs over the (i,n−i)(i, n - i)-unshuffles.

Remarks

For n=1n = 1, clause 3 says l1∘l1=0l_1 \circ l_1 = 0, so (L,l1)(L, l_1) is a cochain complex. For n=2n = 2, it says l1l2(x1,x2)=l2(l1x1,x2)+(−1)∣x1∣l2(x1,l1x2)l_1 l_2(x_1, x_2) = l_2(l_1 x_1, x_2) + (-1)^{\abs{x_1}} l_2(x_1, l_1 x_2), so l1l_1 is a derivation of l2l_2. For n=3n = 3, it says that the graded Jacobi identity for l2l_2 holds up to terms built from l1l_1 and l3l_3.

Example: a differential graded Lie algebra (L,[⋅,⋅],d)(L, [\cdot, \cdot], d) gives an L∞L_\infty-algebra with l1=dl_1 = d, l2=[⋅,⋅]l_2 = [\cdot, \cdot] and lk=0l_k = 0 for k≥3k \ge 3. Clause 2 for k=2k = 2 is graded antisymmetry, and clause 3 for n=3n = 3 becomes the graded Jacobi identity.

Non-example: a Lie algebra 𝔤\mathfrak{g} in degree 00 with l2l_2 its bracket and l1=id⁡l_1 = \id fails clause 1, since l1l_1 must raise the degree by one.

Sign conventions vary between authors; some use a lower grading in which lkl_k has degree k−2k - 2.

Reading path

To understand this page from the ground up, read these 5 pages in order. The foundations come first.

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  1. Differential graded Lie algebra concept
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  3. Symmetric group concept
  4. Vector space concept
  5. L-infinity algebra definition

Further reading

  1. Web https://en.wikipedia.org/wiki/Homotopy_Lie_algebra
About this page
TagNHDWBESKG3
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Kinddefinition
WritingW0 stub
MSC17B55, 18M70, 55P62
DefinesL-infinity algebra
UsesField, Vector space, Symmetric group, Differential graded Lie algebra
Changed3 November 2026

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