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DefinitionDefinition: Literature-sourcedProof: Not applicablePipeline-generatedprecheck passjudge pass (gpt-6-sol)audited 2026-09-30
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The augmented two-sided bar complex

Definition

Let k be a field and A a unital associative k-algebra. Set A⊗k0:=k and, for every n≥0, set

Bar⁡n(A):=A⊗kA⊗kn⊗kA.

Write a pure tensor as a0⊗⋯⊗an+1. For n≥1 define

dn:=∑r=0n(−1)rμr,r+1:Bar⁡n(A)→Bar⁡n−1(A),

where μr,r+1 multiplies slots r and r+1 and leaves the other slots in order. The augmentation is

ε:=μ:Bar⁡0(A)=A⊗kA→A,a0⊗a1↦a0a1.

In degree one, d1(a0⊗a1⊗a2)=a0a1⊗a2−a0⊗a1a2.

The empty middle tensor convention makes Bar⁡0(A)=A⊗kA; there is no unaugmented differential out of degree zero.

Using Enveloping algebra and the bimodule–module dictionary, each term has the following left and right Ae-module structures, considered separately:

(c⊗dop)⋅(a0⊗⋯⊗an+1)=ca0⊗a1⊗⋯⊗an+1d,

(a0⊗⋯⊗an+1)⋅(c⊗dop)=da0⊗a1⊗⋯⊗an+1c.

Every adjacent-multiplication face is linear for each of these module structures: at the first and last faces this is associativity, and at internal faces the outer factors are unchanged. The augmentation is linear on both sides, since ε(ca0⊗a1d)=c(a0a1)d and ε(da0⊗a1c)=d(a0a1)c. This item specifies the bar terms, maps, and outer actions; the asserted zero-composite identities are addressed by the following bar-boundary lemma.

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Sources