2001
DOI: 10.7146/math.scand.a-14337
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Transferring algebra structures up to homology equivalence

Abstract: Given a strong deformation retract M of an algebra A, there are several apparently distinct ways ([9]

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Cited by 21 publications
(29 citation statements)
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“…In our setting, µ 0 is the (background) curvature, and we now indicate briefly how such a curved A ∞ -algebra structure arises. Following [29,30,36], we first work on the level of the chain bundles and define λ m inductively, for m 2, by…”
Section: Curved a ∞ -Algebrasmentioning
confidence: 99%
“…In our setting, µ 0 is the (background) curvature, and we now indicate briefly how such a curved A ∞ -algebra structure arises. Following [29,30,36], we first work on the level of the chain bundles and define λ m inductively, for m 2, by…”
Section: Curved a ∞ -Algebrasmentioning
confidence: 99%
“…Recall (see, for example, [14] The nature and rôle of these side conditions is explained in the following proposition, proved in [26]. The difference between ordinary homotopy diagrams and strongly homotopy ones is measured by the homology of the nerve of the category S. From this point of view, diagram (18) related to moves (M1) and (M3) was very complicated.…”
Section: Structure Of Strongly Homotopy Diagramsmentioning
confidence: 99%
“…Our main references will be [Gug72, LS87, GLS91], papers which contain the results needed for the present application. There are other ways to solve this question, see [Kel01] and [JL01] for instance, however perturbation lemma and its application nicknamed tensor trick have a key advantage for us: they provide explicit formulas for which we can checked that the new higher intersection products still satisfy basic properties such as the projection formula.…”
Section: Perturbation Theory and Intersection Theory For Cycle Complexesmentioning
confidence: 99%