2013
DOI: 10.4310/hha.2013.v15.n1.a5
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Chevalley cohomology for aerial Kontsevich graphs

Abstract: Let T poly (R d ) denote the space of skew-symmetric polyvector fields on R d , turned into a graded Lie algebra by means of the Schouten bracket. Our aim is to explore the cohomology of this Lie algebra, with coefficients in the adjoint representation, arising from cochains defined by linear combination of aerial Kontsevich graphs. We prove that this cohomology is localized at the space of graphs without any isolated vertex, any "hand" or any "foot". As an application, we explicitly compute the cohomology of … Show more

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Cited by 1 publication
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“…Here the inclusion dGC → XGC appeared already in section 3. The last element S is defined as (1) is the unit element (see (1)) and U is the following series of graphs: (1). The operation U corresponds to the scaling operator, acting on multivector fields of degree (joint in x's and ξ's) k as multiplication by k. Let us prove the proposition above.…”
Section: Outmentioning
confidence: 99%
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“…Here the inclusion dGC → XGC appeared already in section 3. The last element S is defined as (1) is the unit element (see (1)) and U is the following series of graphs: (1). The operation U corresponds to the scaling operator, acting on multivector fields of degree (joint in x's and ξ's) k as multiplication by k. Let us prove the proposition above.…”
Section: Outmentioning
confidence: 99%
“…Formality, Deformation Quantization. 1 In the following it will be important that the elements of T poly are polynomials and not power series, as are often considered in physics. The power series version requires different methods, cf.…”
Section: Let Tmentioning
confidence: 99%
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