“…The reason is very clear, Poisson structures are defined by contravariant two-vectors instead of twoforms. So, Vaisman 3 characterized the existence of prequantization bundles of a Poisson manifold M by means of a natural cohomology of multivectors defined by Lichnerowicz, 9 and termed Lichnerowicz-Poisson cohomology of M . This cohomology can be obtained as the cohomology of a subcomplex of the Chevalley-Eilenberg complex associated to the Lie algebra of functions C ϱ (M ,R).…”
Section: Introductionmentioning
confidence: 99%
“…Theorem II.2: Let (M, ⌳, E) be a Jacobi manifold and ͕,͖ the bracket on ⍀ 1 (M )ϫC ϱ (M ,R) defined by (12). Then, the triple (T*M ϫR,͕,͖,(#,E)) is a Lie algebroid over M, where…”
The geometric quantization of Jacobi manifolds is discussed. A natural cohomology ͑termed Lichnerowicz-Jacobi͒ on a Jacobi manifold is introduced, and using it the existence of prequantization bundles is characterized. To do this, a notion of contravariant derivatives is used, in such a way that the procedure developed by Vaisman for Poisson manifolds is naturally extended. A notion of polarization is discussed and the quantization problem is studied. The existence of prequantization representations is also considered.
“…The reason is very clear, Poisson structures are defined by contravariant two-vectors instead of twoforms. So, Vaisman 3 characterized the existence of prequantization bundles of a Poisson manifold M by means of a natural cohomology of multivectors defined by Lichnerowicz, 9 and termed Lichnerowicz-Poisson cohomology of M . This cohomology can be obtained as the cohomology of a subcomplex of the Chevalley-Eilenberg complex associated to the Lie algebra of functions C ϱ (M ,R).…”
Section: Introductionmentioning
confidence: 99%
“…Theorem II.2: Let (M, ⌳, E) be a Jacobi manifold and ͕,͖ the bracket on ⍀ 1 (M )ϫC ϱ (M ,R) defined by (12). Then, the triple (T*M ϫR,͕,͖,(#,E)) is a Lie algebroid over M, where…”
The geometric quantization of Jacobi manifolds is discussed. A natural cohomology ͑termed Lichnerowicz-Jacobi͒ on a Jacobi manifold is introduced, and using it the existence of prequantization bundles is characterized. To do this, a notion of contravariant derivatives is used, in such a way that the procedure developed by Vaisman for Poisson manifolds is naturally extended. A notion of polarization is discussed and the quantization problem is studied. The existence of prequantization representations is also considered.
“…, for X ∈ ΓA, and π : A * → A is defined by π α = ι α π, and set [88]. The Poisson homology H • (A, ∂ π ) of (A, π) is that of the complex (Γ(∧ • A * ), ∂ π ) which has been studied by Huebschmann [55], and which generalizes the Poisson homology of Poisson manifolds [80,12].…”
Section: Lie Algebroids With a Poisson Structurementioning
confidence: 99%
“…Since their introduction by Lichnerowicz in 1977 [88], Poisson geometry and the cohomology of Poisson manifolds have developed into a wide field of research. Lie algebroids are vector bundles with a Lie bracket on their space of sections (see [93,94,16] and Section 1.2).…”
Abstract. After a brief summary of the main properties of Poisson manifolds and Lie algebroids in general, we survey recent work on the modular classes of Poisson and twisted Poisson manifolds, of Lie algebroids with a Poisson or twisted Poisson structure, and of Poisson-Nijenhuis manifolds. A review of the spinor approach to the modular class concludes the paper.
“…a bivector with vanishing Schouten bracket, see [6]). This operator induces the Poisson bracket {F, G} Π = dF, ΠdG on the algebra of smooth functions on M, where ·, · is the dual map between T * M and T M. A smooth real-valued function F on M is called Z-invariant if the Lie derivative L Z F = 0 for any vector field Z ⊂ Z.…”
Section: Geometric Reduction Of Poisson Bivectorsmentioning
Given a foliation S of a manifold M, a distribution Z in M transveral to S and a Poisson bivector Π on M we present a geometric method of reducing this operator on the foliation S along the distribution Z. It encompasses the classical ideas of Dirac (Dirac reduction) and more modern theory of J. Marsden and T. Ratiu, but our method leads to formulas that allow for an explicit calculation of the reduced Poisson bracket. Moreover, we analyse the reduction of Hamiltonian systems corresponding to the bivector Π.
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