词条 | Homological integration |
释义 |
In the mathematical fields of differential geometry and geometric measure theory, homological integration or geometric integration is a method for extending the notion of the integral to manifolds. Rather than functions or differential forms, the integral is defined over currents on a manifold. The theory is "homological" because currents themselves are defined by duality with differential forms. To wit, the space {{math|Dk}} of {{mvar|k}}-currents on a manifold {{mvar|M}} is defined as the dual space, in the sense of distributions, of the space of {{mvar|k}}-forms {{math|Ωk}} on {{mvar|M}}. Thus there is a pairing between {{mvar|k}}-currents {{mvar|T}} and {{mvar|k}}-forms {{mvar|α}}, denoted here by Under this duality pairing, the exterior derivative goes over to a boundary operator defined by for all {{math|α ∈ Ωk}}. This is a homological rather than cohomological construction. References
|last = Federer |first = Herbert |authorlink = Herbert Federer |title = Geometric measure theory |publisher = Springer-Verlag New York Inc. |location = New York |year = 1969 |pages = xiv+676 |isbn = 978-3-540-60656-7 |series = Die Grundlehren der mathematischen Wissenschaften |volume = 153 |mr=0257325 |zbl=0176.00801}}.
|first=H. |last=Whitney |author-link=Hassler Whitney |title=Geometric Integration Theory |series=Princeton Mathematical Series |volume=21 |publisher=Princeton University Press and Oxford University Press |place=Princeton, NJ and London |year=1957 |pages= XV+387 |mr=0087148 |zbl=0083.28204 }}. {{geometry-stub}} 2 : Definitions of mathematical integration|Measure theory |
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