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Current (mathematics) : ウィキペディア英語版
Current (mathematics)
In mathematics, more particularly in functional analysis, differential topology, and geometric measure theory, a k-current in the sense of Georges de Rham is a functional on the space of compactly supported differential k-forms, on a smooth manifold ''M''. Formally currents behave like Schwartz distributions on a space of differential forms. In a geometric setting, they can represent integration over a submanifold, generalizing the Dirac delta function, or more generally even directional derivatives of delta functions (multipoles) spread out along subsets of ''M''.
==Definition==
Let \Omega_c^m(M) denote the space of smooth ''m''-forms with compact support on a smooth manifold M. A current is a linear functional on \Omega_c^m(M) which is continuous in the sense of distributions. Thus a linear functional
:T\colon \Omega_c^m(M)\to \mathbb
is an ''m''-current if it is continuous in the following sense: If a sequence \omega_k of smooth forms, all supported in the same compact set, is such that all derivatives of all their coefficients tend uniformly to 0 when k tends to infinity, then T(\omega_k) tends to 0.
The space \mathcal D_m(M) of ''m''-dimensional currents on M is a real vector space with operations defined by
:(T+S)(\omega):= T(\omega)+S(\omega),\qquad (\lambda T)(\omega):=\lambda T(\omega).
Much of the theory of distributions carries over to currents with minimal adjustments. For example, one may define the support of a current T \in \mathcal_m(M) as the complement of the biggest open set U \subset M such that
:T(\omega) = 0 whenever \omega \in \Omega_c^m(U)
The linear subspace of \mathcal D_m(M) consisting of currents with support (in the sense above) that is a compact subset of M is denoted \mathcal E_m(M).

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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