Diffgeometer1, If (M) is a closed oriented manifold, I've heard that the (k)-th homology groups of (M) with coefficients in (R) (denoted ( H_k(M;\mathbb{R}))) is generated by closed oriented submanifolds of (M). So a (k)-cycle is expressed[c=\sum_{i}a_iZ_i ]where (Z_i) is a closed oriented (k)-submanifold of (M) and (a_i\in \mathbb{R}). From here one has a nondegenerate pairing between de Rham cohomology and (H_k(M;\mathbb{R}))
[H^k_{dR}(M)\times H_k(M;\mathbb{R})\rightarrow \mathbb{R}] given by[\langle[\alpha],[c]\rangle:=\int_c \alpha = \sum_ia_i\int_{Z_i}\alpha.]This is the way physicists do it (for example in the string theory book by Schwartz and Becker). In math, we would define maps (\sigma:\Delta^k\rightarrow M) and then define boundary maps, chain complex, and ultimately the definition of the homology groups (in whatever coefficients (\mathbb{Z}, \mathbb{Q}, \mathbb{R}) ect). These two apporaches have to be equivalent although the physics one is nice and intuitive. Can anyone explain why they're equivalent or give a reference where for why homology classes of (H_k(M;\mathbb{R})) can be expressed as a linear combination of closed oriented (k)-dimensional submanifolds?
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