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Feb 24, 2020 at 21:13 comment added rozu Yes indeed, I meant locally rectifiable.
Feb 24, 2020 at 19:48 history edited Weekkola CC BY-SA 4.0
Clarified where I have my definition from
Feb 24, 2020 at 19:46 comment added Weekkola @rozu Thanks for your comment! However, I think you meant locally rectifiable currents, right? After all, I didn't say anything about the boundary. And yes, the mass (and its (un-)boundedness in case the current has non-compact support) can obviously change when the metric changes. Finally, thanks for pointing me at the bi-Lipschitz property – I'll look into that!
Feb 23, 2020 at 15:24 comment added rozu The way you define it, your class corresponds to the class of "locally integral currents" in Federer's book (see Section 4.1.24 for the definition in Euclidean space). This class is not affected by the change of a metric on a Riemmanian manifold because as metric spaces they are locally bi-Lipschitz equivalent (one can take the identity map). The class of integral currents (assuming they are allowed to have noncompact support) changes in general because a current may have finite mass with respect to one metric but not with respect to another.
S Feb 23, 2020 at 14:50 history edited Weekkola CC BY-SA 4.0
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Feb 18, 2020 at 15:35 history edited Weekkola CC BY-SA 4.0
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