In this paper Tao explains that "The unsigned definite integral generalises to the Lebesgue integral, or more generally to integration on a measure space. Finally, the signed definite integral generalises to the integration of forms, which will be our focus here."
The phrase seems to point to these to kinds of integration being necessarily separate from each other, but is this the case?
On page $100$ of Spivak's Calculus on Manifolds the following definition is made:
If $\omega$ is a $k$-form on $\mathbb{R}^k$, then $\omega = f\ dx_1\land\ldots\land dx_k$ for a unique function $f:\mathbb{R}^k\to\mathbb{R}$. We define $$\int_{[0,1]^k}\omega := \int_{[0,1]^k}f.$$
Can't the right-side be a Lebesgue (as opposed to a Riemann) Integral, allowing us to say we are defining Lebesgue integration on $k$-forms? From what I gather which form of integration we choose (Riemann, Lebesgue, gauge, etc) plays a role in regards to which $k$-forms are integrable.