A little fact is confusing me concerning Differential forms. Besides all kinds of motivation, a differential $p-$form is just the following tensor:
$$\textbf{F} = F_{\mu_{1}...\mu_{p}}(x^{\nu})\textbf{dx} ^{\mu_{1}}\wedge...\wedge \textbf{dx}^{\mu_{p}}\tag{1}$$
Well, it is clear that $F_{\mu_{1}...\mu_{p}}(x^{\nu})$ are components of a covariant tensor field.
On the other hand, a volume integral can be calculated, formally as:
$$ \int_{V}\rho(x^{\nu})\textbf{dx} ^{\alpha}\wedge \textbf{dx}^{\beta} \wedge \textbf{dx}^{\gamma} =: \int_{V}\omega \tag{2}$$
The thing is, since we integrating a $3-$form I would expect a $(0,3)$-tensor field components, instead we have an scalar field $\rho(x^{\nu})$. I mean, I would expect something like:
$$ \int_{V}\rho_{\alpha \beta \gamma}(x^{\nu})\textbf{dx} ^{\alpha}\wedge \textbf{dx}^{\beta} \wedge \textbf{dx}^{\gamma} =: \int_{V}\omega \tag{3}$$
So, my doubt is: what suppose to mean then the object $\omega$ in $(2)$?
3-forms in $\mathbb{R}^3$ form a one-dimensional space. Any three-form has the structure $\rho(x)dx_1\wedge dx_2\wedge dx_3$.