I want to show that
If $M$ is a free $R$-module of rank $n$, for a unital, commutative ring $R$, then the $i^{\operatorname{th}}$ exterior power, $$\bigwedge^{i}(M)$$ is free of dimension $\binom{n}{i}$.
My reasoning:
We have $$M \cong \bigoplus_{k = 1}^{n} R.$$
We also have that $$\bigwedge^i(M) := \mathcal{T}^i(M)/\mathcal{A}^i(M)$$ where $$\mathcal{T}^i(M) = M^{\otimes i}$$ and $$\mathcal{A}^i(M) := \langle m_1 \otimes \cdots \otimes m_\ell \otimes\cdots \otimes \cdots \otimes m_j \otimes \cdots \otimes m_i \;|\; m_p \in M, \ell \neq j \ \text{so that}\ m_\ell = m_j \ \text{for some} \ \ell,j\rangle.$$
Now we take not of the fact that we have a surjective $R$-module homomorphism, that is the projection onto the quotient, i.e. $$f:\mathcal{T}^i(M) = M^{\otimes i} \twoheadrightarrow \mathcal{T}^i(M)/\mathcal{A}^i(M) = \bigwedge^i(M)$$ defined explicitly by $$m_1 \otimes \cdots \otimes m_i \longmapsto m_1 \wedge \cdots \wedge m_i.$$
Now, assume that we have a basis $$\mathcal{B} := \{m'_1,\ldots,m'_n\} \subset M.$$
Then every simple tensor $$m_1 \otimes \cdots \otimes m_i$$ can be written as $$\sum_{k_1 = 1}^{n}r_{k_1} m'_{k_1} \otimes \cdots \otimes \sum_{k_i = 1}^{n} r_{k_i}m'_{k_i}.$$ Now, we can use the multi-additivity of $i$-tensors to find that under $f$, we will see that only the tensors where $k_1 \neq \cdots \neq k_i$ is true, will be sent to a non-zero element.
We thus get that $$f(m_1 \otimes \cdots \otimes m_i)$$$$ = f\Big(\sum_{k_1 = 1}^{n} r_{k_1}m'_{k_1} \otimes \cdots \otimes \sum_{k_i = 1}^{n} r_{k_i} m'_{k_i} \Big) = \sum_{\sigma \in S_i} \operatorname{sgn}(\sigma)(r_{\sigma(k_1)} \cdots r_{\sigma(k_i)})m'_1 \wedge \cdots \wedge m'_i.$$
Now since every element in $M^{\otimes i}$ can be written as a finite sum $$\sum_{\gamma = 1}^{N} m^{\gamma}_1 \otimes \cdots \otimes m^{\gamma}_i$$ who:s image will be $$\sum_{\gamma = 1}^{N}\Bigg(\sum_{\sigma \in S_i}\operatorname{sgn}(\sigma)(r_{\sigma(k^{\gamma}_1)} \cdots r_{\sigma(k^{\gamma}_i)})m^{\gamma '}_1 \wedge \cdots \wedge m^{\gamma '}_i\Bigg)$$ and we have a surjection, we can conclude that every element in $$\bigwedge^i(M)$$ is on (this not so nice) form.
Now, we notice that if $n > i$, then we can choose $\binom{n}{i}$ basis elements for $$\bigwedge^i(M).$$
To conclude, we have that $$\{m'_{k_1} \wedge \cdots \wedge m'_{k_i}\;|\; 1 \leq k_1 < \ldots < k_i \leq n\}$$ for $$k_j \in \{1,\ldots,n\}$$ generates $$\bigwedge^i(M).$$
I have not shown linear independence here, though. Is this idea correct? If not, what is wrong?
If it is correct, is there some nicer (notationally or conceptual) way to show this?
Edit: Thank you Qiachu Yuan. Yes, I realized that $1.$ might work, as you said. I think I encountered a similar exercise in differential geometry.
Am my interpretation correct, that what you mean by $1.$ above is the following:
If $$\{m'_1,\ldots,m'_n\}$$ is a basis for $M$, then it follows that $$\{m^{* '}_{1},\ldots,m^{* '}_{i}\}$$ is a basis for $M^{*}$. Then, assume we have an element $$\omega \in \bigwedge^i(M)$$ such that $$\omega = \sum_{J} r_J m^{J '}$$ for $$m^{J'} = m^{'}_{j_1} \wedge \cdots \wedge m^{'}_{j_i}$$ and $J$ is the set of all increasing indices $(j_1,\ldots,j_i)$ such that $$1 \leq j_1 < \cdots j_i \leq n.$$
Now, if $$\omega = 0$$ we will find that $$\omega(m^{*'}_{j_1},\ldots,m^{*'}_{j_i}) = r_{J'} = 0$$ for that particular choice of $$(j_1,\ldots,j_i)$$ Feeding $\omega$ with all possible choices of $m^{*'}_{j_1},\ldots,m^{*'}_{j_i}$ shows us that all coefficients $$r_{J} \equiv 0.$$
Comment: here we define $m^{*’}_j$ as the element that gives back $1$ when given $m^{’}_j$ and zero otherwise.
Showing linear independence is the hard part and it's not so easy (note that it implies that the determinant exists which is not so trivial). I can think of three approaches off the top of my head, I'm not sure which is standard or if I'm missing an easier one:
You can write down a nondegenerate bilinear pairing $\Lambda^k(M) \times \Lambda^k(M^{\ast}) \to R$ where $M^{\ast} = \text{Hom}_R(M, R)$ is the $R$-linear dual. This will let you show linear independence by acting via wedges of the dual basis in $M^{\ast}$.
You can argue that the exterior algebra takes direct sums to tensor products in the sense that $\Lambda^{\bullet}(M \oplus N) \cong \Lambda^{\bullet}(M) \otimes \Lambda^{\bullet}(N)$. Abstractly this follows from the fact that $\Lambda^{\bullet}(-)$ is the free graded-commutative algebra (the tensor product here has to be understood in the graded sense, with Koszul signs). Then we reduce to the fact that tensor products and direct sums of free modules are free.
You can also (I learned this recently) prove linear independence using noncommutative Grobner basis techniques.