\(\mathbf{1}\) has one point...
Solution.
The lack of a question means we’re proving the given statement, so let’s peice together what we’ve been given.
Our point is defined as a \(\mathcal{C}\)-map \(\mathbf{1} \rightarrow X\text{,}\) where \(\mathbf{1}\) is a terminal object in \(\mathcal{C}\text{.}\) By the definition of terminal object, there exists exactly one \(\mathcal{C}\)-map \(X \rightarrow \mathbf{1}\) for each object of \(X\text{.}\) To help keep these ideas separate, let’s call the point \(\mathbf{1} \xrightarrow{x} X\) and the "terminal map" \(X \xrightarrow{\bar{x}} \mathbf{1}\text{.}\)
If we have some arbitrary map \(X \xrightarrow{f} Y\text{,}\) then we should be able to compose this map with our "point map". Namely, if we have a map \(\mathbf{1} \xrightarrow{x} X\) in our category \(\mathcal{C}\) then our composition \(f \circ x\) should also be in the category. This effectively gives us a map \(\mathbf{1} \xrightarrow{f x} Y\) since we have \(\mathbf{1} \xrightarrow{x} X \xrightarrow{f} Y\text{.}\)
So how do we prove \(f x\) is a point? I think we basically already have done so by establishing the existance of a map \(\mathbf{1} \xrightarrow{f x} Y\) through composition. We might have to also prove that there’s a corresponding map \(Y \xrightarrow{\bar{f x}} \mathbf{1}\) too, which I think we can effectively do by following the arrows backwards since each of these single element sets are isomorphic to every other one by the "Uniqueness of Terminal Objects" theorem.
I think we’re effectively splitting the domain up into points. If we have a map \(X \xrightarrow{f} Y\text{,}\) this terminal object lets us break apart \(X\) into a bunch of individual points \(\mathbf{1} \xrightarrow{x_i} X\text{,}\) and consequently allows us to break up \(f\) into smaller maps where the domain and codomain are both single element sets. For any map \(f: X \rightarrow Y\text{,}\) each point \(x_i\) in \(X\) could be used to construct a map \(f_i: \{x_i\} \rightarrow \{f x_i\}\text{.}\) Each such "mini-map" must be invertable, so there’s precisely one map from \(\{f x_i\}\) to \(\mathbf{1}\) and it’s given by the composition \(\bar{x_i} f_i^{-1}\text{.}\)