I started studying the book of Daniel Huybrechts, Complex Geometry An Introduction. I tried studying backwards as much as possible, but I have been stuck on the concepts of almost complex structures and complexification. I have studied several books and articles on the matter including ones by Keith Conrad, Jordan Bell, Gregory W. Moore, Steven Roman, Suetin, Kostrikin and Mainin, Gauthier
I have several questions on the concepts of almost complex structures and complexification. Here is one:
Question:
Let $L$ be $\mathbb C$-vector space, possibly infinite-dimensional. From Suetin, Kostrikin and Mainin (see 12.13 of Part I), Wikipedia and (implicitly) Daniel Huybrechts, Complex Geometry An Introduction (see Chapter 1.2), we get that $(L_{\mathbb R})^{\mathbb C}$ is $\mathbb C$-isomorphic to an external direct sum: $(L_{\mathbb R})^{\mathbb C} \cong L \ \text{external-}\bigoplus \ \overline L$ in a 'canonical' way.
How exactly does this 'canonical' $\mathbb C$-isomorphism make us think of $(L_{\mathbb R})^{\mathbb C}$ as more like $L \bigoplus \overline L$ than like $L \bigoplus L = L^2$ ? I think of something like 'unique' isomorphisms as asked about in this post. I might be confusing the terms 'canonical' and 'unique'. Also, this post might be relevant.
My understanding of this:
We have the literal (not just isomorphism) internal direct sum $$(L_{\mathbb R})^{\mathbb C} = (L_{\mathbb R}^2,J) = (L^{1,0},J^{1,0}) \ \text{internal-} \ \bigoplus (L^{0,1},J^{0,1})$$
where
$J$ is the almost complex structure on $L_{\mathbb R}^2$, $J(l,m):=(-m,l)$,
$J^{1,0}$ is $J$ with domain and range restricted to $L^{1,0}$ (we can check that $J(L^{1,0}) \subseteq L^{1,0}$) such that $J^{1,0}$ is an almost complex structure on $L^{1,0}$
and $J^{0,1}$ is $J$ with domain and range restricted to $L^{0,1}$ (we can check that $J(L^{0,1}) \subseteq L^{0,1}$) such that $J^{0,1}$ is an almost complex structure on $L^{0,1}$.
Then
Let $\hat i$ be the unique almost complex structure on $L_{\mathbb R}$ such that $L=(L_{\mathbb R}, \hat i)$. We have that $L$ and $(L^{1,0},J^{1,0})$ are $\mathbb C$-isomorphic by $\gamma_L(l)=(l,-\hat i(l))$.
$\overline L=(L_{\mathbb R}, -\hat i)$ and $(L^{0,1},J^{0,1})$ are $\mathbb C$-isomorphic by $\gamma_{\overline L}(l)=(l,\hat i(l))$
Finally, the isomorphism is $f = (\varphi \circ (\gamma_L \ \text{external-}\oplus \ \gamma_{\overline L}))^{-1}$, where $\varphi$ is the standard $\mathbb C$-isomorphism between internal and external direct sums: $\varphi: (L^{1,0},J^{1,0}) \ \text{external-} \ \bigoplus (L^{0,1},J^{0,1}) \to (L^{1,0},J^{1,0}) \ \text{internal-} \ \bigoplus (L^{0,1},J^{0,1})$.
Guess: Based on this post and this post (and 3 of my other posts: Post 1, Post 2, Post 3), I guess canonical/natural just means basis-free, i.e. we don't need axiom of choice, instead of saying that $(L_{\mathbb R})^{\mathbb C}$ is 'more like' $L \bigoplus \overline L$ than like $L \bigoplus L = L^2$ unless an isomorphism constructed without axiom of choice is 'more' of an isomorphism than one constructed with the axiom of choice. I don't really bother to think of 'unique' isomorphism anymore. I think only of 'canonical'/'natural' isomorphism as in basis-free i.e. no axiom of choice.
But, we do not necessarily need the axiom of choice to relate two infinite-dimensional vector spaces. For instance, my answer above works when everything is infinite-dimensional, but does not appeal to the axiom of choice (or something equivalent to it) anywhere.
– Joppy Mar 06 '20 at 05:12