# Where does that dimension equality come from?

I'm reading chapter 3 of Duistermaat's Fourier integral operators. I came across this proof in the process:

$\textbf{Proposition 3.4.1.}$ Let $(E,\sigma)$ be a symplectic vector space. A linear subspace $L$ of $E$ is Lagrangian in $(E,\sigma)$ if and only if $L=L^\sigma$. The dimension of $E$ is even, say $=2n$. An isotropic linear subspace $L$ of $E$ is Lagrangian if and only if $\dim L=n$.

$\textbf{Proof.}$ If $L\varsubsetneqq L^\sigma$ then we can choose $e\in L^\sigma$, $e\notin L$. It follows that $\sigma(\ell _1 +\alpha _1 e, \ell _ 2 +\alpha_2e)=0$ for all $\ell_1,\ell_2\in L$, $\alpha_1,\alpha_2\in k$. So $L+k\cdot e$ is isotropic, $L\varsubsetneqq L+k\cdot e$. This proves the first assertion. Now let $L$ be Lagrangian (the existence of such $L$ is trivial). Then $\dim L=\dim L^\sigma=\dim E-\dim L$, hence $\dim E=2\cdot \dim L$. Conversely $L\subset L^\sigma$, $\dim E=2\cdot\dim L$ implies that $L\subset L^\sigma$, $\dim L=\dim L^\sigma$, hence $L=L^\sigma$. $\tag* {$\square$}$

The only thing I do not understand here is why $\dim L^\sigma=\dim E-\dim L$. How do you prove that? I tried proving $L\oplus L^\sigma$, but of course this isn't true since $L=L^\sigma\neq E$. So where is that equality from?

• If $\beta$ is a non-degenerate bilinear form on a finite-dimensional vector space $E$, then $\dim \{ x : (\forall v\in L)(\beta(x,v) = 0)\} = \dim E - \dim L$ for all subspaces $L\subset E$. A symplectic form is non-degenerate. – Daniel Fischer Aug 10 '15 at 17:07
• And how do I show that? – MickG Aug 10 '15 at 17:13
• Consider the map $\psi \colon E \to E^\ast$ given by $\psi(x) \colon \bigl(y \mapsto \beta(x,y)\bigr)$. What does non-degeneracy say about $\psi$? What relation has $\{ x : (\forall v\in L)(\beta(x,v) = 0)\}$ to $L$ in terms of $\psi$? – Daniel Fischer Aug 10 '15 at 17:18
• It says that its images $\psi(x)$ are nonzero. This means $\ker\psi(x)\neq E$. $\psi(x):E\to\mathbb{R}$ (or whatever field $E$ is built upon), so being nonzero means it is surjective and $\dim\ker\psi(z)=\dim E-1$. In particular, this means that the orthocomplement of a 1D subspace (i.e., if I take the span of a vector $v$, the set $\{x\in E:\beta(x,v)=0\}$) has dimension $n-1$, proving my equality for the case where the subspace is one-dimensional. Then again, saying $\psi(x)$ is nonzero for $x\neq0$ means $\psi$ is an isomorphism, so it preserves the subspace's dimension. Let me think more. – MickG Aug 10 '15 at 17:31
• If $E$ is the space, and $L$ is a subspace, this means $\dim L=\dim\psi(L)$. $\{x:v\in L\implies\beta(x,v)=0\}=\{x:v\in L\implies v\in\ker\psi(x)\}=\{x:L\subseteq\ker\psi(x)\}$. How does that help me? – MickG Aug 10 '15 at 17:41

Daniel Fischer directed me with a few hints to the solution. This happened in comments to the question. I'm posting this to highlight the solution and make it acceptable, so as to get the question off the unanswered.

The first comment said this equality holds for any non-degenerate form, whether it be symmetric, alternating, or neither.

Consider the map $\psi:E\to E^\ast$ given by $\psi(x):(y\mapsto\beta(x,y))$. What does non-degeneracy say about $\psi$? What relation has $\{x:(\forall v\in L)(\beta(x,v)=0)\}$ to $L$ in terms of $\psi$?

The non-degeneracy of $\beta$ implies that if $x\neq0$, $\psi(x)\neq0$, so it is injective, since it is linear, and therefore it is an isomorphism $E\to E^\ast$. As for the set:

$$\{x:v\in L\implies\beta(x,v)=0\}=\{x:v\in L\implies v\in\ker\psi(x)\}=\{x:L\subseteq\ker\psi(x)\}.$$

But that got me stuck again. And Daniel commented:

Do you remember what an annihilator is?

Sort of. I remembered the name, but from another setting. I never used annihilators in linear algebra, only those of rings in abstract algebra. Anyway that set is:

$$\{x:\psi(x)\in L^0\},$$

$L^0$ denoting the annihilator of $L$. Wikipedia came in here with:

If $W$ is a subspace of $V$ then the quotient space $V/W$ is a vector space in its own right, and so has a dual. By the first isomorphism theorem, a functional $f : V \to F$ factors through $V/W$ if and only if $W$ is in the kernel of $f$. There is thus an isomorphism

$$(V/W)^\ast \cong W^0.$$

As a particular consequence, if $V$ is a direct sum of two subspaces $A$ and $B$, then $V^\ast$ is a direct sum of $A^0$ and $B^0$.

Assuming the isomorphism exists, we obtain that $\dim(V/L)^\ast=\dim L^0$, but $V/L$ is canonically isomorphic to its dual as any finite-dimensional vector space, and so:

$$\dim L^0=\dim(V/L)^\ast=\dim V/L=\dim V-\dim L,$$

which is precisely the desired equality.

We are left with the isomorphism to prove. Suppose $f\in L^0$. Since $L\subseteq\ker f$, the map $\phi(f)\in(V/L)^\ast$ defined by $\phi(f)(v+L)=f(v)$ is well-defined and linear, so $\phi:L^0\to(V/L)^\ast$. Linearity is straightforward from the definition, so if $\ker\phi=\{0\}$ and the dimensions are equal (or $\phi$ is surjective) we are done. That the kernel is trivial is easy. Suppose $\phi(f)(v+L)=0$ for all $v+L$. This means $f(v)=0$ for all $v$, so $f=0$. Thus, the kernel is trivial. We can construct the inverse of $\phi$ explicitly. Let $\chi$ be the map that, given $f\in(V/L)^\ast$, maps it to $\chi(f)$ defined by $\chi(f)(v)=f(v+L)$. This new map is well-defined, and linear, so $\chi:(V/L)^\ast\to L^0$. Indeed, because by definition the maps produced by $\chi$ map all $L$ into zero, since $\chi(f)(v)=f(v+L)$, and if $v\in L$, $v+L=0+L$. This is clearly the inverse of $\phi$, as can be checked by trivial computations. So $\phi$ is indeed an isomorphism, and our proof is over.

Note: If you read the comments, you will see I forgot the surjectiveness, or rather implicitly assumed it. It was forgetfulness, and the surjectiveness needed consideration.