Can You Solve This Symplectic Vector Space Problem?

  • Thread starter Thread starter Chris L T521
  • Start date Start date
Click For Summary
SUMMARY

This discussion focuses on the properties of symplectic vector spaces, specifically addressing the existence of a Lagrangian complement for a given Lagrangian subspace $\mathbb{U}$ within an $m$-dimensional vector space $\mathbb{V}$. It establishes that if $\mathbb{V}=\mathbb{U}\oplus\mathbb{W}$ is a Lagrangian splitting, then there exists a unique basis $y_1,\ldots,y_n$ for the Lagrangian complement $\mathbb{W}$ such that the combined basis $x_1,\ldots,x_n,y_1,\ldots,y_n$ forms a symplectic basis for $\mathbb{V}$. The discussion emphasizes the role of the non-degenerate alternating bilinear form $\omega$ in defining these structures.

PREREQUISITES
  • Understanding of symplectic vector spaces and their properties
  • Familiarity with bilinear forms, particularly non-degenerate alternating forms
  • Knowledge of basis concepts in linear algebra, including Lagrangian subspaces
  • Proficiency in matrix representation of linear transformations, specifically the matrix $J$
NEXT STEPS
  • Study the properties of non-degenerate alternating bilinear forms in depth
  • Learn about the construction and significance of symplectic bases in vector spaces
  • Explore Lagrangian subspaces and their applications in symplectic geometry
  • Investigate the implications of Lagrangian splittings in higher-dimensional vector spaces
USEFUL FOR

Mathematicians, physicists, and students studying symplectic geometry, linear algebra, or related fields who seek to deepen their understanding of vector space structures and their applications.

Chris L T521
Gold Member
MHB
Messages
913
Reaction score
0
Here's this week's problem.

-----

Background Info: Let $\mathbb{V}$ be an $m$-dimensional vector space over the field $\mathbb{F}$ (where $\mathbb{F}$ can be either $\mathbb{R}$ or $\mathbb{C}$). If $\omega$ is a non-degenerate alternating bilinear form, then the pairing $(\mathbb{V},\omega)$ is called a symplectic vector space. A symplectic basis for $\mathbb{V}$ is a basis $v_1,\ldots,v_{2n}$ such that $\omega(v_i,v_j)=J_{i,j}$, which is the $(i,j)$-th entry of the $2n\times 2n$ matrix
\[J=\begin{pmatrix} \mathbf{0}_n & I_n\\ -I_n & \mathbf{0}_n\end{pmatrix}.\]A Lagrangian space $\mathbb{U}$ is a subspace of $\mathbb{V}$ of dimension $n$ such that $\omega$ is zero on $\mathbb{U}$; i.e. $\omega(u,w)=0$ for all $u,w\in\mathbb{U}$. A direct sum decomposition $\mathbb{V}=\mathbb{U}\oplus\mathbb{W}$ where $\mathbb{U}$ and $\mathbb{W}$ are Lagrangian subspaces is called a Lagrangian splitting, and $\mathbb{W}$ is called the Lagrangian complement of $\mathbb{U}$.

Problem:
  1. Let $\mathbb{U}$ be a Lagrangian subspace of $\mathbb{V}$. Show that there exists a Lagrangian complement of $\mathbb{U}$
  2. Let $\mathbb{V}=\mathbb{U}\oplus\mathbb{W}$ be a Lagrangian splitting and $x_1,\ldots,x_n$ any basis form $\mathbb{U}$. Show that there exists a unique basis $y_1,\ldots y_n$ of $\mathbb{W}$ such that $x_1,\ldots,x_n,y_1,\ldots,y_n$ is a symplectic basis for $\mathbb{V}$.

-----

Hints:
  1. Take $\mathbb{W}=J\mathbb{U}$ and show that it's a Lagrangian complement to $\mathbb{U}$.
  2. Define the annihilator of $\mathbb{W}$ by $\mathbb{W}^0 = \{f\in\mathbb{V}^{\ast}: f(e)=0\text{ for all $e\in\mathbb{W}$}\}$. Define $\phi_i\in\mathbb{W}^0$ by $\phi_i(w)=\omega(x_i,w)$ for $w\in\mathbb{W}$. Show that $\phi_1,\ldots,\phi_n$ forms a basis for $\mathbb{W}^0$.

 
Physics news on Phys.org
No one answered this week's question. You can find my solution below.

Proof:
  1. The following shows that the complement is not unique. Let $\mathbb{V}=\mathbb{F}^{2n}$ and let $\mathbb{U}\subset\mathbb{F}^{2n}$.
    Claim: $\mathbb{W}=J\mathbb{U}$ is a Lagrangian complement to $\mathbb{U}$.
    Proof of Claim: If $x,y\in\mathbb{W}$, then $x=Ju$, $y=Jv$ where $u,v\in\mathbb{U}$ or $\{u,v\}=0$ (here, $\{\cdot,\cdot\}$ denotes the Poisson bracket). But $\{x,y\}=\{Ju,Jv\}=\{u,v\}=0$, so $\mathbb{W}$ is Lagrangian. If $x\in\mathbb{U}\cap J\mathbb{U}$, the $x=Jy$ with $y\in\mathbb{U}$. So $x,Jx\in\mathbb{U}$ and so $\{x,Jx\}=-\|x\|^2=0$ or $x=0$. Thus, $\mathbb{U}\cap\mathbb{W}=\emptyset$. $\hspace{.25in}\blacksquare$
  2. Define $\phi_i\in\mathbb{W}^0$ by $\phi_i(w)=\omega(x_i,w)$ for $w\in\mathbb{W}$. If $\sum\alpha_i\phi_i=0$, then $\omega\left(\sum\alpha_ix_i,w\right)=0$ for all $w\in\mathbb{W}$ or $\omega\left(\sum\alpha_ix_i,\mathbb{W}\right)=0$. But because $\mathbb{V}=\mathbb{U}\oplus\mathbb{W}$ and $\omega(\mathbb{U},\mathbb{U})=0$, it follows that $\omega\left(\sum\alpha_ix_i,\mathbb{V}\right)=0$. This implies $\sum\alpha_ix_i=0$, because $\omega$ is nondegenerate, and this implies that $\alpha_i=0$ because the $x_i$'s are independent. Thus, $\phi_1,\ldots,\phi_n$ are independent, and so they form a basis for $\mathbb{W}^0$. Let $y_1,\ldots,y_n$ be the dual basis in $\mathbb{W}$; so $\omega(x_i,y_j)=\phi_i(y_j)=\delta_{ij}$. $\hspace{.25in}\blacksquare$
 

Similar threads

  • · Replies 2 ·
Replies
2
Views
3K
  • · Replies 23 ·
Replies
23
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 9 ·
Replies
9
Views
2K
  • · Replies 1 ·
Replies
1
Views
1K
  • · Replies 7 ·
Replies
7
Views
2K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 61 ·
3
Replies
61
Views
13K