- Commit
- e2ec70dd6089a6518c1c393efb9b33b1bf4843ec
- Parent
- 11242f803fae543406ef8cf88bba75a55e1feff3
- Author
- Pablo <pablo-escobar@riseup.net>
- Date
Added TODO items
Source code for my notes on representations of semisimple Lie algebras and Olivier Mathieu's classification of simple weight modules
Added TODO items
1 file changed, 6 insertions, 0 deletions
Status | File Name | N° Changes | Insertions | Deletions |
Modified | sections/sl2-sl3.tex | 6 | 6 | 0 |
diff --git a/sections/sl2-sl3.tex b/sections/sl2-sl3.tex @@ -584,6 +584,9 @@ implemented for \(\mathfrak{sl}_3(K)\) -- and indeed that's what we'll do later down the line -- but instead we would like to focus on the problem of finding the weights of \(V\) for the moment. +% TODO: Move this to before showing V is a highest weight module +% TODO: This would allow us to justify drawing the weight diagrams in the real +% plane as opposed to some abstract 4-dimensional space We'll start out by trying to understand the weights in the boundary of \(\frac{1}{3}\)-plane previously drawn. Since the root spaces act by translation, the action of \(E_{2 1}\) in \(V_\lambda\) will span a subspace @@ -811,6 +814,9 @@ must also be weights of \(V\). The final picture is thus \end{tikzpicture} \end{center} +% TODO: Move this to just after the discussion on the distinguished subalgebras +% TODO: This would allow us to justify the fact we've been drawing the highest +% weight of V as an element of the weight lattice Another important consequence of our analysis is the fact that \(\lambda\) lies in the lattice \(P\) generated by \(\alpha_1\), \(\alpha_2\) and \(\alpha_3\). Indeed, \(\lambda([E_{i j}, E_{j i}])\) is an eigenvalue of \(h\) in a