- Commit
- b1fd8dc0d1cbb7b6543cfcb6bf2d2c8cbbf6a341
- Parent
- 498abf26b9e1049aea20337e8ba0f2169d9641e4
- Author
- Pablo <pablo-escobar@riseup.net>
- Date
Minor tweak in notation
Fixed the notation for the weight lattice of sl3
Source code for my notes on representations of semisimple Lie algebras and Olivier Mathieu's classification of simple weight modules
Minor tweak in notation
Fixed the notation for the weight lattice of sl3
2 files changed, 10 insertions, 10 deletions
Status | File Name | N° Changes | Insertions | Deletions |
Modified | sections/semisimple-algebras.tex | 16 | 8 | 8 |
Modified | sections/sl2-sl3.tex | 4 | 2 | 2 |
diff --git a/sections/semisimple-algebras.tex b/sections/semisimple-algebras.tex @@ -423,14 +423,14 @@ restrictions on the weights of \(V\). Namely, if \(\lambda\) is a weight, Proposition~\ref{thm:weights-fit-in-weight-lattice} is clearly analogous to corollary~\ref{thm:sl3-weights-fit-in-weight-lattice}. In fact, the weight lattice of \(\mathfrak{sl}_3(K)\) -- as in definition~\ref{def:weight-lattice} --- is precisely \(\mathbb{Z} \alpha_1 \oplus \mathbb{Z} \alpha_2 \oplus -\mathbb{Z} \alpha_3\). To proceed further, we would like to take \emph{the -highest weight of \(V\)} as in section~\ref{sec:sl3-reps}, but the meaning of -\emph{highest} is again unclear in this situation. We could simply fix a linear -function \(\mathbb{Q} P \to \mathbb{Q}\) -- as we did in -section~\ref{sec:sl3-reps} -- and choose a weight \(\lambda\) of \(V\) that -maximizes this functional, but at this point it is convenient to introduce some -additional tools to our arsenal. These tools are called \emph{basis}. +-- is precisely \(\mathbb{Z} \langle \alpha_1, \alpha_2, \alpha_3 \rangle\). To +proceed further, we would like to take \emph{the highest weight of \(V\)} as in +section~\ref{sec:sl3-reps}, but the meaning of \emph{highest} is again unclear +in this situation. We could simply fix a linear function \(\mathbb{Q} P \to +\mathbb{Q}\) -- as we did in section~\ref{sec:sl3-reps} -- and choose a weight +\(\lambda\) of \(V\) that maximizes this functional, but at this point it is +convenient to introduce some additional tools to our arsenal. These tools are +called \emph{basis}. \begin{definition}\label{def:basis-of-root} A subset \(\Sigma = \{\beta_1, \ldots, \beta_k\} \subset \Delta\) of linearly
diff --git a/sections/sl2-sl3.tex b/sections/sl2-sl3.tex @@ -610,8 +610,8 @@ In general, we find\dots As a first consequence of this, we show\dots \begin{definition} - The lattice \(P = \mathbb{Z} \alpha_1 \oplus \mathbb{Z} \alpha_2 \oplus \mathbb{Z} \alpha_3\) is - called \emph{the weight lattice of \(\mathfrak{sl}_3(K)\)}. + The lattice \(P = \mathbb{Z} \langle \alpha_1, \alpha_2, \alpha_3 \rangle\) + is called \emph{the weight lattice of \(\mathfrak{sl}_3(K)\)}. \end{definition} \begin{corollary}\label{thm:sl3-weights-fit-in-weight-lattice}