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> [!proposition] Proposition. ([[there exists exactly one root basis per Weyl chamber]])
> Let $(\Phi, E)$ be a [[root system]]. For $\alpha \in \Phi$, let $H_{\alpha}=\{ x \in E: (x,\alpha)=0 \}=\text{span}^{\perp}(\alpha)$ be the $\alpha$-[[reflection|hyperplane]].
>
> By Euclidean geometry, $E \setminus \bigcup_{\alpha \in \Phi}H_{\alpha}\neq \emptyset$. Take any $\gamma \in E \setminus \bigcup_{\alpha \in \Phi}H_{\alpha}$, and suggestively define $\begin{align}
> \Phi_{\gamma}^{+}&:= \{ \alpha \in \Phi: (\alpha, \gamma) > 0 \} \\
> \Phi_{\gamma}^{-}&:= \{ \alpha \in \Phi: (\alpha, \gamma) < 0 \}.
> \end{align}$
> Note that $\Phi=\Phi_{\gamma}^{+} \sqcup \Phi_{\gamma}^{-}$. (Draw a picture with $A_{2}$)
> ![[Pasted image 20250510220159.png]]
>
> Say an element $\alpha \in \Phi_{\gamma}^{+}$ is **decomposable** if $\alpha=\beta_{1}+\beta_{2}$ for $\beta_{1},\beta_{2} \in \Phi_{\gamma}^{+}$ and **indecomposable** otherwise. Let $\Delta_{\gamma}$ be the set of indecomposable elements of $\Phi_{\gamma}^{+}$. Then:
>
> **1.** $\Delta_{\gamma}$ is a [[root basis]] with corresponding set of positive roots $\Phi_{\gamma}^{+}$.
>
> **2.** *Any* [[root basis]] of $E$ is of this form for some $\gamma$.
>
> **3.** If $\gamma,\gamma' \in E \setminus \bigcup_{\alpha \in \Phi}H_{\alpha}$, then $\Delta_{\gamma}=\Delta_{\gamma'}$ if and only if $\gamma,\gamma'$ live in the same [[Weyl chamber]]. Thus, $\gamma \mapsto \Delta_{\gamma}$ defines a [[bijection]] $\{ \text{Weyl chambers} \} \leftrightarrow \{ \text{root bases of } \Phi \}.$
> Its inverse is given by $\Delta_{} \mapsto \mathscr{C}(\Delta)=\{ x \in E: (x, \alpha)>0 \ \fa \alpha \in \Delta \}.$ The set $\mathscr{C}(\Delta)$ is called the **fundamental Weyl chamber attached to $\Delta$**.
> [!proposition] Corollary.
> We extract a useful result of the proof (Claim 2) of the theorem: if $\Delta$ is a root basis and $\alpha, \beta \in \Delta$ are distinct, then $(\alpha, \beta) \leq 0$, i.e., the angle between $\alpha$ and $\beta$ is obtuse.
^proposition
> [!proof]- Proof. ([[there exists exactly one root basis per Weyl chamber]])
> ~
- [ ] (note that lemma 2 from lecture is corollary four in [[angles and lengths in a root system]])
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#### References
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