Coxeter fan

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Coxeter fan

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Let \(W\) be a Weyl group.

  • The Coxeter arrangement \(\mathcal{A}\) for \(W\) is the collection of all reflecting hyperplanes for \(W\). The complement \(V \backslash(\bigcup \mathcal{A})\) of \(\mathcal{A}\) consists of open cones.

  • The chambers are in canonical bijective correspondence with the elements of \(W\). The fundamental chamber \(D:=\bigcap_{s \in S}\left\{v \in V \mathrel{\Big|}\left\langle v, \alpha_{s}\right\rangle \geq 0\right\}\) corresponds to the identity \(e \in W\) and the chamber \(w(D)\) corresponds to \(w \in W\).

  • Subsets above and below hyperplanes:

    • A subset \(U\) of \(V\) is below a hyperplane \(H \in \mathcal{A}\) if every point in \(U\) is on \(H\) or on the same side of \(H\) as \(D\).
    • The subset \(U\) is strictly below \(H \in \mathcal{A}\) if \(U\) is below \(H\) and \(U \cap H=\varnothing\).
    • Similarly, \(U\) is above or strictly above a hyperplane \(H \in \mathcal{A}\). The inversions of \(w \in W\) are the reflections that correspond to the hyperplanes \(H\) which \(w(D)\) is above.
    • For a simple reflection \(s \in S\), we have \(\ell(s w)<\ell(w)\) if and only if \(s \leq w\) in the weak order if and only if \(w(D)\) is above \(H_{s}\). To decide whether \(w(D)\) is above or below \(H_{s}\) is therefore a weak order comparison.
  • See Fans.

  • For a Coxeter arrangement \({\mathcal{A}}\), the chambers and all their faces \(\mathcal{A}\) define the Coxeter fan \(\mathcal{F}\).

    • The Coxeter fan \(\mathcal{F}\) is known to be complete, essential, and simplicial.
    • The fundamental chamber \(D \in \mathcal{F}\) is a (maximal) cone spanned by the (extremal) rays \(\left\{\rho_{s} \mathrel{\Big|}s \in S\right\}\), where \(\rho_{s}\) is the intersection of \(D\) with the subspace orthogonal to the hyperplane spanned by \(\left\{\alpha_{t} \mathrel{\Big|}t \in\langle s\rangle\right\}\).
  • The rays of \(\mathcal{F}\) decompose into \(n\) orbits under the action of \(W\) and each orbit contains exactly one \(\rho_{s}, s \in S\).

    • Thus, any ray \(\rho \in \mathcal{F}^{(1)}\) is \(w\left(\rho_{s}\right)\) for some \(w \in W\) where \(s \in S\) is uniquely determined by \(\rho\) but \(w\) is not unique.
    • In fact, \(w\left(\rho_{s}\right)=g\left(\rho_{s}\right)\) if and only if \(w \in g W_{\langle s\rangle}\).

Examples

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