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Nov 4, 2023 at 13:41 comment added Sam Hopkins Again in Type $A_n$, the hyperplane arrangement you mention at the end is (basically) the so-called "resonance arrangement." This is a classic example of a hyperplane arrangement about which it is very hard to say anything. See e.g. the prior MO questions mathoverflow.net/questions/62764 and mathoverflow.net/questions/372427.
Nov 4, 2023 at 7:28 history edited Dr. Evil CC BY-SA 4.0
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Nov 4, 2023 at 7:22 comment added Dr. Evil Thanks a lot Sam.
Nov 4, 2023 at 7:21 history edited Dr. Evil CC BY-SA 4.0
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Nov 3, 2023 at 13:01 comment added Sam Hopkins In Type A, something special happens: every fundamental weight is minuscule. So you can characterize $X$ as the set of those nonzero coweights $\omega^{\vee}$ which have $(\omega^{\vee}, \alpha) \in \{0,\pm1\}$ for all roots $\alpha \in \Phi$. But this characterization does not extend to other types.
Nov 3, 2023 at 2:32 comment added Sam Hopkins In general, the size of the $W$-orbit of $\omega_i^\vee$ is $\#W/\#W_i$ where $W_i$ is the maximal parabolic subgroup corresponding to node $i$ (i.e., the Weyl group of the Dynkin diagram we get by deleting node $i$). It’s not clear you can get a better formula for $\#X$ than just summing this over all $i$.
Nov 3, 2023 at 2:21 comment added Sam Hopkins If $\Phi$ is of Type $A_n$ then $\# X = 2^{n+1}-2$.
Nov 3, 2023 at 2:04 history asked Dr. Evil CC BY-SA 4.0