'High enough' in an exceptional tube $\implies$ Rigid
Count subspace configurations of ambient dimension $r$ that are high enough in their tubes
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$\underline{\mathrm{CM}}C \cong \frac{\mathcal{D}^b(\operatorname{coh}\mathbb{X})}{\langle \tau^{-}[1]\rangle} \cong \frac{\mathcal{D}^b(\mathrm{mod}\,P)}{\langle \tau^{-}[1]\rangle}$ where $\mathbb{X}$ is a weighted projective line of weight 2,3,6 or 2,4,4.
Cluster tilting object $T$ in $\underline{\mathrm{CM}}C$ whose (opposite) endomorphism ring is isomorphic to the relation extension of $P$.