The flow tree formula for quiver moduli

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Let a KK-node quiver have adjacency matrix αab\alpha_{ab}, dimension vector γ=(N1,…,NK)\gamma=(N_1,\dots,N_K), stability parameters ζ=(ζ1,…,ζK)\zeta=(\zeta_1,\dots,\zeta_K), and generic superpotential W(ϕab,A,ss′)\mathcal{W}(\phi_{ab,A,ss'}). Let Ω(γ,z,y)\Omega(\gamma,z,y) be the rescaled Poincaré polynomial, let Ω‾\overline{\Omega} be its rational counterpart, and let μ\mu be the Möbius function. The quiver flow tree conjecture. The rescaled Poincaré polynomial is conjectured to obey

Ω(γ,z,y)=∑m∣γμ(m) y−1/ym(ym−1/ym) Ω‾(γ/m,z,ym),\Omega(\gamma,z,y)=\sum_{m\mid\gamma}\mu(m)\,\frac{y-1/y}{m(y^m-1/y^m)}\,\overline{\Omega}(\gamma/m,z,y^m),

with

Ω‾(γ,z,y)=∑γ=∑i=1nγigtr({γi,ci},y)∣Aut{γi}∣∏i=1nΩ‾∗(γi,y),\overline{\Omega}(\gamma,z,y)=\sum_{\gamma=\sum_{i=1}^n\gamma_i}\frac{g_{\rm tr}(\{\gamma_i,c_i\},y)}{|{\rm Aut}\{\gamma_i\}|}\prod_{i=1}^n\overline{\Omega}_*(\gamma_i,y),

where the sum is over distinct unordered splittings into vectors with non-negative entries, gtrg_{\rm tr} is the tree index, and Ω‾∗(γi,y)\overline{\Omega}_*(\gamma_i,y) is evaluated using ζ∗,a(γi)=−∑b=1Kαabnib\zeta_{*,a}(\gamma_i)=-\sum_{b=1}^K\alpha_{ab}n_{ib}. This conjectural formula expresses quiver Poincaré polynomials through attractor indices and flow-tree data; the supplied text does not establish it in full generality.

References

Primary source

Sergei Alexandrov and Boris Pioline, “Attractor flow trees, BPS indices and quivers”, arXiv:1804.06928 (2019).

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