The analytically continued hyperbolic matrix-model conjecture

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Let Wn(t;p=4,q)W_n(t;p=4,q) be the disk partition function of the matrix model

S=Ntr⁡(12X2−1q(A~X)q),S=N\operatorname{tr}\left(\frac12X^2-\frac1q(\widetilde A X)^q\right),

with tr⁡A~k=Ntδk,4\operatorname{tr}\widetilde A^k=Nt\delta_{k,4} and loop operator

φ(X)=∑s=0q−2(A~X)sA~.\varphi(X)=\sum_{s=0}^{q-2}(\widetilde A X)^s\widetilde A.

Hyperbolic matrix-model conjecture. The disk partition function admits an analytic continuation in qq near q=4q=4 such that, with

n→∞,ℓ02=πL22(q−4)→0+,t→1,nℓ02=βq,Λ=16πℓ02(1−t)n\to\infty,\quad \ell_0^2=\frac{\pi L^2}{2}(q-4)\to0^+,\quad t\to1,\quad n\ell_0^2=\beta_{\mathrm q},\quad \Lambda=\frac{16\pi}{\ell_0^2}(1-t)

fixed, it yields the UV-complete disk partition function of pure JT gravity with curvature R=−2/L2R=-2/L^2. The conjecture proposes an analytic-continuation route from the hyperbolic lattice matrix model to the UV-complete theory, beyond the effective Schwarzian limit.

References

Primary source

Frank Ferrari, “Random Disks of Constant Curvature: the Lattice Story”, arXiv:2406.06875 (2024).

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