The negative-curvature JT area-tail conjecture

About 2 years old · traced to

Let ρβq−(A)\rho^-_{\beta_{\mathrm q}}(A) be the area distribution of JT gravity with negative curvature −2/L2-2/L^2, coupled to conformal matter with c≤0c\leq0, and let ν\nu be the corresponding critical exponent. Negative-curvature area-tail conjecture. There are a strictly positive constant κν−\kappa^-_\nu and a strictly increasing exponent χν−\chi^-_\nu such that

ln⁡ρβq−(A)∼−κν−(AβqνL)χν−(A→+∞),\ln\rho^-_{\beta_{\mathrm q}}(A)\sim-\kappa^-_\nu\left(\frac{A}{\beta_{\mathrm q}^{\nu}L}\right)^{\chi^-_\nu}\qquad(A\to+\infty),

with

lim⁡ν→1/2+χν−=2,lim⁡ν→1−χν−=+∞.\lim_{\nu\to1/2^+}\chi^-_\nu=2,\qquad\lim_{\nu\to1^-}\chi^-_\nu=+\infty.

The predicted tail is rapidly decaying enough to allow all cosmological constants and is motivated by hyperbolic Brownian-path behavior and the semiclassical limit.

References

Primary source

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

Progress summary

Never refreshed

Nothing recorded yet. Refresh searches the literature and the public web for attempts on this problem, and writes the first summary here.

Solutions 0

No solutions have been posted yet.