The extended-kernel limit for the pentagonal Aztec diamond

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Let XNRX_N^R denote the top line of an Aztec diamond of size NN with a triangle removed from the top corner at height N/2+2−5/6N1/3RN/\sqrt{2}+2^{-5/6}N^{1/3}R. Define

XNR,resc(T)=XNR(2−1/6N2/3T)−N/22−5/6N1/3.X_N^{R,\mathrm{resc}}(T)=\frac{X_N^R(2^{-1/6}N^{2/3}T)-N/\sqrt{2}}{2^{-5/6}N^{1/3}}.

For given observation times T1,…,TkT_1,\ldots,T_k and thresholds U1,…,UkU_1,\ldots,U_k, the pentagonal Aztec-diamond conjecture.

lim⁡N→∞P(⋂ℓ=1k{XNR,resc(Tℓ)≤Uℓ})=det⁡(1−K^ext)L2(E),\lim_{N\to\infty}\mathbf P\left(\bigcap_{\ell=1}^k\{X_N^{R,\mathrm{resc}}(T_\ell)\leq U_\ell\}\right)=\det\left(\mathbb{1}-\widehat K^{\mathrm{ext}}\right)_{L^2(E)},

where

E={(T1,[U1−R,0])×…×(Tk,[Uk−R,0])}.E=\{(T_1,[U_1-R,0])\times\ldots\times(T_k,[U_k-R,0])\}.

This predicts an extended-kernel determinantal scaling limit for the top line when the triangular cutout becomes, after rescaling, a conditioning to remain below the fixed height RR.

References

Primary source

Patrik L. Ferrari and Bálint Vető, “The hard-edge tacnode process for Brownian motion”, arXiv:1608.00394 (2020).

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