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arxiv: 1806.11275 · v1 · pith:WZCRQH2Snew · submitted 2018-06-29 · ❄️ cond-mat.stat-mech · cond-mat.dis-nn· math-ph· math.MP· math.PR

Exact persistence exponent for the 2d-diffusion equation and related Kac polynomials

classification ❄️ cond-mat.stat-mech cond-mat.dis-nnmath-phmath.MPmath.PR
keywords diffusionpolynomialsconnectionequationrandomcomputefieldlarge
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We compute the persistence for the $2d$-diffusion equation with random initial condition, i.e., the probability $p_0(t)$ that the diffusion field, at a given point ${\bf x}$ in the plane, has not changed sign up to time $t$. For large $t$, we show that $p_0(t) \sim t^{-\theta(2)}$ with $\theta(2) = 3/16$. Using the connection between the $2d$-diffusion equation and Kac random polynomials, we show that the probability $q_0(n)$ that Kac polynomials, of (even) degree $n$, have no real root decays, for large $n$, as $q_0(n) \sim n^{-3/4}$. We obtain this result by using yet another connection with the truncated orthogonal ensemble of random matrices. This allows us to compute various properties of the zero-crossings of the diffusing field, equivalently of the real roots of Kac polynomials. Finally, we unveil a precise connection with a fourth model: the semi-infinite Ising spin chain with Glauber dynamics at zero temperature.

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