Statistics of first-passage Brownian functionals

preprint2021arXivOpen access

Abstract

We study the distribution of first-passage functionals A=∫0tfxn(t) dt{\cal A}= \int_0^{t_f} x^n(t)\, dt, where x(t)x(t) is a Brownian motion (with or without drift) with diffusion constant DD, starting at x0>0x_0>0, and tft_f is the first-passage time to the origin. In the driftless case, we compute exactly, for all n>−2n>-2, the probability density Pn(A∣x0)=Prob.(A=A)P_n(A|x_0)=\text{Prob}.(\mathcal{A}=A). This probability density has an essential singular tail as A→0A\to 0 and a power-law tail ∼A−(n+3)/(n+2)\sim A^{-(n+3)/(n+2)} as A→∞A\to \infty. The former is reproduced by the optimal fluctuation method (OFM), which also predicts the optimal paths of the conditioned process for small AA. For the case with a drift toward the origin, where no exact solution is known for general n>−1n>-1, the OFM predicts the distribution tails. For A→0A\to 0 it predicts the same essential singular tail as in the driftless case. For A→∞A\to \infty it predicts a stretched exponential tail −ln⁡Pn(A∣x0)∼A1/(n+1)-\ln P_n(A|x_0)\sim A^{1/(n+1)} for all n>0n>0. In the limit of large Péclet number Pe=μx0/(2D)≫1\text{Pe}= μx_0/(2D)\gg 1, where μμ is the drift velocity, the OFM predicts a large-deviation scaling for all AA: −ln⁡Pn(A∣x0)≃Pe Φn(z=A/Aˉ)-\ln P_n(A|x_0)\simeq\text{Pe}\, Φ_n\left(z= A/\bar{A}\right), where Aˉ=x0n+1/μ(n+1)\bar{A}=x_0^{n+1}/{μ(n+1)} is the mean value of A\mathcal{A}. We compute the rate function Φn(z)Φ_n(z) analytically for all n>−1n>-1. For n>0n>0 Φn(z)Φ_n(z) is analytic for all zz, but for −1<n<0-1<n<0 it is non-analytic at z=1z=1, implying a dynamical phase transition. The order of this transition is 22 for −1/2<n<0-1/2<n<0, while for −1<n<−1/2-1<n<-1/2 the order of transition changes continuously with nn. Finally, we apply the OFM to the case of μ<0μ<0 (drift away from the origin). We show that, when the process is conditioned on reaching the origin, the distribution of A\mathcal{A} coincides with the distribution of A\mathcal{A} for μ>0μ>0 with the same ∣μ∣|μ|.

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