17 research outputs found

    On bounded continuous solutions of the archetypal equation with rescaling

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    The `archetypal' equation with rescaling is given by y(x)=R2y(a(xb))μ(da,db)y(x)=\iint_{\mathbb{R}^2} y(a(x-b))\,\mu(\mathrm{d}a,\mathrm{d}b) (xRx\in\mathbb{R}), where μ\mu is a probability measure; equivalently, y(x)=E{y(α(xβ))}y(x)=\mathbb{E}\{y(\alpha(x-\beta))\}, with random α,β\alpha,\beta and E\mathbb{E} denoting expectation. Examples include: (i) functional equation y(x)=ipiy(ai(xbi))y(x)=\sum_{i} p_{i} y(a_i(x-b_i)); (ii) functional-differential (`pantograph') equation y(x)+y(x)=ipiy(ai(xci))y'(x)+y(x)=\sum_{i} p_{i} y(a_i(x-c_i)) (pi>0p_{i}>0, ipi=1\sum_{i} p_{i}=1). Interpreting solutions y(x)y(x) as harmonic functions of the associated Markov chain (Xn)(X_n), we obtain Liouville-type results asserting that any bounded continuous solution is constant. In particular, in the `critical' case E{lnα}=0\mathbb{E}\{\ln|\alpha|\}=0 such a theorem holds subject to uniform continuity of y(x)y(x); the latter is guaranteed under mild regularity assumptions on β\beta, satisfied e.g.\ for the pantograph equation (ii). For equation (i) with ai=qmia_i=q^{m_i} (miZm_i\in\mathbb{Z}, ipimi=0\sum_i p_i m_i=0), the result can be proved without the uniform continuity assumption. The proofs utilize the iterated equation y(x)=E{y(Xτ)X0=x}y(x)=\mathbb{E}\{y(X_\tau)\,|\,X_0=x\} (with a suitable stopping time τ\tau) due to Doob's optional stopping theorem applied to the martingale y(Xn)y(X_n).Comment: Substantially revised. The title is modifie

    Limit laws for sums of random exponentials

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    We study the limiting distribution of the sum S-N(t) = Sigma(i=1)(N) e(tXi) as t -> infinity, N -> infinity, where (X-i) are i.i.d. random variables. Attention to such exponential sums has been motivated by various problems in random media theory. Examples include the quenched mean population size of a colony of branching processes with random branching rates and the partition function of Derrida's Random Energy Model. In this paper, the problem is considered under the assumption that the log-tail distribution function h(x) = -log P{X-I > x} is regularly varying at infinity with index 1 < rho < infinity. An appropriate scale for the growth of N relative to t is of the form e(lambda H0(t)), where the rate function Ho(t) is a certain asymptotic version of the cumulant. generating function H(t) = log E[e(tXi)] provided by Kasahara's exponential Tauberian theorem. We have found two critical points, 0 < lambda(1) < lambda(2) < infinity, below which the Law of Large Numbers and the Central Limit Theorem, respectively, break down. Below lambda(2), we impose a slightly stronger condition of normalized regular variation of h. The limit laws here appear to be stable, with characteristic exponent alpha = alpha(rho, lambda) ranging from 0 to 2 and with skewness parameter beta = 1. A limit theorem for the maximal value of the sample {e(tXi), i = 1,...,N} is also proved

    Flare Observations

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    Limit laws for sums of random exponentials

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    We study the limiting distribution of the sum S-N(t) = Sigma(i=1)(N) e(tXi) as t -> infinity, N -> infinity, where (X-i) are i.i.d. random variables. Attention to such exponential sums has been motivated by various problems in random media theory. Examples include the quenched mean population size of a colony of branching processes with random branching rates and the partition function of Derrida's Random Energy Model. In this paper, the problem is considered under the assumption that the log-tail distribution function h(x) = -log P{X-I > x} is regularly varying at infinity with index 1 < rho < infinity. An appropriate scale for the growth of N relative to t is of the form e(lambda H0(t)), where the rate function Ho(t) is a certain asymptotic version of the cumulant. generating function H(t) = log E[e(tXi)] provided by Kasahara's exponential Tauberian theorem. We have found two critical points, 0 < lambda(1) < lambda(2) < infinity, below which the Law of Large Numbers and the Central Limit Theorem, respectively, break down. Below lambda(2), we impose a slightly stronger condition of normalized regular variation of h. The limit laws here appear to be stable, with characteristic exponent alpha = alpha(rho, lambda) ranging from 0 to 2 and with skewness parameter beta = 1. A limit theorem for the maximal value of the sample {e(tXi), i = 1,...,N} is also proved

    Correlation effects in the trapping problem: general approach and rigorous results

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    The problem of Brownian survival among randomly located traps is considered with emphasis on the role of trap correlations. We proceed from the general representation of the survival probability as the expected value of the emptiness probability function applied to the Wiener sausage. Using the definition of (pure) trap attraction vs. repulsion in terms of the emptiness probability function, we prove the physical conjecture about the trapping slowdown or acceleration, according to the “sign” of correlations. Two specific models are studied along this line, in which the emptiness probability can be found explicitly; in particular, the long-time survival asymptotics is derived. A remarkable correlation effect of the survival probability dependence on the trap size in one dimension is also discussed
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