242 research outputs found

    One-Dimensional Diffusions That Eventually Stop Down-Crossing

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    Consider a diffusion process corresponding to the operator L=12ad2dx2+bddxL=\frac12a\frac{d^2}{dx^2}+b\frac d{dx} and which is transient to +∞+\infty. For c>0c>0, we give an explicit criterion in terms of the coefficients aa and bb which determines whether or not the diffusion almost surely eventually stops making down-crossings of length cc. As a particular case, we show that if a=1a=1, then the diffusion almost surely stops making down-crossings of length cc if b(x)β‰₯12clog⁑x+Ξ³clog⁑log⁑xb(x)\ge\frac1{2c}\log x+\frac\gamma c\log\log x, for some Ξ³>1\gamma>1 and for large xx, but makes down-crossings of length cc at arbitrarily large times if b(x)≀12clog⁑x+1clog⁑log⁑xb(x)\le\frac1{2c}\log x+\frac1c\log\log x, for large xx

    When the law of large numbers fails for increasing subsequences of random permutations

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    Let the random variable Zn,kZ_{n,k} denote the number of increasing subsequences of length kk in a random permutation from SnS_n, the symmetric group of permutations of {1,...,n}\{1,...,n\}. In a recent paper [Random Structures Algorithms 29 (2006) 277--295] we showed that the weak law of large numbers holds for Zn,knZ_{n,k_n} if kn=o(n2/5)k_n=o(n^{2/5}); that is, lim⁑nβ†’βˆžZn,knEZn,kn=1inprobability.\lim_{n\to\infty}\frac{Z_{n,k_n}}{EZ_{n,k_n}}=1\qquad in probability. The method of proof employed there used the second moment method and demonstrated that this method cannot work if the condition kn=o(n2/5)k_n=o(n^{2/5}) does not hold. It follows from results concerning the longest increasing subsequence of a random permutation that the law of large numbers cannot hold for Zn,knZ_{n,k_n} if knβ‰₯cn1/2k_n\ge cn^{1/2}, with c>2c>2. Presumably there is a critical exponent l0l_0 such that the law of large numbers holds if kn=O(nl)k_n=O(n^l), with l<l0l<l_0, and does not hold if lim sup⁑nβ†’βˆžknnl>0\limsup_{n\to\infty}\frac{k_n}{n^l}>0, for some l>l0l>l_0. Several phase transitions concerning increasing subsequences occur at l=1/2l=1/2, and these would suggest that l0=1/2l_0={1/2}. However, in this paper, we show that the law of large numbers fails for Zn,knZ_{n,k_n} if lim sup⁑nβ†’βˆžknn4/9=∞\limsup_{n\to\infty}\frac{k_n}{n^{4/9}}=\infty. Thus, the critical exponent, if it exists, must satisfy l0∈[2/5,4/9]l_0\in[{2/5},{4/9}].Comment: Published at http://dx.doi.org/10.1214/009117906000000728 in the Annals of Probability (http://www.imstat.org/aop/) by the Institute of Mathematical Statistics (http://www.imstat.org
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