TY - JOUR
T1 - Exact statistics of the gap and time interval between the first two maxima of random walks and Lévy flights
AU - Majumdar, Satya N.
AU - Mounaix, Philippe
AU - Schehr, Grégory
PY - 2013/8/14
Y1 - 2013/8/14
N2 - We investigate the statistics of the gap Gn between the two rightmost positions of a Markovian one-dimensional random walker (RW) after n time steps and of the duration Ln which separates the occurrence of these two extremal positions. The distribution of the jumps ηi 's of the RW, f(η), is symmetric and its Fourier transform has the small k behavior 1-f(k)∼|k|μ, with 0<μ≤2. For μ=2, the RW converges, for large n, to Brownian motion, while for 0<μ<2 it corresponds to a Lévy flight of index μ. We compute the joint probability density function (PDF) Pn(g,l) of Gn and Ln and show that, when n→∞, it approaches a limiting PDF p(g,l). The corresponding marginal PDFs of the gap, pgap(g), and of L n, ptime(l), are found to behave like p gap(g)∼g-1- μ for gâ‰1 and 0<μ<2, and ptime(l)∼l- γμ for lâ‰1 with γ(1<μ≤2)=1+1/μ and γ(0<μ<1)=2. For l, gâ‰1 with fixed lg -μ, p(g,l) takes the scaling form p(g,l)∼g-1 -2μpËœμ(lg-μ), where p Ëœμ(y) is a (μ-dependent) scaling function. We also present numerical simulations which verify our analytic results.
AB - We investigate the statistics of the gap Gn between the two rightmost positions of a Markovian one-dimensional random walker (RW) after n time steps and of the duration Ln which separates the occurrence of these two extremal positions. The distribution of the jumps ηi 's of the RW, f(η), is symmetric and its Fourier transform has the small k behavior 1-f(k)∼|k|μ, with 0<μ≤2. For μ=2, the RW converges, for large n, to Brownian motion, while for 0<μ<2 it corresponds to a Lévy flight of index μ. We compute the joint probability density function (PDF) Pn(g,l) of Gn and Ln and show that, when n→∞, it approaches a limiting PDF p(g,l). The corresponding marginal PDFs of the gap, pgap(g), and of L n, ptime(l), are found to behave like p gap(g)∼g-1- μ for gâ‰1 and 0<μ<2, and ptime(l)∼l- γμ for lâ‰1 with γ(1<μ≤2)=1+1/μ and γ(0<μ<1)=2. For l, gâ‰1 with fixed lg -μ, p(g,l) takes the scaling form p(g,l)∼g-1 -2μpËœμ(lg-μ), where p Ëœμ(y) is a (μ-dependent) scaling function. We also present numerical simulations which verify our analytic results.
U2 - 10.1103/PhysRevLett.111.070601
DO - 10.1103/PhysRevLett.111.070601
M3 - Article
AN - SCOPUS:84882716417
SN - 0031-9007
VL - 111
JO - Physical Review Letters
JF - Physical Review Letters
IS - 7
M1 - 070601
ER -