1983
DOI: 10.1007/bf02894735
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First passage time distributions for finite one-dimensional random walks

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Cited by 33 publications
(28 citation statements)
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“…0 in order to keep those moments finite. Such relations have been previously proposed for certain random processes in discrete space [14,15] and have been anticipated without proof in [16] also for the present continuous dynamics (1). A proof will be given at the end of this Letter (see also [17]).…”
mentioning
confidence: 66%
“…0 in order to keep those moments finite. Such relations have been previously proposed for certain random processes in discrete space [14,15] and have been anticipated without proof in [16] also for the present continuous dynamics (1). A proof will be given at the end of this Letter (see also [17]).…”
mentioning
confidence: 66%
“…To derive this expression, we needed to correct an error in Khantha and Balakrishnan (1983) in going from their equation 6 to equation 7: the inner expression in their equation 7 should read (m − m 0 )…”
Section: Appendix D: Analysis Of the Dlif Modelmentioning
confidence: 99%
“…The membrane potential V(t) for this model is a continuous-time Markov random walk, and the output spike trains are renewal processes. The Laplace transform of the first passage time densities for reflected random walks are obtained by Khantha and Balakrishnan (1983). The moments of the first passage times can be found from the derivatives of these Laplace transforms (Feller, 1991).…”
Section: Appendix D: Analysis Of the Dlif Modelmentioning
confidence: 99%
“…Paul L evy was a French mathematician who was interested in probability distributions with certain properties, most notably that the probability distribution for a sum of independent, identically distributed random variables takes the same form as the probability distribution for each component variable (L evy 1937). His work found application within physics, especially since about the early 1980s, when it was realized that various kinds of random walk, considered to reflect certain physical processes, could lead to outcomes with L evy probability distributions (Hughes, Shlesinger & Montroll 1981;Khantha & Balakrishnan 1983;Mukamel, Stern & Ronis 1983). In this context, the L evy walk has proven particularly useful in studies of processes involving 'super diffusion', where diffusion occurs at a faster rate than the 'normal diffusion' resulting from Brownian motion (Eliazar & Klafter 2011;Eliazar & Shlesinger 2013).…”
Section: The L Evy and Other 'Random Walks'mentioning
confidence: 99%