2022
DOI: 10.21203/rs.3.rs-2202581/v1
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The inverse first-passage time problem as hydrodynamic limit of a particle system

Abstract: Given a distribution on the positive real line, the two-sided inverse first-passage time problem for Brownian motion asks for a function, such that the first-passage time of this function by a reflected Brownian motion has the given distribution. We present a particle system without branching but with selection at timepoints depending on the given distribution on the positive real line, whose hydrodynamic limit is the distribution of a Brownian motion conditioned to not have passed the solution of the inverse … Show more

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“…Heuristically, q(n) k is an empirical version of q (n) (kδ (n) ) from (2.6). A proof for the validity of this choice, namely that q(n) k → q (n) (kδ (n) ) almost surely as N → ∞, can be found in [18,Theorem 3.3.2].…”
Section: Monte Carlo Methods For An Approximate Solutionmentioning
confidence: 99%
“…Heuristically, q(n) k is an empirical version of q (n) (kδ (n) ) from (2.6). A proof for the validity of this choice, namely that q(n) k → q (n) (kδ (n) ) almost surely as N → ∞, can be found in [18,Theorem 3.3.2].…”
Section: Monte Carlo Methods For An Approximate Solutionmentioning
confidence: 99%