2018
DOI: 10.1016/j.spl.2018.05.020
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Exact simulation of reciprocal Archimedean copulas

Abstract: The decreasing enumeration of the points of a Poisson random measure whose mean measure is Radon on (0, ∞] can be represented as a non-increasing function of the jump times of a standard Poisson process. This observation allows to generalize the essential idea from a well-known exact simulation algorithm for arbitrary extreme-value copulas to copulas of a more general family of max-infinitely divisible distributions, with reciprocal Archimedean copulas being a particular example.

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Cited by 4 publications
(13 citation statements)
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“…Proof. By (10), µ j is a finite measure for each j ∈ J 0 . Thus, Xj is obtained by the simulation of a finite PRM with intensity µ j .…”
Section: Exact Simulation Of Continuous Max-id Processesmentioning
confidence: 99%
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“…Proof. By (10), µ j is a finite measure for each j ∈ J 0 . Thus, Xj is obtained by the simulation of a finite PRM with intensity µ j .…”
Section: Exact Simulation Of Continuous Max-id Processesmentioning
confidence: 99%
“…For example, a common representation of an exponent measure of a max-id random vector is a scale mixture of a probability distribution on the non-negative unit sphere of some norm on R d . Two famous representatives of this class of exponent measures are the exponent measures of max-stable random vectors with unit Fréchet margins [16, Chapter 5] and random vectors with reciprocal Archimedean copula [7,10], see Example 3.10 below. In both cases, a simulation of X via Algorithm 1 would require to deviate from the natural description of the exponent measure to simulate the PRM with intensity 1 {f (t)≥c} dµ(f ).…”
Section: Exact Simulation Of Max-id Random Vectorsmentioning
confidence: 99%
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