2015
DOI: 10.1007/978-3-319-19039-6_6
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Extended Marshall–Olkin Model and Its Dual Version

Abstract: We propose an extension of the generalized bivariate Marshall-Olkin model assuming dependence between the random variables involved. Probabilistic, aging properties, and survival copula representation of the extended model are obtained and illustrated by examples. Bayesian analysis is performed and possible applications are discussed. A dual version of extended Marshall-Olkin model is introduced and related stochastic order comparisons are presented. IntroductionA variety of bivariate (multivariate) extensions… Show more

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Cited by 11 publications
(12 citation statements)
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“…With this additional source of dependence extended Marshall-Olkin's distributions allow modeling both positive and negative quadrant dependence between its components. Moreover, the model may be non-exchangeable even if the marginals have the same distribution, consult Pinto and Kolev (2015) for details.…”
Section: Discussion and Possible Further Investigationsmentioning
confidence: 99%
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“…With this additional source of dependence extended Marshall-Olkin's distributions allow modeling both positive and negative quadrant dependence between its components. Moreover, the model may be non-exchangeable even if the marginals have the same distribution, consult Pinto and Kolev (2015) for details.…”
Section: Discussion and Possible Further Investigationsmentioning
confidence: 99%
“…The corresponding joint distributions do not possess BLMP, i.e., are "aging". As a further step, Pinto and Kolev (2015) introduced the Extended MO model assuming dependence between variables T 1 and T 2 , but keeping T 3 independent of them. The motivation is that the individual shocks might be dependent if the items share a common environment.…”
Section: B J P S -Accepted Manuscriptmentioning
confidence: 99%
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“…In 2014 the model was extended to the multidimensional case by Lin and Li [4]. As an added step, in 2015 Pinto and Kolev [5] introduced the extended BLMP model assuming the dependence between individual shocks, but keeping the third one independent of the previous two. Their motivation is that the individual shocks might be dependent if the items share a common environment.…”
Section: Introductionmentioning
confidence: 99%
“…More specifically, let the distribution of the pair (X m , X f ) be defined via the joint survival functionF X m ,X f (x, y) = P(X m > x, X f > y) for x, y ≥ 0, and consider a continuous non-negative random variable Z with survival functionF Z (x) = P(Z > x), independent of X m and X f . Thus, we arrive to the Extended Marshall-Olkin (EMO) model introduced in Pinto and Kolev (2015) and defined as follows:…”
Section: Introductionmentioning
confidence: 99%