Modèles spatiaux bayésiens pour l’estimation des moyennes pour petites régions échantillonnées et non échantillonnées
Section 3. Simulation de distributions a posteriori

Dans la présente section, nous illustrons les étapes d’échantillonnage de rejet pour obtenir des échantillons indépendants a posteriori à partir des distributions a posteriori des modèles proposés. Nous supposons que les composantes du vecteur de la moyenne de petites régions θ MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8rrps0l bbf9q8WrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaGaaiaadaaakeaacaWH4oaaaa@32F1@  sont disposées de façon que θ= ( θ (1) T , θ (2) T ) T , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8rrps0l bbf9q8WrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaGaaiaadaaakeaacaWH4oGaaGjbVlabg2da9iaaysW7ca GGOaGaaCiUdmaaDaaaleaacaaIOaGaaGymaiaaiMcaaeaaruWqHXwA IjxAGWuANHgDaGabaiaa=rfaaaGccaaISaGaaGjbVlaahI7adaqhaa WcbaGaaGikaiaaikdacaaIPaaabaGaa8hvaaaakiaaiMcadaahaaWc beqaaiaa=rfaaaGccaGGSaaaaa@4A40@  où θ (1) m 1 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8rrps0l bbf9q8WrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaGaaiaadaaakeaacaWH4oWaaSbaaSqaaiaaiIcacaaIXa GaaGykaaqabaGccaaMe8UaeyicI4meaaaaaaaaa8qacqWIDesOpaWa aWbaaSqabeaacaWGTbWaaSbaaWqaaiaaigdaaeqaaaaaaaa@3BFE@  et θ (2) m 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8rrps0l bbf9q8WrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaGaaiaadaaakeaacaWH4oWaaSbaaSqaaiaaiIcacaaIYa GaaGykaaqabaGccaaMe8UaeyicI4meaaaaaaaaa8qacqWIDesOpaWa aWbaaSqabeaacaWGTbWaaSbaaWqaaiaaikdaaeqaaaaaaaa@3C00@  sont les vecteurs de la moyenne de petites régions correspondant aux régions non échantillonnées et échantillonnées, respectivement. Pour des raisons de commodité, nous désignons la matrice de précision du k e MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8rrps0l bbf9q8WrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaGaaiaadaaakeaacaWGRbWaaWbaaSqabeaacaqGLbaaaa aa@33B2@  modèle spatial par Ω= ( σ v 2 ) 1 Ω k (ρ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8rrps0l bbf9q8WrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaGaaiaadaaakeaacaWHPoGaaGjbVlabg2da9iaaysW7ca aIOaGaeq4Wdm3aa0baaSqaaiaadAhaaeaacaaIYaaaaOGaaGykamaa CaaaleqabaGaeyOeI0IaaGymaaaakiaaykW7caWHPoWaaSbaaSqaai aadUgaaeqaaOGaaGPaVlaaiIcacqaHbpGCcaaIPaaaaa@468D@  et l’intervalle admissible de ρ MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8rrps0l bbf9q8WrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaGaaiaadaaakeaacqaHbpGCaaa@336D@  par (l,u) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8rrps0l bbf9q8WrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaGaaiaadaaakeaacaaIOaGaamiBaiaaiYcacaaMe8Uaam yDaiaaiMcaaaa@3740@  en supprimant l’indice du modèle k. MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8rrps0l bbf9q8WrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaGaaiaadaaakeaacaWGRbGaaiOlaaaa@334F@

Nous calculons d’abord la densité a posteriori marginale de ( σ v 2 ,ρ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8rrps0l bbf9q8WrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaGaaiaadaaakeaacaaIOaGaeq4Wdm3aa0baaSqaaiaadA haaeaacaaIYaaaaOGaaGilaiaaysW7cqaHbpGCcaaIPaaaaa@3AC6@  et nous fournissons les procédures d’échantillonnage subséquentes. Supposons que 0 m 2 × m 1 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8rrps0l bbf9q8WrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaGaaiaadaaakeaacaWHWaWaaSbaaSqaaiaad2gadaWgaa adbaGaaGOmaaqabaWccaaMe8Uaey41aqRaaGjbVlaad2gadaWgaaad baGaaGymaaqabaaaleqaaaaa@3B8E@  est la matrice nulle m 2 × m 1 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8rrps0l bbf9q8WrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaGaaiaadaaakeaacaWGTbWaaSbaaSqaaiaaikdaaeqaaO GaaGjbVlabgEna0kaaysW7caWGTbWaaSbaaSqaaiaaigdaaeqaaaaa @3A9B@  et que M=[ 0 m 2 × m 1 , I m 2 ], MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8rrps0l bbf9q8WrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaGaaiaadaaakeaacaWHnbGaaGjbVlabg2da9iaaysW7ca aIBbGaaCimamaaBaaaleaacaWGTbWaaSbaaWqaaiaaikdaaeqaaSGa aGPaVlabgEna0kaaykW7caWGTbWaaSbaaWqaaiaaigdaaeqaaaWcbe aakiaaiYcacaaMe8UaaCysamaaBaaaleaacaWGTbWaaSbaaWqaaiaa ikdaaeqaaaWcbeaakiaai2facaGGSaaaaa@4837@  de sorte que θ (2) =Mθ. MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8rrps0l bbf9q8WrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaGaaiaadaaakeaacaWH4oWaaSbaaSqaaiaaiIcacaaIYa GaaGykaaqabaGccaaMe8Uaeyypa0JaaGjbVlaah2eacaWH4oGaaiOl aaaa@3C34@  Supposons également que X (2) =MX. MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8rrps0l bbf9q8WrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaGaaiaadaaakeaacaWHybWaaSbaaSqaaiaaiIcacaaIYa GaaGykaaqabaGccaaMe8Uaeyypa0JaaGjbVlaah2eacaWHybGaaiOl aaaa@3B6E@  Si l’on n’intègre pas θ MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8rrps0l bbf9q8WrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaGaaiaadaaakeaacaWH4oaaaa@32F1@  dans le modèle (2.11) et (2.12), nous avons Y (2) |β, σ v 2 ,ρ~ N m 2 ( X (2) β,Δ), MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8rrps0l bbf9q8WrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaGaaiaadaaakeaadaabceqaaiaahMfadaWgaaWcbaGaaG ikaiaaikdacaaIPaaabeaakiaaykW7aiaawIa7aiaaykW7caWHYoGa aGilaiaaysW7cqaHdpWCdaqhaaWcbaGaamODaaqaaiaaikdaaaGcca aISaGaaGjbVlabeg8aYjaaysW7ieaacaWF+bGaaGjbVlaad6eadaWg aaWcbaGaamyBamaaBaaameaacaaIYaaabeaaaSqabaGccaaMc8UaaG ikaiaahIfadaWgaaWcbaGaaGikaiaaikdacaaIPaaabeaakiaaykW7 caWHYoGaaGilaiaaysW7caWHuoGaaGykaiaacYcaaaa@58DD@  où Δ= D (2) +M Ω 1 M T . MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8rrps0l bbf9q8WrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaGaaiaadaaakeaacaWHuoGaaGjbVlabg2da9iaaysW7ca WHebWaaSbaaSqaaiaaiIcacaaIYaGaaGykaaqabaGccaaMe8Uaey4k aSIaaGjbVlaah2eacaWHPoWaaWbaaSqabeaacqGHsislcaaIXaaaaO GaaCytamaaCaaaleqabaqefmuySLMyYLgimL2zOrhaiqaacaWFubaa aOGaaiOlaaaa@497B@  La marginalisation subséquente de β MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8rrps0l bbf9q8WrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaGaaiaadaaakeaacaWHYoaaaa@32EB@  donne la densité a posteriori marginale p( σ v 2 , ρ| y (2) ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8rrps0l bbf9q8WrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaGaaiaadaaakeaacaWGWbGaaGPaVlaaiIcacqaHdpWCda qhaaWcbaGaamODaaqaaiaaikdaaaGccaaISaGaaGjbVpaaeiqabaGa eqyWdiNaaGPaVdGaayjcSdGaaGPaVlaahMhadaWgaaWcbaGaaGikai aaikdacaaIPaaabeaakiaaiMcaaaa@454C@  comme suit :

p( σ v 2 , ρ| y (2) ) exp[ 1 2 y (2) T Δ 1 { Δ X (2) ( X (2) T Δ 1 X (2) ) 1 X (2) T } Δ 1 y (2) ] | Δ | 1/2 | X (2) T Δ 1 X (2) | 1/2 I(l<ρ<u).(3.1) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8rrps0l bbf9q8WrFfeuY=Hhbbf9G8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaGaaiaadaaakeaacaWGWbGaaGPaVlaaiIcacqaHdpWCda qhaaWcbaGaamODaaqaaiaaikdaaaGccaaISaGaaGjbVpaaeiqabaGa eqyWdiNaaGPaVdGaayjcSdGaaGPaVlaahMhadaWgaaWcbaGaaGikai aaikdacaaIPaaabeaakiaaiMcacaaMe8UaaGjbVlabg2Hi1kaaysW7 caaMe8+aaSaaaeaaciGGLbGaaiiEaiaacchadaWadaqaaiabgkHiTm aaleaaleaacaaIXaaabaGaaGOmaaaakiaaykW7caWH5bWaa0baaSqa aiaaiIcacaaIYaGaaGykaaqaaerbdfgBPjMCPbctPDgA0baceaGaa8 hvaaaakiaaykW7caWHuoWaaWbaaSqabeaacqGHsislcaaIXaaaaOGa aGPaVpaacmaabaGaaCiLdiaaysW7cqGHsislcaaMe8UaaCiwamaaBa aaleaacaaIOaGaaGOmaiaaiMcaaeqaaOGaaGPaVlaaiIcacaWHybWa a0baaSqaaiaaiIcacaaIYaGaaGykaaqaaiaa=rfaaaGccaaMc8UaaC iLdmaaCaaaleqabaGaeyOeI0IaaGymaaaakiaaykW7caWHybWaaSba aSqaaiaaiIcacaaIYaGaaGykaaqabaGccaaIPaWaaWbaaSqabeaacq GHsislcaaIXaaaaOGaaGPaVlaahIfadaqhaaWcbaGaaGikaiaaikda caaIPaaabaGaa8hvaaaaaOGaay5Eaiaaw2haaiaaysW7caWHuoWaaW baaSqabeaacqGHsislcaaIXaaaaOGaaGPaVlaahMhadaWgaaWcbaGa aGikaiaaikdacaaIPaaabeaaaOGaay5waiaaw2faaaqaamaaemqaba GaaGPaVlaahs5acaaMc8oacaGLhWUaayjcSdWaaWbaaSqabeaadaWc gaqaaiaaigdaaeaacaaIYaaaaaaakiaaysW7daabdeqaaiaaykW7ca WHybWaa0baaSqaaiaaiIcacaaIYaGaaGykaaqaaiaa=rfaaaGccaWH uoWaaWbaaSqabeaacqGHsislcaaIXaaaaOGaaCiwamaaBaaaleaaca aIOaGaaGOmaiaaiMcaaeqaaOGaaGPaVdGaay5bSlaawIa7amaaCaaa leqabaWaaSGbaeaacaaIXaaabaGaaGOmaaaaaaaaaOGaaGjbVlaadM eacaaMc8UaaGikaiaadYgacaaMe8UaeyipaWJaaGjbVlabeg8aYjaa ysW7cqGH8aapcaaMe8UaamyDaiaaiMcacaaIUaGaaGzbVlaaywW7ca aMf8UaaGzbVlaaywW7caGGOaGaaG4maiaac6cacaaIXaGaaiykaaaa @CB12@

De plus, nous avons des distributions a posteriori conditionnelles de β MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8rrps0l bbf9q8WrFfeuY=Hhbbf9G8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaGaaiaadaaakeaacaWHYoaaaa@32F6@  et θ MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8rrps0l bbf9q8WrFfeuY=Hhbbf9G8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaGaaiaadaaakeaacaWH4oaaaa@32FC@  qui sont :

β| σ v 2 ,ρ,y~ N p (γ,Γ),(3.2) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8rrps0l bbf9q8WrFfeuY=Hhbbf9G8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaGaaiaadaaakeaadaabceqaaiaahk7acaaMc8oacaGLiW oacaaMc8Uaeq4Wdm3aa0baaSqaaiaadAhaaeaacaaIYaaaaOGaaGil aiaaysW7cqaHbpGCcaaISaGaaGjbVlaahMhacaaMe8UaaGjbVJqaai aa=5hacaaMe8UaaGjbVlaad6eadaWgaaWcbaGaamiCaaqabaGccaaM c8UaaGikaiaaho7acaaISaGaaGjbVlaaho5acaaIPaGaaGilaiaayw W7caaMf8UaaGzbVlaaywW7caaMf8UaaiikaiaaiodacaGGUaGaaGOm aiaacMcaaaa@5F66@

θ|β, σ v 2 ,ρ,y~ N m (μ,Ψ),(3.3) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8rrps0l bbf9q8WrFfeuY=Hhbbf9G8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaGaaiaadaaakeaadaabceqaaiaahI7acaaMc8oacaGLiW oacaaMc8UaaCOSdiaaiYcacaaMe8Uaeq4Wdm3aa0baaSqaaiaadAha aeaacaaIYaaaaOGaaGilaiaaysW7cqaHbpGCcaaISaGaaGjbVlaahM hacaaMe8UaaGjbVJqaaiaa=5hacaaMe8UaaGjbVlaad6eadaWgaaWc baGaamyBaaqabaGccaaMc8UaaGikaiaahY7acaaISaGaaGjbVlaahI 6acaaIPaGaaGilaiaaywW7caaMf8UaaGzbVlaaywW7caaMf8Uaaiik aiaaiodacaGGUaGaaG4maiaacMcaaaa@6309@

Γ= ( X (2) T Δ 1 X (2) ) 1 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8rrps0l bbf9q8WrFfeuY=Hhbbf9G8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaGaaiaadaaakeaacaWHtoGaaGjbVJGabiab=1da9iaays W7caaIOaGaaCiwamaaDaaaleaacaaIOaGaaGOmaiaaiMcaaeaaruWq HXwAIjxAGWuANHgDaGabaiaa+rfaaaGccaaMc8UaaCiLdmaaCaaale qabaGaeyOeI0IaaGymaaaakiaaykW7caWHybWaaSbaaSqaaiaaiIca caaIYaGaaGykaaqabaGccaaIPaWaaWbaaSqabeaacqGHsislcaaIXa aaaOGaaiilaaaa@4D39@   γ=Γ X (2) T Δ 1 y (2) , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8rrps0l bbf9q8WrFfeuY=Hhbbf9G8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaGaaiaadaaakeaacaWHZoGaaGjbVlabg2da9iaaysW7ca WHtoGaaCiwamaaDaaaleaacaaIOaGaaGOmaiaaiMcaaeaaruWqHXwA IjxAGWuANHgDaGabaiaa=rfaaaGccaWHuoWaaWbaaSqabeaacqGHsi slcaaIXaaaaOGaaCyEamaaBaaaleaacaaIOaGaaGOmaiaaiMcaaeqa aOGaaiilaaaa@483C@   μ= y * ΨΩ( y * Xβ), MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8rrps0l bbf9q8WrFfeuY=Hhbbf9G8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaGaaiaadaaakeaacaWH8oGaaGypaiaahMhadaWgaaWcba GaaiOkaaqabaGccqGHsislcaWHOoGaaCyQdiaaykW7caaIOaGaaCyE amaaBaaaleaacaGGQaaabeaakiaaysW7cqGHsislcaaMe8UaaCiwai aahk7acaaIPaGaaiilaaaa@44AF@   y * = ( 0 m 1 T , y (2) T ) T , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8rrps0l bbf9q8WrFfeuY=Hhbbf9G8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaGaaiaadaaakeaacaWH5bWaaSbaaSqaaiaacQcaaeqaaO GaaGjbVlabg2da9iaaysW7caaIOaGaaCimamaaDaaaleaacaWGTbWa aSbaaWqaaiaaigdaaeqaaaWcbaqefmuySLMyYLgimL2zOrhaiqaaca WFubaaaOGaaGilaiaaysW7caWH5bWaa0baaSqaaiaaiIcacaaIYaGa aGykaaqaaiaa=rfaaaGccaaIPaWaaWbaaSqabeaacaWFubaaaOGaai ilaaaa@49EB@  et Ψ 1 = M T D (2) 1 M+Ω. MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8rrps0l bbf9q8WrFfeuY=Hhbbf9G8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaGaaiaadaaakeaacaWHOoWaaWbaaSqabeaacqGHsislca aIXaaaaOGaaGjbVlabg2da9iaaysW7caWHnbWaaWbaaSqabeaaruWq HXwAIjxAGWuANHgDaGabaiaa=rfaaaGccaaMc8UaaCiramaaDaaale aacaaIOaGaaGOmaiaaiMcaaeaacqGHsislcaaIXaaaaOGaaGPaVlaa h2eacaaMe8Uaey4kaSIaaGjbVlaahM6acaGGUaaaaa@4E59@  Par conséquent, nous pouvons obtenir un échantillon indépendant a posteriori par échantillonnage de rejet à partir de (3.1) et d’échantillonnages subséquents à partir de (3.2) et de (3.3). Pour les données sans région non échantillonnée, nous obtenons des procédures d’échantillonnage souhaitées en établissant que M= I m MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8rrps0l bbf9q8WrFfeuY=Hhbbf9G8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaGaaiaadaaakeGabaaVhiaah2eacaaMe8Uaeyypa0JaaG jbVlaahMeadaWgaaWcbaGaamyBaaqabaaaaa@3964@  et y * =y. MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8rrps0l bbf9q8WrFfeuY=Hhbbf9G8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaGaaiaadaaakeaacaWH5bWaaSbaaSqaaiaacQcaaeqaaO GaaGjbVlabg2da9iaaysW7caWH5bGaaiOlaaaa@3972@


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