Bayesian benchmarking of the Fay-Herriot model using random deletion
Section 2. Bayesian Fay-Herriot model

Assume that the observed data are ( θ ^ i , s i ) , i = 1, , l , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWaaeWaaeaacu aH4oqCgaqcamaaBaaaleaacaWGPbaabeaakiaaiYcacaaMe8Uaam4C amaaBaaaleaacaWGPbaabeaaaOGaayjkaiaawMcaaiaaiYcacaaMe8 UaamyAaiaai2dacaaIXaGaaGilaiaaysW7cqWIMaYscaaISaGaaGjb VlabloriSjaacYcaaaa@4B05@ where θ ^ i MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafqiUdeNbaK aadaWgaaWcbaGaamyAaaqabaaaaa@38D7@ and s i MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaam4CamaaBa aaleaacaWGPbaabeaaaaa@3809@ are respectively an estimate and its standard error (for simplicity, assumed known) of a quantity under study, e.g., the i th MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamyAamaaCa aaleqabaGaaeiDaiaabIgaaaaaaa@38F4@ area total θ i . MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiUde3aaS baaSqaaiaadMgaaeqaaOGaaiOlaaaa@3983@ The BFH model is

θ ^ i | θ i ind Normal ( θ i , s i 2 ) , MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWaaqGaaeaacu aH4oqCgaqcamaaBaaaleaacaWGPbaabeaakiaaykW7aiaawIa7aiaa ykW7cqaH4oqCdaWgaaWcbaGaamyAaaqabaGccaaMe8+aaybyaeqale qabaGaaeyAaiaab6gacaqGKbaabaqeeuuDJXwAKbsr4rNCHbacfaqc LbwacqWF8iIoaaGccaaMe8UaaeOtaiaab+gacaqGYbGaaeyBaiaabg gacaqGSbWaaeWaaeaacqaH4oqCdaWgaaWcbaGaamyAaaqabaGccaaI SaGaaGjbVlaadohadaqhaaWcbaGaamyAaaqaaiaaikdaaaaakiaawI cacaGLPaaacaaISaaaaa@5D10@

θ i | β , σ 2 ind Normal ( x i β , σ 2 ) , MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWaaqGaaeaacq aH4oqCdaWgaaWcbaGaamyAaaqabaGccaaMc8oacaGLiWoacaaMc8Ua aCOSdiaaiYcacaaMe8Uaeq4Wdm3aaWbaaSqabeaacaaIYaaaaOGaaG jbVpaawagabeWcbeqaaiaabMgacaqGUbGaaeizaaqaaebbfv3ySLgz GueE0jxyaGqbaKqzGfGae8hpIOdaaOGaaGjbVlaab6eacaqGVbGaae OCaiaab2gacaqGHbGaaeiBamaabmaabaGaaCiEamaaDaaaleaacaWG PbaabaqcLbwacWaGyBOmGikaaOGaaCOSdiaacYcacaaMe8Uaeq4Wdm 3aaWbaaSqabeaacaaIYaaaaaGccaGLOaGaayzkaaGaaGilaaaa@646D@

π ( β , σ 2 ) , ( 2.1 ) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiWda3aae WaaeaacaWHYoGaaiilaiaaysW7cqaHdpWCdaahaaWcbeqaaiaaikda aaaakiaawIcacaGLPaaacaaISaGaaGzbVlaaywW7caaMf8UaaGzbVl aaywW7caGGOaGaaGOmaiaac6cacaaIXaGaaiykaaaa@4B6B@

where i = 1, , l , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamyAaiaai2 dacaaIXaGaaGilaiaaysW7cqWIMaYscaaISaGaaGjbVlabloriSjaa cYcaaaa@3FF0@ x i MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaaCiEamaaBa aaleaacaWGPbaabeaaaaa@3812@ are a set of covariates with p MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamiCaaaa@36EC@ components (including intercept) and π ( β , σ 2 ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiWda3aae WaaeaacaWHYoGaaiilaiaaysW7cqaHdpWCdaahaaWcbeqaaiaaikda aaaakiaawIcacaGLPaaaaaa@3F6E@ is the joint prior distribution for ( β , δ 2 ) . MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWaaeWaaeaaca WHYoGaaiilaiaaysW7cqaH0oazdaahaaWcbeqaaiaaikdaaaaakiaa wIcacaGLPaaacaGGUaaaaa@3E45@ A priori it is assumed that π ( β , σ 2 ) = π ( β ) π ( σ 2 ) , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiWda3aae WaaeaacaWHYoGaaiilaiaaysW7cqaHdpWCdaahaaWcbeqaaiaaikda aaaakiaawIcacaGLPaaacqGH9aqpcqaHapaCdaqadaqaaiaahk7aai aawIcacaGLPaaacqaHapaCdaqadaqaaiabeo8aZnaaCaaaleqabaGa aGOmaaaaaOGaayjkaiaawMcaaiaacYcaaaa@4BA4@ i.e., β MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaaCOSdaaa@3735@ and σ 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeq4Wdm3aaW baaSqabeaacaaIYaaaaaaa@38A3@ are independent, with

π ( β ) 1 and π ( σ 2 ) = 1 / ( 1 + σ 2 ) 2 . ( 2.2 ) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiWda3aae WaaeaacaWHYoaacaGLOaGaayzkaaGaeyyhIuRaaGymaiaaywW7caqG HbGaaeOBaiaabsgacaaMf8UaeqiWda3aaeWaaeaacqaHdpWCdaahaa WcbeqaaiaaikdaaaaakiaawIcacaGLPaaacaaI9aWaaSGbaeaacaaI XaaabaWaaeWaaeaacaaIXaGaey4kaSIaeq4Wdm3aaWbaaSqabeaaca aIYaaaaaGccaGLOaGaayzkaaWaaWbaaSqabeaacaaIYaaaaaaakiaa c6cacaaMf8UaaGzbVlaaywW7caaMf8UaaGzbVlaacIcacaaIYaGaai OlaiaaikdacaGGPaaaaa@5CEB@

By Bayes’ theorem, the joint posterior density of l + p + 1 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeS4eHWMaey 4kaSIaamiCaiabgUcaRiaaigdaaaa@3A9C@ model parameters is

π ( θ , β , σ 2 | θ ^ ) 1 ( 1 + σ 2 ) 2 ( 1 σ 2 ) l / 2 i = 1 l { exp [ 1 2 { 1 s i 2 ( θ ^ i θ i ) 2 + 1 σ 2 ( θ i x i β ) 2 } ] } . ( 2.3 ) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiWda3aae WaaeaacaWH4oGaaGilaiaaysW7caWHYoGaaGilaiaaysW7daabcaqa aiabeo8aZnaaCaaaleqabaGaaGOmaaaakiaaykW7aiaawIa7aiaayk W7ceWH4oGbaKaaaiaawIcacaGLPaaacqGHDisTdaWcaaqaaiaaigda aeaadaqadaqaaiaaigdacqGHRaWkcqaHdpWCdaahaaWcbeqaaiaaik daaaaakiaawIcacaGLPaaadaahaaWcbeqaaiaaikdaaaaaaOWaaeWa aeaadaWcaaqaaiaaigdaaeaacqaHdpWCdaahaaWcbeqaaiaaikdaaa aaaaGccaGLOaGaayzkaaWaaWbaaSqabeaadaWcgaqaaiabloriSbqa aiaaikdaaaaaaOWaaebCaeqaleaacaWGPbGaaGypaiaaigdaaeaacq WItecBa0Gaey4dIunakmaacmaabaGaciyzaiaacIhacaGGWbWaamWa aeaacqGHsisldaWcaaqaaiaaigdaaeaacaaIYaaaamaacmaabaWaaS aaaeaacaaIXaaabaGaam4CamaaDaaaleaacaWGPbaabaGaaGOmaaaa aaGcdaqadaqaaiqbeI7aXzaajaWaaSbaaSqaaiaadMgaaeqaaOGaey OeI0IaeqiUde3aaSbaaSqaaiaadMgaaeqaaaGccaGLOaGaayzkaaWa aWbaaSqabeaacaaIYaaaaOGaey4kaSYaaSaaaeaacaaIXaaabaGaeq 4Wdm3aaWbaaSqabeaacaaIYaaaaaaakmaabmaabaGaeqiUde3aaSba aSqaaiaadMgaaeqaaOGaeyOeI0IaaCiEamaaDaaaleaacaWGPbaaba qcLbwacWaGyBOmGikaaOGaaCOSdaGaayjkaiaawMcaamaaCaaaleqa baGaaGOmaaaaaOGaay5Eaiaaw2haaaGaay5waiaaw2faaiaaykW7ai aawUhacaGL9baacaaIUaGaaGzbVlaaywW7caGGOaGaaGOmaiaac6ca caaIZaGaaiykaaaa@9245@

In (2.2), π ( σ 2 ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiWda3aae WaaeaacqaHdpWCdaahaaWcbeqaaiaaikdaaaaakiaawIcacaGLPaaa aaa@3BF3@ is a proper prior distribution, flatter than π ( σ 2 ) 1 / σ 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiWda3aae WaaeaacqaHdpWCdaahaaWcbeqaaiaaikdaaaaakiaawIcacaGLPaaa cqGHDisTdaWcgaqaaiaaigdaaeaacqaHdpWCdaahaaWcbeqaaiaaik daaaaaaaaa@40F0@ near zero, with no moments. In fact, any proper prior for σ 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeq4Wdm3aaW baaSqabeaacaaIYaaaaaaa@38A3@ is fine; an improper prior on σ 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeq4Wdm3aaW baaSqabeaacaaIYaaaaaaa@38A3@ may lead to improper posterior density. Because π ( β ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiWda3aae WaaeaacaWHYoaacaGLOaGaayzkaaaaaa@3A7B@ is improper, the product π ( β , σ 2 ) = π ( β ) π ( σ 2 ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiWda3aae WaaeaacaWHYoGaaiilaiaaysW7cqaHdpWCdaahaaWcbeqaaiaaikda aaaakiaawIcacaGLPaaacqGH9aqpcqaHapaCdaqadaqaaiaahk7aai aawIcacaGLPaaacqaHapaCdaqadaqaaiabeo8aZnaaCaaaleqabaGa aGOmaaaaaOGaayjkaiaawMcaaaaa@4AF4@ is improper, and this could cause the joint posterior density of ( θ , β , σ 2 ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWaaeWaaeaaca WH4oGaaiilaiaaysW7caWHYoGaaiilaiaaysW7cqaHdpWCdaahaaWc beqaaiaaikdaaaaakiaawIcacaGLPaaaaaa@4132@ to be improper, an undesirable scenario. Theorem 1 below establishes the propriety of the joint posterior density (2.3).

More details about the BFH model are presented in Appendix B. Specifically, letting λ i = σ 2 s i 2 + σ 2 , i = 1, , l , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeq4UdW2aaS baaSqaaiaadMgaaeqaaOGaaGypamaaleaaleaacqaHdpWCdaahaaad beqaaiaaikdaaaaaleaacaWGZbWaa0baaWqaaiaadMgaaeaacaaIYa aaaSGaey4kaSIaeq4Wdm3aaWbaaWqabeaacaaIYaaaaaaakiaaiYca caaMe8UaamyAaiaai2dacaaIXaGaaGilaiaaysW7cqWIMaYscaaISa GaaGjbVlabloriSjaacYcaaaa@4F1A@ we have shown that

θ i | β , σ 2 , θ ^ ind Normal { λ i θ ^ i + ( 1 λ i ) x i β , ( 1 λ i ) σ 2 } , i = 1, , l , ( 2.4 ) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWaaqGaaeaacq aH4oqCdaWgaaWcbaGaamyAaaqabaGccaaMc8oacaGLiWoacaaMc8Ua aCOSdiaaiYcacaaMe8Uaeq4Wdm3aaWbaaSqabeaacaaIYaaaaOGaaG ilaiaaysW7ceWH4oGbaKaacaaMe8+aaybyaeqaleqabaGaaeyAaiaa b6gacaqGKbaabaqeeuuDJXwAKbsr4rNCHbacfaqcLbwacqWF8iIoaa GccaaMe8UaaeOtaiaab+gacaqGYbGaaeyBaiaabggacaqGSbWaaiWa aeaacqaH7oaBdaWgaaWcbaGaamyAaaqabaGccuaH4oqCgaqcamaaBa aaleaacaWGPbaabeaakiabgUcaRmaabmaabaGaaGymaiabgkHiTiab eU7aSnaaBaaaleaacaWGPbaabeaaaOGaayjkaiaawMcaaiaahIhada qhaaWcbaGaamyAaaqaaKqzGfGamai2gkdiIcaakiaahk7acaaISaGa aGjbVpaabmaabaGaaGymaiabgkHiTiabeU7aSnaaBaaaleaacaWGPb aabeaaaOGaayjkaiaawMcaaiabeo8aZnaaCaaaleqabaGaaGOmaaaa aOGaay5Eaiaaw2haaiaaiYcacaaMe8UaamyAaiaai2dacaaIXaGaaG ilaiaaysW7cqWIMaYscaaISaGaaGjbVlabloriSjaaiYcacaaMf8Ua aGzbVlaaywW7caaMf8UaaGzbVlaacIcacaaIYaGaaiOlaiaaisdaca GGPaaaaa@923F@

β | σ 2 , θ ^ Normal ( β ^ , Σ ^ ) , ( 2.5 ) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWaaqGaaeaaca WHYoGaaGPaVdGaayjcSdGaaGPaVlabeo8aZnaaCaaaleqabaGaaGOm aaaakiaaiYcacaaMe8UabCiUdyaajaqeeuuDJXwAKbsr4rNCHbacfa Gae8hpIOJaaeOtaiaab+gacaqGYbGaaeyBaiaabggacaqGSbWaaeWa aeaaceWHYoGbaKaacaGGSaGaaGjbVlqbfo6atzaajaaacaGLOaGaay zkaaGaaGilaiaaywW7caaMf8UaaGzbVlaaywW7caaMf8Uaaiikaiaa ikdacaGGUaGaaGynaiaacMcaaaa@600B@

π 3 ( σ 2 | θ ^ ) Q ( σ 2 ) 1 ( 1 + σ 2 ) 2 , ( 2.6 ) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiWda3aaS baaSqaaiaaiodaaeqaaOWaaeWaaeaadaabcaqaaiabeo8aZnaaCaaa leqabaGaaGOmaaaakiaaykW7aiaawIa7aiaaykW7ceWH4oGbaKaaai aawIcacaGLPaaacqGHDisTcaWGrbWaaeWaaeaacqaHdpWCdaahaaWc beqaaiaaikdaaaaakiaawIcacaGLPaaadaWcaaqaaiaaigdaaeaada qadaqaaiaaigdacqGHRaWkcqaHdpWCdaahaaWcbeqaaiaaikdaaaaa kiaawIcacaGLPaaadaahaaWcbeqaaiaaikdaaaaaaOGaaGilaiaayw W7caaMf8UaaGzbVlaaywW7caaMf8UaaiikaiaaikdacaGGUaGaaGOn aiaacMcaaaa@5D17@

where

β ^ = Σ ^ i = 1 l θ ^ i x i s i 2 + σ 2 , Σ ^ 1 = i = 1 l x i x i s i 2 + σ 2 , MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGabCOSdyaaja GaaGypaiqbfo6atzaajaWaaabCaeqaleaacaWGPbGaaGypaiaaigda aeaacqWItecBa0GaeyyeIuoakmaalaaabaGafqiUdeNbaKaadaWgaa WcbaGaamyAaaqabaGccaWH4bWaaSbaaSqaaiaadMgaaeqaaaGcbaGa am4CamaaDaaaleaacaWGPbaabaGaaGOmaaaakiabgUcaRiabeo8aZn aaCaaaleqabaGaaGOmaaaaaaGccaaISaGaaGjbVlqbfo6atzaajaWa aWbaaSqabeaacqGHsislcaaIXaaaaOGaaGypamaaqahabeWcbaGaam yAaiaai2dacaaIXaaabaGaeS4eHWganiabggHiLdGcdaWcaaqaaiaa hIhadaWgaaWcbaGaamyAaaqabaGccaWH4bWaa0baaSqaaiaadMgaae aajugybiadaITHYaIOaaaakeaacaWGZbWaa0baaSqaaiaadMgaaeaa caaIYaaaaOGaey4kaSIaeq4Wdm3aaWbaaSqabeaacaaIYaaaaaaaki aaiYcaaaa@66B9@

Q ( σ 2 ) = | Σ ^ | 1 / 2 i = 1 l 1 ( s i 2 + σ 2 ) 1 / 2 exp { 1 2 i = 1 l 1 s i 2 + σ 2 ( θ ^ i x i β ^ ) 2 } . MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamyuamaabm aabaGaeq4Wdm3aaWbaaSqabeaacaaIYaaaaaGccaGLOaGaayzkaaGa aGypamaaemaabaGaaGPaVlqbfo6atzaajaGaaGPaVdGaay5bSlaawI a7amaaCaaaleqabaGaaGymaiaai+cacaaIYaaaaOWaaebCaeqaleaa caWGPbGaaGypaiaaigdaaeaacqWItecBa0Gaey4dIunakmaalaaaba GaaGymaaqaamaabmaabaGaam4CamaaDaaaleaacaWGPbaabaGaaGOm aaaakiabgUcaRiabeo8aZnaaCaaaleqabaGaaGOmaaaaaOGaayjkai aawMcaamaaCaaaleqabaWaaSGbaeaacaaIXaaabaGaaGOmaaaaaaaa aOGaciyzaiaacIhacaGGWbWaaiWaaeaacqGHsisldaWcaaqaaiaaig daaeaacaaIYaaaamaaqahabeWcbaGaamyAaiaai2dacaaIXaaabaGa eS4eHWganiabggHiLdGcdaWcaaqaaiaaigdaaeaacaWGZbWaa0baaS qaaiaadMgaaeaacaaIYaaaaOGaey4kaSIaeq4Wdm3aaWbaaSqabeaa caaIYaaaaaaakmaabmaabaGafqiUdeNbaKaadaWgaaWcbaGaamyAaa qabaGccqGHsislcaWH4bWaa0baaSqaaiaadMgaaeaajugybiadaITH YaIOaaGcceWHYoGbaKaaaiaawIcacaGLPaaadaahaaWcbeqaaiaaik daaaaakiaawUhacaGL9baacaaIUaaaaa@7943@

Theorem 1

The joint posterior density (2.3) is proper provided the design matrix is full rank.

Proof of Theorem 1

Because the design matrix is full rank, β ^ MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGabCOSdyaaja aaaa@3745@ and Σ ^ MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafu4OdmLbaK aaaaa@378B@ are well defined for all σ 2 . MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeq4Wdm3aaW baaSqabeaacaaIYaaaaOGaaiOlaaaa@395F@ This implies that Q ( σ 2 ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamyuamaabm aabaGaeq4Wdm3aaWbaaSqabeaacaaIYaaaaaGccaGLOaGaayzkaaaa aa@3B0C@ is bounded in σ 2 . MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeq4Wdm3aaW baaSqabeaacaaIYaaaaOGaaiOlaaaa@395F@ Therefore, as π ( σ 2 ) = 1 ( 1 + σ 2 ) 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiWda3aae WaaeaacqaHdpWCdaahaaWcbeqaaiaaikdaaaaakiaawIcacaGLPaaa cqGH9aqpdaWcbaWcbaGaaGymaaqaamaabmaabaGaaGymaiabgUcaRi abeo8aZnaaCaaameqabaGaaGOmaaaaaSGaayjkaiaawMcaamaaCaaa meqabaGaaGOmaaaaaaaaaa@4498@ is proper, the posterior density π 3 ( σ 2 | θ ^ ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiWda3aaS baaSqaaiaaiodaaeqaaOWaaeWaaeaadaabcaqaaiabeo8aZnaaCaaa leqabaGaaGOmaaaakiaaykW7aiaawIa7aiaaykW7ceWH4oGbaKaaai aawIcacaGLPaaaaaa@42E6@ is proper. Then, by applying the multiplication rule of probability, it follows that the joint posterior density, π ( θ , β , σ 2 | θ ^ ) , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiWda3aae WaaeaacaWH4oGaaiilaiaaysW7caWHYoGaaiilaiaaysW7daabcaqa aiabeo8aZnaaCaaaleqabaGaaGOmaaaakiaaykW7aiaawIa7aiaayk W7ceWH4oGbaKaaaiaawIcacaGLPaaacaGGSaaaaa@499F@ is proper.

With propriety assured, sampling from the joint posterior density and inference about θ i MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiUde3aaS baaSqaaiaadMgaaeqaaaaa@38C7@ can be achieved through a simple Monte Carlo procedure. Using the multiplication rule and drawing samples from (2.6), (2.5) and (2.4), the procedure follows. First, draw a sample from π 3 ( σ 2 | θ ^ ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiWda3aaS baaSqaaiaaiodaaeqaaOWaaeWaaeaadaabcaqaaiabeo8aZnaaCaaa leqabaGaaGOmaaaakiaaykW7aiaawIa7aiaaykW7ceWH4oGbaKaaai aawIcacaGLPaaaaaa@42E6@ in (2.6). Draws from this distribution can be made using a grid method; see Appendix B. It is then easy to draw samples from the conditional posterior density of β MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaaCOSdaaa@3735@ in (2.5). Finally, samples of the θ i MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiUde3aaS baaSqaaiaadMgaaeqaaaaa@38C7@ can be drawn independently from (2.4). Sampling in this manner from the joint posterior density under the unconstrained BFH model does not need monitoring (unlike Markov chain Monte Carlo methods). The unconstrained BFH model will provide a basis for comparison of the estimates and related measures of uncertainty obtained under the proposed random deletion benchmarking method.


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