Bayesian benchmarking of the Fay-Herriot model using random deletion
Section 5. Concluding remarks

The Bayesian Fay-Herriot (BFH) model is discussed in detail. We show that the BFH can be fit using random samples rather than a Markov chain Monte Carlo sampler. Since random samples required no monitoring, this method is beneficial because there is little time at NASS between receiving the county-level survey summary data and presenting the final estimates. In support to the BFH model, we show that the posterior density under the BFH model is proper, providing a baseline for benchmarking. The effects of benchmarking are studied in a simulation study, comparing the BFH model without benchmarking to the BFH model with two benchmarking methods.

In this study, we assume that the benchmarking constraint is of the form i = 1 l θ i = a . MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWaaabmaeaacq aH4oqCdaWgaaWcbaGaamyAaaqabaGccqGH9aqpcaWGHbGaaiOlaaWc baGaamyAaiabg2da9iaaigdaaeaacqWItecBa0GaeyyeIuoaaaa@4151@ A straightforward generalization of the benchmarking methods may be developed for the constraint of the form i = 1 l w i θ i = a , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWaaabmaeaaca WG3bWaaSbaaSqaaiaadMgaaeqaaOGaeqiUde3aaSbaaSqaaiaadMga aeqaaOGaeyypa0JaamyyaiaacYcaaSqaaiaadMgacqGH9aqpcaaIXa aabaGaeS4eHWganiabggHiLdaaaa@436F@ where the w i MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaam4DamaaBa aaleaacaWGPbaabeaaaaa@380D@ are weights. For example, this latter situation occurs for benchmarking yield, ratio of production and harvested acres.

Our major contribution is the extension of BFH model to accommodate benchmarking. Previous approaches delete the last area, giving rise to the question “Does it matter which area is deleted?”. In this paper, we develop and illustrate a method that gives each area a chance to be deleted. We show how to fit this extended BFH model using the Gibbs sampler. Because of the complexity of the joint posterior density, a sampling based method, without Markov chains, cannot be used. Using empirical studies, we show that the differences in the posterior means over no benchmarking, deleting the last county and random deletion are very small.

The effects of changing the benchmarking target are studied in a sensitivity analysis. As expected, changing the benchmarking target leads to different estimates, but, unexpectedly, the changes in the posterior standard deviations are small. Small changes in the estimates are noted for the benchmarking methods using different probabilities of deletion.

It is expected that the posterior standard deviations from deleting the last one benchmarking and random benchmarking be larger than those from the BFH model because of the jittering effect from benchmarking. However, in the empirical studies we present, deleting the last one benchmarking and random benchmarking have about the same posterior standard deviations with a small reduction when random benchmarking is used. The key strength of the random benchmarking approach is that there is no preferential treatment for any area/county.

Disclaimer and acknowledgements

The Findings and Conclusions in This Preliminary Publication Have Not Been Formally Disseminated by the U.S. Department of Agriculture and Should Not Be Construed to Represent Any Agency Determination or Policy. This research was supported in part by the intramural research program of the U.S. Department of Agriculture, National Agriculture Statistics Service.

Dr. Nandram’s work was supported by a grant from the Simons Foundation (353953, Balgobin Nandram). The authors thank the Associate Editor and the referees for their comments and suggestions. The work of Erciulescu was completed as a Research Associate at the National Institute of Statistical Sciences (NISS) working on NASS projects.

Appendix A

Exemplification of the sensitivity of deletion

Let y i ind Normal ( μ i , σ i 2 ) , i = 1 , 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamyEamaaBa aaleaacaWGPbaabeaakiaaysW7daGfGbqabSqabeaacaqGPbGaaeOB aiaabsgaaeaarqqr1ngBPrgifHhDYfgaiuaajugybiab=XJi6aaaki aaysW7caqGobGaae4BaiaabkhacaqGTbGaaeyyaiaabYgadaqadaqa aiabeY7aTnaaBaaaleaacaWGPbaabeaakiaacYcacaaMe8Uaeq4Wdm 3aa0baaSqaaiaadMgaaeaacaaIYaaaaaGccaGLOaGaayzkaaGaaiil aiaaysW7caWGPbGaeyypa0JaaGymaiaacYcacaaMe8UaaGOmaiaacY caaaa@5D67@ such that y 1 + y 2 = a , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamyEamaaBa aaleaacaaIXaaabeaakiabgUcaRiaadMhadaWgaaWcbaGaaGOmaaqa baGccqGH9aqpcaWGHbGaaiilaaaa@3D54@ and λ = σ 2 2 / ( σ 1 2 + σ 2 2 ) . MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeq4UdWMaey ypa0ZaaSGbaeaacqaHdpWCdaqhaaWcbaGaaGOmaaqaaiaaikdaaaaa keaadaqadaqaaiabeo8aZnaaDaaaleaacaaIXaaabaGaaGOmaaaaki abgUcaRiabeo8aZnaaDaaaleaacaaIYaaabaGaaGOmaaaaaOGaayjk aiaawMcaaaaacaGGUaaaaa@4639@ Then, if we start by deleting y 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamyEamaaBa aaleaacaaIYaaabeaakiaacYcaaaa@3897@ the joint density of ( y 1 , y 2 ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWaaeWaaeaaca WG5bWaaSbaaSqaaiaaigdaaeqaaOGaaiilaiaaysW7caWG5bWaaSba aSqaaiaaikdaaeqaaaGccaGLOaGaayzkaaaaaa@3D9C@ is

f ( y 1 , y 2 | ϕ = 0 ) = δ y 2 ( a y 1 ) Normal { λ μ 1 + ( 1 λ ) ( a μ 2 ) , ( 1 λ ) σ 2 2 } , MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamOzamaabm aabaGaamyEamaaBaaaleaacaaIXaaabeaakiaacYcacaaMe8+aaqGa aeaacaWG5bWaaSbaaSqaaiaaikdaaeqaaOGaaGPaVdGaayjcSdGaaG PaVlabew9aMjabg2da9iaaicdaaiaawIcacaGLPaaacqGH9aqpcqaH 0oazdaWgaaWcbaGaamyEaiaaikdaaeqaaOWaaeWaaeaacaWGHbGaey OeI0IaamyEamaaBaaaleaacaaIXaaabeaaaOGaayjkaiaawMcaaiaa b6eacaqGVbGaaeOCaiaab2gacaqGHbGaaeiBamaacmaabaGaeq4UdW 2aaSbaaSqaaiabeY7aTnaaBaaameaacaaIXaaabeaaaSqabaGccqGH RaWkdaqadaqaaiaaigdacqGHsislcqaH7oaBaiaawIcacaGLPaaada qadaqaaiaadggacqGHsislcqaH8oqBdaWgaaWcbaGaaGOmaaqabaaa kiaawIcacaGLPaaacaGGSaGaaGjbVpaabmaabaGaaGymaiabgkHiTi abeU7aSbGaayjkaiaawMcaaiabeo8aZnaaDaaaleaacaaIYaaabaGa aGOmaaaaaOGaay5Eaiaaw2haaiaacYcaaaa@73EE@

where δ a ( b ) = 1 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiTdq2aaS baaSqaaiaadggaaeqaaOWaaeWaaeaacaWGIbaacaGLOaGaayzkaaGa eyypa0JaaGymaaaa@3CE9@ if a = b MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamyyaiabg2 da9iaadkgaaaa@38CA@ and δ a ( b ) = 0 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiTdq2aaS baaSqaaiaadggaaeqaaOWaaeWaaeaacaWGIbaacaGLOaGaayzkaaGa eyypa0JaaGimaaaa@3CE8@ if a b . MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamyyaiabgc Mi5kaadkgacaGGUaaaaa@3A3D@ However, if we start by deleting y 1 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamyEamaaBa aaleaacaaIXaaabeaakiaacYcaaaa@3896@ the joint density of ( y 1 , y 2 ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWaaeWaaeaaca WG5bWaaSbaaSqaaiaaigdaaeqaaOGaaiilaiaaysW7caWG5bWaaSba aSqaaiaaikdaaeqaaaGccaGLOaGaayzkaaaaaa@3D9C@ is

g ( y 1 , y 2 | ϕ = 0 ) = δ y 1 ( a y 2 ) Normal { λ ( a μ 1 ) + ( 1 λ ) μ 2 , ( 1 λ ) σ 2 2 } . MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaam4zamaabm aabaGaamyEamaaBaaaleaacaaIXaaabeaakiaacYcacaaMe8+aaqGa aeaacaWG5bWaaSbaaSqaaiaaikdaaeqaaOGaaGPaVdGaayjcSdGaaG PaVlabew9aMjabg2da9iaaicdaaiaawIcacaGLPaaacqGH9aqpcqaH 0oazdaWgaaWcbaGaamyEaiaaigdaaeqaaOWaaeWaaeaacaWGHbGaey OeI0IaamyEamaaBaaaleaacaaIYaaabeaaaOGaayjkaiaawMcaaiaa b6eacaqGVbGaaeOCaiaab2gacaqGHbGaaeiBamaacmaabaGaeq4UdW 2aaeWaaeaacaWGHbGaeyOeI0IaeqiVd02aaSbaaSqaaiaaigdaaeqa aaGccaGLOaGaayzkaaGaey4kaSYaaeWaaeaacaaIXaGaeyOeI0Iaeq 4UdWgacaGLOaGaayzkaaGaeqiVd02aaSbaaSqaaiaaikdaaeqaaOGa aiilaiaaysW7daqadaqaaiaaigdacqGHsislcqaH7oaBaiaawIcaca GLPaaacqaHdpWCdaqhaaWcbaGaaGOmaaqaaiaaikdaaaaakiaawUha caGL9baacaGGUaaaaa@73B9@

It will matter in the estimation procedure which variable is deleted because the two joint distributions are different. Note that the two distributions are the same if and only if

λ μ 1 + ( 1 λ ) ( a μ 2 ) = λ ( a μ 1 ) + ( 1 λ ) μ 2 , MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeq4UdWMaeq iVd02aaSbaaSqaaiaaigdaaeqaaOGaey4kaSYaaeWaaeaacaaIXaGa eyOeI0Iaeq4UdWgacaGLOaGaayzkaaWaaeWaaeaacaWGHbGaeyOeI0 IaeqiVd02aaSbaaSqaaiaaikdaaeqaaaGccaGLOaGaayzkaaGaeyyp a0Jaeq4UdW2aaeWaaeaacaWGHbGaeyOeI0IaeqiVd02aaSbaaSqaai aaigdaaeqaaaGccaGLOaGaayzkaaGaey4kaSYaaeWaaeaacaaIXaGa eyOeI0Iaeq4UdWgacaGLOaGaayzkaaGaeqiVd02aaSbaaSqaaiaaik daaeqaaOGaaiilaaaa@57F8@

which gives

λ ( μ 1 a / 2 ) = ( 1 λ ) ( μ 2 a / 2 ) . MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeq4UdW2aae WaaeaacqaH8oqBdaWgaaWcbaGaaGymaaqabaGccqGHsisldaWcgaqa aiaadggaaeaacaaIYaaaaaGaayjkaiaawMcaaiabg2da9maabmaaba GaaGymaiabgkHiTiabeU7aSbGaayjkaiaawMcaamaabmaabaGaeqiV d02aaSbaaSqaaiaaikdaaeqaaOGaeyOeI0YaaSGbaeaacaWGHbaaba GaaGOmaaaaaiaawIcacaGLPaaacaGGUaaaaa@4BF2@

Even if we assume that σ 1 2 = σ 2 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeq4Wdm3aa0 baaSqaaiaaigdaaeaacaaIYaaaaOGaeyypa0Jaeq4Wdm3aa0baaSqa aiaaikdaaeaacaaIYaaaaOGaaiilaaaa@3E90@ the two distributions are different. However, under this assumption, λ = 1 / 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeq4UdWMaey ypa0ZaaSGbaeaacaaIXaaabaGaaGOmaaaacaGGSaaaaa@3AEE@ and the condition for the two distributions to be the same is that μ 1 = μ 2 . MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiVd02aaS baaSqaaiaaigdaaeqaaOGaeyypa0JaeqiVd02aaSbaaSqaaiaaikda aeqaaOGaaiOlaaaa@3CFE@ That is, overall the condition for the two joint distributions to be the same is that μ 1 = μ 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiVd02aaS baaSqaaiaaigdaaeqaaOGaeyypa0JaeqiVd02aaSbaaSqaaiaaikda aeqaaaaa@3C42@ and σ 1 = σ 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeq4Wdm3aaS baaSqaaiaaigdaaeqaaOGaeyypa0Jaeq4Wdm3aaSbaaSqaaiaaikda aeqaaOGaaiilaaaa@3D16@ thereby making y 1 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamyEamaaBa aaleaacaaIXaaabeaaaaa@37DC@ and y 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamyEamaaBa aaleaacaaIYaaabeaaaaa@37DD@ exchangeable. However, this is a very restricted situation.

One way out of this diffculty is to actually delete both y 1 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamyEamaaBa aaleaacaaIXaaabeaaaaa@37DC@ and y 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamyEamaaBa aaleaacaaIYaaabeaaaaa@37DD@ in the following way. Let z = 1 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamOEaiabg2 da9iaaigdaaaa@38B7@ if y 1 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamyEamaaBa aaleaacaaIXaaabeaaaaa@37DC@ is deleted and let z = 0 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamOEaiabg2 da9iaaicdaaaa@38B6@ if y 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamyEamaaBa aaleaacaaIYaaabeaaaaa@37DD@ is deleted. Then,

p ( y 1 , y 2 , z | ϕ = 0 ) = [ p g ( y 1 , y 2 | ϕ = 0 ) ] z [ ( 1 p ) f ( y 1 , y 2 | ϕ = 0 ) ] 1 z , MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamiCamaabm aabaGaamyEamaaBaaaleaacaaIXaaabeaakiaacYcacaaMe8UaamyE amaaBaaaleaacaaIYaaabeaakiaacYcacaaMe8+aaqGaaeaacaWG6b GaaGPaVdGaayjcSdGaaGPaVlabew9aMjabg2da9iaaicdaaiaawIca caGLPaaacqGH9aqpdaWadaqaaiaadchacaWGNbWaaeWaaeaacaWG5b WaaSbaaSqaaiaaigdaaeqaaOGaaiilaiaaysW7daabcaqaaiaadMha daWgaaWcbaGaaGOmaaqabaGccaaMc8oacaGLiWoacaaMc8Uaeqy1dy Maeyypa0JaaGimaaGaayjkaiaawMcaaaGaay5waiaaw2faamaaCaaa leqabaGaamOEaaaakmaadmaabaWaaeWaaeaacaaIXaGaeyOeI0Iaam iCaaGaayjkaiaawMcaaiaadAgadaqadaqaaiaadMhadaWgaaWcbaGa aGymaaqabaGccaGGSaGaaGjbVpaaeiaabaGaamyEamaaBaaaleaaca aIYaaabeaakiaaykW7aiaawIa7aiaaykW7cqaHvpGzcqGH9aqpcaaI WaaacaGLOaGaayzkaaaacaGLBbGaayzxaaWaaWbaaSqabeaacaaIXa GaeyOeI0IaamOEaaaakiaacYcaaaa@7A52@

where we have taken z Bernoulli ( p ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamOEaebbfv 3ySLgzGueE0jxyaGqbaiab=XJi6iaabkeacaqGLbGaaeOCaiaab6ga caqGVbGaaeyDaiaabYgacaqGSbGaaeyAamaabmaabaGaamiCaaGaay jkaiaawMcaaaaa@4774@ and, because z MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamOEaaaa@36F6@ is not really identifiable, we will take p = 1 / 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamiCaiabg2 da9maalyaabaGaaGymaaqaaiaaikdaaaaaaa@397F@ (i.e., we randomly delete one or the other). However, note that

z | y 1 , y 2 , ϕ = 0 Bernoulli { p g ( y 1 , y 2 | ϕ = 0 ) [ p g ( y 1 , y 2 | ϕ = 0 ) ] + [ ( 1 p ) f ( y 1 , y 2 | ϕ = 0 ) ] } . MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWaaqGaaeaaca WG6bGaaGPaVdGaayjcSdGaaGPaVlaadMhadaWgaaWcbaGaaGymaaqa baGccaGGSaGaaGjbVlaadMhadaWgaaWcbaGaaGOmaaqabaGccaGGSa GaaGjbVlabew9aMjabg2da9iaaicdarqqr1ngBPrgifHhDYfgaiuaa cqWF8iIocaqGcbGaaeyzaiaabkhacaqGUbGaae4BaiaabwhacaqGSb GaaeiBaiaabMgadaGadaqaamaalaaabaGaamiCaiaadEgadaqadaqa aiaadMhadaWgaaWcbaGaaGymaaqabaGccaGGSaGaaGjbVpaaeiaaba GaamyEamaaBaaaleaacaaIYaaabeaakiaaykW7aiaawIa7aiaaykW7 cqaHvpGzcqGH9aqpcaaIWaaacaGLOaGaayzkaaaabaWaamWaaeaaca WGWbGaam4zamaabmaabaGaamyEamaaBaaaleaacaaIXaaabeaakiaa cYcacaaMe8+aaqGaaeaacaWG5bWaaSbaaSqaaiaaikdaaeqaaOGaaG PaVdGaayjcSdGaaGPaVlabew9aMjabg2da9iaaicdaaiaawIcacaGL PaaaaiaawUfacaGLDbaacqGHRaWkdaWadaqaamaabmaabaGaaGymai abgkHiTiaadchaaiaawIcacaGLPaaacaWGMbWaaeWaaeaacaWG5bWa aSbaaSqaaiaaigdaaeqaaOGaaiilaiaaysW7daabcaqaaiaadMhada WgaaWcbaGaaGOmaaqabaGccaaMc8oacaGLiWoacaaMc8Uaeqy1dyMa eyypa0JaaGimaaGaayjkaiaawMcaaaGaay5waiaaw2faaaaaaiaawU hacaGL9baacaGGUaaaaa@9599@

Appendix B

Fitting the Bayesian Fay-Herriot model

The Bayesian Fay-Herriot (BFH) model is given in (2.1) and the joint posterior density under the BFH model is given in (2.3), which for convenience we state here,

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 } ] } . ( B .1 ) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiWda3aae WaaeaacaWH4oGaaiilaiaaysW7caWHYoGaaiilaiaaysW7daabcaqa aiabeo8aZnaaCaaaleqabaGaaGOmaaaakiaaykW7aiaawIa7aiaayk W7ceWH4oGbaKaaaiaawIcacaGLPaaacqGHDisTdaWcaaqaaiaaigda aeaadaqadaqaaiaaigdacqGHRaWkcqaHdpWCdaahaaWcbeqaaiaaik daaaaakiaawIcacaGLPaaadaahaaWcbeqaaiaaikdaaaaaaOWaaeWa aeaadaWcaaqaaiaaigdaaeaacqaHdpWCdaahaaWcbeqaaiaaikdaaa aaaaGccaGLOaGaayzkaaWaaWbaaSqabeaadaWcgaqaaiabloriSbqa aiaaikdaaaaaaOWaaebCaeaadaGadaqaaiGacwgacaGG4bGaaiiCam aadmaabaGaeyOeI0YaaSaaaeaacaaIXaaabaGaaGOmaaaadaGadaqa amaalaaabaGaaGymaaqaaiaadohadaqhaaWcbaGaamyAaaqaaiaaik daaaaaaOWaaeWaaeaacuaH4oqCgaqcamaaBaaaleaacaWGPbaabeaa kiabgkHiTiabeI7aXnaaBaaaleaacaWGPbaabeaaaOGaayjkaiaawM caamaaCaaaleqabaGaaGOmaaaakiabgUcaRmaalaaabaGaaGymaaqa aiabeo8aZnaaCaaaleqabaGaaGOmaaaaaaGcdaqadaqaaiabeI7aXn aaBaaaleaacaWGPbaabeaakiabgkHiTiaahIhadaqhaaWcbaGaamyA aaqaaKqzGfGamai2gkdiIcaakiaahk7aaiaawIcacaGLPaaadaahaa WcbeqaaiaaikdaaaaakiaawUhacaGL9baaaiaawUfacaGLDbaacaaM c8oacaGL7bGaayzFaaGaaiOlaaWcbaGaamyAaiabg2da9iaaigdaae aacqWItecBa0Gaey4dIunakiaaywW7caaMf8UaaiikaiaabkeacaqG UaGaaeymaiaacMcaaaa@9270@

We show how to fit the joint posterior density of the parameters using random samples (not even a Gibbs sampler), thereby avoiding any monitoring. We will use the multiplication rule to write

π ( θ , β , σ 2 | θ ^ ) = π 1 ( θ | β , σ 2 , θ ^ ) π 2 ( β | σ 2 , θ ^ ) π 3 ( σ 2 | θ ^ ) , MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiWda3aae WaaeaacaWH4oGaaGilaiaaysW7caWHYoGaaGilaiaaysW7daabcaqa aiabeo8aZnaaCaaaleqabaGaaGOmaaaakiaaykW7aiaawIa7aiaayk W7ceWH4oGbaKaaaiaawIcacaGLPaaacaaI9aGaeqiWda3aaSbaaSqa aiaaigdaaeqaaOWaaeWaaeaadaabcaqaaiaahI7acaaMc8oacaGLiW oacaaMc8UaaCOSdiaaiYcacaaMe8Uaeq4Wdm3aaWbaaSqabeaacaaI YaaaaOGaaGilaiaaysW7ceWH4oGbaKaaaiaawIcacaGLPaaacqaHap aCdaWgaaWcbaGaaGOmaaqabaGcdaqadaqaamaaeiaabaGaaCOSdiaa ykW7aiaawIa7aiaaykW7cqaHdpWCdaahaaWcbeqaaiaaikdaaaGcca aISaGaaGjbVlqahI7agaqcaaGaayjkaiaawMcaaiabec8aWnaaBaaa leaacaaIZaaabeaakmaabmaabaWaaqGaaeaacqaHdpWCdaahaaWcbe qaaiaaikdaaaGccaaMc8oacaGLiWoacaaMc8UabCiUdyaajaaacaGL OaGaayzkaaGaaGilaaaa@7BCA@

where π 1 ( θ | β , σ 2 , θ ^ ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiWda3aaS baaSqaaiaaigdaaeqaaOWaaeWaaeaadaabcaqaaiaahI7acaaMc8oa caGLiWoacaaMc8UaaCOSdiaacYcacaaMe8Uaeq4Wdm3aaWbaaSqabe aacaaIYaaaaOGaaiilaiaaysW7ceWH4oGbaKaaaiaawIcacaGLPaaa aaa@49E0@ and π 2 ( β | σ 2 , θ ^ ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiWda3aaS baaSqaaiaaikdaaeqaaOWaaeWaaeaadaabcaqaaiaahk7acaaMc8oa caGLiWoacaaMc8Uaeq4Wdm3aaWbaaSqabeaacaaIYaaaaOGaaiilai aaysW7ceWH4oGbaKaaaiaawIcacaGLPaaaaaa@4660@ have standard forms and π 3 ( σ 2 | θ ^ ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiWda3aaS baaSqaaiaaiodaaeqaaOWaaeWaaeaadaabcaqaaiabeo8aZnaaCaaa leqabaGaaGOmaaaakiaaykW7aiaawIa7aiaaykW7ceWH4oGbaKaaai aawIcacaGLPaaaaaa@42E6@ is nonstandard but it is density of a single parameter.

Momentarily, we will drop the term, 1 ( 1 + σ 2 ) 2 ( 1 σ 2 ) l / 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWaaSqaaSqaai aaigdaaeaadaqadaqaaiaaigdacqGHRaWkcqaHdpWCdaahaaadbeqa aiaaikdaaaaaliaawIcacaGLPaaadaahaaadbeqaaiaaikdaaaaaaO WaaeWaaeaadaWcbaWcbaGaaGymaaqaaiabeo8aZnaaCaaameqabaGa aGOmaaaaaaaakiaawIcacaGLPaaadaahaaWcbeqaamaalyaabaGaeS 4eHWgabaGaaGOmaaaaaaGccaGGSaaaaa@45A1@ because it only affects the posterior density of σ 2 . MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeq4Wdm3aaW baaSqabeaacaaIYaaaaOGaaiOlaaaa@395F@ That is,

π 1 ( θ | β , σ 2 , θ ^ ) i = 1 l { exp [ 1 2 { 1 s i 2 ( θ ^ i θ i ) 2 + 1 σ 2 ( θ i x i β ) 2 } ] } . MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiWda3aaS baaSqaaiaaigdaaeqaaOWaaeWaaeaadaabcaqaaiaahI7acaaMc8oa caGLiWoacaaMc8UaaCOSdiaaiYcacaaMe8Uaeq4Wdm3aaWbaaSqabe aacaaIYaaaaOGaaGilaiaaysW7ceWH4oGbaKaaaiaawIcacaGLPaaa cqGHDisTdaqeWbqabSqaaiaadMgacaaI9aGaaGymaaqaaiabloriSb qdcqGHpis1aOWaaiWaaeaaciGGLbGaaiiEaiaacchadaWadaqaaiab gkHiTmaalaaabaGaaGymaaqaaiaaikdaaaWaaiWaaeaadaWcaaqaai aaigdaaeaacaWGZbWaa0baaSqaaiaadMgaaeaacaaIYaaaaaaakmaa bmaabaGafqiUdeNbaKaadaWgaaWcbaGaamyAaaqabaGccqGHsislcq aH4oqCdaWgaaWcbaGaamyAaaqabaaakiaawIcacaGLPaaadaahaaWc beqaaiaaikdaaaGccqGHRaWkdaWcaaqaaiaaigdaaeaacqaHdpWCda ahaaWcbeqaaiaaikdaaaaaaOWaaeWaaeaacqaH4oqCdaWgaaWcbaGa amyAaaqabaGccqGHsislcaWH4bWaa0baaSqaaiaadMgaaeaajugybi adaITHYaIOaaGccaWHYoaacaGLOaGaayzkaaWaaWbaaSqabeaacaaI YaaaaaGccaGL7bGaayzFaaaacaGLBbGaayzxaaGaaGPaVdGaay5Eai aaw2haaiaai6caaaa@7DB8@

Standard calculations reduce the argument (without 1 / 2 ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeyOeI0YaaS GbaeaacaaIXaaabaGaaGOmaaaacaGGPaaaaa@391E@ of the exponential term to

1 ( 1 λ i ) σ 2 { θ i ( λ i θ ^ i + ( 1 λ i ) x i β ) } 2 + λ i σ 2 ( θ ^ i x i β ) 2 , λ i = σ 2 s i 2 + σ 2 , i = 1 , , l . MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWaaSaaaeaaca aIXaaabaWaaeWaaeaacaaIXaGaeyOeI0Iaeq4UdW2aaSbaaSqaaiaa dMgaaeqaaaGccaGLOaGaayzkaaGaeq4Wdm3aaWbaaSqabeaacaaIYa aaaaaakmaacmaabaGaeqiUde3aaSbaaSqaaiaadMgaaeqaaOGaeyOe I0YaaeWaaeaacqaH7oaBdaWgaaWcbaGaamyAaaqabaGccuaH4oqCga qcamaaBaaaleaacaWGPbaabeaakiabgUcaRmaabmaabaGaaGymaiab gkHiTiabeU7aSnaaBaaaleaacaWGPbaabeaaaOGaayjkaiaawMcaai aahIhadaqhaaWcbaGaamyAaaqaaKqzGfGamai2gkdiIcaakiaahk7a aiaawIcacaGLPaaaaiaawUhacaGL9baadaahaaWcbeqaaiaaikdaaa GccqGHRaWkdaWcaaqaaiabeU7aSnaaBaaaleaacaWGPbaabeaaaOqa aiabeo8aZnaaCaaaleqabaGaaGOmaaaaaaGcdaqadaqaaiqbeI7aXz aajaWaaSbaaSqaaiaadMgaaeqaaOGaeyOeI0IaaCiEamaaDaaaleaa caWGPbaabaqcLbwacWaGyBOmGikaaOGaaCOSdaGaayjkaiaawMcaam aaCaaaleqabaGaaGOmaaaakiaacYcacaaMe8UaaGPaVlabeU7aSnaa BaaaleaacaWGPbaabeaakiabg2da9maalaaabaGaeq4Wdm3aaWbaaS qabeaacaaIYaaaaaGcbaGaam4CamaaDaaaleaacaWGPbaabaGaaGOm aaaakiabgUcaRiabeo8aZnaaCaaaleqabaGaaGOmaaaaaaGccaGGSa GaaGjbVlaadMgacqGH9aqpcaaIXaGaaiilaiaaysW7cqWIMaYscaGG SaGaaGjbVlabloriSjaac6caaaa@8CE2@

Hence, for π 1 ( θ | β , σ 2 , θ ^ ) , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiWda3aaS baaSqaaiaaigdaaeqaaOWaaeWaaeaadaabcaqaaiaahI7acaaMc8oa caGLiWoacaaMc8UaaCOSdiaacYcacaaMe8Uaeq4Wdm3aaWbaaSqabe aacaaIYaaaaOGaaiilaiaaysW7ceWH4oGbaKaaaiaawIcacaGLPaaa caGGSaaaaa@4A90@

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 . ( B .2 ) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWaaqGaaeaacq aH4oqCdaWgaaWcbaGaamyAaaqabaGccaaMc8oacaGLiWoacaaMc8Ua aCOSdiaaiYcacaaMe8Uaeq4Wdm3aaWbaaSqabeaacaaIYaaaaOGaaG ilaiaaysW7ceWH4oGbaKaacaaMe8UaaGjbVpaawagabeWcbeqaaiaa bMgacaqGUbGaaeizaaqaaebbfv3ySLgzGueE0jxyaGqbaKqzGfGae8 hpIOdaaOGaaGjbVlaaysW7caqGobGaae4BaiaabkhacaqGTbGaaeyy aiaabYgadaGadaqaaiabeU7aSnaaBaaaleaacaWGPbaabeaakiqbeI 7aXzaajaWaaSbaaSqaaiaadMgaaeqaaOGaey4kaSYaaeWaaeaacaaI XaGaeyOeI0Iaeq4UdW2aaSbaaSqaaiaadMgaaeqaaaGccaGLOaGaay zkaaGaaCiEamaaDaaaleaacaWGPbaabaqcLbwacWaGyBOmGikaaOGa aCOSdiaaiYcacaaMe8+aaeWaaeaacaaIXaGaeyOeI0Iaeq4UdW2aaS baaSqaaiaadMgaaeqaaaGccaGLOaGaayzkaaGaeq4Wdm3aaWbaaSqa beaacaaIYaaaaaGccaGL7bGaayzFaaGaaGilaiaaysW7caWGPbGaaG ypaiaaigdacaaISaGaaGjbVlablAciljaaiYcacaaMe8UaeS4eHWMa aGOlaiaaywW7caaMf8UaaGzbVlaaywW7caaMf8Uaaiikaiaabkeaca qGUaGaaeOmaiaacMcaaaa@955A@

Momentarily, we will drop the term, i = 1 l [ ( 1 λ i ) σ 2 ] 1 / 2 . MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWaaebmaeqale aacaWGPbGaaGypaiaaigdaaeaacqWItecBa0Gaey4dIunakmaadmaa baWaaeWaaeaacaaIXaGaeyOeI0Iaeq4UdW2aaSbaaSqaaiaadMgaae qaaaGccaGLOaGaayzkaaGaeq4Wdm3aaWbaaSqabeaacaaIYaaaaaGc caGLBbGaayzxaaWaaWbaaSqabeaadaWcgaqaaiaaigdaaeaacaaIYa aaaaaakiaac6caaaa@48BB@ Then, integrating out the θ i , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiUde3aaS baaSqaaiaadMgaaeqaaOGaaiilaaaa@3981@ we get

π 2 ( β | σ 2 , θ ^ ) exp { 1 2 i = 1 l λ i σ 2 ( θ ^ i x i β ) 2 } . MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiWda3aaS baaSqaaiaaikdaaeqaaOWaaeWaaeaadaabcaqaaiaahk7acaaMc8oa caGLiWoacaaMc8UaaGjcVlabeo8aZnaaCaaaleqabaGaaGOmaaaaki aaiYcacaaMe8UabCiUdyaajaaacaGLOaGaayzkaaGaeyyhIuRaciyz aiaacIhacaGGWbWaaiWaaeaacqGHsisldaWcaaqaaiaaigdaaeaaca aIYaaaamaaqahabeWcbaGaamyAaiaai2dacaaIXaaabaGaeS4eHWga niabggHiLdGcdaWcaaqaaiabeU7aSnaaBaaaleaacaWGPbaabeaaaO qaaiabeo8aZnaaCaaaleqabaGaaGOmaaaaaaGcdaqadaqaaiqbeI7a XzaajaWaaSbaaSqaaiaadMgaaeqaaOGaeyOeI0IaaCiEamaaDaaale aacaWGPbaabaqcLbwacWaGyBOmGikaaOGaaCOSdaGaayjkaiaawMca amaaCaaaleqabaGaaGOmaaaaaOGaay5Eaiaaw2haaiaai6caaaa@6AA0@

Hence, the exponent (without 1 / 2 ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeyOeI0YaaS GbaeaacaaIXaaabaGaaGOmaaaacaGGPaaaaa@391E@ can be written as,

i = 1 l λ i σ 2 ( θ ^ i x i β ^ ) 2 + ( β β ^ ) Σ ^ 1 ( β β ^ ) , MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWaaabCaeqale aacaWGPbGaaGypaiaaigdaaeaacqWItecBa0GaeyyeIuoakmaalaaa baGaeq4UdW2aaSbaaSqaaiaadMgaaeqaaaGcbaGaeq4Wdm3aaWbaaS qabeaacaaIYaaaaaaakmaabmaabaGafqiUdeNbaKaadaWgaaWcbaGa amyAaaqabaGccqGHsislcaWH4bWaa0baaSqaaiaadMgaaeaajugybi adaITHYaIOaaGcceWHYoGbaKaaaiaawIcacaGLPaaadaahaaWcbeqa aiaaikdaaaGccqGHRaWkdaqadaqaaiaahk7acqGHsislceWHYoGbaK aaaiaawIcacaGLPaaadaahaaWcbeqaaOGamaiYgkdiIcaacuqHJoWu gaqcamaaCaaaleqabaGaeyOeI0IaaGymaaaakmaabmaabaGaaCOSdi abgkHiTiqahk7agaqcaaGaayjkaiaawMcaaiaaiYcaaaa@610E@

where

β ^ = Σ ^ i = 1 l θ ^ i x i s i 2 + σ 2 and 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 aaCaaaleqabaGaaGOmaaaaaaGccaaMf8Uaaeyyaiaab6gacaqGKbGa aGzbVlqbfo6atzaajaWaaWbaaSqabeaacqGHsislcaaIXaaaaOGaaG ypamaaqahabeWcbaGaamyAaiaai2dacaaIXaaabaGaeS4eHWganiab ggHiLdGcdaWcaaqaaiaahIhadaWgaaWcbaGaamyAaaqabaGccaWH4b Waa0baaSqaaiaadMgaaeaajugybiadaITHYaIOaaaakeaacaWGZbWa a0baaSqaaiaadMgaaeaacaaIYaaaaOGaey4kaSIaeq4Wdm3aaWbaaS qabeaacaaIYaaaaaaakiaai6caaaa@6A50@

It is worth noting that 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 baaSqabeaacaaIYaaaaaaa@38A3@ provided that the design matrix, X , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamiwaiaacY caaaa@3784@ where X = ( x 1 , , x l ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGabmiwayaafa Gaeyypa0ZaaeWaaeaacaWH4bWaaSbaaSqaaiaaigdaaeqaaOGaaiil aiaaysW7cqWIMaYscaGGSaGaaGjbVlaahIhadaWgaaWcbaGaeS4eHW gabeaaaOGaayjkaiaawMcaaaaa@4365@ is full rank. Then,

π 2 ( β | σ 2 , θ ^ ) exp { 1 2 i = 1 l λ i σ 2 ( θ ^ i x i β ^ ) 2 1 2 ( β β ^ ) Σ ^ 1 ( β β ^ ) } . MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiWda3aaS baaSqaaiaaikdaaeqaaOWaaeWaaeaadaabcaqaaiaahk7acaaMc8oa caGLiWoacaaMc8Uaeq4Wdm3aaWbaaSqabeaacaaIYaaaaOGaaiilai aaysW7ceWH4oGbaKaaaiaawIcacaGLPaaacqGHDisTciGGLbGaaiiE aiaacchadaGadaqaaiabgkHiTmaalaaabaGaaGymaaqaaiaaikdaaa WaaabCaeaadaWcaaqaaiabeU7aSnaaBaaaleaacaWGPbaabeaaaOqa aiabeo8aZnaaCaaaleqabaGaaGOmaaaaaaGcdaqadaqaaiqbeI7aXz aajaWaaSbaaSqaaiaadMgaaeqaaOGaeyOeI0IaaCiEamaaDaaaleaa caWGPbaabaqcLbwacWaGyBOmGikaaOGabCOSdyaajaaacaGLOaGaay zkaaWaaWbaaSqabeaacaaIYaaaaOGaeyOeI0YaaSaaaeaacaaIXaaa baGaaGOmaaaadaqadaqaaiaahk7acqGHsislceWHYoGbaKaaaiaawI cacaGLPaaadaahaaWcbeqaaOGamaiYgkdiIcaacuqHJoWugaqcamaa CaaaleqabaGaeyOeI0IaaGymaaaakmaabmaabaGaaCOSdiabgkHiTi qahk7agaqcaaGaayjkaiaawMcaaaWcbaGaamyAaiabg2da9iaaigda aeaacqWItecBa0GaeyyeIuoaaOGaay5Eaiaaw2haaiaac6caaaa@7C43@

That is,

β | σ 2 , θ ^ Normal ( β ^ , Σ ^ ) . ( B .3 ) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWaaqGaaeaaca WHYoGaaGPaVdGaayjcSdGaaGPaVlabeo8aZnaaCaaaleqabaGaaGOm aaaakiaacYcacaaMe8UabCiUdyaajaGaaGjbVlaaykW7rqqr1ngBPr gifHhDYfgaiuaacqWF8iIocaaMc8UaaGjbVlaab6eacaqGVbGaaeOC aiaab2gacaqGHbGaaeiBamaabmaabaGabCOSdyaajaGaaiilaiaays W7cuqHJoWugaqcaaGaayjkaiaawMcaaiaac6cacaaMf8UaaGzbVlaa ywW7caaMf8UaaGzbVlaacIcacaqGcbGaaeOlaiaaiodacaGGPaaaaa@6637@

Now, integrating out β MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaaCOSdaaa@3735@ and incorporating the terms in σ 2 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeq4Wdm3aaW baaSqabeaacaaIYaaaaOGaaiilaaaa@395D@ which were dropped, we have

π 3 ( σ 2 | θ ^ ) Q ( σ 2 ) 1 ( 1 + σ 2 ) 2 , ( B .4 ) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiWda3aaS baaSqaaiaaiodaaeqaaOWaaeWaaeaadaabcaqaaiabeo8aZnaaCaaa leqabaGaaGOmaaaakiaaykW7aiaawIa7aiaaykW7ceWH4oGbaKaaai aawIcacaGLPaaacqGHDisTcaWGrbWaaeWaaeaacqaHdpWCdaahaaWc beqaaiaaikdaaaaakiaawIcacaGLPaaadaWcaaqaaiaaigdaaeaada qadaqaaiaaigdacqGHRaWkcqaHdpWCdaahaaWcbeqaaiaaikdaaaaa kiaawIcacaGLPaaadaahaaWcbeqaaiaaikdaaaaaaOGaaGilaiaayw W7caaMf8UaaGzbVlaaywW7caaMf8UaaiikaiaabkeacaqGUaGaaein aiaacMcaaaa@5D16@

where

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 a7amaaCaaaleqabaWaaSGbaeaacaaIXaaabaGaaGOmaaaaaaGcdaqe WbqabSqaaiaadMgacaaI9aGaaGymaaqaaiabloriSbqdcqGHpis1aO WaaSaaaeaacaaIXaaabaWaaeWaaeaacaWGZbWaa0baaSqaaiaadMga aeaacaaIYaaaaOGaey4kaSIaeq4Wdm3aaWbaaSqabeaacaaIYaaaaa GccaGLOaGaayzkaaWaaWbaaSqabeaadaWcgaqaaiaaigdaaeaacaaI YaaaaaaaaaGcciGGLbGaaiiEaiaacchadaGadaqaaiabgkHiTmaala aabaGaaGymaaqaaiaaikdaaaWaaabCaeqaleaacaWGPbGaaGypaiaa igdaaeaacqWItecBa0GaeyyeIuoakmaalaaabaGaaGymaaqaaiaado hadaqhaaWcbaGaamyAaaqaaiaaikdaaaGccqGHRaWkcqaHdpWCdaah aaWcbeqaaiaaikdaaaaaaOWaaeWaaeaacuaH4oqCgaqcamaaBaaale aacaWGPbaabeaakiabgkHiTiaahIhadaqhaaWcbaGaamyAaaqaaKqz GfGamai2gkdiIcaakiqahk7agaqcaaGaayjkaiaawMcaamaaCaaale qabaGaaGOmaaaaaOGaay5Eaiaaw2haaiaai6caaaa@78A0@

To obtain a random sample from (B.1), we sample σ 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeq4Wdm3aaW baaSqabeaacaaIYaaaaaaa@38A3@ from (B.4), β MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaaCOSdaaa@3735@ from (B.3) and the θ i MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiUde3aaS baaSqaaiaadMgaaeqaaaaa@38C7@ independently from (B.2). The conditional posterior density in (B.4) is nonstandard, and to draw a sample from it, we use a grid method (e.g., Nandram and Yin, 2016). First, we transform σ 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeq4Wdm3aaW baaSqabeaacaaIYaaaaaaa@38A3@ to ϕ = σ 2 / ( 1 + σ 2 ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqy1dyMaey ypa0ZaaSGbaeaacqaHdpWCdaahaaWcbeqaaiaaikdaaaaakeaadaqa daqaaiaaigdacqGHRaWkcqaHdpWCdaahaaWcbeqaaiaaikdaaaaaki aawIcacaGLPaaaaaaaaa@416D@ so that 0 < ϕ < 1 . MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaaGimaGqaai aa=XdacqaHvpGzcaWF8aGaa8xmaiaa=5caaaa@3B5D@ Then, we divide (0, 1) into 100 grids. Actually, we have located the range of ϕ MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqy1dygaaa@37BF@ in (0, 1) and we have divided this interval into 100 grids. This gives us a probability mass function that we sample. Jittering is used in the selected grid to get deviates, which are different with probability one; see Nandram and Yin (2016) for more details.

Appendix C

Proof of Theorem 2

It is convenient to make the following transformations,

θ i = θ i , i = 1 , , l 1 , ϕ = i = 1 l θ i a . MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiUde3aaS baaSqaaiaadMgaaeqaaOGaeyypa0JaeqiUde3aaSbaaSqaaiaadMga aeqaaOGaaiilaiaaysW7caWGPbGaeyypa0JaaGymaiaacYcacaaMe8 UaeSOjGSKaaiilaiaaysW7cqWItecBcqGHsislcaaIXaGaaiilaiaa ysW7cqaHvpGzcqGH9aqpdaaeWbqaaiabeI7aXnaaBaaaleaacaWGPb aabeaakiabgkHiTiaadggaaSqaaiaadMgacqGH9aqpcaaIXaaabaGa eS4eHWganiabggHiLdGccaGGUaaaaa@5AA7@

Here, ϕ MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqy1dygaaa@37BF@ is a dummy variable, which holds the benchmarking constraint, and it ensures a non-singular transformation. The Jacobian is unity and the inverse transformation is

θ i = θ i , i = 1 , , l 1 , θ l = ϕ + a i = 1 l 1 θ i . MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiUde3aaS baaSqaaiaadMgaaeqaaOGaeyypa0JaeqiUde3aaSbaaSqaaiaadMga aeqaaOGaaiilaiaaysW7caWGPbGaeyypa0JaaGymaiaacYcacaaMe8 UaeSOjGSKaaiilaiaaysW7cqWItecBcqGHsislcaaIXaGaaiilaiaa ysW7cqaH4oqCdaWgaaWcbaGaeS4eHWgabeaakiabg2da9iabew9aMj abgUcaRiaadggacqGHsisldaaeWbqaaiabeI7aXnaaBaaaleaacaWG PbaabeaaaeaacaWGPbGaeyypa0JaaGymaaqaaiabloriSjabgkHiTi aaigdaa0GaeyyeIuoakiaac6caaaa@6039@

The transformed density is

π ˜ ( θ 1 , , θ l 1 , ϕ ) . MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafqiWdaNbaG aadaqadaqaaiabeI7aXnaaBaaaleaacaaIXaaabeaakiaacYcacaaM e8UaeSOjGSKaaiilaiaaysW7cqaH4oqCdaWgaaWcbaGaeS4eHWMaey OeI0IaaGymaaqabaGccaGGSaGaaGjbVlabew9aMbGaayjkaiaawMca aiaac6caaaa@4B0A@

Then, the density that holds the benchmarking constraint exactly is

π ˜ ( θ 1 , , θ l 1 | ϕ = 0 ) , θ l = a i = 1 l 1 θ i . MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafqiWdaNbaG aadaqadaqaamaaeiaabaGaeqiUde3aaSbaaSqaaiaaigdaaeqaaOGa aiilaiaaysW7cqWIMaYscaGGSaGaaGjbVlabeI7aXnaaBaaaleaacq WItecBcqGHsislcaaIXaaabeaakiaaykW7aiaawIa7aiaaykW7cqaH vpGzcqGH9aqpcaaIWaaacaGLOaGaayzkaaGaaiilaiaaysW7cqaH4o qCdaWgaaWcbaGaeS4eHWgabeaakiabg2da9iaadggacqGHsisldaae WbqaaiabeI7aXnaaBaaaleaacaWGPbaabeaakiaac6caaSqaaiaadM gacqGH9aqpcaaIXaaabaGaeS4eHWMaeyOeI0IaaGymaaqdcqGHris5 aaaa@6210@

Therefore,

π ( θ 1 , , θ l 1 | ϕ = 0 ) exp { 1 2 δ 2 [ i = 1 l 1 ( θ i u i β ) 2 + { i = 1 l 1 θ i ( a u i β ) } 2 ] } . MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiWda3aae WaaeaadaabcaqaaiabeI7aXnaaBaaaleaacaaIXaaabeaakiaacYca caaMe8UaeSOjGSKaaiilaiaaysW7cqaH4oqCdaWgaaWcbaGaeS4eHW MaeyOeI0IaaGymaaqabaGccaaMc8oacaGLiWoacaaMc8Uaeqy1dyMa eyypa0JaaGimaaGaayjkaiaawMcaaiabg2Hi1kGacwgacaGG4bGaai iCamaacmaabaGaeyOeI0YaaSaaaeaacaaIXaaabaGaaGOmaiabes7a KnaaCaaaleqabaGaaGOmaaaaaaGcdaWadaqaamaaqahabaWaaeWaae aacqaH4oqCdaWgaaWcbaGaamyAaaqabaGccqGHsislcaWH1bWaa0ba aSqaaiaadMgaaeaajugybiadaITHYaIOaaGccaWHYoaacaGLOaGaay zkaaWaaWbaaSqabeaacaaIYaaaaOGaey4kaScaleaacaWGPbGaeyyp a0JaaGymaaqaaiabloriSjabgkHiTiaaigdaa0GaeyyeIuoakmaacm aabaWaaabCaeaacqaH4oqCdaWgaaWcbaGaamyAaaqabaGccqGHsisl daqadaqaaiaadggacqGHsislcaWH1bWaa0baaSqaaiaadMgaaeaaju gybiadaITHYaIOaaGccaWHYoaacaGLOaGaayzkaaaaleaacaWGPbGa eyypa0JaaGymaaqaaiabloriSjabgkHiTiaaigdaa0GaeyyeIuoaaO Gaay5Eaiaaw2haamaaCaaaleqabaGaaGOmaaaaaOGaay5waiaaw2fa aiaaykW7aiaawUhacaGL9baacaGGUaaaaa@8D73@

Dropping terms that do not involve θ ( l ) = ( θ 1 , , θ l 1 ) , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaaCiUdmaaBa aaleaadaqadaqaaiabloriSbGaayjkaiaawMcaaaqabaGccqGH9aqp daqadaqaaiabeI7aXnaaBaaaleaacaaIXaaabeaakiaacYcacaaMe8 UaeSOjGSKaaiilaiaaysW7cqaH4oqCdaWgaaWcbaGaeS4eHWMaeyOe I0IaaGymaaqabaaakiaawIcacaGLPaaadaahaaWcbeqaaOGamaiYgk diIcaacaGGSaaaaa@4D79@ it is easy to show that the exponent is

1 2 δ 2 { θ ( l ) ( I + J ) θ ( l ) 2 [ ( u 1 u l ) β , , ( u l 1 u l ) β + a j ] θ ( l ) } . MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWaaSaaaeaaca aIXaaabaGaaGOmaiabes7aKnaaCaaaleqabaGaaGOmaaaaaaGcdaGa daqaaiaahI7adaqhaaWcbaWaaeWaaeaacqWItecBaiaawIcacaGLPa aaaeaajugybiadaITHYaIOaaGcdaqadaqaaiaadMeacqGHRaWkcaWG kbaacaGLOaGaayzkaaGaaCiUdmaaBaaaleaadaqadaqaaiabloriSb GaayjkaiaawMcaaaqabaGccqGHsislcaaIYaWaamWaaeaadaqadaqa aiaahwhadaWgaaWcbaGaaGymaaqabaGccqGHsislcaWH1bWaaSbaaS qaaiabloriSbqabaaakiaawIcacaGLPaaadaahaaWcbeqaaOGamaiY gkdiIcaacaWHYoGaaiilaiaaysW7cqWIMaYscaGGSaGaaGjbVpaabm aabaGaaCyDamaaBaaaleaacqWItecBcqGHsislcaaIXaaabeaakiab gkHiTiaahwhadaWgaaWcbaGaeS4eHWgabeaaaOGaayjkaiaawMcaam aaCaaaleqabaGccWaGiBOmGikaaiaahk7acqGHRaWkcaWGHbGabCOA ayaafaaacaGLBbGaayzxaaGaaCiUdmaaBaaaleaadaqadaqaaiablo riSbGaayjkaiaawMcaaaqabaaakiaawUhacaGL9baacaGGUaaaaa@7586@

Then, using the properties of a multivariate normal density, we have

θ ( l ) | ϕ = 0 Normal ( ( I + J ) 1 ( a j + ( u 1 u l ) β , , ( u l 1 u l ) β ) , δ 2 ( I + J ) 1 ) . MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWaaqGaaeaaca WH4oWaaSbaaSqaamaabmaabaGaeS4eHWgacaGLOaGaayzkaaaabeaa kiaaykW7aiaawIa7aiaaykW7cqaHvpGzcqGH9aqpcaaIWaGaaGjbVl aaykW7rqqr1ngBPrgifHhDYfgaiuaacqWF8iIocaaMe8UaaGPaVlaa b6eacaqGVbGaaeOCaiaab2gacaqGHbGaaeiBamaabmaabaWaaeWaae aacaWGjbGaey4kaSIaamOsaaGaayjkaiaawMcaamaaCaaaleqabaGa eyOeI0IaaGymaaaakmaabmaabaGaamyyaiqahQgagaqbaiabgUcaRm aabmaabaGaaCyDamaaBaaaleaacaaIXaaabeaakiabgkHiTiaahwha daWgaaWcbaGaeS4eHWgabeaaaOGaayjkaiaawMcaamaaCaaaleqaba GccWaGiBOmGikaaiaahk7acaGGSaGaaGjbVlablAciljaacYcacaaM e8+aaeWaaeaacaWH1bWaaSbaaSqaaiabloriSjabgkHiTiaaigdaae qaaOGaeyOeI0IaaCyDamaaBaaaleaacqWItecBaeqaaaGccaGLOaGa ayzkaaWaaWbaaSqabeaakiadaISHYaIOaaGaaCOSdaGaayjkaiaawM caamaaCaaaleqabaGccWaGiBOmGikaaiaacYcacaaMe8UaeqiTdq2a aWbaaSqabeaacaaIYaaaaOWaaeWaaeaacaWGjbGaey4kaSIaamOsaa GaayjkaiaawMcaamaaCaaaleqabaGaeyOeI0IaaGymaaaaaOGaayjk aiaawMcaaiaac6caaaa@8BCF@

Finally, using the Sherman-Morrison formula, ( I + J ) 1 = I 1 l J , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWaaeWaaeaaca WGjbGaey4kaSIaamOsaaGaayjkaiaawMcaamaaCaaaleqabaGaeyOe I0IaaGymaaaakiabg2da9iaadMeacqGHsisldaWcbaWcbaGaaGymaa qaaiabloriSbaakiaadQeacaGGSaaaaa@4230@ we have

θ ( l ) | ϕ = 0 Normal { ( I 1 l J ) ( a j + ( u 1 u l ) β , , ( u l 1 u l ) β ) , δ 2 ( I 1 l J ) } . MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWaaqGaaeaaca WH4oWaaSbaaSqaamaabmaabaGaeS4eHWgacaGLOaGaayzkaaaabeaa kiaaykW7aiaawIa7aiaaykW7cqaHvpGzcqGH9aqpcaaIWaGaaGjbVl aaykW7rqqr1ngBPrgifHhDYfgaiuaacqWF8iIocaaMe8UaaGPaVlaa b6eacaqGVbGaaeOCaiaab2gacaqGHbGaaeiBamaacmaabaWaaeWaae aacaWGjbGaeyOeI0YaaSaaaeaacaaIXaaabaGaeS4eHWgaaiaadQea aiaawIcacaGLPaaadaqadaqaaiaadggaceWHQbGbauaacqGHRaWkda qadaqaaiaahwhadaWgaaWcbaGaaGymaaqabaGccqGHsislcaWH1bWa aSbaaSqaaiabloriSbqabaaakiaawIcacaGLPaaadaahaaWcbeqaaO GamaiYgkdiIcaacaWHYoGaaiilaiaaysW7cqWIMaYscaGGSaGaaGjb VpaabmaabaGaaCyDamaaBaaaleaacqWItecBcqGHsislcaaIXaaabe aakiabgkHiTiaahwhadaWgaaWcbaGaeS4eHWgabeaaaOGaayjkaiaa wMcaamaaCaaaleqabaGccWaGiBOmGikaaiaahk7aaiaawIcacaGLPa aadaahaaWcbeqaaOGamaiYgkdiIcaacaGGSaGaaGjbVlabes7aKnaa CaaaleqabaGaaGOmaaaakmaabmaabaGaamysaiabgkHiTmaalaaaba GaaGymaaqaaiabloriSbaacaWGkbaacaGLOaGaayzkaaaacaGL7bGa ayzFaaGaaiOlaaaa@8CC7@

It is worth noting that the matrix determinant lemma gives det ( I + J ) = l MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaciizaiaacw gacaGG0bWaaeWaaeaacaWGjbGaey4kaSIaamOsaaGaayjkaiaawMca aiabg2da9iabloriSbaa@3F01@ and so det ( δ 2 ( I 1 l J ) ) = 1 l ( δ 2 ) l 1 . MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpgpC0xc9LqFf0xc9 qqpeuf0xe9q8qiYRWFGCk9vi=dbbf9v8Gq0db9qqpm0dXdHqpq0=vr 0=vr0=edbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaciizaiaacw gacaGG0bWaaeWaaeaacqaH0oazdaahaaWcbeqaaiaaikdaaaGcdaqa daqaaiaadMeacqGHsisldaWcbaWcbaGaaGymaaqaaiabloriSbaaki aadQeaaiaawIcacaGLPaaaaiaawIcacaGLPaaacqGH9aqpdaWcbaWc baGaaGymaaqaaiabloriSbaakmaabmaabaGaeqiTdq2aaWbaaSqabe aacaaIYaaaaaGccaGLOaGaayzkaaWaaWbaaSqabeaacqWItecBcqGH sislcaaIXaaaaOGaaiOlaaaa@4E03@

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