A note on the concept of invariance in two-phase sampling designs Section 3. Implications of the invariance property

3.1 Weak invariance

For an arbitrary two-phase sampling design, the inclusion probability of unit i , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpipu0de9LqFf0de9 vqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9=e0dfrpm0dXdHqVu0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamyAaiaacY caaaa@364E@ π i , i s 1 , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpipu0de9LqFf0de9 vqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9=e0dfrpm0dXdHqVu0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiWda3aaS baaSqaaiaadMgaaeqaaOGaaGilaiaadMgacqGHiiIZcaWGZbWaaSba aSqaaiaaigdaaeqaaOGaaGilaaaa@3D58@ is generally unknown and is defined as

π i = E ( I 1 i I 2 i ) = E { I 1 i E ( I 2 i | I 1 ) } = i 1 : i 1 i = 1 π 2 i ( I 1 ) P ( I 1 = i 1 ) , ( 3.1 ) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpipu0de9LqFf0de9 vqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9=e0dfrpm0dXdHqVu0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaqbaeaabmGaaa qaaiabec8aWnaaBaaaleaacaWGPbaabeaaaOqaaiaai2dacaqGfbWa aeWaaeaacaWGjbWaaSbaaSqaaiaaigdacaWGPbaabeaakiaadMeada WgaaWcbaGaaGOmaiaadMgaaeqaaaGccaGLOaGaayzkaaaabaaabaGa aGypaiaabweadaGadaqaaiaadMeadaWgaaWcbaGaaGymaiaadMgaae qaaOGaaeyramaabmaabaWaaqGaaeaacaWGjbWaaSbaaSqaaiaaikda caWGPbaabeaakiaaykW7aiaawIa7aiaaysW7caWHjbWaaSbaaSqaai aahgdaaeqaaaGccaGLOaGaayzkaaaacaGL7bGaayzFaaaabaaabaGa aGypamaaqafabeWcbaGaaCyAamaaBaaameaacaaIXaaabeaaliaayg W7caaI6aGaaGjbVlaadMgadaWgaaadbaGaaGymaiaadMgaaeqaaSGa aGypaiaaigdaaeqaniabggHiLdGccqaHapaCdaWgaaWcbaGaaGOmai aadMgaaeqaaOWaaeWaaeaacaWHjbWaaSbaaSqaaiaahgdaaeqaaaGc caGLOaGaayzkaaGaamiuamaabmaabaGaaCysamaaBaaaleaacaaIXa aabeaakiaai2dacaWHPbWaaSbaaSqaaiaaigdaaeqaaaGccaGLOaGa ayzkaaGaaGilaaaacaaMf8UaaGzbVlaaywW7caaMf8UaaGzbVlaacI cacaaIZaGaaiOlaiaaigdacaGGPaaaaa@78A9@

where i 1 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpipu0de9LqFf0de9 vqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9=e0dfrpm0dXdHqVu0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaaCyAamaaBa aaleaacaaIXaaabeaaaaa@3689@ denotes a realisation of the random vector I 1 . MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpipu0de9LqFf0de9 vqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9=e0dfrpm0dXdHqVu0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaaCysamaaBa aaleaacaaIXaaabeaakiaac6caaaa@3725@ Therefore, the π i s MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpipu0de9LqFf0de9 vqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9=e0dfrpm0dXdHqVu0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiWda3aaS baaSqaaiaadMgaaeqaaGqaaOGaa8xgGiaabohaaaa@394A@ are generally unknown because they require the knowledge of P ( I 1 = i 1 ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpipu0de9LqFf0de9 vqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9=e0dfrpm0dXdHqVu0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamiuamaabm aabaGaaCysamaaBaaaleaacaaIXaaabeaakiaai2dacaWHPbWaaSba aSqaaiaaigdaaeqaaaGccaGLOaGaayzkaaaaaa@3B7B@ for every possible I 1 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpipu0de9LqFf0de9 vqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9=e0dfrpm0dXdHqVu0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaaCysamaaBa aaleaacaaIXaaabeaaaaa@3669@ (in many cases, we do) but also of π 2 i ( I 1 ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpipu0de9LqFf0de9 vqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9=e0dfrpm0dXdHqVu0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiWda3aaS baaSqaaiaaikdacaWGPbaabeaakmaabmaabaGaaCysamaaBaaaleaa caWHXaaabeaaaOGaayjkaiaawMcaaaaa@3B98@ for every I 1 . MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpipu0de9LqFf0de9 vqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9=e0dfrpm0dXdHqVu0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaaCysamaaBa aaleaacaWHXaaabeaakiaac6caaaa@3724@ The latter are generally unknown because π 2 i ( I 1 ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpipu0de9LqFf0de9 vqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9=e0dfrpm0dXdHqVu0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiWda3aaS baaSqaaiaaikdacaWGPbaabeaakmaabmaabaGaaCysamaaBaaaleaa caWHXaaabeaaaOGaayjkaiaawMcaaaaa@3B98@ may depend on the outcome of phase 1. However, if the sampling design is weakly invariant, then π 2 i ( I 1 ) = π 2 i MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpipu0de9LqFf0de9 vqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9=e0dfrpm0dXdHqVu0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiWda3aaS baaSqaaiaaikdacaWGPbaabeaakmaabmaabaGaaCysamaaBaaaleaa caWHXaaabeaaaOGaayjkaiaawMcaaiaai2dacqaHapaCdaWgaaWcba GaaGOmaiaadMgaaeqaaaaa@3FF2@ and (3.1) reduces to

π i = π 2 i i 1 : i 1 i = 1 P ( I 1 = i 1 ) = π 1 i π 2 i . ( 3.2 ) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpipu0de9LqFf0de9 vqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9=e0dfrpm0dXdHqVu0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiWda3aaS baaSqaaiaadMgaaeqaaOGaaGypaiabec8aWnaaBaaaleaacaaIYaGa amyAaaqabaGcdaaeqbqabSqaaiaahMgadaWgaaadbaGaaGymaaqaba WccaaI6aGaaGjbVlaadMgadaWgaaadbaGaaGymaiaadMgaaeqaaSGa aGypaiaaigdaaeqaniabggHiLdGccaWGqbWaaeWaaeaacaWHjbWaaS baaSqaaiaaigdaaeqaaOGaaGypaiaahMgadaWgaaWcbaGaaGymaaqa baaakiaawIcacaGLPaaacaaI9aGaeqiWda3aaSbaaSqaaiaaigdaca WGPbaabeaakiabec8aWnaaBaaaleaacaaIYaGaamyAaaqabaGccaaI UaGaaGzbVlaaywW7caaMf8UaaGzbVlaaywW7caGGOaGaaG4maiaac6 cacaaIYaGaaiykaaaa@6176@

Suppose that we are interested in estimating the population total t y = i U y i . MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpipu0de9LqFf0de9 vqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9=e0dfrpm0dXdHqVu0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamiDamaaBa aaleaacaWG5baabeaakiaai2dadaaeqaqabSqaaiaadMgacqGHiiIZ caWGvbaabeqdcqGHris5aOGaaGPaVlaadMhadaWgaaWcbaGaamyAaa qabaGccaGGUaaaaa@413D@ Since the π i s MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpipu0de9LqFf0de9 vqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9=e0dfrpm0dXdHqVu0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiWda3aaS baaSqaaiaadMgaaeqaaGqaaOGaa8xgGiaabohaaaa@394A@ are generally unknown, the Horvitz-Thompson estimator of t y , MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpipu0de9LqFf0de9 vqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9=e0dfrpm0dXdHqVu0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamiDamaaBa aaleaacaWG5baabeaakiaacYcaaaa@378D@

t ^ H T = i s 2 π i 1 y i , MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpipu0de9LqFf0de9 vqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9=e0dfrpm0dXdHqVu0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGabmiDayaaja WaaSbaaSqaaiaadIeacaWGubaabeaakiaai2dadaaeqbqabSqaaiaa dMgacqGHiiIZcaWGZbWaaSbaaWqaaiaaikdaaeqaaaWcbeqdcqGHri s5aOGaaGPaVlabec8aWnaaDaaaleaacaWGPbaabaGaeyOeI0IaaGym aaaakiaadMhadaWgaaWcbaGaamyAaaqabaGccaaISaaaaa@47D4@

cannot be used, in general. Instead, it is common practice to use the double expansion estimator

t ^ D E = i s 2 π 1 i 1 π 2 i ( I 1 ) 1 y i . MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpipu0de9LqFf0de9 vqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9=e0dfrpm0dXdHqVu0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGabmiDayaaja WaaSbaaSqaaiaadseacaWGfbaabeaakiaai2dadaaeqbqabSqaaiaa dMgacqGHiiIZcaWGZbWaaSbaaWqaaiaaikdaaeqaaaWcbeqdcqGHri s5aOGaaGPaVlabec8aWnaaDaaaleaacaaIXaGaamyAaaqaaiabgkHi TiaaigdaaaGccqaHapaCdaWgaaWcbaGaaGOmaiaadMgaaeqaaOWaae WaaeaacaWHjbWaaSbaaSqaaiaaigdaaeqaaaGccaGLOaGaayzkaaWa aWbaaSqabeaacqGHsislcaaIXaaaaOGaamyEamaaBaaaleaacaWGPb aabeaakiaai6caaaa@5146@

In general, both t ^ H T MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpipu0de9LqFf0de9 vqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9=e0dfrpm0dXdHqVu0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGabmiDayaaja WaaSbaaSqaaiaadIeacaWGubaabeaaaaa@378B@ and t ^ D E MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpipu0de9LqFf0de9 vqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9=e0dfrpm0dXdHqVu0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGabmiDayaaja WaaSbaaSqaaiaadseacaWGfbaabeaaaaa@3778@ differ. However, for weakly invariant two-phase designs, it is clear from (3.2), that both are identical.

3.2 Strong invariance

Let θ MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpipu0de9LqFf0de9 vqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9=e0dfrpm0dXdHqVu0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiUdehaaa@3665@ be a finite population parameter and θ ^ MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpipu0de9LqFf0de9 vqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9=e0dfrpm0dXdHqVu0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafqiUdeNbaK aaaaa@3676@ be an estimator of θ . MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpipu0de9LqFf0de9 vqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9=e0dfrpm0dXdHqVu0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqiUdeNaai Olaaaa@3718@ The total variance of θ ^ MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpipu0de9LqFf0de9 vqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9=e0dfrpm0dXdHqVu0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafqiUdeNbaK aaaaa@3676@ can be expressed as

V ( θ ^ ) = V E ( θ ^ | I 1 ) + E V ( θ ^ | I 1 ) . ( 3.3 ) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpipu0de9LqFf0de9 vqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9=e0dfrpm0dXdHqVu0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamOvamaabm aabaGafqiUdeNbaKaaaiaawIcacaGLPaaacaaI9aGaamOvaiaadwea daqadaqaamaaeiaabaGafqiUdeNbaKaacaaMc8oacaGLiWoacaaMe8 UaaCysamaaBaaaleaacaWHXaaabeaaaOGaayjkaiaawMcaaiabgUca RiaadweacaWGwbWaaeWaaeaadaabcaqaaiqbeI7aXzaajaGaaGPaVd GaayjcSdGaaGjbVlaahMeadaWgaaWcbaGaaCymaaqabaaakiaawIca caGLPaaacaaIUaGaaGzbVlaaywW7caaMf8UaaGzbVlaaywW7caGGOa GaaG4maiaac6cacaaIZaGaaiykaaaa@5D4D@

Decomposition (3.3) is often called the two-phase decomposition of the variance; e.g., Särndal et al. (1992). If the two-phase sampling design is strongly invariant, the total variance of θ ^ MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpipu0de9LqFf0de9 vqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9=e0dfrpm0dXdHqVu0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGafqiUdeNbaK aaaaa@3676@ can alternatively be decomposed as

V ( θ ^ ) = E V ( θ ^ | I 2 ) + V E ( θ ^ | I 2 ) . ( 3.4 ) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpipu0de9LqFf0de9 vqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9=e0dfrpm0dXdHqVu0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamOvamaabm aabaGafqiUdeNbaKaaaiaawIcacaGLPaaacaaI9aGaamyraiaadAfa daqadaqaamaaeiaabaGafqiUdeNbaKaacaaMc8oacaGLiWoacaaMe8 UaaCysamaaBaaaleaacaWHYaaabeaaaOGaayjkaiaawMcaaiabgUca RiaadAfacaWGfbWaaeWaaeaadaabcaqaaiqbeI7aXzaajaGaaGPaVd GaayjcSdGaaGjbVlaahMeadaWgaaWcbaGaaCOmaaqabaaakiaawIca caGLPaaacaaIUaGaaGzbVlaaywW7caaMf8UaaGzbVlaaywW7caGGOa GaaG4maiaac6cacaaI0aGaaiykaaaa@5D50@

The decomposition (3.4) is often called the reverse decomposition of the variance as the order of sampling is reversed, which can only be justified provided the two-phase design is strongly invariant. The decomposition (3.4) cannot be used in the case of weakly invariant two-phase design as the vector I 2 MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpipu0de9LqFf0de9 vqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9=e0dfrpm0dXdHqVu0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaaCysamaaBa aaleaacaaIYaaabeaaaaa@366A@ cannot be generated prior to the vector I 1 . MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiFu0Je9sqqrpepC0xbbL8F4rqqrpipu0de9LqFf0de9 vqaqFeFr0xbbG8FaYPYRWFb9fi0lXxbvc9=e0dfrpm0dXdHqVu0=vr 0=vr0=fdbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaaCysamaaBa aaleaacaaIXaaabeaakiaai6caaaa@372B@ The reverse decomposition was studied in the context of nonresponse by Fay (1991), Shao and Steel (1999) and Kim and Rao (2009), among others. In a nonresponse context, assuming that the units respond independently of one another, the set of respondents can be viewed as a second-phase sample selected according to Poisson sampling with unknown inclusion probabilities, called response probabilities. If the latter remain the same from one realization of the sample to another, we are essentially in the presence of a strongly invariant two-phase sampling design. Decomposition (3.4) can be used to justify simplified variance estimators for two-phase sampling designs; see Beaumont, Béliveau and Haziza (2015).

Acknowledgements

The authors are grateful to an Associate Editor and a reviewer for their comments and suggestions, which improved the quality of this paper. David Haziza’s research was funded by a grant from the Natural Sciences and Engineering Research Council of Canada.

References

Beaumont, J.-F., Béliveau, A. and Haziza, D. (2015). Clarifying some aspects of variance estimation in two-phase sampling. Journal of Survey Statistics and Methodology, 3, 524-542.

Fay, R.E. (1991). A design-based perspective on missing data variance. Proceedings of the 1991 Annual Research Conference, US Bureau of the Census, 429-440.

Kim, J.K., and Rao, J.N.K. (2009). A unified approach to linearization variance estimation from survey data after imputation for item nonresponse. Biometrika, 96, 917-932.

Särndal, C.-E., Swensson, B. and Wretman, J. (1992). Model Assisted Survey Sampling. Springer-Verlag, New York.

Shao, J., and Steel, P. (1999). Variance estimation for survey data with composite imputation and nonnegligible sampling fractions. Journal of the American Statistical Association, 94, 254-265.

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