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The backward Gaussian kernel remains valid after future observations

Statement

Assume AC. Let (X0,…,XT,Y1,…,YT) follow a finite-horizon linear-Gaussian model as in Linear-Gaussian state-space models with independent noises. Suppose the Kalman filter of Exact linear-Gaussian Kalman filter is admissible: every innovation covariance Sj it solves is positive definite. Fix 0≤k<T, and let mk∣k,Pk∣k and mk+1∣k,Pk+1∣k be the corresponding filtered and one-step predicted quantities. Assume in addition that Pk+1∣k≻0. Put Ck=Pk∣kFk+1TPk+1∣k−1,Vk=Pk∣k−CkPk+1∣kCkT. Then Vk⪰0, and the formula Qk(y1:k,xk+1,⋅)=N ⁣(mk∣k(y1:k)+Ck(xk+1−mk+1∣k(y1:k)),Vk) defines an everywhere probability kernel. It is a conditional law of Xk given (Y1:k,Xk+1) and also a version of the conditional law of Xk given (Y1:T,Xk+1) under the full finite-horizon model. Thus future observations do not change this backward kernel once Xk+1 is also given. The inverse is the ordinary inverse of the positive-definite forecast covariance; no singular-forecast extension is asserted.

Facts & Assumptions

Given: AC, the finite-horizon model in the Statement, admissible filter histories, and Pk+1∣k≻0.

[A1]

AC is the Axiom of Choice assumed by the Gaussian-law and conditional-Gaussian suppliers. The Axiom of Choice.

[F1]

The model has affine state and observation equations; its initial, process, and measurement Gaussian vectors are mutually independent, and the process covariance Qk+1 is positive semidefinite. Linear-Gaussian state-space models with independent noises.

[F2]

The Kalman algorithm predicts mk+1∣k=Fk+1mk∣k and Pk+1∣k=Fk+1Pk∣kFk+1T+Qk+1. Exact linear-Gaussian Kalman filter.

[F3]

For every observation history, the filtered law of Xk is the probability kernel N(mk∣k,Pk∣k); its covariance is positive semidefinite. The finite-horizon linear-Gaussian Kalman filter is exact.

[F4]

An independent process noise extends the supplied filtering kernel to the joint conditional law, and measurable pushforwards remain conditional laws. Independent noise extends and pushes forward a conditional law.

[F5]

A finite independent stack of Gaussian vectors is jointly Gaussian even when covariance blocks are singular. A finite stack of independent Gaussian vectors is jointly Gaussian.

[F6]

For a jointly Gaussian pair with positive-semidefinite block covariance and positive-definite observed covariance B, the everywhere conditional kernel is Gaussian with the Schur-complement covariance, which is positive semidefinite. Conditional law of a jointly Gaussian block with positive-definite observed covariance.

[F7]

The finite linear-Gaussian path law is the ordered product of its transition and observation kernels. The finite linear-Gaussian state-space path is jointly Gaussian.

[F8]

Integration of a nonnegative product-measurable function against a finite probability kernel is measurable in its parameter. Measurability of integration against a kernel.

[F9]

A data-indexed state-space conditional law is an everywhere probability kernel whose composition with the data vector is an RCD; its values on null-data sets may vary. Filtering, predictive, and smoothing laws in a finite-horizon state-space model.

[F10]

Under AC, Nd(m,P) is defined for every finite-dimensional symmetric positive-semidefinite P, including singular P. Multivariate normal law, including singular covariance.

Proof

Given: The hypotheses in the Statement.

1.1A1F1F2F3F4F5F6F8F10givenalgebra

Fix a history h=y1:k. By [F3], the conditional law of Xk is N(mk∣k(h),Pk∣k). The next process noise is independent of the past by [F1], so [F4] extends this filtering kernel by qk+1 and pushes it forward through (x,q)↦(x,Fk+1x+q). By [F5], (Xk,qk+1) is jointly Gaussian, and the projection characterization in [F10] makes its linear image (Xk,Xk+1) jointly Gaussian. Its mean is (mk∣k,Fk+1mk∣k), its state covariance is Pk∣k, its cross-covariance is Pk∣kFk+1T, and its next-state covariance is Pk+1∣k. The latter block is positive definite by hypothesis. Apply [F6] with that observed block: the conditional mean and covariance are exactly the displayed Qk parameters, so Vk⪰0. The history mean is affine by [F2], and representing each Gaussian section as a translate of fixed N(0,Vk) plus [F8] gives joint measurability in (h,xk+1). Thus Qk is an everywhere probability kernel.

2.1F1F3F4F7F8F9step 1.1construct

Write H=Y1:k, V=Xk+1, and Z=Yk+1:T. By [F7], the full path law factors by taking the law of (H,Xk), applying the transition kernel at k+1, and then a future observation kernel R(V,dz) formed by the remaining transition and observation kernels. The first two factors disintegrate as πk(h,dxk)Kk+1(xk,dv)=ρk(h,dv)Qk(h,v,dxk) by step 1.1, where ρk is the one-step predictive law. Substitution gives the joint factorization as the law of H followed by ρk, Qk, and R. The future kernel depends on the past only through V, and its iterated integrals are measurable by [F8].

3.1F7F8F9step 1.1step 2.1algebra∎

For any Borel set A of Xk and any Borel set D in the product space of (H,V,Z), integrate 1A(xk)1D(h,v,z) in the factorization from step 2.1. This gives P(Xk∈A,(H,V,Z)∈D)=∫DQk(h,v,A) P(H,V,Z)(dh,dv,dz). This is the RCD event identity for Qk given (H,V,Z); its kernel properties were established in step 1.1. Since (H,Z)=Y1:T, it is also a version of the conditional law given (Y1:T,Xk+1). The factorization uses model kernels rather than observation densities, and the only inverse is of Pk+1∣k≻0.

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