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The backward Gaussian kernel remains valid after future observations
Statement
Assume AC. Let 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 it solves is positive definite. Fix , and let and be the corresponding filtered and one-step predicted quantities. Assume in addition that . Put Then , and the formula defines an everywhere probability kernel. It is a conditional law of given and also a version of the conditional law of given under the full finite-horizon model. Thus future observations do not change this backward kernel once 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 .
AC is the Axiom of Choice assumed by the Gaussian-law and conditional-Gaussian suppliers. The Axiom of Choice.
The model has affine state and observation equations; its initial, process, and measurement Gaussian vectors are mutually independent, and the process covariance is positive semidefinite. Linear-Gaussian state-space models with independent noises.
The Kalman algorithm predicts and . Exact linear-Gaussian Kalman filter.
For every observation history, the filtered law of is the probability kernel ; its covariance is positive semidefinite. The finite-horizon linear-Gaussian Kalman filter is exact.
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.
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.
For a jointly Gaussian pair with positive-semidefinite block covariance and positive-definite observed covariance , 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.
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.
Integration of a nonnegative product-measurable function against a finite probability kernel is measurable in its parameter. Measurability of integration against a kernel.
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.
Under AC, is defined for every finite-dimensional symmetric positive-semidefinite , including singular . Multivariate normal law, including singular covariance.
Proof
Given: The hypotheses in the Statement.
Fix a history . By [F3], the conditional law of is . The next process noise is independent of the past by [F1], so [F4] extends this filtering kernel by and pushes it forward through . By [F5], is jointly Gaussian, and the projection characterization in [F10] makes its linear image jointly Gaussian. Its mean is , its state covariance is , its cross-covariance is , and its next-state covariance is . The latter block is positive definite by hypothesis. Apply [F6] with that observed block: the conditional mean and covariance are exactly the displayed parameters, so . The history mean is affine by [F2], and representing each Gaussian section as a translate of fixed plus [F8] gives joint measurability in . Thus is an everywhere probability kernel.
Write , , and . By [F7], the full path law factors by taking the law of , applying the transition kernel at , and then a future observation kernel formed by the remaining transition and observation kernels. The first two factors disintegrate as by step 1.1, where is the one-step predictive law. Substitution gives the joint factorization as the law of followed by , , and . The future kernel depends on the past only through , and its iterated integrals are measurable by [F8].
For any Borel set of and any Borel set in the product space of , integrate in the factorization from step 2.1. This gives . This is the RCD event identity for given ; its kernel properties were established in step 1.1. Since , it is also a version of the conditional law given . The factorization uses model kernels rather than observation densities, and the only inverse is of .
Depends on
- The Axiom of Choice
- Linear-Gaussian state-space models with independent noises
- Multivariate normal law, including singular covariance
- Filtering, predictive, and smoothing laws in a finite-horizon state-space model
- Exact linear-Gaussian Kalman filter
- Independent noise extends and pushes forward a conditional law
- A finite stack of independent Gaussian vectors is jointly Gaussian
- The finite-horizon linear-Gaussian Kalman filter is exact
- The finite linear-Gaussian state-space path is jointly Gaussian
- Measurability of integration against a kernel
- Conditional law of a jointly Gaussian block with positive-definite observed covariance
Used by
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Sources
- Simo Särkkä, Bayesian Filtering and Smoothing, Chapter 8, §§8.1–8.2 (standard reference, not scraped)
- Kody Law, Andrew M. Stuart, and Konstantinos Zygalakis, Data Assimilation: A Mathematical Introduction, Chapter 3, §3.1 (standard reference, not scraped)