Alphabeta Math
DefinitionDefinition: AI-adaptedProof: Not applicablePipeline-generatedverified 2026-10-22 (gpt-6.1-sol)
How statement and proof provenance work

The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.

  • Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
  • AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
  • AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.

These labels describe origin, not correctness: citations and verification chips remain separate evidence.

Posterior computation error budget

Definition

Fix a measurable space (E,E) and a bounded measurable functional f:E→R, with ∥f∥∞:=sup⁡x∈E∣f(x)∣<∞. All target laws below are probability measures on this same space. If a model or discretization originally uses another state space, specify its measurable embedding into E and compare its pushforward law; no identification of different state spaces is implicit. A posterior law here is the probability law for the unknown at the specified computation stage, conditional on the same fixed observed data. For a probability law μ, write μ(f):=∫Ef dμ.

Name the successive posterior laws as follows: μ⋆ is the intended target; μmodel is the posterior under the selected statistical or physical model; μsolver is the posterior after replacing the exact forward or PDE solution by the declared numerical solver output; and μdisc is the posterior after the declared finite-dimensional discretization. These labels refer to the exact adjacent laws recorded for the computation, even when two stages happen to agree.

Let K be the implemented probability kernel on (E,E). An invariant law πK for K is a probability measure satisfying ∫EK(x,A) πK(dx)=πK(A)(A∈E). Choose and report which invariant law is used if K has more than one. If no invariant law has been established, the invariant-kernel and burn-in terms below are unavailable; they are not set to zero. Let (Xn)n≥0 be a time-homogeneous Markov chain with transition kernel K relative to its natural filtration, with initial probability law λ. For burn-in length b∈{0,1,2,…} and retained sample size N∈{1,2,3,…}, set fˉb,N:=1N∑j=1Nf(Xb+j), and let Eλ denote expectation under this initial law and the chain's transition randomness.

When all stages are present, define the component errors δmodel:=∣μ⋆(f)−μmodel(f)∣,δsolver:=∣μmodel(f)−μsolver(f)∣,δdisc:=∣μsolver(f)−μdisc(f)∣,δK:=∣μdisc(f)−πK(f)∣,δburn:=∣πK(f)−Eλfˉb,N∣,δMC:=∣Eλfˉb,N−fˉb,N∣. The last component is random and the earlier components are fixed for the declared data and computation. The posterior computation error budget is Bf:=δmodel+δsolver+δdisc+δK+δburn+δMC. If a computation stops before one of these stages, report the shorter reference chain and its component terms. The term δK measures the invariant-law discrepancy induced by the implemented transition rule; it is not a one-step distance between kernels. A one-step kernel error cannot replace it without a separate perturbation theorem with its own hypotheses.

The successive scalar references are arranged as this directed error chain; each arrow is labelled by the absolute difference of its endpoints.

¹?(f)¹model(f)¹solver(f)¹disc(f)¼K(f)E¸¹fb;N¹fb;N±model±solver±disc±K±burn±MC

The budget is a bookkeeping bound only when its components are supplied with estimators or verified bounds; an unavailable component is reported as unquantified rather than silently set to zero. In particular, invariance alone does not provide a burn-in estimate, a mixing rate, or a Monte Carlo error estimate.

Depends on

Used by

Dependency tree · two levels

21 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.

Sources