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.
Exact variance against propagated variance for a nonlinear observation map
Example
Let carry the weights , , let and let on the open convex set , which contains the three values of . Then is with constant Hessian and operator norm , the mean is , and The linearization has variance so the propagated variance is not the exact variance of . The linearization error satisfies so both displayed bounds of Mean, mean-square and covariance bounds for second-order linearization error are attained in this example. The example contains no measured quantity and asserts no physical model.
Facts & Assumptions
Given: The finite weighted set and the random variable displayed in the Example; the function on .
The finite probability space determines a probability measure on with , and expectations of finite-valued random variables computed by the finite weighted sum agree with their expectations as random variables on that probability space. (Finite probability spaces are exactly finite full-power-set probability spaces, Expectation of a real random variable on a finite probability space, Finite probability spaces, outcome weights, events, and event probabilities)
If is on the open convex set , on , takes values in with and , then the linearization error satisfies , and when the fourth moment is finite. (Mean, mean-square and covariance bounds for second-order linearization error)
For a square-integrable random variable with mean , the covariance matrix of the one-dimensional random vector is the matrix , and the linearization has covariance matrix . (Mean vector and covariance matrix of a square-integrable random vector, The covariance of the linearization is )
The derivative of is , and variance is for square-integrable . (For a natural the function is differentiable everywhere with derivative ; for it is the constant , with derivative ; for a natural the function is differentiable at every with derivative ; consequently every polynomial function is differentiable at every real, with the derivative computed term by term, Moments, variance, and covariance on a probability space)
Verification
By [L1] the weights make a probability space and the expectations below are the finite weighted sums of Expectation of a real random variable on a finite probability space: and .
The function is on the open convex set , with , so and ; its Hessian is the constant matrix , of operator norm by [L3] and [L4], and the values of and the mean all lie in .
By [L4], and .
The linearization error is .
By [L3] the propagated covariance is , while step 2.1 gives ; these differ, so the propagated covariance is not the exact variance of in this model.
With and the moments of step 1.1, the bounds of [L2] read and ; since by step 2.2, one has and , so both bounds are attained.
Depends on
Mean, mean-square and covariance bounds for second-order linearization error
Mean vector and covariance matrix of a square-integrable random vector
Expectation of a real random variable on a finite probability space
Finite probability spaces, outcome weights, events, and event probabilities
Moments, variance, and covariance on a probability space
The covariance of the linearization is
For a natural the function is differentiable everywhere with derivative ; for it is the constant , with derivative ; for a natural the function is differentiable at every with derivative ; consequently every polynomial function is differentiable at every real, with the derivative computed term by term
Finite probability spaces are exactly finite full-power-set probability spaces