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Finite-history linear prediction — Examples

1 · Prerequisites

2 · Summary

These examples compute a singular-history forecast whose coefficient vectors are nonunique but whose predictor class is fixed, and a three-state stationary cycle whose conditional mean is nonlinear in the observed history. A causal AR(1) process then gives the h-step forecast μ+ϕh(Xn−μ) and its innovation-sum error variance under centered, uncorrelated finite-variance innovations.

3 · Logical flowchart

4 · Definitions, theorems and proofs

None yet.

5 · Examples, counterexamples and false statements

ExampleConstruction: AI-generatedVerification: AI-generatedprecheck passjudge pass (gpt-6-luna)Open item page →

One-step and multistep forecasts for a causal AR(1)

Example

Let ∣ϕ∣<1, σ2>0, and let (ϵt)t∈Z be centered, square-integrable white noise: E[ϵt2]=σ2 and Cov⁡(ϵs,ϵt)=0 for s≠t. Suppose a weakly stationary process has the causal L2 representation Xt−μ=∑j=0∞ϕjϵt−j and hence satisfies Xt−μ=ϕ(Xt−1−μ)+ϵt. For every n,h≥1, its forecast is X^n+h=μ+ϕh(Xn−μ) and its error variance is σ2∑j=0h−1ϕ2j.

Facts & Assumptions

Given: The weakly stationary causal AR(1) representation and the centered, finite-variance, pairwise uncorrelated innovations specified above.

[F1]

Weak stationarity gives square-integrability of every coordinate and a common mean. Strict and weak stationarity for integer-indexed time series

[F2]

The finite-history best linear forecast is the unique class minimizing squared L2 error over the affine span of the observed history. Best linear forecast from a finite history

[F3]

Variance and covariance are centered second moments and covariance is bilinear on finite sums. Moments, variance, and covariance on a probability space Variance and covariance identities for random variables

[F4]

Cauchy–Schwarz bounds the absolute expectation of a product of two square-integrable variables by the product of their L2 norms. Cauchy-Schwarz for random variables

Verification

1.1givenalgebra

Reindexing the convergent causal series gives Xt−μ=ϕ(Xt−1−μ)+ϵt; repeating this identity gives Xn+h−μ=ϕh(Xn−μ)+Rh, where Rh=∑r=0h−1ϕrϵn+h−r. Every innovation in Rh has index greater than n, while the causal series for each Xj−μ, 1≤j≤n, uses only indices at most j.

2.1givenF1F3F4step 1.1

For each j≤n, every finite partial sum for Xj−μ uses innovation indices at most j, so its covariance with each future term of Rh is zero by the uncorrelated-noise assumption; [F4] passes this covariance identity to the L2 limit. Thus Cov⁡(Rh,Xj)=0 and E[Rh]=0, making the residual orthogonal to the constant and every history variable.

3.1F2F3step 1.1step 2.1algebra∎

Let H=μ+ϕh(Xn−μ) and let any competing affine forecast Z be in the history span; then D:=H−Z is also in that span. Step 2.1 gives E[Rh]=0 and Cov⁡(Rh,Xj)=0 for every j; bilinearity [F3] gives Cov⁡(Rh,D)=0, hence E[RhD]=0. Since Xn+h−Z=Rh+D, expansion yields E[(Xn+h−Z)2]=E[Rh2]+E[D2]≥E[Rh2], with equality exactly when D=0 as an L2 class. Thus H is the unique best class by [F2]. The innovations in Rh are pairwise uncorrelated, so [F3] gives Var⁡(Rh)=σ2∑r=0h−1ϕ2r. This proves both formulas without Gaussian or independent innovations.

ExampleConstruction: AI-generatedVerification: AI-generatedprecheck passjudge pass (gpt-6-luna)Open item page →

A singular history covariance can have nonunique coefficients

Example

Let Ω={−1,1} have equal probability, let Z(ω)=ω, and set Xt=Z for every t∈Z. For n=2 and h=1, the history covariance matrix is singular and the normal equations have multiple coefficient vectors, but they all give the unique predictor class [Z].

Facts & Assumptions

Given: The two-point uniform probability space, Z(ω)=ω, Xt=Z for all integer t, and the prediction target X3 with history X1,X2.

[F1]

A real random variable on a finite probability space is a map from outcomes to R; event probabilities and expectations are the corresponding finite weighted sums. Finite probability spaces, outcome weights, events, and event probabilities Real random variables on finite probability spaces and their finite distributions Expectation of a real random variable on a finite probability space

[F2]

Variance and covariance are expectations of centered products. Variance, standard deviation, and covariance on a finite probability space

[F3]

A process is weakly stationary when its second moments are finite, its mean is constant, and its covariance depends only on the lag. Strict and weak stationarity for integer-indexed time series

[F4]

Finite affine L2 projection gives a unique minimizing class, and its covariance normal equations may have multiple coefficient solutions that represent that same class. Normal equations for best affine L2 prediction

Verification

1.1givenF1F3

Each outcome has weight 1/2, so [F1] gives E[Z]=0 and E[Z2]=1. Every Xt=Z is square-integrable with mean zero, and every finite-dimensional law is shift-invariant because each coordinate is the same Z; hence X is weakly stationary.

2.1givenF2F4step 1.1algebra

The reversed history is (Y1,Y2)=(X2,X1)=(Z,Z) and the target is X3=Z. Direct covariance calculation gives Γ=(1111) and γh=(1,1)T; by [F4] the normal equations reduce to a1+a2=1, so the matrix is singular and has solutions (1,0)T and (0,1)T.

3.1F2F4step 2.1∎

The intercept is zero because every variable has mean zero; either displayed solution gives forecast a1Z+a2Z=Z and zero error, so they represent the same unique minimizing class by [F4].

ExampleConstruction: AI-generatedVerification: AI-generatedprecheck passjudge pass (gpt-6-luna)Open item page →

A finite-history conditional mean can be nonlinear

Example

Take Ω={0,1,2} with equal probability and define v(0)=−1, v(1)=0, and v(2)=1. For every integer t, let Xt(ω)=v(ω+t−1) mod 3. This process is strictly stationary. For n=h=1, the conditional expectation of X2 given X1 is not affine in X1, whereas the best affine forecast is −X1/2.

Facts & Assumptions

Given: The three-point uniform probability space and the process Xt(ω)=v(ω+t−1) mod 3 with v=(−1,0,1).

[F2]

Variance and covariance are expectations of centered products. Variance, standard deviation, and covariance on a finite probability space

[F3]

Strict stationarity means invariance of every finite-dimensional law under common integer shifts; weak stationarity has the stated finite-moment and covariance conditions. Strict and weak stationarity for integer-indexed time series

[F4]

For a one-variable history with positive variance, the affine forecast coefficient is covariance divided by history variance, with the intercept adjusted to the means. Finite-history forecast equations and error variance

[F5]

A conditional-expectation version is measurable with respect to the conditioning sigma-algebra and has the defining event integrals. Conditional expectation given a sigma algebra

[F6]

A random variable measurable with respect to the conditioning sigma-algebra is its own conditional expectation. Conditioning a known variable and an independent variable

Verification

1.1givenF1F3

A common shift s changes phase ω to (ω+s) mod 3, a permutation of the equally weighted outcomes, so every shifted finite coordinate vector has the original law. One-coordinate laws give a common mean, pair laws at each lag give covariance independent of t, and boundedness gives finite moments; hence the process is weakly stationary by [F3].

2.1givenF1F2F4step 1.1algebra

The values of (X1,X2) at ω=0,1,2 are (−1,0),(0,1),(1,−1); hence both means are zero, Var⁡(X1)=2/3, and Cov⁡(X2,X1)=−1/3. By [F4], the unique best affine forecast from this one-variable history is (−1/3)/(2/3)X1=−X1/2.

3.1F5F6step 2.1algebra∎

Since X1:Ω→{−1,0,1} is bijective, σ(X1) is the full event sigma-algebra and X2 is measurable with respect to it. The conditional-expectation definition and known-variable property give E[X2∣σ(X1)]=X2, with values (0,1,−1) at ω=0,1,2. Every outcome has positive probability; if X2=a+bX1 almost surely, the outcomes with X1=0 and X1=−1 force a=b=1, which would give X2=2 when X1=1, contrary to its value −1. Thus the conditional mean is not affine in X1, while step 2.1 gives the best affine forecast −X1/2.

Sources