Calculation of the First Few \(\psi\)-weights for a Specific ARMA(1,1) Model

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The Formal Theorem

Consider an ARMA(1,1) process defined by Yt=ϕYt1+ϵt+θϵt1 Y_t = \phi Y_{t-1} + \epsilon_t + \theta \epsilon_{t-1} , where {ϵt} \{ \epsilon_t \} is a white noise process with E[ϵt]=0 E[\epsilon_t] = 0 and Var(ϵt)=σϵ2 Var(\epsilon_t) = \sigma_{\epsilon}^2 , and ϕ<1 |\phi| < 1 for stationarity. The ψ\psi-weights, ψj \psi_j for j0 j \ge 0 , are defined by the MA( \infty ) representation Yt=j=0ψjϵtj Y_t = \sum_{j=0}^{\infty} \psi_j \epsilon_{t-j} . The first few ψ\psi-weights are given by:
ψ0=1 \psi_0 = 1
ψ1=ϕ+θ \psi_1 = \phi + \theta
ψj=ϕψj1 \psi_j = \phi \psi_{j-1}
for j2 j \ge 2 .

Analytical Intuition.

Imagine a complex ripple in a pond, where the current state Yt Y_t is influenced by its immediate past Yt1 Y_{t-1} and a 'shock' ϵt \epsilon_t that also lingers from the previous moment ϵt1 \epsilon_{t-1} . The ψ\psi-weights are like a chain reaction, quantifying how each past shock ϵtj \epsilon_{t-j} contributes to the current observation Yt Y_t . ψ0 \psi_0 is the direct impact of the current shock (always 1, representing the shock itself). ψ1 \psi_1 captures the combined effect of the current shock and the 'memory' of the previous shock carried forward by the AR(1) component. For subsequent shocks, the influence fades geometrically, dictated solely by the AR(1) parameter ϕ \phi , like an echo diminishing over time.
CAUTION

Institutional Warning.

Students often struggle to see why ψj \psi_j for j2 j \ge 2 only depends on ϕ \phi and not θ \theta , forgetting that θ \theta 's influence is fully captured in ψ0 \psi_0 and ψ1 \psi_1 .

Academic Inquiries.

01

What is the MA(infinity) representation and why is it important?

The MA(infinity) representation expresses any stationary ARMA process as an infinite moving average of past white noise innovations. It's crucial because it allows us to understand the unconditional dependence structure of the process and forms the basis for calculating forecast error variances and impulse response functions.

02

How is the ARMA(1,1) process related to the MA(infinity) representation?

By repeatedly substituting the AR(1) part of the ARMA(1,1) equation into itself, we can express Yt Y_t solely as a linear combination of current and past error terms ϵ \epsilon , effectively transforming it into an infinite moving average process.

03

Does the value of σϵ2 \sigma_{\epsilon}^2 affect the ψ\psi-weights?

No, the ψ\psi-weights themselves are determined by the AR and MA parameters (ϕ \phi and θ \theta ) and represent the structure of the dependence. The variance σϵ2 \sigma_{\epsilon}^2 scales the magnitude of these weights when calculating the variance of Yt Y_t or covariances.

04

What happens if ϕ1 |\phi| \ge 1 ?

If ϕ1 |\phi| \ge 1 , the ARMA(1,1) process is not stationary. In this case, the MA(infinity) representation might not converge, and the ψ\psi-weights would not be well-defined in the usual sense, or they would grow infinitely.

Standardized References.

  • Definitive Institutional SourceBrockwell, P. J., & Davis, R. A. (2016). Introduction to Time Series and Forecasting. Springer.

Institutional Citation

Reference this proof in your academic research or publications.

NICEFA Visual Mathematics. (2026). Calculation of the First Few \(\psi\)-weights for a Specific ARMA(1,1) Model: Visual Proof & Intuition. Retrieved from https://nicefa.org/library/time-series-analysis/calculation-of-the-first-few---psi--weights-for-a-specific-arma-1-1--model

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