Derivation of the Method of Moments Estimators for an AR(1) Model with a Constant Term

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The Formal Theorem

Consider a stationary Autoregressive model of order 1 (AR(1)) with a constant term, defined as:
Yt=c+ϕYt1+ϵt Y_t = c + \phi Y_{t-1} + \epsilon_t
where Yt Y_t is the time series at time t t , c c is a constant, ϕ \phi is the autoregressive parameter, and ϵt \epsilon_t is a white noise error term such that E[ϵt]=0 E[\epsilon_t] = 0 , Var[ϵt]=σ2 Var[\epsilon_t] = \sigma^2 , and Cov(ϵt,ϵs)=0 Cov(\epsilon_t, \epsilon_s) = 0 for ts t \neq s . Additionally, ϵt \epsilon_t is uncorrelated with Ys Y_s for s<t s < t . For stationarity, we assume ϕ<1 |\phi| < 1 . The Method of Moments (MoM) estimators for c c , ϕ \phi , and σ2 \sigma^2 are derived by equating the first three theoretical (population) moments to their corresponding sample moments. **1. Population Mean (μ \mu ):** For a stationary process, E[Yt]=E[Yt1]=μ E[Y_t] = E[Y_{t-1}] = \mu . Taking the expectation of the AR(1) equation: E[Yt]=E[c+ϕYt1+ϵt] E[Y_t] = E[c + \phi Y_{t-1} + \epsilon_t] μ=c+ϕμ+0 \mu = c + \phi \mu + 0 Solving for μ \mu : μ(1ϕ)=c    μ=c1ϕ \mu(1 - \phi) = c \implies \mu = \frac{c}{1 - \phi} **2. Population Variance (γ0 \gamma_0 ):** For a stationary process, Var[Yt]=Var[Yt1]=γ0 Var[Y_t] = Var[Y_{t-1}] = \gamma_0 . Taking the variance of the AR(1) equation: Var[Yt]=Var[c+ϕYt1+ϵt] Var[Y_t] = Var[c + \phi Y_{t-1} + \epsilon_t] Since c c is a constant and Yt1 Y_{t-1} is uncorrelated with ϵt \epsilon_t : γ0=ϕ2Var[Yt1]+Var[ϵt] \gamma_0 = \phi^2 Var[Y_{t-1}] + Var[\epsilon_t] γ0=ϕ2γ0+σ2 \gamma_0 = \phi^2 \gamma_0 + \sigma^2 Solving for γ0 \gamma_0 : γ0(1ϕ2)=σ2    γ0=σ21ϕ2 \gamma_0(1 - \phi^2) = \sigma^2 \implies \gamma_0 = \frac{\sigma^2}{1 - \phi^2} **3. Population Autocovariance at Lag 1 (γ1 \gamma_1 ):** γ1=Cov(Yt,Yt1)=E[(Ytμ)(Yt1μ)] \gamma_1 = Cov(Y_t, Y_{t-1}) = E[(Y_t - \mu)(Y_{t-1} - \mu)] We can rewrite the AR(1) model in terms of deviations from the mean: Ytμ=ϕ(Yt1μ)+ϵt Y_t - \mu = \phi (Y_{t-1} - \mu) + \epsilon_t . (To see this, substitute μ=c1ϕ \mu = \frac{c}{1-\phi} into Ytμ Y_t - \mu ) γ1=E[(ϕ(Yt1μ)+ϵt)(Yt1μ)] \gamma_1 = E[ (\phi (Y_{t-1} - \mu) + \epsilon_t) (Y_{t-1} - \mu) ] γ1=E[ϕ(Yt1μ)2+ϵt(Yt1μ)] \gamma_1 = E[ \phi (Y_{t-1} - \mu)^2 + \epsilon_t (Y_{t-1} - \mu) ] Since ϵt \epsilon_t is uncorrelated with Yt1 Y_{t-1} , E[ϵt(Yt1μ)]=E[ϵt]E[Yt1μ]=00=0 E[\epsilon_t (Y_{t-1} - \mu)] = E[\epsilon_t] E[Y_{t-1} - \mu] = 0 \cdot 0 = 0 . γ1=ϕE[(Yt1μ)2]=ϕVar[Yt1] \gamma_1 = \phi E[(Y_{t-1} - \mu)^2] = \phi Var[Y_{t-1}] For a stationary process, γ1=ϕγ0 \gamma_1 = \phi \gamma_0 **Method of Moments Estimators:** We equate the theoretical moments to their sample counterparts for a given time series {Y1,,YN} \{Y_1, \dots, Y_N\} : μ^=Yˉ=1Nt=1NYt \hat{\mu} = \bar{Y} = \frac{1}{N} \sum_{t=1}^N Y_t γ^0=sY2=1Nt=1N(YtYˉ)2 \hat{\gamma}_0 = s_Y^2 = \frac{1}{N} \sum_{t=1}^N (Y_t - \bar{Y})^2 γ^1=s1=1Nt=2N(YtYˉ)(Yt1Yˉ) \hat{\gamma}_1 = s_1 = \frac{1}{N} \sum_{t=2}^N (Y_t - \bar{Y})(Y_{t-1} - \bar{Y}) From γ1=ϕγ0 \gamma_1 = \phi \gamma_0 , we get the estimator for ϕ \phi :
ϕ^=γ^1γ^0=1Nt=2N(YtYˉ)(Yt1Yˉ)1Nt=1N(YtYˉ)2\hat{\phi} = \frac{\hat{\gamma}_1}{\hat{\gamma}_0} = \frac{\frac{1}{N} \sum_{t=2}^N (Y_t - \bar{Y})(Y_{t-1} - \bar{Y})}{\frac{1}{N} \sum_{t=1}^N (Y_t - \bar{Y})^2}
From μ=c1ϕ \mu = \frac{c}{1 - \phi} , we solve for c c and substitute the estimators: c=μ(1ϕ) c = \mu(1 - \phi)
c^=Yˉ(1ϕ^)\hat{c} = \bar{Y}(1 - \hat{\phi})
From γ0=σ21ϕ2 \gamma_0 = \frac{\sigma^2}{1 - \phi^2} , we solve for σ2 \sigma^2 and substitute the estimators: σ2=γ0(1ϕ2) \sigma^2 = \gamma_0 (1 - \phi^2)
σ^2=γ^0(1ϕ^2)=(1Nt=1N(YtYˉ)2)(1(γ^1γ^0)2)\hat{\sigma}^2 = \hat{\gamma}_0 (1 - \hat{\phi}^2) = \left( \frac{1}{N} \sum_{t=1}^N (Y_t - \bar{Y})^2 \right) \left( 1 - \left( \frac{\hat{\gamma}_1}{\hat{\gamma}_0} \right)^2 \right)
These three equations provide the Method of Moments estimators for ϕ \phi , c c , and σ2 \sigma^2 for an AR(1) model with a constant term.

Analytical Intuition.

Imagine you're a forensic detective in a high-stakes cinematic thriller, tasked with understanding the hidden 'operating system' of a seemingly chaotic sequence of events – our time series Yt Y_t . The AR(1) model with a constant term, Yt=c+ϕYt1+ϵt Y_t = c + \phi Y_{t-1} + \epsilon_t , is the complex 'blueprint' we suspect is at play, but the true parameters c c , ϕ \phi , and σ2 \sigma^2 are unknown, like encrypted codes. The Method of Moments is your ingenious decryption tool. Instead of trying to crack the entire code directly, you look for its 'fingerprints' – specific characteristics or moments – in the observed data. The 'mean' tells you the average level of activity, the 'variance' indicates its overall volatility, and the 'autocovariance at lag 1' reveals how strongly the current event is influenced by the immediate past. You calculate these same 'fingerprints' from your observed data (sample moments) and then, in a moment of cinematic revelation, you equate them to the theoretical 'fingerprints' predicted by the model's blueprint (population moments). By solving these equations, you reverse-engineer the unknown parameters, c^ \hat{c} , ϕ^ \hat{\phi} , and σ^2 \hat{\sigma}^2 , effectively 'unlocking' the model and revealing its underlying dynamics. It's about matching the model's expected statistical signature with the signature found in reality.
CAUTION

Institutional Warning.

Students often confuse population moments (theoretical values from the model's distribution) with sample moments (calculated directly from data). Another common pitfall is the correct handling of \sum limits and denominators (N N vs. Nk N-k ) when defining sample autocovariances, which can impact estimator bias, though MoM typically uses N N for direct analogy.

Academic Inquiries.

01

Why use the Method of Moments (MoM) instead of Maximum Likelihood Estimation (MLE) for AR(1) models?

MoM estimators are generally simpler to compute and require fewer assumptions about the error distribution (e.g., ϵt \epsilon_t only needs to be white noise, not necessarily Gaussian). However, MLE estimators are often asymptotically more efficient (have smaller variance) if the distributional assumptions are correct, particularly for large sample sizes. For AR(1) with Gaussian errors, MLE is preferred, but MoM provides a good starting point and can be robust.

02

What happens if the stationarity condition ϕ<1 |\phi| < 1 is violated?

If ϕ1 |\phi| \ge 1 , the AR(1) process is non-stationary. The population moments (mean, variance, autocovariance) would not be constant over time, making the derivation of theoretical moments invalid. The MoM estimators derived would not consistently estimate the true parameters, and standard statistical inference would not apply. Such processes exhibit explosive behavior or unit roots, requiring different modeling approaches.

03

How does the constant term c c affect the mean of the AR(1) process?

The constant term c c directly determines the long-run mean of the stationary AR(1) process. As derived, μ=c1ϕ \mu = \frac{c}{1 - \phi} . If c=0 c=0 , the mean μ \mu would be zero. A positive c c pushes the mean upwards, and a negative c c pulls it downwards, with the effect amplified by 11ϕ \frac{1}{1-\phi} . It represents the baseline level around which the series fluctuates.

Standardized References.

  • Definitive Institutional SourceShumway, R. H., & Stoffer, D. S. (2017). Time Series Analysis and Its Applications: With R Examples. Springer.

Institutional Citation

Reference this proof in your academic research or publications.

NICEFA Visual Mathematics. (2026). Derivation of the Method of Moments Estimators for an AR(1) Model with a Constant Term: Visual Proof & Intuition. Retrieved from https://nicefa.org/library/time-series-analysis/derivation-of-the-method-of-moments-estimators-for-an-ar-1--model-with-a-constant-term

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