Unit Root Tests

unit-rootstructural-breaks

Definition

Unit root tests evaluate whether a time series has an autoregressive root equal to one — i.e., whether ytI(1)y_t \sim I(1) with permanent shocks rather than ytI(0)y_t \sim I(0) with transitory shocks. Under the unit root null, standard ordinary least squares (OLS) estimators of the AR coefficient converge to non-standard functionals of Brownian motion rather than Gaussian limits, requiring simulation-based critical values. The tests are foundational for applied time series work because I(1) versus I(0) classification governs whether cointegration analysis applies, whether differencing is required, and how forecast uncertainty accumulates with horizon.

Key Ideas

How It Works

Dickey-Fuller and ADF Tests

The baseline model is yt=αyt1+uty_t = \alpha y_{t-1} + u_t (or with deterministic terms). White (1958) showed that under α=1\alpha=1 with i.i.d. errors, T(α^1)T(\hat\alpha-1) has the non-standard limiting distribution:

T(α^1)(01W(r)dW(r))(01W(r)2dr)1T(\hat\alpha-1) \Rightarrow \left(\int_0^1 W(r)\,dW(r)\right)\left(\int_0^1 W(r)^2\,dr\right)^{-1}

where W(r)W(r) is a standard Brownian motion on [0,1][0,1]. The augmented DF regression

Δyt=b0yt1+j=1kbjΔytj+etk\Delta y_t = b_0 y_{t-1} + \sum_{j=1}^k b_j \Delta y_{t-j} + e_{tk}

extends this to ARMA errors of unknown order (Said-Dickey 1984). The ADF tt-statistic tρt_\rho for b0=0b_0=0 has the same Dickey-Fuller limiting distribution. Critical values with a constant and no trend are 2.86-2.86 (5%) and 3.43-3.43 (1%) for T=T=\infty.

Phillips-Perron Tests

Phillips (1987) and Phillips-Perron (1988) proposed two non-parametric corrections for serially correlated errors:

Zα=T(α^1)(s2su2)(2T2t=1Tyt12)1Z_\alpha = T(\hat\alpha-1) - (s^2-s^2_u)\left(2T^{-2}\sum_{t=1}^T y^2_{t-1}\right)^{-1}

Zt=sustα12(s2su2)(s2T2t=1Tyt12)1/2Z_t = \frac{s_u}{s}\,t_\alpha - \frac{1}{2}(s^2-s^2_u)\left(s^2 T^{-2}\sum_{t=1}^T y^2_{t-1}\right)^{-1/2}

where su2=T1u^t2s^2_u = T^{-1}\sum \hat u_t^2 (innovation variance) and s2s^2 is any consistent estimator of σ2=2πfu(0)\sigma^2 = 2\pi f_u(0) (the non-normalized spectral density at frequency zero). Under standard asymptotics, ZαZ_\alpha and ZtZ_t have the same Dickey-Fuller limiting distributions as T(α^1)T(\hat\alpha-1) and tαt_\alpha respectively. The practical problem is size distortion: when s2s^2 is estimated inconsistently (e.g., by a kernel estimator when α^\hat\alpha is inconsistent), the correction factor explodes and the statistics diverge from their asymptotic distributions.

M Statistics (Stock 1990; Perron-Ng 1996)

Stock (1990) proposed a class of statistics with different normalization rates under H0H_0 and H1H_1:

MZα=(T1yT2s2)(2T2t=1Tyt12)1MZ_\alpha = \left(T^{-1}y_T^2 - s^2\right)\left(2T^{-2}\sum_{t=1}^T y^2_{t-1}\right)^{-1}

MSB=(T2t=1Tyt12/s2)1/2,MZt=MSBMZαMSB = \left(T^{-2}\sum_{t=1}^T y^2_{t-1}/s^2\right)^{1/2}, \qquad MZ_t = MSB \cdot MZ_\alpha

The key identity is MZα=Zα+(T/2)(α^1)2MZ_\alpha = Z_\alpha + (T/2)(\hat\alpha-1)^2: the modification factor (T/2)(α^1)2(T/2)(\hat\alpha-1)^2 is Op(1)O_p(1) in the near-cancellation cases where T(α^1)T(\hat\alpha-1) \to -\infty, providing an offsetting term that keeps MZαMZ_\alpha bounded. Under standard asymptotics, (α^1)2=Op(T2)(\hat\alpha-1)^2 = O_p(T^{-2}) and the modification is Op(T1)0O_p(T^{-1}) \to 0, so MZαMZ_\alpha and ZαZ_\alpha are asymptotically equivalent. The relation Zt=MSBZαZ_t = MSB \cdot Z_\alpha (eq. 2.9 of Perron-Ng) gives the corresponding MZt=MSBMZαMZ_t = MSB \cdot MZ_\alpha by analogy.

MSBMSB is bounded below by zero and tests the unit root hypothesis by checking whether T2yt12T^{-2}\sum y^2_{t-1} is of order Op(T2)O_p(T^2) (consistent with I(1)) or Op(T)O_p(T) (consistent with I(0)). Critical values (5%): MZα8.1MZ_\alpha \leq -8.1, MSB0.168MSB \leq 0.168 (constant only); MZα17.3MZ_\alpha \leq -17.3, MSB0.148MSB \leq 0.148 (constant and trend).

Autoregressive Spectral Density Estimator

The AR estimator sAR2s^2_{AR} is constructed from the augmented autoregression on first differences:

Δyt=b0yt1+j=1kbjΔytj+etk,sAR2=sek2/(1b^(1))2\Delta y_t = b_0 y_{t-1} + \sum_{j=1}^k b_j \Delta y_{t-j} + e_{tk}, \qquad s^2_{AR} = s^2_{ek}/(1-\hat b(1))^2

where sek2=T1t=k+1Te^tk2s^2_{ek} = T^{-1}\sum_{t=k+1}^T \hat e^2_{tk} and b^(1)=j=1kb^j\hat b(1) = \sum_{j=1}^k \hat b_j. Because this regression is formulated in first differences of yty_t rather than on OLS residuals u^t\hat u_t, the estimate of σ2\sigma^2 does not depend on α^\hat\alpha at first order. In the three local asymptotic frameworks analyzed by Perron-Ng (1996), sAR2s^2_{AR} converges to the correct limit σT2\sigma^2_T in each case, while sWA2s^2_{WA} does not.

Local-to-Unity Framework

Setting yt=(1+c/T)yt1+uty_t = (1+c/T)y_{t-1} + u_t, with c=0c=0 the exact unit root null and c<0c<0 the stationary alternative, yields tractable non-degenerate limits for all statistics as TT\to\infty. The non-centrality cc measures distance from the unit root boundary in units of T1T^{-1}. This framework (Nabeya-Perron 1994; Perron-Ng 1996) diagnoses test behavior in the three regimes where standard asymptotics fail: near-MA-cancellation, near-twice-integration, and near-seasonal-integration.

Why It Matters

Open Questions

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