Lecture Notes 2: Limit Theorems, OLS, And

Lecture Notes 2: Limit Theorems, OLS, And

Limit Theorems 1 14.384 Time Series Analysis, Fall 2007 Professor Anna Mikusheva Paul Schrimpf, scribe September 11, 2007 revised September 9, 2013 Lecture 2 Limit Theorems, OLS, and HAC Limit Theorems What are limit theorems? They are laws describing behavior of sums of many random variables. The mostly used are the Law of Large Numbers and Central Limit Theorem. In fact, these are two sets of theorems, rather than just two theorems (different assumptions about moments conditions, dependence and the way of summing can lead to similar statements). The most generic form is: If fxig is a sequence of independent identically distributed (iid) random variables, with Exi = µ, 2 Var(xi) = σ then P 1 n ! L2 1. Law of large numbers (LLN) { n i=1 xi µ (in , a.s., in probability) p P n 1 n − ) 2. Central limit theorems (CLT) {σ ( n i=1 xi µ) N(0; 1) We stated these while assuming independence. In time series, we usually don't have independence. Let us explore where independence may have been used. First, let's start at the simplest proof of LLN: !2 ! 1 Xn 1 Xn E x − µ =Var x (1) n i n i i=1 i=1 ! 1 Xn = Var x (2) n2 i i=1 1 Xn = Var(x ) (3) n2 i i=1 nσ2 = ! 0 (4) n2 We used independence to go from (2) to (3). Without independence, we'd have ! 1 Xn 1 Xn Xn Var x = cov(x ; x ) n i n2 i j i=1 i=1 j=1 1 = (nγ + 2(n − 1)γ + 2(n − 2)γ + :::) n2 0 1 2 " ( ) # 1 Xn k = 2 γ 1 − + γ n k n 0 k=1 Cite as: Anna Mikusheva, course materials for 14.384 Time Series Analysis, Fall 2007. MIT OpenCourseWare (http://ocw.mit.edu), Massachusetts Institute of Technology. Downloaded on [DD Month YYYY]. Limit Theorems 2 P 1 j j 1 If we assume absolute summability, i.e. j=−∞ γ j < , then " ( ) # 1 Xn k lim γk 1 − + γ0 = 0 n!1 n n k=1 Thus, we have: Lemma 1. If xt is a weakly stationary time series(with mean µ) with absolutely summable auto-covariances then a law of large numbers holds (in probability and L2). ∼ 2 8 2 8 Remark 2. Stationarity is not enough. Let z N(0; σ ). Suppose xt = z t. Then cov(xt; xs) = σ Pt; s, so f g 1 n we do not have absolute summability, and clearly we do not have a LLN for xt since the average n i=1 xi equals to z, which is random. P P 1 j j 1 1 j j 1 Remark 3. For an MA, xt = c(L)et, we have j=1 cj < implies −∞ γj < The proof is easy. Last time we showed that X1 γk = cjcj+k j=0 then X1 X1 X1 jγk j = j cjcj+kj k=0 k=0 j=0 XX1 1 ≤ jcj jjcj+k j k=0 j=0 XX1 1 ≤ jcjjjclj l=0 j=0 0 12 X1 @ A = jcjj < 1 j=0 From the new proof of LLN one can guess that the variance in a central limit theorem should change. Remember that we wish to normalize the sum in such a way that the limit variance would be 1. ! ( ) 1 Xn Xn k Var p x =γ + 2 γ 1 − n i 0 k n i=1 k=1 X1 !γ0 + 2 γk = J k=1 J is called the long-run variance and is a correct scale measure. There are many Central Limit Theorems for serially correlated observations. The simplest is for MA(1). P P 1 1 j j 1 Theorem 4. Let yt = µ + j=0 cjet− j, where et is independent white noise and j=0 cj < , then ! p 1 XT T y − µ)J N(0; ) T t t=1 For another version we have to introduce the following notations. Cite as: Anna Mikusheva, course materials for 14.384 Time Series Analysis, Fall 2007. MIT OpenCourseWare (http://ocw.mit.edu), Massachusetts Institute of Technology. Downloaded on [DD Month YYYY]. Limit Theorems 3 • f gt Let It be information available at time t, i.e. It is the sigma-algebra generated by yj j=−∞ • Let τt;k = E[ytjIt− k] − E[ytjI t− k −1] is the revision of forecast about yt as the new information arrives at time t − k. Definition 5. A strictly stationary process fytg is ergodic if for any t; k; l and any bounded functions, g and h, lim cov(g(yt; :::; yt+k); h(yt+k+n; :::yt+k+n+l)) = 0 n!1 f g 2 Theorem 6 (Gordon's CLT). Assume that we have a strictly stationary and ergodic series yt with Eyt < 1 satisfying: P 2 1=2 1 1. j(Eτt;j) < 2 2. E[ytjIt− j] ! 0 in L as j ! 1 then 1 XT p yt ) N(0; J ); T t=1 P J 1 where = γ0 + 2 k=1 γk is a long-run variance. P1 Remark 7. Notice, that yt = j=0 τt;j. The condition 1 is intended to make the dependence between distant observations to decrease to 0. Condition 1 can be checked (see an example below). I'm not sure how the ergodicity can be easily checked. Condition 2 is aimed at the correct centering, in particular, it implies that E[yt] = 0 Example 8. AR(1) yt = ρyt−1 + et j − j k 2 2k 2 We can check condition 2. We have E[yt It−k] E[yt It−k−1] = ρ et−k and Eτt;j = ρ σ , so condition 2 is satisfied. More generally, if the MA has absolutely summable coefficients, then condition 2 will hold. One k can notice that E[ytj=It− k] ρ yt− k, so condition 3 holds. Now let's calculate the long-run variance: σ2ρk γ = k 1 − ρ2 ! 1 1 X σ2 X σ2 J = γ + 2 γ = 1 + 2 ρk = 0 k 1 − ρ2 (1 − ρ)2 k=1 k=1 Remark 9. X1 X1 J = γ0 + 2 γk = γk = γ(1) k=1 k=−∞ where γ(1) is the covariance function from last lecture evaluated at 1. Recall: X1 i γ(ξ) = γiξ i=−∞ and if a(L)yt = b(L)et, then b(ξ)b(ξ−1) γ(ξ) = σ2 a(ξ)a(ξ−1) so ( ) b(1) 2 J = σ2 a(1) Cite as: Anna Mikusheva, course materials for 14.384 Time Series Analysis, Fall 2007. MIT OpenCourseWare (http://ocw.mit.edu), Massachusetts Institute of Technology. Downloaded on [DD Month YYYY]. OLS 4 P1 Remark 10. If fytg is a vector, then let Γk = cov(yt; yt+k) and J = −∞ Γk. The only thing that's different 6 0 from the scalar case is that Γk = Γ−k. Instead, Γk = Γ−k. All the formulas above also hold, except in matrix notation. For example, for a VARMA, 0 J =A−1BΣB0A−1 2 Remark 11. If yt is a martingale difference: E[ytjIt−1] = 0, then there is no serial correlation and J = σ : OLS Suppose yt = xtβ + ut . In cross-section xt is always independent from us if s =6 t due to iid assumption, so the exclusion restriction is formulated as E(utjxt) = 0. In time series, however, we have to describe the dependence between error terms and all regressors. Definition 12. xt is weakly exogenous if E(utjxt; xt−1; :::) = 0 jf g1 Definition 13. xt is strictly exogenous if E(ut xt t=−∞) = 0 Usually, strict exogeneity is too strong an assumption, it is difficult to find a good empirical example for it. The weak exogeneity is much more functional (and we will mainly assume it). OLS estimator: β^ = (X0X)−1(X0y) What is the asymptotic distribution? p 1 1 T (β^ − β) =( X0X)−1(p X0u) T T 1 X 1 X =( x x0 )−1(p x u ) T t t t t t T t P 1 0 ! Appropriate assumptions will gives us a LLN for ( T t xtxt) M. Assume also Gordon'sP condition for z = x u . If u is weakly exogenous, then centering is OK. Gordon's CLT gives ( p1 x u ) ) N(0; J ), t t t t T t t t which means that p T (β^ − β) ) N(0;M −1J M −1) P1 The only thing that is different from usual is the J . J = −∞ γj (where γj are the autocovariances of zt = xtut) is called the long-run variance. The long-run variance usually arise from potentially auto-dependent error terms ut. The errors usually contains everything that is not in the regression, which is arguably auto- correlated. It also may arise from xt being autocorrelated and from conditional heteroskedasticity of the error terms. We need to figure out how to estimate J . This is called HAC (heteroskedasticity autocorrelation consistent) standard errors. Remark 14. A side note on GLS. If one believes in strict exogeneity, then the estimation can be done more efficiently by using GLS. However, GLS is generally invalid if only weak exogeneity holds. The logic here is the following. In many settings error terms ut are arguably auto-correlated, one may think that estimation is not fully efficient (as Gauss-Markov theorem assumes that observations are uncrre- lated) and could be improved. Assume for a moment that yt = βxt + ut; and ut = ρut−1 + et: Assume also for a moment that ρ is known and et are serially uncorrelated(white noise).

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