Short run and long run causality in time series:...
Transcript of Short run and long run causality in time series:...
Short run and long run causality in time series: inference∗
Jean-Marie Dufour,† Denis Pelletier‡ and Éric Renault§
Université de Montréal
September 2003
∗ This work was supported by the Canada Research Chair Program (Chair in Econometrics, Université de Mon-tréal), the Alexander-von-Humboldt Foundation (Germany), the Institut de Finance mathématique de Montréal (IFM2),the Canadian Network of Centres of Excellence [program onMathematics of Information Technology and Complex Sys-tems(MITACS)], the Canada Council for the Arts (Killam Fellowship), the Natural Sciences and Engineering ResearchCouncil of Canada, the Social Sciences and Humanities Research Council of Canada, and the Fonds FCAR (Governmentof Québec). The authors thank Jörg Breitung, Helmut Lütkepohl, Peter Schotman, participants at the EC2 Meeting onCausality and Exogeneity in Louvain-la-Neuve (December 2001), two anonymous referees, and the Editors Luc Bauwens,Peter Boswijk and Jean-Pierre Urbain for several useful comments. This paper is a revised version of Dufour and Renault(1995).
† Canada Research Chair Holder (Econometrics). Centre interuniversitaire de recherche en analyse des organisa-tions (CIRANO), Centre interuniversitaire de recherche en économie quantitative (CIREQ), and Département de scienceséconomiques, Université de Montréal. Mailing address: Département de sciences économiques, Université de Montréal,C.P. 6128 succursale Centre-ville, Montréal, Québec, Canada H3C 3J7. TEL: 1 514 343 2400; FAX: 1 514 343 5831;e-mail: [email protected]. Web page: http://www.fas.umontreal.ca/SCECO/Dufour .
‡ CIRANO, CIREQ, Université de Montréal (Département de sciences économiques), and North Carolina StateUniversity. Mailing address: Department of Economics, North Carolina State University, Campus Box 8110, Raleigh,NC, USA 27695-8110. E-mail: [email protected] .
§CIRANO, CIREQ, and Université de Montréal (Département de sciences économiques). Mailing address: Départe-ment de sciences économiques, Université de Montréal, C.P. 6128 succursale Centre-ville, Montréal, Québec, CanadaH3C 3J7. TEL: 1 514 343 2398; FAX: 1 514 343 5831; e-mail: [email protected] .
ABSTRACT
We propose methods for testing hypothesis of non-causality at various horizons, as defined in Du-four and Renault (1998,Econometrica). We study in detail the case of VAR models and we proposelinear methods based on running vector autoregressions at different horizons. While the hypothesesconsidered are nonlinear, the proposed methods only require linear regression techniques as well asstandard Gaussian asymptotic distributional theory. Bootstrap procedures are also considered. Forthe case of integrated processes, we propose extended regression methods that avoid nonstandardasymptotics. The methods are applied to a VAR model of the U.S. economy.
Key words: time series; Granger causality; indirect causality; multiple horizon causality; autore-gression; autoregressive model; vector autoregression; VAR; stationary process; nonstationary pro-cess; integrated process; unit root; extended autoregression; bootstrap; Monte Carlo; macroeco-nomics; money; interest rates; output; inflation.
JEL classification numbers: C1; C12; C15; C32; C51; C53; E3; E4; E52.
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RÉSUMÉ
Nous proposons des méthodes pour tester des hypothèses de non-causalité à différents horizons, telque défini dans Dufour et Renault (1998,Econometrica). Nous étudions le cas des modèles VARen détail et nous proposons des méthodes linéaires basées sur l’estimation d’autorégressions vecto-rielles à différents horizons. Même si les hypothèses considérées sont non linéaires, les méthodesproposées ne requièrent que des techniques de régression linéaire de même que la théorie distribu-tionnelle asymptotique gaussienne habituelle. Dans le cas des processus intégrés, nous proposonsdes méthodes de régression étendue qui ne requièrent pas de théorie asymptotique non standard.L’application du bootstrap est aussi considérée. Les méthodes sont appliquées à un modèle VAR del’économie américaine.
Mots clés : séries chronologiques; causalité; causalité indirecte; causalité à différents horizons;autorégression; modèle autorégressif; autorégression vectorielle; VAR; processus stationnaire; pro-cessus non stationnaire; processus intégré; racine unitaire; autorégression étendue; bootstrap; MonteCarlo; macroéconomie; monnaie; taux d’intérêt; production; inflation.
Classification JEL: C1; C12; C15; C32; C51; C53; E3; E4; E52.
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Contents
List of Definitions, Propositions and Theorems iv
1. Introduction 1
2. Multiple horizon autoregressions 2
3. Estimation of (p, h) autoregressions 7
4. Causality tests based on stationary(p, h)-autoregressions 9
5. Causality tests based on nonstationary(p, h)-autoregressions 12
6. Empirical illustration 15
7. Conclusion 22
iii
List of Tables
1 Rejection frequencies using the asymptotic distribution and the simulated proce-dure when the true DGP is an i.i.d. Gaussian sequence. . . . . . . . . . . . . . 15
2 Causality tests and simulated p-values for series in first differences (of logarithm)for the horizons 1 to 12. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 19
3 Causality tests and simulated p-values for series in first differences (of logarithm)for the horizons 13 to 24. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 20
4 Summary of causality relations at various horizons for series in first difference. . 215 Causality tests and simulated p-values for extended autoregressions at the horizons
1 to 12 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 236 Causality tests and simulated p-values for extended autoregressions at the horizons
13 to 24 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 247 Summary of causality relations at various horizons for series in first difference with
extended autoregressions. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 25
List of Definitions, Propositions and Theorems
3.1 Proposition : Asymptotic normality of LS in a(p, h) stationary VAR. . . . . . . . . 94.1 Proposition : Asymptotic distribution of test criterion for non-causality at horizonh
in a stationary VAR . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 11
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1. Introduction
The concept of causality introduced by Wiener (1956) and Granger (1969) is now a basic notion forstudying dynamic relationships between time series. The literature on this topic is considerable; see,for example, the reviews of Pierce and Haugh (1977), Newbold (1982), Geweke (1984), Lütkepohl(1991) and Gouriéroux and Monfort (1997, Chapter 10). The original definition of Granger (1969),which is used or adapted by most authors on this topic, refers to the predictability of a variableX(t),wheret is an integer, from its own past, the one of another variableY (t) and possibly a vectorZ(t)of auxiliary variables,one period ahead: more precisely, we say thatY causesX in the sense ofGranger if the observation ofY up to timet (Y (τ) : τ ≤ t) can help one to predictX(t + 1)when the corresponding observations onX andZ are available(X(τ), Z(τ) : τ ≤ t); a moreformal definition will be given below.
Recently, however, Lütkepohl (1993) and Dufour and Renault (1998) have noted that, for multi-variate models where a vector of auxiliary variablesZ is used in addition to the variables of interestX andY, it is possible thatY does not causeX in this sense, but can still help to predictX severalperiods ahead; on this issue, see also Sims (1980), Renault, Sekkat and Szafarz (1998) and Giles(2002). For example, the valuesY (τ) up to timet may help to predictX(t + 2), even though theyare useless to predictX(t+1). This is due to the fact thatY may help to predictZ one period ahead,which in turn has an effect onX at a subsequent period. It is clear that studying such indirect effectscan have a great interest for analyzing the relationships between time series. In particular, one candistinguish in this way properties of “short-run (non-)causality” and “long-run (non-)causality”.
In this paper, we study the problem of testing non-causality at various horizons as defined inDufour and Renault (1998) for finite-order vector autoregressive (VAR) models. In such models,the non-causality restriction at horizon one takes the form of relatively simple zero restrictions onthe coefficients of the VAR [see Boudjellaba, Dufour and Roy (1992) and Dufour and Renault(1998)]. However non-causality restrictions at higher horizons (greater than or equal to 2) aregenerally nonlinear, taking the form of zero restrictions on multilinear forms in the coefficientsof the VAR. When applying standard test statistics such as Wald-type test criteria, such forms caneasily lead to asymptotically singular covariance matrices, so that standard asymptotic theory wouldnot apply to such statistics. Further, calculation of the relevant covariance matrices _ which involvethe derivatives of potentially large numbers of restrictions _ can become quite awkward.
Consequently, we propose simple tests for non-causality restrictions at various horizons [asdefined in Dufour and Renault (1998)] which can be implemented only through linear regressionmethods and do not involve the use of artificial simulations [e.g., as in Lütkepohl and Burda (1997)].This will be done, in particular, by considering multiple horizon vector autoregressions [called(p, h)-autoregressions] where the parameters of interest can be estimated by linear methods. Re-strictions of non-causality at different horizons may then be tested through simple Wald-type (orFisher-type) criteria after taking into account the fact that such autoregressions involve autocorre-lated errors [following simple moving average processes] which are orthogonal to the regressors.The correction for the presence of autocorrelation in the errors may then be performed by using anautocorrelation consistent [or heteroskedasticity-autocorrelation-consistent (HAC)] covariance ma-trix estimator. Further, we distinguish between the case where the VAR process considered is stable
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(i.e., the roots of the determinant of the associated AR polynomial are all outside the unit circle)and the one where the process may be integrated of an unknown order (although not explosive). Inthe first case, the test statistics follow standard chi-square distributions while, in the second case,they may follow nonstandard asymptotic distributions involving nuisance parameters, as already ob-served by several authors for the case of causality tests at horizon one [see Sims, Stock and Watson(1990), Toda and Phillips (1993, 1994), Toda and Yamamoto (1995), Dolado and Lütkepohl (1996)and Yamada and Toda (1998)]. To meet the objective of producing simple procedures that can beimplemented by least squares methods, we propose to deal with such problems by using an exten-sion to the case of multiple horizon autoregressions of the lag extension technique suggested byChoi (1993) for inference on univariate autoregressive models and by Toda and Yamamoto (1995)and Dolado and Lütkepohl (1996) for inference on standard VAR models. This extension will al-low us to use standard asymptotic theory in order to test non-causality at different horizons withoutmaking assumption on the presence of unit roots and cointegrating relations. Finally, to alleviatethe problems of finite-sample unreliability of asymptotic approximations in VAR models (on bothstationary and nonstationary series), we propose the use of bootstrap methods to implement theproposed test statistics.
In section 2, we describe the model considered and introduce the notion of autoregression athorizonh [or (p, h)-autoregression] which will be the basis of our method. In section 3, we studythe estimation of(p, h)-autoregressions and the asymptotic distribution of the relevant estimatorsfor stable VAR processes. In section 4, we study the testing of non-causality at various horizons forstationary processes, while in section 5, we consider the case of processes that may be integrated.In section 6, we illustrate the procedures on a monthly VAR model of the U.S. economy involv-ing a monetary variable (nonborrowed reserves), an interest rate (federal funds rate), prices (GDPdeflator) and real GDP, over the period 1965-1996. We conclude in section 7.
2. Multiple horizon autoregressions
In this section, we develop the notion of “autoregression at horizonh” and the relevant notations.Consider aVAR(p) process of the form:
W (t) = µ(t) +p∑
k=1
πkW (t− k) + a (t) , t = 1, . . . , T, (2.1)
whereW (t) =(w1t, w2t, . . . , wmt
)′is anm× 1 random vector,µ(t) is a deterministic trend, and
E[a (s) a (t)′
]= Ω, if s = t ,= 0, if s 6= t ,
(2.2)
det(Ω) 6= 0 . (2.3)
The most common specification forµ(t) consists in assuming thatµ(t) is a constant vector,i.e.
µ(t) = µ , (2.4)
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although other deterministic trends could also be considered.TheVAR(p) in equation (2.1) is an autoregression at horizon 1. We can then also write for the
observation at timet + h:
W (t + h) = µ(h)(t) +p∑
k=1
π(h)k W (t + 1− k) +
h−1∑
j=0
ψja (t + h− j) , t = 0, . . . , T − h ,
whereψ0 = Im andh < T . The appropriate formulas for the coefficientsπ(h)k , µ(h)(t) andψj are
given in Dufour and Renault (1998), namely:
π(h+1)k = πk+h +
h∑
l=1
πh−l+1π(l)k = π
(h)k+1 + π
(h)1 πk , π
(0)1 = Im , π
(1)k = πk , (2.5)
µ(h)(t) =h−1∑
k=0
π(k)1 µ(t + h− k) , ψh = π
(h)1 , ∀h ≥ 0 . (2.6)
Theψh matrices are the impulse response coefficients of the process, which can also be obtainedfrom the formal series:
ψ(z) = π(z)−1 = Im +∞∑
k=1
ψkzk , π(z) = Im −
∞∑
k=1
πkzk . (2.7)
Equivalently, the above equation forW (t + h) can be written in the following way:
W (t + h)′ = µ(h)(t)′+
p∑
k=1
W (t + 1− k)′ π(h)′k + u(h) (t + h)′
= µ(h)(t)′+ W (t, p)′ π(h) + u(h) (t + h)′ , t = 0, . . . , T − h , (2.8)
whereW (t, p)′ =[W (t)′ , W (t− 1)′ , . . . , W (t− p + 1)′
], π(h) =
[π
(h)1 , . . . , π
(h)p
]′and
u(h) (t + h)′ =[u
(h)1 (t + h) , . . . , u(h)
m (t + h)]
=h−1∑
j=0
a (t + h− j)′ ψ′j .
It is straightforward to see thatu(h) (t + h) has a non-singular covariance matrix.We call (2.8) an “autoregression of orderp at horizonh” or a “(p, h)-autoregression”. In the
sequel, we will assume that the deterministic part of each autoregression is a linear function of afinite-dimensional parameter vector,i.e.
µ(h)(t) = γ(h)D(h)(t) (2.9)
whereγ(h) is am×n coefficient vector andD(h)(t) is an×1 vector of deterministic regressors. If
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µ(t) is a constant vector,i.e. µ(t) = µ, thenµ(h)(t) is simply a constant vector (which may dependonh):
µ(h)(t) = µh . (2.10)
To derive inference procedures, it will be convenient to consider a number of alternative formu-lations of(p, h)-autoregression autoregressions.a) Matrix (p, h)-autoregression_ First, we can put (2.8) in matrix form, which yields:
wh (h) = W p (h) Π(h) + Uh (h) , h = 1, . . . , H , (2.11)
wherewh (k) andUh (k) are(T − k + 1)×m matrices andW p (k) is a(T − k + 1)× (n + mp)matrix defined as
wh (k) =
W (0 + h)′
W (1 + h)′...
W (T − k + h)′
= [w1 (h, k) , . . . , wm (h, k)] , (2.12)
W p (k) =
Wp (0)′
Wp (1)′...
Wp (T − k)′
, Wp (t) =
[D(h)(t)
′
W (t, p)
], (2.13)
Π(h) =[
γ(h)′
π(h)
]= [β1 (h) , β2 (h) , . . . , βm (h)] , (2.14)
Uh (k) =
u(h) (0 + h)′
u(h) (1 + h)′...
u(h) (T − k + h)′
= [u1 (h, k) , . . . , um (h, k)] , (2.15)
ui (h, k) =[u
(h)i (0 + h) , u
(h)i (1 + h) , . . . , u
(h)i (T − k + h)
]′. (2.16)
We shall call the formulation (2.11) a “(p, h)-autoregression in matrix form”.b) Rectangular stacked(p, H)-autoregression_ To get the same regressor matrix on the right-hand side of (2.11), we can also consider:
wh (H) = W p (H) Π(h) + Uh (H) , h = 1, . . . , H. (2.17)
This, however, involves losing observations. Using (2.17), we can also stack theH systems aboveas follows:
wH = W p (H) ΠH + UH (2.18)
wherewH andUH are(T −H + 1)×(mH) matrices andWp (H) is an(mp)×(mH) matrix such
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that
wH = [w1 (H) , w2 (H) , . . . , wH (H)] ,
ΠH =[Π(1), Π(2), . . . , Π(H)
],
UH = [U1 (H) , U2 (H) , . . . , UH (H)] .
Since the elements ofUH are linear transformations of the random vectorsa (t) , t = 1, . . . , T,which containTm random variables, it is clear that the vectorvec (Um) will have a singular covari-ance matrix when
Tm < (T −H) mH = TmH −mH2,
which will be the case whenH ≥ 2 andTm > H.
c) Vec-stacked(p, H)-autoregression_ We can also write equation (2.8) as
w (t + h) =[Im ⊗Wp (t)′
]Π(h) + u(h) (t + h)
= W p (t)′ Π(h) + u(h) (t + h) , t = 0, . . . , T − h, (2.19)
where
Π(h) = vec(Π(h)
)=
β(h)1
β(h)2...
β(h)m
,
W p (t)′ =
Wp (t)′ 0 · · · 00 Wp (t)′ · · · 0...
......
...0 0 · · · Wp (t)′
,
which yields the linear modelwh = ZhΠ(h) + uh (2.20)
where
wh =
W (0 + h)W (1 + h)
...W (T )
= vec
[wh (h)′
],
Zh =
W p (0)′
W p (1)′...
W p (T − h)′
=
Im ⊗Wp (0)′
Im ⊗Wp (1)′...
Im ⊗Wp (T − h)′
,
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uh =
u(h) (0 + h)u(h) (1 + h)
...u(h) (T )
= vec
[Uh (h)′
].
It is also possible to stack together the models (2.20) forh = 1, . . . , H :
w (H) = Z (H) ΠH + u (H) (2.21)
where
w (H) =
w1
w2...
wH
, u (H) =
u1
u2...
uH
, Z (H) =
Z1 0 · · · 00 Z2 · · · 0...
......
0 0 · · · ZH
.
d) Individual (p, H)-autoregressions_ Consider finally a single dependent variable
Wi (t + h) = Wp (t)′ βi (h) + u(h)i (t + h) , t = 0, . . . , T −H, (2.22)
for 1 ≤ h ≤ H, where1 ≤ i ≤ m. We can also write:
Wi (t + H) =[IH ⊗Wp (t)′
]βi (H) + ui (t + H) , t = 0, . . . , T −H , (2.23)
where
Wi (t + H) =
Wi (t + 1)Wi (t + 2)
...Wi (t + H)
, ui (t + H) =
ui (t + 1)ui (t + 2)
...ui (t + H)
, βi (H) =
βi (1)βi (2)
...βi (H)
,
which yields the linear modelWi (H) = ZH βi (H) + uH (2.24)
where
Wi (H) =
Wi (0 + H)Wi (1 + H)
...Wi (T )
, βi (H) =
βi (1)βi (2)
...βi (H)
,
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ZH =
IH ⊗Wp (0)′
IH ⊗Wp (1)′...
IH ⊗Wp (T −H)′
, uH =
ui (0 + H)ui (1 + H)
...ui (T )
.
In the sequel, we shall focus on prediction equations for individual variables and the matrix(p, h)-autoregressive form of the system in (2.11).
3. Estimation of (p, h) autoregressions
Let us now consider each autoregression of orderp at horizonh as given by (2.11):
wh (h) = W p (h) Π(h) + Uh (h) , h = 1, . . . , H . (3.1)
We can estimate (3.1) by ordinary least squares (OLS), which yields the estimator:
Π(h) =[W p (h)′W p (h)
]−1W p (h)′wh (h) = Π(h) +
[W p (h)′W p (h)
]−1W p (h)′ Uh (h) ,
hence √T [Π(h) −Π(h) ] =
[1T
W p (h)′W p (h)]−1 1√
TW p (h)′ Uh (h)
where
1T
W p (h)′W p (h) =1T
T−h∑
t=0
Wp (t) Wp (t)′ ,1√T
W p (h)′ Uh (h) =1√T
T−h∑
t=0
Wp (t) u(h) (t + h)′ .
Suppose now that
1T
T−h∑
t=0
Wp (t)Wp (t)′ p−→T→∞
Γp with det(Γp) 6= 0 . (3.2)
In particular, this will be the case if the processW (t) is second-order stationary, strictly indeter-ministic and regular, in which case
E[Wp (t) Wp (t)′
]= Γp , ∀t. (3.3)
Cases where the process does not satisfy these conditions are covered in section 5. Further, since
u(h) (t + h) = a (t + h) +h−1∑
k=1
ψka (t + h− k)
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(where, by convention, any sum of the form∑h−1
k=1 with h < 2 is zero), we have:
E[Wp (t) u(h) (t + h)′
]= 0 , for h = 1, 2, ... ,
V
vec[Wp (t) u(h) (t + h)′
]= ∆p (h) .
If the processW (t) is strictly stationary with i.i.d. innovationsa(t) and finite fourth moments, wecan write:
E[Wp (s)u(h)i (s + h) u
(h)j (t + h) Wp (t)′] = Γij(p, h, t− s) = Γij(p, h, s− t) (3.4)
where1 ≤ i ≤ m, 1 ≤ j ≤ m, with
Γij(p, h, 0) = E[Wp (t) u
(h)i (t + h) u
(h)j (t + h) Wp (t)′
]
= σij (h) E[Wp (t) Wp (t)′
]= σij (h) Γp , (3.5)
Γij(p, h, t− s) = 0 , if |t− s| ≥ h . (3.6)
In this case,1
∆p (h) = [σij (h) Γp]i, j=1, ... , m = Σ(h)⊗ Γp (3.7)
whereΣ(h) is nonsingular, and thus∆p (h) is also nonsingular. The nonsingularity ofΣ(h) followsfrom the identity
u(h) (t + h) =[ψh−1, ψh−2, . . . , ψ1, Im
] [a (t + 1)′ , a (t + 2)′ , . . . , a (t + h)′
]′.
Under usual regularity conditions,
1√T
T−h∑
t=0
vec[Wp (t) u(h) (t + h)′ ] L−→T→∞
N[0, ∆p (h)
](3.8)
where∆p (h) is a nonsingular covariance matrix which involves the variance and the autocovari-ances ofWp (t)u(h) (t + h)′ [and possibly other parameters, if the processW (t) is not linear].Then,
√T vec
[Π(h) −Π(h)
]=
Im ⊗
[1T
W p (h)′W p (h)]−1
vec
[1√T
W p (h)′ Uh (h)]
=
Im ⊗
[1T
W p (h)′W p (h)]−1
1√T
T−h∑
t=0
vec[Wp (t) u(h) (t + h)′
]
1Note that (3.5) holds under the assumption of martingale difference sequence ona (t) . But to get (3.6) and allow theuse of simpler central limit theorems, we maintain the stronger assumption that the innovationsa(t) are i.i.d. accordingto some distribution with finite fourth moments (not necessarily Gaussian).
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L−→T→∞
N[0,
(Im ⊗ Γ−1
p
)∆p (h)
(Im ⊗ Γ−1
p
) ]. (3.9)
For convenience, we shall summarize the above observations in the following proposition.
Proposition 3.1 ASYMPTOTIC NORMALITY OF LS IN A (p, h) STATIONARY VAR. Underthe assumptions(2.1), (3.2), and (3.8), the asymptotic distribution of
√T vec
[Π(h) − Π(h)
]is
N [0, Σ(Π(h))] , whereΣ(Π(h)) =(Im ⊗ Γ−1
p
)∆p (h)
(Im ⊗ Γ−1
p
).
4. Causality tests based on stationary(p, h)-autoregressions
Consider thei-th equation(1 ≤ i ≤ m) in system (2.11):
wi (h) = W p (h) βi (h) + ui (h) , 1 ≤ i ≤ m , (4.1)
wherewi (h) = wi (h, h) andui (h) = ui (h, h) , wherewi (h, h) andui (h, h) are defined in(2.12) and (2.15). We wish to test:
H0(h) : Rβi (h) = r (4.2)
whereR is a q × (n + mp) matrix of rankq. In particular, if we wish to test the hypothesis thatwjt does not causewit at horizonh [i.e., using the notation of Dufour and Renault (1998),wj 9
h
wi | I(j), whereI(j)(t) is the Hilbert space generated by the basic information setI(t) and thevariableswkτ , ω < τ ≤ t, k 6= j, ω being an appropriate starting time(ω ≤ −p + 1)], therestriction would take the form:
H(h)j9i : π
(h)ijk = 0 , k = 1, . . . , p , (4.3)
where π(h)k =
[π
(h)ijk
]i, j=1, ... , m
, k = 1, . . . , p . In other words, the null hypothesis takes
the form of a set of zero restrictions on the coefficients ofβi (h) as defined in (2.14).The matrix of restrictionsR in this case takes the formR = R(j), where R(j) ≡[δ1( j), δ2( j), . . . , δp( j)]′ is a p × (n + mp) matrix, δk( j) is a (n + pm) × 1 vector whoseelements are all equal to zero except for a unit value at positionn + (k − 1)m + j, i.e.δk( j) = [δ (1, n + (k − 1)m + j) , . . . , δ (n + pm, n + (k − 1)m + j)]′ , k = 1, . . . , p, withδ(i, j) = 1 if i = j, andδ(i, j) = 0 if i 6= j. Note also that the conjunction of the hypothesis
H(h)j9i, h = 1, . . . , (m − 2)p + 1, is sufficient to obtain noncausality at all horizons [see Dufour
and Renault (1998, section 4)]. Non-causality up to horizonH is the conjunction of the hypothesisH
(h)j9i, h = 1, . . . , H.
We have:βi (h) = βi (h) +
[W p (h)′W p (h)
]−1W p (h)′ ui (h) ,
9
hence
√T
[βi (h)− βi (h)
]=
[1T
W p (h)′W p (h)]−1 1√
T
T−h∑
t=0
Wp (t) u(h)i (t + h) .
Under standard regularity conditions [see White (1999, chap. 5-6)],
√T
[βi (h)− βi (h)
] L−→T→∞
N[0, V
(βi
)]
with det[V
(βi
)] 6= 0, whereV(βi
)can be consistently estimated:
VT
(βi
) p−→T→∞
V(βi
).
More explicit forms forVT
(βi
)will be discussed below. Note also that
Γp = plimT→∞
1T
W p (h)′W p (h) , det (Γp) 6= 0 .
Let
Vip (T ) = Var
[1√T
W p (h)′ ui (h)]
=1T
Var
[T−h∑
t=0
Wp (t)u(h)i (t + h)
]
=1T
T−h∑
t=0
E[Wp (t) u
(h)i (t + h)u
(h)i (t + h) Wp (t)′
]
+h−1∑
τ=1
T−h∑
t=τ+1
[E[Wp (t) u
(h)i (t + h)u
(h)i (t− τ + h) Wp (t− τ)′
]
+E[Wp (t− τ) u
(h)i (t− τ + h) u
(h)i (t + h) Wp (t)′
]].
Let us assume thatVip (T ) −→
T→∞Vip , det (Vip) 6= 0 , (4.4)
whereVip can be estimated by a computable consistent estimatorVip (T ) :
Vip (T )p−→
T→∞Vip . (4.5)
Then, √T
[βi (h)− βi (h)
]p−→
T→∞N
[0, Γ−1
p VipΓ−1p
]
10
so thatV(βi
)= Γ−1
p VipΓ−1p . Further, in this case,
VT
(βi
)= Γ−1
p Vip (T ) Γ−1p
p−→T→∞
V(βi
),
Γp =1T
T−h∑
t=0
Wp (t) Wp (t)′ =1T
W p (h)′W p (h)p−→
T→∞Γp .
We can thus state the following proposition.
Proposition 4.1 ASYMPTOTIC DISTRIBUTION OF TEST CRITERION FOR NON-CAUSALITY AT
HORIZON h IN A STATIONARY VAR. Suppose the assumptions of Proposition3.1hold jointly with(4.4)− (4.5). Then, under any hypothesis of the formH0(h) in (4.2), the asymptotic distribution of
W[H0(h)] = T[Rβi (h)− r
]′[RVT
(βi
)R′]−1[
Rβi (h)− r]
(4.6)
is χ2 (q). In particular, under the hypothesisH(h)j9i of non-causality at horizonh from wjt to
wit
(wj 9
hwi | I(j)
), the asymptotic distribution of the corresponding statisticW[H0(h)] is χ2 (p) .
The problem now consists in estimatingVip. Let ui (h) =[u
(h)i (t + h) : t = 0, . . . , T − h
]′
be the vector of OLS residuals from the regression (4.1),g(h)i (t + h) = Wp (t) u
(h)i (t + h) , and
set
R(h)i (τ) =
1T − h
T−h∑t=τ
g(h)i (t + h) g
(h)i (t + h− τ)′ , τ = 0, 1, 2, . . . .
If the innovations are i.i.d. or, more generally, if (3.6) holds, a natural estimator ofVip, which wouldtake into account the fact that the prediction errorsu(h) (t + h) follow an MA(h− 1) process, isgiven by:
V(W )ip (T ) = R
(h)i (0) +
h−1∑
τ=1
[R
(h)i (τ) + R
(h)i (τ)′
].
Under regularity conditions studied by White (1999, Section 6.3),
V(W )ip (T )− Vip
p−→T→∞
0.
A problem withV(W )ip (T ) is that it is not necessarily positive-definite.
An alternative estimator which is automatically positive-semidefinite is the one suggested byDoan and Litterman (1983), Gallant (1987) and Newey and West (1987):
V(NW )ip (T ) = R
(h)i (0) +
m(T )−1∑
τ=1
κ (τ , m (T ))[R
(h)i (τ) + R
(h)i (τ)′
], (4.7)
11
whereκ (τ , m) = 1− [τ/ (m + 1)] , limT→∞
m (T ) = ∞, and limT→∞
[m (T ) /T 1/4
]= 0 . Under the
regularity conditions given by Newey and West (1987),
V(NW )ip (T )− Vip −→
T→∞0 .
Other estimators that could be used here includes various heteroskedasticity-autocorrelation-consistent (HAC) estimators; see Andrews (1991), Andrews and Monahan (1992), Cribari-Neto,Ferrari and Cordeiro (2000), Cushing and McGarvey (1999), Den Haan and Levin (1997), Hansen(1992), Newey and McFadden (1994), Wooldridge (1989).
The cost of having a simple procedure that sidestep all the nonlinearities associated with thenon-causality hypothesis is a loss of efficiency. There are two places where we are not using allinformation. The constraints on theπ(h)
k ’s are giving information on theψj ’s and we are not usingit. We are also estimating the VAR by OLS and correcting the variance-covariance matrix insteadof doing a GLS-type estimation. These two sources of inefficiencies could potentially be overcomebut it would lead to less user-friendly procedures.
The asymptotic distribution provided by Proposition4.1, may not be very reliable in finite sam-ples, especially if we consider a VAR system with a large number of variables and/or lags. Due toautocorrelation, a larger horizon may also affect the size an power of the test. So an alternative tousing the asymptotic distribution chi-square ofW[H0(h)], consists in using Monte Carlo test tech-niques [see Dufour (2002)] or bootstrap methods [see, for example, Paparoditis (1996), Paparoditisand Streitberg (1991), Kilian (1998a, 1998b)]. In view of the fact that the asymptotic distribution ofW[H0(h)] is nuisance-parameter-free, such methods yield asymptotically valid tests when appliedto W[H0(h)] and typically provide a much better control of test level in finite samples. It is alsopossible that using better estimates would improve size control, although this is not clear, for impor-tant size distortions can occur in multivariate regressions even when unbiased efficient estimatorsare available [see, for example, Dufour and Khalaf (2002)].
5. Causality tests based on nonstationary(p, h)-autoregressions
In this section, we study how the tests described in the previous section can be adjusted in order toallow for non-stationary possibly integrated processes. In particular, let us assume that
W (t) = µ(t) + η(t) , (5.1)
µ(t) = δ0 + δ1t + · · ·+ δqtq , η (t) =
p∑
k=1
πkη (t− k) + a (t) , (5.2)
t = 1, . . . , T, whereδ0, δ1, . . . , δq arem × 1 fixed vectors, and the processη (t) is at mostI(d)whered is an integer greater than or equal to zero. Typical values ford are0, 1 or 2. Note that theseassumptions allow for the presence (or the absence) of cointegration relationships.
12
Under the above assumptions, we can also write:
W (t) = γ0 + γ1t + · · ·+ γqtq +
p∑
k=1
πkW (t− k) + a (t) , t = 1, . . . , T, (5.3)
whereγ0, γ1, . . . , γq arem× 1 fixed vectors (which depend onδ0, δ1, . . . , δq, andπ1, . . . , πp);see Toda and Yamamoto (1995). Under the specification (5.3), we have:
W (t + h) = µ(h)(t) +p∑
k=1
π(h)k W (t + 1− k) + u(h) (t + h) , t = 0, . . . , T − h. (5.4)
whereµ(h)(t) = γ(h)0 + γ
(h)1 t + · · ·+ γ
(h)q tq andγ
(h)0 , γ
(h)1 , . . . , γ
(h)q arem× 1 fixed vectors. For
h = 1, this equation is identical with (5.3). Forh ≥ 2, the errorsu(h) (t + h) follow a MA(h− 1)process as opposed to being i.i.d. . For any integerj, we have:
W (t + h) = µ(h)(t) +p∑
k=1k 6=j
π(h)k
[W (t + 1− k)−W (t + 1− j)
]
+
(p∑
k=1
π(h)k
)W (t + 1− j) + u(h) (t + h) , (5.5)
W (t + h)−W (t + 1− j) = µ(h)(t) +p∑
k=1k 6=j
π(h)k
[W (t + 1− k)−W (t + 1− j)
]
−(Im −
p∑
k=1
π(h)k
)W (t + 1− j) + u(h) (t + h) , (5.6)
for t = 0, . . . , T − h . The two latter expressions can be viewed as extensions to(p, h)-autoregressions of the representations used by Dolado and Lütkepohl (1996, pp. 372-373) forVAR(p) processes. Further, on takingj = p + 1 in (5.6), we see that
W (t + h)−W (t− p) = µ(h)(t) +p∑
k=1
A(h)k ∆W (t + 1− k)
+B(h)p W (t− p) + u(h) (t + h) (5.7)
where∆W (t) = W (t) −W (t − 1), A(h)k =
∑kj=1 π
(h)k ,andB
(h)k = A
(h)k − Im . Equation (5.7)
may be interpreted as an error-correction form at the horizonh,with baseW (t− p).
13
Let us now consider the extended autoregression
W (t + h) = µ(h)(t) +p∑
k=1
π(h)k W (t + 1− k) +
p+d∑
k=p+1
π(h)k W (t + 1− k) + u(h) (t + h) , (5.8)
t = d, . . . , T−h. Under model (5.3), the actual values of the coefficient matricesπ(h)p+1, . . . , π
(h)p+d
are equal to zero(π(h)p+1 = · · · = π
(h)p+d = 0), but we shall estimate the(p, h)-autoregressions
without imposing any restriction onπ(h)p+1, . . . , π
(h)p+d.
Now, suppose the processη (t) is eitherI(0) or I(1), and we taked = 1 in (5.8). Then, onreplacingp by p + 1 and settingj = p in the representation (5.6), we see that
W (t + h)−W (t− p− 1) = µ(h)(t) +p∑
k=1
π(h)k
[W (t + 1− k)−W (t− p− 1)
]
−B(h)p+1 W (t− p− 1) + u(h) (t + h) , (5.9)
whereB(h)p+1 =
(Im −
∑p+1k=1 π
(h)k
). In the latter equation,π(h)
1 , . . . , π(h)p all affect trend-stationary
variables (in an equation where a trend is included along with the other coefficients). Using argu-ments similar to those of Sims et al. (1990), Park and Phillips (1989) and Dolado and Lütkepohl(1996), it follows that the estimates ofπ
(h)1 , . . . , π
(h)p based on estimating (5.9) by ordinary least
squares (without restrictingB(h)p+1 ) _ or, equivalently, those obtained from (5.8) without restricting
π(h)p+1 _ are asymptotically normal with the same asymptotic covariance matrix as the one obtained
for a stationary process of the type studied in section 4.2 Consequently, the asymptotic distributionof the statisticW[H(h)
j9i] for testing the null hypothesisH(h)j9i of non-causality at horizonh from wj
to wi
(wj 9
hwi | I(j)
), based on estimating(5.8), is χ2(p). When computingH(h)
j9i as defined in
(4.3), it is important that only the coefficients ofπ(h)1 , . . . , π
(h)p are restricted (but notπ(h)
p+1).If the processη (t) is integrated up to orderd, whered ≥ 0, we can proceed similarly and addd
extra lags to the VAR process studied. Again, the null hypothesis is tested by considering the restric-tions entailed onπ(h)
1 , . . . , π(h)p . Further, in view of the fact the test statistics are asymptotically
pivotal under the null hypothesis, it is straightforward to apply bootstrap methods to such statistics.Note finally that the precision of the VAR estimates in such augmented regressions may eventuallybe improved with respect to the OLS estimates considered here by applying bias corrections suchas those proposed by Kurozumi and Yamamoto (2000)]. Adapting and applying such corrections to(p, h)-autoregressions would go beyond the scope of the present paper.
2For related results, see also Choi (1993), Toda and Yamamoto (1995), Yamamoto (1996), Yamada and Toda (1998),and Kurozumi and Yamamoto (2000).
14
Table 1. Rejection frequencies using the asymptotic distribution and the bootstrap procedurea) i.i.d. Gaussian sequence
h = 1 2 3 4 5 6 7 8 9 10 11 12
Asymptotic5% level 27.0 27.8 32.4 36.1 35.7 42.6 47.9 48.5 51.0 55.7 59.7 63.610% level 37.4 39.4 42.2 46.5 47.8 52.0 58.1 59.3 60.3 66.3 69.2 72.5
Bootstrap5% level 5.5 5.7 4.7 6.5 4.0 5.1 5.5 3.9 4.7 6.1 5.2 3.810% level 10.0 9.1 10.1 10.9 9.6 10.6 10.2 9.4 9.5 10.9 10.3 8.9
b) VAR(16) without causality up to horizonh
Asymptotic5% level 24.1 27.9 35.8 37.5 55.9 44.3 52.3 55.9 54.1 60.1 62.6 72.010% level 35.5 38.3 46.6 47.2 65.1 55.0 64.7 64.6 64.8 69.8 72.0 79.0
Bootstrap5% level 6.0 5.1 3.8 6.1 4.6 4.7 4.4 4.5 4.3 6.3 4.9 5.810% level 9.8 8.8 8.7 10.4 10.3 9.9 8.7 7.4 10.3 11.1 9.3 9.7
6. Empirical illustration
In this section, we present an application of these causality tests at various horizons to macroeco-nomic time series. The data set considered is the one used by Bernanke and Mihov (1998) in orderto study United States monetary policy. The data set considered consists of monthly observationson nonborrowed reserves (NBR, also denotedw1), the federal funds rate(r, w2), the GDP deflator(P, w3) and real GDP(GDP, w4). The monthly data on GDP and GDP deflator were constructedby state space methods from quarterly observations [see Bernanke and Mihov (1998) for more de-tails]. The sample goes from January 1965 to December 1996 for a total of 384 observations. Inwhat follows, all the variables were first transformed by a logarithmic transformation.
Before performing the causality tests, we must specify the order of the VAR model. First, inorder to get apparently stationary time series, all variables were transformed by taking first differ-ences of their logarithms. In particular, for the federal funds rate, this helped to mitigate the effectsof a possible break in the series in the years 1979-1981.3 Starting with 30 lags, we then tested thehypothesis ofK lags versusK + 1 lags using the LR test presented in Tiao and Box (1981). Thisled to a VAR(16) model. Tests of a VAR(16) against a VAR(K) for K = 17, . . . , 30 also failed toreject the VAR(16) specification, and the AIC information criterion [see McQuarrie and Tsai (1998,chapter 5)] is minimized as well by this choice. Calculations were performed using the Ox program(version 3.00) working on Linux [see Doornik (1999)].
3Bernanke and Mihov (1998) performed tests for arbitrary break points, as in Andrews (1993), and did not findsignificant evidence of a break point. They considered a VAR(13) with two additional variables (total bank reserves andDow-Jones index of spot commodity prices and they normalize both reserves by a 36-month moving average of totalreserves.)
15
Vector autoregressions of orderp at horizonh were estimated as described in section 4 andthe matrixV (NW )
ip , required to obtain covariance matrices, were computed using formula (4.7) withm(T )−1 = h−1.4 On looking at the values of the test statistics and their correspondingp-values atvarious horizons it quickly becomes evident that theχ2(q) asymptotic approximation of the statisticW in equation (4.6) is very poor. As a simple Monte Carlo experiment, we replaced the data bya 383 × 4 matrix of random draw from anN(0, 1), ran the same tests and looked at the rejectionfrequencies over 1000 replications using the asymptotic critical value. The results are in Table 1a.We see important size distortions even for the tests at horizon 1 where there is no moving averagepart.
We next illustrate that the quality of the asymptotic approximation is even worse when we moveaway from an i.i.d. Gaussian setup to a more realistic case. We now take as the DGP the VAR(16)estimated with our data in first difference but we impose that some coefficients are zero such that thefederal funds rate does not causeGDP up to horizonh and then we test ther 9
hGDP hypothesis.
The constraints of non-causality fromj to i up to horizonh that we impose are:
πijl = 0 for 1 ≤ l ≤ p , (6.1)
πikl = 0 for 1 ≤ l ≤ h, 1 ≤ k ≤ m. (6.2)
Rejection frequencies for this case are given in Table 1b.In light of these results we computed thep-values by doing a parametric bootstrap,i.e. doing
an asymptotic Monte Carlo test based on a consistent point estimate [see Dufour (2002)]. Theprocedure to test the hypothesiswj 9
hwi | I(j) is the following.
1. An unrestricted VAR(p) model is fitted for the horizon one, yielding the estimatesΠ(1) andΩ for Π(1) andΩ .
2. An unrestricted(p, h)-autoregression is fitted by least squares, yielding the estimateΠ(h) ofΠ(h).
3. The test statisticW for testing noncausality at the horizonh from wj to wi
[H
(h)j9i : wj 9
h
wi | I(j)
]is computed. We denote byW(h)
j9i(0) the test statistic based on the actual data.
4. N simulated samples from (2.8) are drawn by Monte Carlo methods, usingΠ(h) = Π(h) andΩ = Ω [and the hypothesis thata(t) is Gaussian]. We impose the constraints of non-causality,
π(h)ijk = 0, k = 1, . . . , p. Estimates of the impulse response coefficients are obtained from
Π(1) through the relations described in equation (2.5). We denote byW(h)j9i(n) the test statis-
tic for H(h)j9i based on then-th simulated sample(1 ≤ n ≤ N).
4The covariance estimator used here is relatively simple and exploits the truncation property (3.6). In view of the vastliterature on HAC estimators [see Den Haan and Levin (1997) and Cushing and McGarvey (1999)], several alternativeestimators forVip could have been considered (possibly allowing for alternative assumptions on the innovation distribu-tion). It would certainly be of interest to compare the performances of alternative covariance estimators, but this wouldlead to a lengthy study, beyond the scope of the present paper.
16
5. The simulatedp-valuepN [W(h)j9i(0)] is obtained, where
pN [x] =
1 +
N∑
n=1
I[W(h)j9i(n)− x]
/(N + 1) ,
I[z] = 1 if z ≥ 0 andI[z] = 0 if z < 0.
6. The null hypothesisH(h)j9i is rejected at levelα if pN [W(0)
j9i(h)] ≤ α.
From looking at the results in Table 1, we see that we get a much better size control by usingthis bootstrap procedure. The rejection frequencies over 1000 replications (withN = 999) are veryclose to the nominal size. Although the coefficientsψj ’s are functions of theπi’s we do not constrain
them in the bootstrap procedure because there is no direct mapping fromπ(h)k to πk andψj . This
certainly produces a power loss but the procedure remains valid because theψj ’s are computed withtheπk, which are consistent estimates of the trueπk both under the null and alternative hypothesis.To illustrate that our procedure has power for detecting departure from the null hypothesis of non-causality at a given horizon we ran the following Monte Carlo experiment. We again took a VAR(16)fitted on our data in first differences and we imposed the constraints (6.1) - (6.2) so that there wasno causality fromr to GDP up to horizon 12 (DGP under the null hypothesis). Next the value ofone coefficient previously set to zero was changed to induce causality fromr to GDP at horizons4 and higher:π3(1, 3) = θ . As θ increases from zero to one the strength of the causality fromrto GDP is higher. Under this setup, we could compute the power of our simulated test procedureto reject the null hypothesis of non-causality at a given horizon. In Figure 1, the power curves areplotted as a function ofθ for the various horizons. The level of the tests was controlled through thebootstrap procedure. In this experiment we took againN = 999 and we did 1000 simulations. Asexpected, the power curves are flat at around 5% for horizons one to three since the null is true forthese horizons. For horizons four and up we get the expected result that power goes up asθ movesfrom zero to one, and the power curves gets flatter as we increase the horizon.
Now that we have shown that our procedure does have power we present causality tests athorizon one to 24 for every pair of variables in tables 2 and 3. For every horizon we have twelvecausality tests and we group them by pairs. When we say that a given variable cause or does notcause another, it should be understood that we mean the growth rate of the variables. Thep-valuesare computed by takingN = 999. Table 4 summarize the results by presenting the significantresults at the 5% and 10% level.
The first thing to notice is that we have significant causality results at short horizons for somepairs of variables while we have it at longer horizons for other pairs. This is an interesting illustrationof the concept of causality at horizonh of Dufour and Renault (1998).
The instrument of the central bank, the nonborrowed reserves, cause the federal funds rate athorizon one, the prices at horizon 1, 2, 3 and 9 (10% level). It does not cause the other two variablesat any horizon and except the GDP at horizon 12 and 16 (10% level) nothing is causing it. We seethat the impact of variations in the nonborrowed reserves is over a very short term. Another variable,the GDP, is also causing the federal funds rates over short horizons (one to five months).
17
0.0 0.5 1.0
50
100horizon 1
0.0 0.5 1.0
50
100horizon 2
0.0 0.5 1.0
50
100horizon 3
0.0 0.5 1.0
50
100horizon 4
0.0 0.5 1.0
50
100horizon 5
0.0 0.5 1.0
50
100horizon 6
0.0 0.5 1.0
50
100horizon 7
0.0 0.5 1.0
50
100horizon 8
0.0 0.5 1.0
50
100horizon 9
0.0 0.5 1.0
50
100horizon 10
0.0 0.5 1.0
50
100horizon 11
0.0 0.5 1.0
50
100horizon 12
Figure 1. Power of the test at the 5% level for given horizons.The abscissa (x axis) represents the values ofθ.
18
Tabl
e2.
Cau
salit
yte
sts
and
sim
ulat
edp-va
lues
for
serie
sin
first
diffe
renc
es(o
flog
arith
m)
for
the
horiz
ons
1to
12.
p-v
alue
sar
ere
port
edin
pare
nthe
sis.
h1
23
45
67
89
1011
12N
BR
9r
38.5
205
26.3
851
24.3
672
22.5
684
24.2
294
27.0
748
21.4
347
17.2
164
21.8
217
18.4
775
18.5
379
19.6
482
(0.0
41)
(0.2
40)
(0.3
27)
(0.3
95)
(0.3
79)
(0.3
13)
(0.5
50)
(0.7
99)
(0.6
03)
(0.7
80)
(0.8
24)
(0.7
89)
r9
NB
R22
.539
020
.862
117
.235
717
.422
217
.894
418
.646
225
.205
940
.989
641
.688
238
.165
641
.220
336
.127
8(0
.386
)(0
.467
)(0
.706
)(0
.738
)(0
.734
)(0
.735
)(0
.495
)(0
.115
)(0
.142
)(0
.214
)(0
.206
)(0
.346
)N
BR
9P
50.5
547
45.2
498
49.1
408
33.8
545
33.8
943
35.3
923
39.1
767
40.0
218
36.4
089
39.0
916
28.4
933
26.5
439
(0.0
04)
(0.0
14)
(0.0
09)
(0.1
21)
(0.1
62)
(0.1
57)
(0.0
99)
(0.1
41)
(0.2
34)
(0.2
02)
(0.4
85)
(0.6
09)
P9
NB
R17
.069
618
.950
416
.688
021
.238
128
.726
420
.035
918
.229
123
.670
423
.341
927
.842
730
.917
136
.515
9(0
.689
)(0
.601
)(0
.741
)(0
.550
)(0
.307
)(0
.664
)(0
.771
)(0
.596
)(0
.649
)(0
.492
)(0
.462
)(0
.357
)N
BR
9G
DP
27.8
029
25.0
122
25.5
123
23.6
799
15.0
040
17.5
748
16.6
781
19.6
643
29.9
020
34.0
930
32.3
917
34.8
183
(0.1
84)
(0.3
02)
(0.2
94)
(0.3
93)
(0.8
30)
(0.7
57)
(0.7
90)
(0.7
46)
(0.3
68)
(0.3
00)
(0.3
70)
(0.3
57)
GD
P9
NB
R17
.633
820
.656
824
.533
418
.322
018
.312
332
.874
633
.997
939
.670
140
.735
626
.342
440
.226
253
.348
2(0
.644
)(0
.520
)(0
.348
)(0
.670
)(0
.682
)(0
.211
)(0
.242
)(0
.145
)(0
.161
)(0
.551
)(0
.216
)(0
.092
)r
9P
32.2
481
32.9
207
32.0
362
25.0
124
25.2
441
25.8
110
29.2
553
29.6
021
36.0
771
43.2
116
30.2
530
20.8
982
(0.1
04)
(0.1
08)
(0.1
38)
(0.3
42)
(0.3
83)
(0.3
94)
(0.3
28)
(0.3
51)
(0.2
41)
(0.1
38)
(0.4
22)
(0.7
63)
P9
r22
.438
516
.445
514
.307
314
.293
214
.014
816
.713
811
.559
916
.573
113
.069
714
.575
915
.031
724
.407
7(0
.413
)(0
.670
)(0
.790
)(0
.826
)(0
.844
)(0
.774
)(0
.951
)(0
.809
)(0
.936
)(0
.909
)(0
.899
)(0
.659
)r
9G
DP
26.3
362
28.6
645
35.9
768
38.8
680
37.6
788
39.8
145
64.1
500
80.2
396
89.6
998
101.
4143
105.
9138
110.
3551
(0.2
62)
(0.1
59)
(0.0
73)
(0.0
59)
(0.0
82)
(0.0
79)
(0.0
06)
(0.0
02)
(0.0
02)
(0.0
02)
(0.0
01)
(0.0
03)
GD
P9
r42
.532
743
.007
849
.836
641
.108
241
.794
536
.096
529
.547
225
.789
827
.980
739
.636
639
.047
740
.154
5(0
.016
)(0
.017
)(0
.005
)(0
.033
)(0
.044
)(0
.109
)(0
.263
)(0
.429
)(0
.366
)(0
.148
)(0
.178
)(0
.205
)P
9G
DP
20.6
903
24.1
099
27.4
106
23.3
585
22.9
095
18.5
543
20.8
172
23.6
942
30.5
340
28.8
286
24.9
477
25.7
552
(0.4
95)
(0.3
22)
(0.2
33)
(0.4
23)
(0.4
97)
(0.7
13)
(0.6
39)
(0.5
55)
(0.3
75)
(0.4
14)
(0.6
12)
(0.6
29)
GD
P9
P24
.336
824
.492
524
.612
522
.816
026
.790
040
.082
536
.485
549
.616
146
.257
436
.319
726
.852
024
.011
3(0
.329
)(0
.365
)(0
.380
)(0
.470
)(0
.348
)(0
.081
)(0
.157
)(0
.058
)(0
.072
)(0
.262
)(0
.540
)(0
.666
)
19
Tabl
e3.
Cau
salit
yte
sts
and
sim
ulat
edp-va
lues
for
serie
sin
first
diffe
renc
es(o
flog
arith
m)
for
the
horiz
ons
13to
24
h13
1415
1617
1819
2021
2223
24N
BR
9r
20.7
605
21.1
869
18.6
062
17.6
750
22.2
838
34.0
098
28.7
769
33.7
855
66.1
538
38.7
272
28.8
194
34.8
015
(0.7
83)
(0.7
71)
(0.8
52)
(0.9
05)
(0.8
11)
(0.5
32)
(0.6
96)
(0.6
32)
(0.1
43)
(0.5
58)
(0.8
03)
(0.7
08)
r9
NB
R42
.292
443
.819
632
.811
328
.177
531
.232
631
.758
725
.694
234
.668
037
.747
051
.419
633
.289
727
.336
2(0
.245
)(0
.254
)(0
.533
)(0
.707
)(0
.625
)(0
.651
)(0
.832
)(0
.682
)(0
.625
)(0
.406
)(0
.755
)(0
.869
)N
BR
9P
38.0
451
39.0
293
43.2
101
37.9
049
22.4
428
20.0
337
38.8
919
66.1
541
55.0
460
64.8
568
54.8
929
42.2
509
(0.3
36)
(0.3
51)
(0.3
15)
(0.4
13)
(0.8
35)
(0.8
83)
(0.4
88)
(0.1
49)
(0.2
55)
(0.1
80)
(0.3
32)
(0.5
62)
P9
NB
R29
.545
729
.454
327
.242
528
.754
731
.485
144
.125
436
.031
947
.160
850
.274
345
.807
854
.196
156
.786
5(0
.565
)(0
.667
)(0
.688
)(0
.703
)(0
.627
)(0
.400
)(0
.581
)(0
.427
)(0
.379
)(0
.486
)(0
.401
)(0
.399
)N
BR
9G
DP
30.3
906
25.2
694
29.7
274
23.3
347
16.7
784
18.7
922
26.8
942
30.2
550
39.0
652
43.6
661
56.9
724
67.7
764
(0.4
93)
(0.7
16)
(0.6
03)
(0.8
14)
(0.9
42)
(0.9
01)
(0.7
52)
(0.7
45)
(0.5
45)
(0.5
05)
(0.3
14)
(0.2
51)
GD
P9
NB
R44
.226
441
.579
559
.330
165
.764
753
.357
950
.464
551
.516
343
.113
240
.705
136
.396
038
.716
240
.846
6(0
.219
)(0
.292
)(0
.106
)(0
.086
)(0
.225
)(0
.282
)(0
.311
)(0
.466
)(0
.513
)(0
.659
)(0
.665
)(0
.644
)r
9P
27.3
588
37.7
170
37.2
499
37.1
005
27.3
052
35.4
128
39.2
469
53.2
675
57.1
530
54.6
753
69.6
377
59.2
184
(0.5
88)
(0.3
41)
(0.3
81)
(0.4
43)
(0.7
00)
(0.5
34)
(0.4
77)
(0.2
66)
(0.2
29)
(0.3
14)
(0.1
64)
(0.2
93)
P9
r22
.372
026
.358
828
.493
023
.015
226
.421
136
.363
234
.392
217
.426
916
.965
231
.933
628
.837
730
.001
3(0
.750
)(0
.608
)(0
.633
)(0
.794
)(0
.747
)(0
.512
)(0
.536
)(0
.956
)(0
.958
)(0
.715
)(0
.801
)(0
.795
)r
9G
DP
123.
8280
80.3
638
95.0
727
83.2
773
76.6
169
84.1
068
76.8
979
81.3
505
65.5
025
71.3
334
63.1
942
64.8
020
(0.0
01)
(0.0
18)
(0.0
05)
(0.0
18)
(0.0
33)
(0.0
40)
(0.0
55)
(0.0
73)
(0.1
61)
(0.1
53)
(0.2
41)
(0.2
86)
GD
P9
r35
.708
633
.020
040
.171
330
.322
720
.558
219
.114
417
.738
622
.641
038
.817
538
.711
038
.998
725
.057
7(0
.319
)(0
.420
)(0
.273
)(0
.545
)(0
.838
)(0
.898
)(0
.930
)(0
.856
)(0
.515
)(0
.565
)(0
.549
)(0
.860
)P
9G
DP
9.42
909.
9870
12.1
148
15.1
682
14.2
883
21.2
701
29.0
528
47.5
841
66.5
988
59.2
137
71.5
165
67.1
851
(0.9
88)
(0.9
94)
(0.9
74)
(0.9
47)
(0.9
70)
(0.8
68)
(0.7
08)
(0.3
63)
(0.1
62)
(0.2
56)
(0.1
65)
(0.2
31)
GD
P9
P29
.764
237
.009
533
.467
642
.219
031
.157
352
.375
751
.956
740
.379
031
.659
854
.068
465
.828
453
.082
3(0
.521
)(0
.351
)(0
.470
)(0
.328
)(0
.605
)(0
.238
)(0
.226
)(0
.459
)(0
.675
)(0
.244
)(0
.215
)(0
.342
)
20
Table 4. Summary of causality relations at various horizons for series in first difference
h 1 2 3 4 5 6 7 8 9 10 11 12NBR 9 r ??
r 9 NBR
NBR 9 P ?? ?? ?? ?P 9 NBR
NBR 9 GDPGDP 9 NBR ?
r 9 PP 9 r
r 9 GDP ? ? ? ? ?? ?? ?? ?? ?? ??GDP 9 r ?? ?? ?? ?? ??
P 9 GDPGDP 9 P ? ? ?
h 13 14 15 16 17 18 19 20 21 22 23 24NBR 9 r
r 9 NBR
NBR 9 PP 9 NBR
NBR 9 GDPGDP 9 NBR ?
r 9 PP 9 r
r 9 GDP ?? ?? ?? ?? ?? ?? ? ?GDP 9 r
P 9 GDPGDP 9 P
Note _ The symbols? and?? indicate rejection of the non-causality hypothesis at the 10% and 5%levels respectively.
An interesting result is the causality from the federal funds rate to the GDP. Over the first fewmonths the funds rate does not cause GDP, but from horizon 3 (up to 20) we do find significantcausality. This result can easily be explained by, e.g. the theory of investment. Notice that wehave the following indirect causality. Nonborrowed reserves do not cause GDP directly over anyhorizon, but they cause the federal funds rate which in turn causes GDP. Concerning the observationthat there are very few causality results for long horizons, this may reflect the fact that, for stationaryprocesses, the coefficients of prediction formulas converge to zero as the forecast horizon increases.
Using the results of Proposition 4.5 in Dufour and Renault (1998), we know that for this examplethe highest horizon that we have to consider is 33 since we have a VAR(16) with four time series.Causality tests for the horizons 25 through 33 were also computed but are not reported. Somep-values smaller or equal to 10% are scattered over horizons 30 to 33 but no discernible patternemerges.
We next consider extended autoregressions to illustrate the results of section 5. To cover thepossibility that the first difference of the logarithm of the four series may not be stationary, we ranextended autoregressions on the series analyzed. Since we used a VAR(16) with non-zero mean for
21
the first difference of the series a VAR(17),i.e. d = 1, with a non-zero mean was fitted. The MonteCarlo samples withN = 999 are drawn in the same way as before except that the constraints on theVAR parameters at horizonh is π
(h)jik = 0 for k = 1, . . . , p and notk = 1, . . . , p + d.
Results of the extended autoregressions are presented in Table 5 (horizons 1 to 12) and 6 (hori-zons 13 to 24). Table 7 summarize these results by presenting the significant results at the 5% and10% level. These results are very similar to the previous ones over all the horizons and variableevery pairs. A few causality tests are not significant anymore (GDP 9 r at horizon 5,r 9 GDPat horizons 5 and 6) and some causality relations are now significant (r 9 P at horizon one) but webroadly have the same causality patterns.
7. Conclusion
In this paper, we have proposed a simple linear approach to the problem of testing non-causalityhypotheses at various horizons in finite-order vector autoregressive models. The methods describedallow for both stationary (or trend-stationary) processes and possibly integrated processes (whichmay involve unspecified cointegrating relationships), as long as an upper bound is set on the orderof integration. Further, we have shown that these can be easily implemented in the context of afour-variable macroeconomic model of the U.S. economy.
Several issues and extensions of interest warrant further study. The methods we have proposedwere, on purpose, designed to be relatively simple to implement. This may, of course, involve ef-ficiency losses and leave room for improvement. For example, it seems quite plausible that moreefficient tests may be obtained by testing directly the nonlinear causality conditions described inDufour and Renault (1998) from the parameter estimates of the VAR model. However, such proce-dures will involve difficult distributional problems and may not be as user-friendly as the proceduresdescribed here. Similarly, in nonstationary time series, information about integration order and thecointegrating relationships may yield more powerful procedures, although at the cost of complexity.These issues are the topics of on-going research.
Another limitation comes from the fact we consider VAR models with a known finite order. Weshould however note that the asymptotic distributional results established in this paper continue tohold as long as the orderp of the model is selected according to a consistent order selection rule [seeDufour, Ghysels and Hall (1994), Pötscher (1991)]. So this is not an important restriction. Otherproblems of interest would consist in deriving similar tests applicable in the context of VARMAor VARIMA models, as well as more general infinite-order vector autoregressive models, usingfinite-order VAR approximations based on data-dependent truncation rules [such as those used byLütkepohl and Poskitt (1996) and Lütkepohl and Saikkonen (1997)]. These problems are also thetopics of on-going research.
22
Tabl
e5.
Cau
salit
yte
sts
and
sim
ulat
edp-va
lues
for
exte
nded
auto
regr
essi
ons
atth
eho
rizon
s1
to12
h1
23
45
67
89
1011
12N
BR
9r
37.4
523
24.0
148
24.9
365
22.9
316
25.4
508
26.6
763
19.5
377
19.3
805
21.9
278
19.8
541
21.2
947
19.5
569
(0.0
51)
(0.3
37)
(0.3
09)
(0.4
10)
(0.3
33)
(0.3
33)
(0.6
60)
(0.6
88)
(0.6
09)
(0.7
16)
(0.7
10)
(0.7
95)
r9
NB
R25
.918
517
.797
716
.618
517
.382
019
.642
520
.203
239
.849
644
.017
243
.992
839
.421
736
.780
235
.088
3(0
.281
)(0
.650
)(0
.747
)(0
.759
)(0
.673
)(0
.676
)(0
.129
)(0
.075
)(0
.130
)(0
.207
)(0
.286
)(0
.375
)N
BR
9P
50.8
648
44.8
472
56.5
028
33.8
112
36.1
026
42.1
714
38.7
204
38.8
076
35.3
353
33.8
049
28.6
205
26.9
863
(0.0
04)
(0.0
15)
(0.0
07)
(0.1
52)
(0.1
24)
(0.0
61)
(0.1
52)
(0.1
61)
(0.2
59)
(0.3
16)
(0.4
98)
(0.6
09)
P9
NB
R20
.749
117
.277
216
.389
126
.161
029
.732
918
.758
322
.782
123
.174
327
.007
624
.376
331
.186
938
.334
9(0
.506
)(0
.704
)(0
.764
)(0
.339
)(0
.276
)(0
.730
)(0
.605
)(0
.629
)(0
.508
)(0
.655
)(0
.484
)(0
.336
)N
BR
9G
DP
27.2
102
23.8
072
25.9
561
24.3
384
14.4
893
17.8
928
15.9
036
17.9
592
30.7
472
33.5
333
33.7
687
36.3
343
(0.2
24)
(0.3
46)
(0.3
17)
(0.4
02)
(0.8
37)
(0.7
32)
(0.8
21)
(0.8
17)
(0.3
68)
(0.3
33)
(0.3
55)
(0.3
48)
GD
P9
NB
R16
.132
219
.447
120
.679
819
.103
529
.122
936
.105
337
.119
440
.357
843
.783
537
.733
748
.300
452
.244
2(0
.746
)(0
.571
)(0
.537
)(0
.658
)(0
.269
)(0
.166
)(0
.167
)(0
.163
)(0
.138
)(0
.247
)(0
.125
)(0
.123
)r
9P
32.5
147
31.2
909
25.6
717
24.4
449
21.7
640
25.4
747
27.6
313
31.4
581
43.2
611
38.2
020
30.6
394
19.9
687
(0.1
00)
(0.1
28)
(0.3
52)
(0.3
90)
(0.5
68)
(0.3
97)
(0.3
53)
(0.3
11)
(0.1
11)
(0.2
12)
(0.4
20)
(0.8
12)
P9
r22
.737
415
.945
315
.200
115
.193
316
.233
415
.747
213
.419
615
.250
614
.432
415
.858
921
.363
721
.994
9(0
.415
)(0
.704
)(0
.762
)(0
.790
)(0
.768
)(0
.830
)(0
.905
)(0
.859
)(0
.909
)(0
.887
)(0
.749
)(0
.731
)r
9G
DP
27.0
435
29.5
913
37.5
271
35.7
130
34.9
901
35.1
715
79.9
402
92.6
009
94.9
068
107.
6638
108.
0581
138.
0570
(0.2
44)
(0.1
58)
(0.0
61)
(0.0
94)
(0.1
17)
(0.1
64)
(0.0
02)
(0.0
01)
(0.0
04)
(0.0
01)
(0.0
03)
(0.0
01)
GD
P9
r41
.847
541
.944
944
.759
738
.035
830
.477
628
.184
030
.586
727
.074
526
.587
639
.950
239
.861
833
.485
5(0
.032
)(0
.019
)(0
.019
)(0
.060
)(0
.209
)(0
.286
)(0
.250
)(0
.369
)(0
.431
)(0
.157
)(0
.181
)(0
.347
)P
9G
DP
23.7
424
26.7
148
24.6
605
24.6
507
23.3
233
19.8
483
20.3
581
28.9
318
29.0
384
27.2
509
26.3
318
22.6
991
(0.3
68)
(0.2
37)
(0.3
42)
(0.3
73)
(0.4
79)
(0.6
68)
(0.6
66)
(0.3
76)
(0.4
27)
(0.5
05)
(0.5
58)
(0.7
40)
GD
P9
P25
.126
424
.194
125
.568
319
.212
737
.598
438
.031
837
.625
445
.221
945
.245
836
.991
223
.168
722
.993
4(0
.278
)(0
.358
)(0
.350
)(0
.639
)(0
.108
)(0
.110
)(0
.153
)(0
.088
)(0
.092
)(0
.237
)(0
.647
)(0
.698
)
23
Tabl
e6.
Cau
salit
yte
sts
and
sim
ulat
edp-va
lues
for
exte
nded
auto
regr
essi
ons
atth
eho
rizon
s13
to24
h13
1415
1617
1819
2021
2223
24N
BR
9r
19.5
845
30.2
847
17.4
893
24.9
745
21.2
814
27.4
800
36.9
567
27.8
970
59.3
731
34.9
153
27.3
241
31.9
143
(0.8
14)
(0.5
13)
(0.9
01)
(0.7
50)
(0.8
58)
(0.7
06)
(0.5
37)
(0.7
70)
(0.2
36)
(0.6
40)
(0.8
32)
(0.7
71)
r9
NB
R41
.736
047
.850
130
.961
329
.180
935
.765
422
.996
629
.086
929
.139
638
.067
552
.551
229
.613
325
.487
2(0
.282
)(0
.212
)(0
.592
)(0
.692
)(0
.540
)(0
.847
)(0
.757
)(0
.766
)(0
.665
)(0
.401
)(0
.838
)(0
.917
)N
BR
9P
36.7
787
37.7
357
33.4
273
35.3
241
20.6
330
23.6
911
44.5
735
55.5
420
53.7
340
68.0
270
52.3
332
47.5
614
(0.3
59)
(0.3
66)
(0.5
12)
(0.4
55)
(0.8
60)
(0.8
25)
(0.3
79)
(0.2
49)
(0.2
90)
(0.1
65)
(0.3
63)
(0.4
81)
P9
NB
R29
.504
939
.207
618
.083
130
.648
639
.551
734
.836
339
.960
843
.656
340
.671
344
.025
461
.691
462
.934
6(0
.582
)(0
.401
)(0
.920
)(0
.671
)(0
.441
)(0
.606
)(0
.535
)(0
.471
)(0
.551
)(0
.553
)(0
.296
)(0
.286
)N
BR
9G
DP
30.9
525
22.0
737
30.1
165
22.7
429
17.2
546
22.2
686
28.6
752
31.8
817
39.5
031
53.6
466
58.8
413
79.0
569
(0.5
01)
(0.8
22)
(0.5
99)
(0.7
93)
(0.9
37)
(0.8
63)
(0.7
49)
(0.7
17)
(0.5
91)
(0.3
67)
(0.3
27)
(0.1
53)
GD
P9
NB
R46
.453
838
.042
464
.226
960
.879
257
.579
857
.223
742
.085
143
.168
343
.437
941
.714
139
.829
241
.712
3(0
.186
)(0
.347
)(0
.071
)(0
.125
)(0
.169
)(0
.205
)(0
.453
)(0
.491
)(0
.501
)(0
.568
)(0
.631
)(0
.632
)r
9P
30.7
883
37.3
585
30.4
331
35.8
788
26.9
960
39.2
961
44.7
334
46.6
740
56.9
680
53.1
830
67.3
818
61.2
522
(0.5
03)
(0.3
64)
(0.5
66)
(0.4
48)
(0.7
12)
(0.4
29)
(0.3
58)
(0.3
52)
(0.2
23)
(0.3
10)
(0.1
82)
(0.2
41)
P9
r25
.308
533
.102
728
.736
233
.575
833
.899
139
.303
129
.422
814
.309
517
.858
829
.957
225
.034
729
.190
3(0
.654
)(0
.450
)(0
.624
)(0
.546
)(0
.525
)(0
.451
)(0
.707
)(0
.984
)(0
.957
)(0
.764
)(0
.883
)(0
.825
)r
9G
DP
109.
5052
84.9
556
88.4
433
80.9
836
79.9
549
75.1
199
94.8
986
65.5
929
67.2
913
71.6
331
75.5
123
67.4
315
(0.0
02)
(0.0
11)
(0.0
21)
(0.0
16)
(0.0
31)
(0.0
73)
(0.0
26)
(0.1
47)
(0.1
36)
(0.1
64)
(0.1
51)
(0.2
54)
GD
P9
r34
.818
541
.421
838
.276
128
.532
622
.611
616
.799
220
.809
731
.876
938
.708
334
.466
335
.627
920
.500
7(0
.340
)(0
.264
)(0
.318
)(0
.606
)(0
.809
)(0
.923
)(0
.866
)(0
.644
)(0
.519
)(0
.649
)(0
.637
)(0
.949
)P
9G
DP
8.80
398.
9511
17.0
182
9.76
0816
.477
219
.694
246
.324
041
.742
964
.592
860
.287
556
.031
572
.282
3(0
.995
)(0
.995
)(0
.933
)(0
.995
)(0
.923
)(0
.916
)(0
.349
)(0
.484
)(0
.207
)(0
.250
)(0
.332
)(0
.215
)G
DP
9P
23.8
773
39.5
163
34.3
832
34.5
734
36.8
350
54.8
088
54.8
048
36.4
102
29.4
543
58.0
095
58.1
341
59.5
283
(0.7
09)
(0.3
31)
(0.4
68)
(0.4
88)
(0.4
72)
(0.2
12)
(0.2
18)
(0.5
57)
(0.7
39)
(0.2
54)
(0.2
65)
(0.2
86)
24
Table 7. Summary of causality relations at various horizons for series in first difference withextended autoregressions
h 1 2 3 4 5 6 7 8 9 10 11 12NBR 9 r ?
r 9 NBR ?
NBR 9 P ?? ?? ?? ?P 9 NBR
NBR 9 GDPGDP 9 NBR
r 9 P ?P 9 r
r 9 GDP ? ? ?? ?? ?? ?? ?? ??GDP 9 r ?? ?? ?? ?
P 9 GDPGDP 9 P ? ?
h 13 14 15 16 17 18 19 20 21 22 23 24NBR 9 r
r 9 NBR
NBR 9 PP 9 NBR
NBR 9 GDPGDP 9 NBR ?
r 9 PP 9 r
r 9 GDP ?? ?? ?? ?? ?? ? ??GDP 9 r
P 9 GDPGDP 9 P
Note _ The symbols? and?? indicate rejection of the non-causality hypothesis at the 10% and 5%levels respectively.
25
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