Non-Identiability of VMA and VARMA Systems in the Mixed Frequency Case 1 2 3 Manfred Deistler , Lukas Koelbl , Brian D.O. Anderson Abstract This paper is concerned with results on non-identiability of VMA and VARMA systems from mixed frequency data. Recently, identiability results for VAR systems have been shown in a number of papers. These results have been extended to VARMA systems, where the MA order is smaller than or equal to the AR order. In this paper we show that in the VMA case and in the VARMA case, where the MA order exceeds the AR order, results are completely dierent. Then, for the case, where the innovation covariance matrix is non-singular, we typically have non-identiability - not even local identiability. This is due to the fact that, e.g., in the VMA case, as opposed to the VAR case, the not directly observed autocovariances of the output can vary freely. In the singular case, i.e., when the innovation covariance matrix is singular, things may be dierent. Keywords: VARMA, VMA, mixed frequency, non-identiability 1 Corresponding author. Manfred Deistler is with the Institute of Statistics and Mathemat- ical Methods in Economics, Vienna University of Technology, Vienna, Austria, and Institute for Advanced Studies, Vienna, Austria, e-mail: [email protected]. 2 Lukas Koelbl is with the Institute of Statistics and Mathematical Methods in Economics, Vienna University of Technology, Vienna, Austria, e-mail: [email protected] 3 Brian D.O. Anderson is with the Research School of Engineering, Australian National University, Canberra, Australia, and Canberra Research Laboratory, National ICT Australia Ltd., e-mail: [email protected] Preprint submitted to Elsevier July 8, 2016 1. Introduction In many applications we encounter mixed frequency (MF) data in multivariate time series, i.e., the univariate component processes often are available only at dierent sampling frequencies. Problems associated with MF data have been considered, e.g., in Nijman [15], Kohn and Ansley [13], Chen and Zadrozny [5], Ghysels et al. [8], Wohlrabe [17], Marcellino and Schumacher [14], Foroni and Marcellino [6], Ghysels [7]. Here, we are interested in the problem of retrieving the parameters of the underlying high frequency system, i.e., the system generating the output at the highest sampling frequency available in the data, from MF data and, in particular, in identiability. Many papers dealing with mixed frequency data use the framework of VAR systems. G(eneric)-identiability from MF data has been shown in Anderson et al. [3, 2] for the case of VAR systems and in Anderson et al. [4], Zadrozny [18] for the case of VARMA systems, where the MA order is smaller than or equal to the AR order. Here, we show that the situation is completely dierent in case of VMA systems and of VARMA systems with MA order exceeding the AR order. This is a consequence of the fact that non-observed autocovariances of the VMA output process can freely vary in a certain neighborhood without violating the assumptions. For the VARMA case considered here, this is true for special non-observed autocovariances. In Section 2 we give a detailed analysis of non-identiability of VMA systems from MF data for the case of stock as well as for the case of ow variables. In Section 3 we show non-identiability for the VARMA case, where the MA order exceeds the AR order. Whereas Section 2 and 3 deal with the case, where the innovation variance matrix is non-singular, Section 4 gives generic identiability results for the case, where the innovation variance matrix is singular with rank being suciently small. 2 2. High Frequency VMA Systems and MF Data: Non-Identiability Results We consider (high frequency) multivariate MA(r) systems of the form t∈Z yt = νt + B1 νt−1 + ... + Br νt−r , where r is a specied integer, T Σ = E νt νt . Bi ∈ Rn×n and (νt |t ∈ Z) (2.1) is white noise with In addition, we impose the strict miniphase condition det b(z) 6= 0, |z| ≤ 1 (2.2) where b(z) = In + B1 z + ... + Br z r is the corresponding VMA transfer function. We use well as for the backward shift on Z. z (2.3) for a complex variable as In this and in the next section we assume that q = rank (Σ) = n (2.4) holds. The VMA parameter space considered is of the form ΘMA = n o 2 ∈ Rn r | det b(z) 6= 0, |z| ≤ 1 × | {z } SMA n o n(n+1) 2 vech (Σ) ∈ R | Σ = ΣT , Σ > 0 . | {z } vec (B1 , . . . , Br ) Σ Before going into the details let us outline the basic ideas in the ow of arguments behind Lemma 1, Theorem 1, Theorem 2 and Theorem 3. Consider 3 ΓMA gure 2.1 below. In this gure to ΘMA , ιF is the set of autocovariances corresponding is the mapping describing this correspondence, ιM relates autoco- variances to spectra and ιP MA parameters to transfer functions. The basic idea is as follows: First we show for the MA(r) case, for every corresponding spectrum there is a neighborhood, which is contained in the set of MA(r) spectra, not violating the strict miniphase assumption. In the next step we demonstrate that by the bijective nature of the mapping between parameters and spectral densities in the high frequency case, we obtain that varying a particular autocovariance, that cannot be directly observed from mixed frequency data, leads to a corresponding variation of parameters; thus giving a (non-singleton) subset of a class of observationally equivalent parameters under mixed frequency observations. Let ΘMA be endowed with the usual Euclidean norm. (as det is a continuous mapping) the set and Σ is open in ιP (τ ) = b(e−iλ ) R n(n+1) 2 . For every τ = SMA As can be seen easily dened above is open in vec (B1 , . . . , Br ) ∈ SMA , is uniquely given by (2.3). Conversely, for given 2 Rn r of course, b(e−iλ ), τ is uniquely given by 1 2π Bj = Thus, ιP is a bijection between SMA and ιP (SMA ). Lemma 1. SMA Z π b −iλ e iλj e dλ. −π SMA and ιP (SMA ) and in this sense we identify The following lemma is straightforward to show: (endowed with the Euclidean metric) and ιP (SMA ) endowed with the supremum norm b −iλ e are homeomorphic. Here, sup k.kmax = sup λ∈[−π,π] b −iλ e max (2.5) denotes the max norm for matrices with com- plex entries. 4 In other words, the above lemma says that SMA , when endowed with the Eu- clidean metric and then endowed with the sup norm (2.5) has the same open sets, i.e., the two metrics are topologically equivalent. Now consider the autocovariance sequence γ : Z → Rn×n of the VMA(r) process (2.1), where γ (j) = E yj y0T . (2.6) The corresponding spectral density is given by f (λ) where ∗ r 1 X γ (j) e−iλj 2π j=−r = b e−iλ Σb∗ e−iλ = (2.7) denotes the conjugate transpose. As is well known, there is a bijection between the covariances and the corresponding spectral density; let us write ιM (γ) = f . The set of all autocovariance sequences has to be non-negative denite; in addition, for the MA case considered here Moreover, γ (0) γ (j) = 0, ∀|j| > r. is symmetric and positive denite and due to (2.2) we have f (λ) > 0, ∀λ ∈ [−π, π]. Thus, for the VMA(r) case, we can parametrize the set of all autocovariances by ΓMA = γ= vech (γ T (0)) , vec (γ (1) , . . . , γ (r)) f (λ) = ιM (γ) (λ) > 0, ∀λ ∈ [−π, π] . Here, we have identied above, we identify vech (γ T T T ∈R T (0)) , vec (γ (1) , . . . , γ (r)) n(n+1) +n2 r 2 T with γ. | As ΓMA and ιM (ΓMA ) and we can endow ΓMA with the Euclidean norm as well as with the sup norm for spectral densities and these norms are topologically equivalent. We have: 5 Theorem 1. Proof. Let Under the assumptions (2.2) and (2.4) γ ∈ ΓMA . principal minors of f tinuous functions in neighborhood of f >0 f Then, f (λ) > 0 ∀λ ∈ [−π, π] being positive on γ, [−π, π]. ΓMA R n(n+1) +n2 r 2 . is equivalent to all leading Since these minors are con- they are bounded away from zero. Thus, there is a (in the sup and therefore also in the Euclidean norm), where and thus a neighborhood of γ which is contained in In the next step, let us consider the relation between denoted by ιF is open in (θ) = γ , dened by (2.7). ΓMA . θ ∈ ΘMA and γ ∈ ΓMA , Clearly ιF is continuous. By the spectral factorization theorem (see Rozanov [16], Hannan [9], Hannan and Deistler [11]), ιF is bijective. In Anderson [1], the continuity of the spectral factorization with the sup norm for spectra and the ΘMA As can be seen easily, on L2 the norm for transfer functions has been stated. L2 and the Euclidean norm are the same up to normalization. Thus, we have: Theorem 2. ιF : ΘMA → ΓMA The mapping is a homeomorphism. Summarizing, this can be depicted in the following diagram: Note that, strictly speaking, ιP maps τ onto −iλ b e , but the extension of ιP to ΘMA is evident. ιF θ ∈ ΘMA γ ∈ ΓMA ιP ιM (b(e−iλ ), Σ) f Figure 2.1: Diagram of the homeomorphisms In this diagram the index and P M stands for moments, for parameters. 6 F stands for the factorization Now consider the MF case: Let f yt yt = , yts where the the nf -dimensional fast component ns -dimensional slow component yts ytf (2.8) is observed for every is observed only for t∈Z t ∈ N Z (N and being an integer larger than one). Thus, we consider the MF stock case here. Throughout we assume that nf ≥ 1 ourselves to the case and N =2 ns ≥ 1. Without loss of generality we restrict here. Let ff fs γ (j) γ (j) γ (j) = γ sf (j) γ ss (j) denote the corresponding partitioned autocovariance matrices. Then, γ f s (j), γ sf (j) and γ ss (2j), j ∈ Z can be directly observed, i.e., directly es- timated from data, but this is not the case for instance, the case r = 1; ΓMA due to its openness. dimension ns × ns γ ss (j), j odd. Consider, for then, under the mixed frequency scheme described above, the autocovariances neighborhood of the true γ f f (j), γ ss (1) ∈ Rns ×ns vech (γ T can be freely varied in a certain T (0)) , vec (γ (1)) T without leaving the set This variation corresponds to a set say, and, by what was stated before ι−1 F (O) O ⊆ ΓMA of is a subset of the class of observationally equivalent VMA systems of topological dimension ns × ns . Thus, we have shown: Theorem 3. Under the assumptions (2.2) and (2.4) in the MF stock case, the MA(r) parameters are not identiable. As immediately can be seen we do not even have local identiability in this case. A heuristic argument concerning the non-identiability can be given by the 7 counting condition, e.g., for the case n = 2, r = 1, N = 2 we can directly observe 6 autocovariances whereas the corresponding VMA(1) system is described by 7 free parameters. As shown in the following example, such an argument may be misleading: Example. Consider the VMA(1) system, where ff b B1 = bsf and |bf f |, |bss | < 1. ff 0 σ , Σ = bss σ sf n = 2, bf s = 0 is xed σf s >0 σ ss (2.9) Now let us dene an equivalent (in terms of directly observ- able autocovariances) VMA(1) system with B̄1 σ̄ ss where ff fs 0 0 σ σ = B1 + δ f s , Σ̄ = σ sf ss − σf f 1 σ σ̄ sf 2 ss 2 ss ss 2 (σ ) 1 + (b ) σ + 2δb + δ σf f = > 0, 2 1 + (bss + δ) δ ∈ (−1−bss , 1−bss ) is the free variation. ΘMA , γ̄(0) = γ(0) γ̄ ss (1) 6= γ ss (1) for δ 6= 0. VMA(1) systems satises varying δ, vec B̄1 T b̄f s = 0, 0 2 (σ f s ) ss σ̄ − σf f If we assume that the class of equivalent it can be shown that the formulas above, by dene a class of observationally equivalent systems, which is not a singleton. Note that in this case we have 6 unknown parameters (3 for 3 for Σ) , vech Σ̄ but 0 γ̄(1) = B̄1 Σ̄ = γ(1) + δ 0 and therefore It follows that B1 and and 6 directly observable autocovariances and therefore the counting condition fails. 8 T T ∈ Until now, only the case where stock variables are observed, has been considered. Now we assume that the observed slow component wt is obtained by the linear observation scheme s s wt = k0 yts + k1 yt−1 + · · · + kN −1 yt−N +1 , where ki ∈ Rns ×ns are known and k0 t ∈ NZ (2.10) is non-singular. Then, the corresponding autocovariances which can be directly observed, are T γ f f (j) = E yjf y0f , = E yjf w0T , T γ wf (j) = E wj y0f , γ ww (N j) = E wN j w0T , j ∈ Z. γ f w (j) As shown in Anderson et al. [2], Section 5, structed from struct γ ss (j) γ f f (j) and γ f w (j). γ f s (j) and γ sf (j) can be recon- Therefore, in a last step, we have to recon- from γ ww (N j) = N −1 X ki γ ss (N j + i − h) khT , j∈Z (2.11) i,h=0 since γ ww (N j) γ ss (j). are the only directly observed autocovariances depending on Note that γ ww (N j) = 0 for largest integer smaller than or equal to |j| > γ ss N +1 , where bαc α, and therefore we only have 1 directly obsered autocovariances from γ ww from r−1 and denotes the r−1 N +1 + r +1 unknown autocovariances (with non-negative lags) which are unequal to zero. For simplicity, we only consider the case ns = 1 , generalizations being straightforward. In this PN −1 ss γ ww (N j) = i,h=0 ki kh γ (N j + i − h) and thus we r−1 equations with N + 1 + 1 equations and r + 1 unknown case (2.11) changes to obtain a system of autocovariances γ ss . Under the additional assumption that 9 kN −1 is unequal to zero, we can uniquely reconstruct the γ ss obtain identiability. Nevertheless, in the case autocovariances For the case PN −1 i=0 γ ss r >1 and therefore we we have more unknown than equations and thus we do not obtain identiability. r = 1, ns ≥ 1 ki ⊗ ki , r=1 for the case where ⊗ and N ∈ N we have to assume that kN −1 and denotes the Kronecker product, are non-singular to obtain identiability. Note that this excludes the case of stock variables. If we relax the strict miniphase assumption (2.2), in the sense that we allow roots on and outside the unit circle, we may have g(eneric)-identiability in certain extreme cases, e.g., for r = 1, n = 2 and b (z) has zeros at 1 and −1. Here, we say that a subset of a given set is generic, if it contains an open and dense subset of this set. 3. High Frequency VARMA Systems and MF Data: Non-Identiability Results In this section we consider VARMA(p, r) systems yt + A1 yt−1 + ... + Ap yt−p = νt + B1 νt−1 + ... + Br νt−r , where Ai , Bi ∈ Rn×n (νt |t ∈ Z) and are parameter matrices, is white noise with T Σ = E νt νt b(z) = In + B1 z + ... + Br z r . . t∈Z (3.1) p, r ∈ N are specied integers and Let a(z) = In + A1 z + ... + Ap z p We impose the usual stability condition det a(z) 6= 0, |z| ≤ 1 as well as the strict miniphase condition (2.2). (3.2) Throughout this section we assume that r > p. 10 (3.3) The case (yt ) r≤p has been treated in Anderson et al. [4]. The spectral density of is given by f (λ) = = 1 −1 −iλ −iλ a e b(e )Σb∗ (e−iλ )a−∗ 2π ∞ 1 X γ (j) e−iλj . 2π j=−∞ −iλ e (3.4) The parameter space considered here is of the form ΘARMA = {(A1 , . . . , Ap , B1 , . . . , Br ) | det a(z) 6= 0, |z| ≤ 1, det b(z) 6= 0, |z| ≤ 1 rank (Ap ) = rank (Br ) = n, (a(z), b(z)) Σ | Σ = ΣT , Σ > 0 . Note that in the high frequency case ΘARMA = rank (Br ) = n × (3.5) is identiable (see Hannan [10], Hannan and Deistler [11]) and that the conditions and rank (Ap ) is left co-prime} (a(z), b(z)) are generically fullled. is left co-prime In the next step we (A1 , . . . , Ap ) are generically identiable from MF T f postmultiply (3.1) by yt−j , j = r + 1, . . . , r + np, and take show that the AR parameters stock data. If we the expectation, we obtain analogously to Chen and Zadrozny [5] f yt−r−1 T T T f f , yt−r−2 , . . . , yt−r−np E yt y t−1 T T T . f f .. y f (−A1 , . . . , −Ap ) E , y , . . . , y t−r−np t−r−1 t−r−2 yt−p {z } | ZARMA where ZARMA ∈ Rnp×npnf . [2, 4], it can be shown that Theorem 4. = (3.6) With the same techniques as in Anderson et al. ZARMA has generically full row rank. Thus, we get: Under the assumptions (3.2), (2.2) and (2.4) the AR parameters 11 of (3.1) are g-identiable. Let G = (In , 0, . . . , 0) and −A1 ··· In A= .. −Ap−1 . be the companion form of the system parameters a (z). For equal to k= α, , where N dαe In r−p+1 −Ap 0 (A1 , . . . , Ap ) corresponding to denotes the smallest integer larger than or we obtain the following system of equations γ (kN ) γ ((k + 1) N ) γ ((k + 2) N ) . . . γ ((k + np − 1)N ) | {z } = O1 kN −r GA GAkN −r AN γ (r) . . . GAkN −r A2N . . . γ (r − p + 1) . GAkN −r A(np−1)N | {z } O Analogously to Koelbl [12], Anderson et al. [4] it can be shown that generically full column rank. Thus, we can uniquely obtain O has γ ss (j), r ≥ |j| ≥ r − p + 1 ≥ 2 from (A1 , . . . , Ap ) and the second moments contained in O1 , which can be directly observed in the case of stock data, by using the formula γ (r) . = OT O −1 OT O1 . . . γ (r − p + 1) 12 (3.7) γ ss (j), |j| > r We obtain γ ss (1) cannot reconstruct n2s r − p − r−p N Theorem 5. case, for from γ (j) = − from (3.7). Pp i=1 Ai γ (j − i). Obviously, we To be more specic, there are still autocovariances missing. Under the assumptions (3.2), (2.2) and (2.4) in the MF stock r > p, ΘARMA is not identiable. Proof. Let the VARMA spectral density f (λ) of notation, we restrict ourselves to the case 0 f¯ (λ, δ) = f (λ) + 0 be given by (3.4). For simplicity ns = 1. We dene 0 δ −iλ e iλ e + (3.8) and a −iλ e f¯ (λ, δ) a∗ −iλ e = f (λ) a∗ 0 +a e−iλ 0 δ a −iλ e −iλ e (3.9) 0 −iλ e ∗ a iλ −iλ e . +e Note that the left hand side of (3.9) is a trigonometric polynomial matrix of degree r. As can be seen easily, Theorem 1 implies that for δ in a suitable neighborhood of zero this left hand side is a spectral density of an MA(r) system. Thus, (3.8) corresponds to a VARMA(p, r) spectral density where all (yt ) second moments of course γ ss (−1)), stay the same with the exception of which has been disturbed by δ, where neighborhood of zero. Because left co-primeness of conditions rank (Ap ) sponding to f¯ (λ, δ) = rank (Br ) = n δ γ ss (1) (and of varies in a certain (a (z) , b (z)) and the rank are open properties, the system corre- can be described in the parameter space ΘARMA . Since the mapping between the second moments and the parameters is homeomorphic, the variation of δ gives the corresponding variation in the parameter space. 13 Note that the basic idea of the proof is not applicable for the case p ≥ r. Now we consider the more general observation scheme (2.10). First of all, observe that again γ f s (j) and γ sf (j) can be reconstructed from γ f f (j) and Therefore, we can g-identify the system parameters, see (3.6). step, we want to reconstruct the missing autocovariances (2.11). For simplicity, we just investigate the case straightforward. For k = r−p N +1 γ ns = 1, ss γ f w (j). In a second (j), j ∈ N from generalizations are we can arrange the following system of equations γ ww (αN ) γ ww ((α + 1) N ) γ ww ((α + 2) N ) . . . ww γ ((α + np − 1)N ) | {z } = F O1 where O1F γ f s (r) ss (r) γ . . . . . f s . γ (r − p + 1) P N −1 ss (r − p + 1) i−h+kN −r A(np−1)N γ (0, 1) G k k A i h i,h=0 | {z } OF and OF can be constructed from the observed autocovariances and the system parameters. Again it can be shown that rank and therefore we obtain OF has generically full column γ ss (j) , j ≥ r − p + 1 ≥ 2. to reconstruct the remaining unknown autocovariances with the help of with r−p N P N −1 i−h+kN −r (0, 1) G i,h=0 ki kh A P N −1 i−h+kN −r AN (0, 1) G i,h=0 ki kh A P N −1 i−h+kN −r A2N (0, 1) G i,h=0 ki kh A +1 γ ww (N j), j = 0, . . . , equations and r−p N r−p+1 In a last step, we have γ ss (j), j = 0, . . . , r − p . Thus, we get a system of equations unknown autocovariances and therefore we cannot expect to uniquely reconstruct the remaining autocovariances except for the case r = p+1 (under the additional assumption that summarize, VARMA(p, p not for + 1) kN −1 6= 0). To systems are g-identiable in the ow case, but r > p + 1. 4. High Frequency VARMA Systems and MF Data: The Singular Case Here, we consider the singular case, i.e., the case rank (Σ) = q < n. as is shown below, as opposed to the regular case rank (Σ) 14 = n, In this case, we may have identiability for VMA and VARMA systems with r > p, if q is smaller than or nf . equal to In an evident notation we write the spectral density as f (λ) of the VARMA system ff fs f (λ) f (λ) f (λ) = . f sf (λ) f ss (λ) Clearly, f has normal rank equal to q. (4.1) Let ff Σ Σ= Σsf Σf s Σss it follows that f f f (λ) be partitioned accordingly. Lemma 2. For Σf f > 0 is non-singular almost every- where. Proof. Let H(t) = span {yj : j ≤ t} and Hf (t) = span n o yjf : j ≤ t be the Hilbert spaces spanned by all univariate components of the yj , j ≤ t f the yj , be the projec- j ≤ t, f tion of yt onto ytf = f yt|t−1 +νtf and thus respectively. f Furthermore, let y t|t−1 and H(t − 1) Hf (t − 1), = zt +ηt . Σf f > 0 , and Now respectively. f Then, it follows that ηt ηtT H (t) ⊆ H(t) implies E which is generically fullled, implies zt and ≥E f f f (λ) > 0 νtf T νtf almost ev- erywhere. If q = nf holds, then generically (in the parameter space of singular VARMA systems, where rank equal to q = q. rank (Σ) has been prescribed) already In the mixed frequency case obtained from mixed frequency data. f f f (λ) f f f (λ), f f s (λ) and has normal f sf (λ) are This is true for the stock, but also for the more general linear observation scheme (2.10). 15 Then, we obtain f ss (λ) (according to the Wiener ltering formula) as −1 f ss (λ) = f sf (λ) f f f (λ) and thus, in this case, i.e., if f f s (λ) (4.2) f f f (λ) has already normal rank equal to q , f (λ) is generically unique from the second moments which can be directly observed or reconstructed in the case of more general linear observation schemes. As is easily seen, this argument can also be applied to the case q. q < nf , if f f f (λ) has rank In this way we have directly reconstructed, generically, the high frequency spectral density and therefore the well known high frequency identiability result holds. Note that this result hold for all between p and Theorem 6. p, r, not depending on the relation r. For nf ≥ q , the VARMA(p, r) classes are g-identiable. 5. Conclusions This paper deals with the non-identiability of VMA and VARMA(p, r) r>p systems in the case of mixed frequency observations. The main result is that opposed to the classes of VAR and VARMA systems, where the MA order is smaller than or equal to the AR order, generic identiability cannot be obtained in case of regular systems and stock variables. With some modications, these results hold through for more general observation schemes. For the singular case q = rank (Σ) ≤ nf generic identiability can be obtained. 6. Acknowledgments Support by the Oesterreichische Nationalbank (Oesterreichische Nationalbank, Anniversary Fund, project number: 16546), the FWF (Austrian Science Fund 16 under contract P24198/N18) and NICTA is gratefully acknowledged. NICTA is funded by the Australian Government. References [1] Anderson, B. D. O. 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