Box and Jenkins (1970) (Autoregressive Moving Average model ARMA ) Box-Jenkins ARMA Hannan (1970) Anderson (1971) Fuller (
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1 41, 1, From Time Series Analysis to Spatio-Temporal Statistical Analysis Yoshihiro Yajima We review developments of time series analysis and spatio-temporal statistical analysis and envisage a future of them. : 1. Gelfand et al. (2010) Finkenstät et al. (2007) ( ) ( yajima@e.u-tokyo.ac.jp)
2 Box and Jenkins (1970) (Autoregressive Moving Average model ARMA ) Box-Jenkins ARMA Hannan (1970) Anderson (1971) Fuller (1976) Priestley (1981) ARMA 2 (Brockwell and Davis (1991) Chapter 8) 1980 (Autoregressive Conditional Heteroskedasticity model) (Stochastic Volatility model) (Tong (1990) Taylor (1994) Guouriéroux (1997) Fan and Yao (2003) (2003))
3 221 (Banerjee et al. (1993) Beran (1994) Doukhan et al. (2002) Johansen (1996) (2003) Robinson (2003)) 3. 2 (strictly stationary process) (weakly stationary process) (Brockwell and Davis (1991)) t t R = (, ) Z = {0, ±1, ±2, } K 3.1 {X t t K} 2 (i){x t } t E(X t ) = µ µ = 0 (ii)cov(x t, X s ) t s {γ(h)} γ(h) = Cov(X t+h, X t ) γ(h) = exp(ihλ)df (λ) (i 2 = 1) (3.1) T K = R T = (, ) K = Z T = [ π, π] F (λ) F (λ) (3.1) f(λ) γ(h) = exp(ihλ)f(λ)dλ T
4 F (λ) f(λ) X t = T exp(itλ)dz(λ) (3.2) {Z(λ)} λ 1 λ 2 (λ 1, λ 2 T ) E Z(λ 2 ) Z(λ 1 ) 2 = λ2 λ 1 df (λ) dz(λ) λ λ E dz(λ) 2 df (λ) f(λ)dλ K = Z 2 γ(h) < (3.3) h=0 {X t } (short-memory) (short range dependent) (weakly dependent) γ(h) = (3.4) h=0 (long-memory) (long range dependent) (strongly dependent) ARMA {X t } X t φ 1 X t 1... φ p X t p = U t θ 1 U t 1... θ q U t q (3.5) {X t } (p, q) ARMA {U t } (white noise) V ar(u t ) = σ 2 Cov(U t, U s ) = 0(t s) {U t } f U (λ) = σ2 2π B BX t = X t 1 (3.5) (3.6) φ(b)x t = θ(b)u t φ(b) = 1 φ 1... φ p B p θ(b) = 1 θ 1... θ q B q
5 223 φ(z) = 0 ( z = 1) ARMA X t U s (s t) (causality) h 0 γ(h) Ka h (0 < a < 1) h (3.7) K (3.3) f(λ) = σ2 θ(e iλ ) 2 2π φ(e iλ ) 2 (3.8) 0 (3.7) (3.8) 2 ARMA ARFIMA (Granger and Joyeux (1980) Hosking (1981)) FI fractionally integrated d (fractional diffrence operator) d d = (1 B) d = j=0 ( ) d d(d 1)... (d j + 1) = = j j! ( ) d ( B) j (3.9) j Γ(d + 1) Γ(j + 1)Γ(d j + 1) Γ(x) d ( d j) = 0(j > d) (3.9) d (Yajima (1985)) d {X t } φ(b) d X(t) = θ(b)u t {X t } (p, d, q) ARFIMA d < 1/2 {X t } f(λ) = σ2 θ(e iλ ) 2 2π φ(e iλ )(1 e iλ ) d 2 (3.10) ARMA (3.8) (3.10) d (1 e iλ ) d 0 < d < 1/2 λ 0 f(λ)
6 (Fractional Gaussian Noise FGN ) (Manderbrot and van Ness (1968)) (Fractional Brownian Motion FBM ) {B H (t) 0 t < } 2 E(B H (t)) = 0 t E( B H (t) B H (s) 2 ) = σ 2 t s 2H (0 < H < 1) FBM H = 1/2 FBM {X t t = 1, 2,...} X t = B H (t) B H (t 1) {X t } FGN H = 1/2( ) FGN N(0, σ 2 ) H 1/2 1/2 < H ARFIMA λ 0 (Sinai (1976)) ARFIMA FGN f(λ) λ α 1 (λ 0) γ(h) h α (h ) α = 1 2d = 2 2H (3.11) 0 < α < 1(0 < d < 1/2, 1/2 < H < 1) f(λ) (λ 0) (3.4) 4. {X t } θ ARMA φ i (i = 1,..., p), θ j (j = 1,..., q) σ 2 = V ar(u t ) ARFIMA FGN
7 225 d H f(λ; θ) γ(h; θ) θ X N = (X 1,, X N ) log L N (θ; X N ) = 1 2 log det(γ N ) 1 2 (X N µ) Γ 1 N (X N µ) µ = (µ, µ,..., µ) Γ N X N (i, j) Cov(X i, X j ) = γ(i j; θ) Γ 1 N det(γ N) θ Whittle µ = 0 2(2π/N) log L N (θ; X N ) = (2π/N)[log detγ N + X N Γ 1 N X N] N N (2π/N) log τ j N + [ π,π] j=1 m n=1 [ π,π] N m n=1 X mx n e i(m n)λ (2π) 2 dλ (4.1) f(λ; θ) ( log f(λ; θ) + I ) N(λ) dλ (4.2) f(λ; θ) = L N(θ; X N ) (say). I N (λ) I N (λ) = P N t=1 Xt exp( itλ) 2 2πN τ i,n Γ N L N (θ; X N ) θ Whittle (4.1) Γ 1 N Γ N = (γmn ) γ mn e i(m n)λ = (2π) 2 f(λ; θ) dλ [ π,π] Γ N Γ 1 N (Shaman (1976)) (3.6) Γ 1 N = Γ N = I N /σ 2 I N N N f(λ) 0 G(x) lim (2π/N) N G(τ j N ) = N j=1 [ π,π] G(f(λ))dλ (4.3) (Grenander and Szegö (1984)) (4.3) G(x) = log x (4.2) Whittle
8 Idea: Whittle (1961) Univariate Short-Memory: Walker (1964) Hannan (1973) Multivariate Short-Memory: Dunsmuir (1979) Univariate Short-Memory (Irregularly Spaced): Dunsmuir and Robinson (1981) Multivariate Short-Memory (Misspecified): Hosoya and Taniguchi (1982) Long-Memory Gaussian: Yajima (1985) Fox and Taqqu (1986) Long-Memory Gaussian (Misspecified): Yajima (1992) Long-Memory Non Gaussian: Giraitis and Surgailis (1990) Hosoya (1997) f(λ) ( log f(λ; θ) + f(λ) ) dλ f(λ; θ) [ π,π] θ θ 0 f(λ) = f(λ; θ), λ θ θ N (i) ˆθ ˆθ θ 0 a.s. (ii) N(ˆθ N θ 0 ) N(0 4πW (θ 0 ) 1 ) W (θ) = h(λ; θ) = f 1 (λ; θ) [ π,π] [ ] [ ] h(λ; θ) h(λ; θ) f(λ) 2 dλ θ θ f(λ) f(λ; θ), θ f(λ; θ)
9 4.2 N 227 (i) ˆθ θ 0 a.s. (ii)(a) (3.11) 1/2 < α < 1 N(ˆθ N θ 0 ) N(0, 4πV (θ 0 ) 1 W (θ 0 )V (θ 0 ) 1 ) [ 2 ] h(λ; θ) V (θ) = θ θ f(λ)dλ [ π,π] (b) α = 1/2 N/ log N(ˆθ N θ 0 ) 1 (c) 0 < α < 1/2 (N α / log N)(ˆθ N θ 0 ) (ii)(a) f(λ) = f(λ; θ 0 ) V (θ 0 ) = W (θ 0 ) (Hosoya and Taniguchi (1982)) 4.2.(ii)(a) 4.1.(ii) 4.1.(ii) 4.2.(ii) Whittle X N 2 Q N = X NB N X N E(X NB N X N ) B N = (b mn ) N N (m, n) ˆb(λ)( π λ π) b mn = e i(m n)λˆb(λ)dλ [ π,π] f(λ)ˆb(λ) [ π, π] 2 NQN 0 [ π,π] (f(λ)ˆb(λ)) 2 dλ (Fox and Taqqu (1987) Giraitis and Surgailis (1990)) 2 1/ N (Noncentral limit theorem) (Fox and Taqqu (1985)) Whittle h(λ; θ)/ θ θ = θ 0 ˆb(λ) f(λ) ˆb(λ) f(λ)ˆb(λ) (ii) ˆb(0) = 0 f(λ) (λ 0) 4.2(ii)(a) f(λ) 2 ˆb(λ) f(λ)ˆb(λ) 2
10 (ii)(b) (c) ˆb(0) (ii) Fox and Taqqu (1987) 1/ N f(λ)ˆb(λ) 2 Lavancier and Philippe (2011) 5. One-parameter Stochastic Process {X t t R Z} ( ) Multi-parameter Stochastic Process {X t t R d Z d }(2 d) (half sapce) Z d (Guyon (1995)) t Z d ARMA (Guyon (1995)) ARMA R d Z = {0, ±1, ±2,...} d K d (site) s( K d ) Y (s) 1 1 d = 2 s
11 229 Y (s) d = 3 s Y (s) d = 4 t Y (s, t) D( K d ) s {Y (s) : s D} (random field) 5.2 {Y (s) : s K d } 2 (i){y (s)} s E(Y (s)) = µ µ = 0 (ii) t s C(t s) = E(Y (t)y (s)), t, s K d {C(h), h = t s K d } d = 1 (3.1) (3.2) Y (s) = exp(is λ)dm(λ) T d C(h) = exp(ih λ)df (λ) T d (Gikhman and Skorokhod (1974) Rosenblatt (1985) Yaglom (1987)) s = (s 1,..., s d ), h = (h 1,..., h d ), λ = (λ 1,..., λ d ) K = Z T = [ π, π] K = R T = (, ) M = {M(λ), λ T d } d F (λ) d E M( ) 2 = F ( )( T d ) E(M( 1 )M( 2 )) = 0( 1, 2 T d, 1 2 = φ) F (λ) F (λ) f(λ) 6. Ma (2008) 3 A Simple Stochastic Representation A Closed-Form Spectral Density Function A Closed-Form of the Covariance Function
12 Ma (2008)..., just as a stationary discrete-time ARMA time series. In general, however, only one or two tractable forms may be available for a spatial or spatio-temporal stationary random field,... (3.5) (3.7) (3.8) ARMA 3 (i)y (s) (ii) ( ) Cressie (1993) Guyon (1995) Gelfand et al. (2010) 2 2 (isotropic) (separable) C(h) h = d i=1 h2 i 1 (positive definite) C 0 (x)(x R) x h C(h) = C 0 ( h ) C 0 (x) d 2 C(h) (Christakos (1984) Cressie (1993 p. 84)) d C(h) C 0 (x) = 0 exp( x 2 u 2 )dg(x) G(x) g(x) = C 0 (x 1/2 ) g(x)(x 0) (completely monotone) g(x) x 0 n n ( 1) n d n g(x)/dx n 0(0 < x < ) (Schoenberg (1938) Feller (1971) Cressie (1993) Stein (1999)) g(x) = exp( αx γ )(0 < α, 0 < γ 1) C 0 (x) Matérn (Matérn class) (Matérn ( ) Handcock and Stein (1993) Stein (1999)) C 0 (x) = π 1/2 φ 2 ν 1 Γ(ν + 1/2)α 2ν (α x )ν K ν (α x ) (Stein (1999)) K ν 2 (Modified Bessel function of the second kind) α, ν, φ φ α ν ν 2 ν = 1/2 C 0 (x) = πφα 1 exp( α x )
13 231 ν = 3/2 C 0 (x) = 1 2 πφα 3 exp( α x )(1 + α x ) ω = λ f(ω) = φ π (d 1)/2 (α 2 + ω 2 ) ν+d/2 Guttorp and Gneiting (2006) Matérn Matérn Matérn 1947 (Matérn (1947)) ( Harald Cramér) 1960 (Matérn (1960)) (Matérn (1986)) von Kármán (1948a b) ν = 1/3 Whittle (1954) ν = 1 1 σ 2 α ν = 0.5, 1.0, 1.5 ( )Matérn ν ν (Separable Model) 2 h C(h) = C 1 ( h 1 )C 2 ( h 2 ) h 1 = (h 1,..., h m ), h2 = (h m+1,..., h d ) C i ( h i )(i = 1, 2, ) C i ( h i )(i = 1, 2, ) f i ( λ i )(i = 1, 2) f(λ) = f 1 ( λ 1 )f 2 ( λ 2 ) λ = (λ 1,..., λ d ) λ 1 = (λ 1,..., λ m ) λ 2 = (λ m+1,..., λ d ) d = 2 f(λ) λ 1 d 1 λ 2 d 2 (0 < d 1, d 2 < 1) f(λ) (λ λ 2 2) d (0 < d < 2) (Ludeña and Lavielle (1999))
14 Simulation of Matérn class (2010) Sherman (2011) 7. 4 Whittle Spatial Short-Memory (Regularly Spaced): Dahlhaus and Künsch (1987) Spatial Long-Memory (Regularly Spaced): Ludeña and Lavielle (1999) Spatial Short-Memory Gaussian (Irregularly Spaced): Matsuda and Yajima (2009) Spatial Long-Memory (Non)Gaussin (Irregularlry Spaced): Who? When? Whittle
15 233 Regularly Spaced Increasing Domain Asymptotics P n = d i=1 [1, 2,..., n i] n = d i=1 n i n i (i = 1, 2,..., d) Whittle d = 1 I n (λ) = s P n exp( is λ)y (s) 2 (2π) d n d 2 (edge effect) Ĉ(h) = s s+h P n Y (s)y (s + h)/n d E(Ĉ(h)) C(h) = O(n 1/d ) (7.1) (Guyon (1995)) n(ĉ(h) C(h)) d 2 (7.1) d = 1( ) d = 2 d = 3 d tapered Y (s) = 0(s / P n ) taper h(u) : [0, 1] [0, 1] lim u 0,1 h(u) = 0 h(u) Y (s) h(s)y (s) h(s) = d i=1 h(s i/n i ) s P n 0 tapered I T n (λ) = s P n exp( is λ)h(s)y (s) 2 (2π) d H n H n = s P n h 2 (s) h(u) 1 I n (λ) Y n θ L n(θ; Y n ) = ( π,π] d ( log f(λ; θ) + IT n (λ) f(λ; θ) ) dλ d 2 Whittle d d 3 (Dahlhaus and Künsch (1987)) d 4
16 Irregularly Spaced s i s i = (A 1 u i,1,..., A d u i,d ) i = 1,..., n u i = (u i,1,..., u i,d ) (i = 1,..., n) d i.i.d. g(x) [0, 1] d compact support A j (j = 1, 2,..., d) n Infill Asymptotics k k (n = n k ) (A j (k) (j = 1,..., d)) Mixed Domain Asymptotics (discrete Fourier transform) J k (λ) = (2π) d 2 G 1/2 S k 1 2 n 1 k I k (λ) = J k (λ) 2 n k p=1 Y (s p ) exp( is pλ) G = g(s) 2 ds S [0,1] d k S k = [0, A 1 ]... [0, A d ] S k S k = A 1... A d J k (λ) (2π) d 2 S k 1 2 S k Y (s) exp( is λ)ds G Ĝ = m d m i 1 m i d =1 ĝ(x 1,, x d ) = 1 n k δ d ( i1 ĝ m,, i d m n k j=1 ) 2 ( uj,1 x 1 K,, u j,d x d δ δ K R d δ L k (θ) = D [ ] I k (λ) log{f(λ; θ) + c k (θ)} + dλ f(λ; θ) + c k (θ) θ(ˆθ 0 ) Whittle D (λ D λ D) c k (θ) L k (θ) k d ˆθ θ 0 ( ) d 3 S k 1/2 (ˆθ k θ 0 ) L N(0, 2bW (θ 0 ) 1 ) )
17 (Matsuda and Yajima (2009)) 235 g(s) 4 ds [0,1] b = d ( g(s) [0,1] 2 ds) 2 d ( ) ( ) log f(λ; θ) log f(λ; θ) W (θ) = (2π) d dλ θ θ D b 1 g(x) 1 8. (1) 6 4 (Ma (2008)) 3 (a) d = 1 ( ) d dt + α Y (t) = ɛ(t) (8.1) ɛ(t) 0 σ 2 dy (t) = αy (t)dt + σdw (t)
18 {W (t)} 3 (B 1/2 (t), σ = 1) Ornstein-Uhlenbeck Y (t) = Y (0) exp( αt) + σ t 0 exp( α(t s))dw (s) (Karatzas and Shreve (1991)) Y (0) N(0, σ 2 /2α) {Y (t)} C(h) = (σ 2 /2α)e α h f(λ) = σ 2 /(λ 2 +α 2 ) {Y (t)}(t = 0, 1, 2,...) φ = e α AR(1) Whittle (1954) d = 2 ( ) 2 s s 2 φ 2 Y (s 1, s 2 ) = ɛ(s 1, s 2 ) (8.2) 2 6 C(h 1, h 2 ) = φ h K 1 (φ h ) σ 2 f(λ 1, λ) = (λ λ2 2 + φ2 ) 2 (8.2) (8.1) ɛ(s 1, s 2 ) 0 σ 2 Jones and Zhang (1997) d [( d ) p ] 2 φ 2 c Y (s, t) = ɛ(s, t) (8.3) t s 2 i=1 i C(h, t) = h d/2+1 σ 2 2(2π) d/2 c f(λ, τ) = σ 2 ( λ 2 +φ 2 ) 2p + c 2 τ 2 u d/2 e (u2 +φ 2 ) p t/c 0 (u 2 + φ 2 ) p J d/2 1 (u h )du J ν Bessel (8.2) (8.3) Ruiz-Medina et al. (2004) Kelbert et al. (2005) (8.2) (8.3)
19 237 (b) 2 Stein (2005) f(λ τ) = {c 1 (a 2 1+ λ 2 ) α 1 + c 2 (a τ 2 ) α 2 } β (λ τ) R d R c 1 = σ 2, c 2 = c 2 σ 2, a 2 = 0, α 1 = 2p, α 2 = 1, β = 1 Jones and Zhang (1997) Fuentes et al. (2008) f(λ, τ) = γ(α 2 β 2 + β 2 λ 2 +α 2 τ 2 + ɛ λ 2 τ 2 ) ν, (λ, τ) R d R ɛ ɛ = 1 f(λ, τ) = γ(α 2 + λ 2 ) ν (β 2 + τ 2 ) ν ɛ = 0 f(λ, τ) = γ(α 2 β 2 + β 2 λ 2 +α 2 τ 2 ) ν Matérn (c) Gneiting (2002) σ 2 ( ) h 2 C(h, t) = ψ(t 2 ) φ d/2 ψ(t 2, (h, u) R d R ) φ(t)(t 0) ψ(t)(t 0) Stein (2005) a laundry list of potential models (2) 2
20 (a) (intrinsic stationary random field) h 2 {Y (s)} E(Y (s + h) Y (s)) = 0 E[Y (s + h) Y (s)] 2 = 2γ(h) 2γ(h) (variogram) γ(h) (semivariogram) 3 FBM (multidimensional)fbm exp(is λ) 1 Y (s) = S(λ/ λ )dw (λ) R d λ d/2+h W (λ) 5 M(λ) de W (λ) 2 = dλ S (Istas (2007)) 2γ(h) = R d exp(ih λ) 1 2 λ d+2h S 2 (λ/ λ )dλ S(λ/ λ ) 1 2γ(h) = C h 2H C 1 FBM (Samorodnitsky and Taqqu (1994)) exp(is λ) 1 Y (s) = dw (λ) R d λ d/2+h(λ) H(λ) 0 c( 0) H(cλ) = H(λ) (Bonami and Estrade (2003)) exp(ih λ) 1 2 2γ(h) = dλ λ d+2h(λ) R d H λ 2 S(λ/ λ ) H(λ)
21 239 (b) Priestley (1965) (evolutionary) Y (s, t) = R d R exp(is λ + iτt)φs,t(λ, τ)dm(λ, τ) E dm(λ, τ) 2 = dλdτ φs t(λ τ) (Fuentes et al. (2008)) Cov(Y (s 1, t 1 ), Y (s 2, t 2 )) C(s 1, t 1 ; s 2, t 2 ) = R d R exp(i(s 1 s 2 ) λ + i(t 1 t 2 )τ) φs 1,t 1 (λ τ)φs 2,t 2 (λ τ)dλ dτ φs,t(λ τ) φs,t(λ, τ) = φ (1) s (λ)φ(2) t (τ) Cov(Y (s 1, t 1 ), Y (s 2, t 2 )) = C (1) (s 1, s 2 )C (2) (t 1, t 2 ) K s j (j = 1,..., K) φs j (λ, τ) s s j K(s s j ) φs,t(λ, τ) = k K(s s j )φs j (λ, τ) j=1 s j φs,t(λ, τ) (3) n s i (i = 1,..., n) Y (s i ) C = (c ij ) n n, c ij = Cov(Y (s i ), Y (s j )) (Best Linear Unbiased Predictor (BLUP) (Kriging) ( (2010)) C 1 n 3
22 Covariance Taper with theta=0.8 Product distance 2 Overview of Covariance Tapering n = 1, covariance tapering C(h) C θ (h)( C θ (0) = 1) C tap (h) = C(h)C θ (h) θ C θ (h) = 0, h > θ 2(θ = 0.8) n n Σ tap = (σ ij,tap )(n n) σ ij,tap = C tap (s i s j ) σ ij,tap = 0, s i s j > θ Σ tap 0 sparse C
23 241 Matérn (Du et al. (2009) Furrer et al. (2006) Kaufman et al. (2008) Wang and Loh (2011)) covariance tapering MA AR covariance tapering (4) Arbia (2006) Arbia and Baltagi (2009) Cressie (1993) Gelfand et al. (2010) LeSage and Pace (2009) (A)No Anderson, T. W. (1971). The Statistical Analysis of Time Series, Wiley. Arbia, G. (2006). Spatial Econometrics: Statistical Foundations and Applications to Regional Convergence, Springer. Arbia, G. and Baltagi, B. H. (2009). Spatial Econometrics: Methods and Applications, Springer. Banerjee, A., Dolad, J., Galbraith, J. W. and Hendry, D. F. (1993). Co-integration, Error Correction, and the Econometric Analysis of Non-Stationary Data, Oxford Univeristy Press. Beran, J. (1992). Statistics for Long-Memory Processes, Chapman and Hall. Bonami, A. and Estrade, A. (2003). Anisotropic analysis of some Gaussian models, J. Fourier Anal. Appl., 9, Box, G. E. P. and Jenkins, G. M. (1970). Time Series Analysis: Forecasting and Control (1st. ed.), Holden Day.
24 Brockwell, P. J. and Davis, R. A. (1991). Time Series : Theory and Methods (2nd ed.), Springer. Christakos, G. (1984). On the problem of permissible covariance and variogram models, Water Resour. Res., 20, Cressie, N. (1993). Statistics for Spatial Data (rev. ed.), Wiley. Dahlhaus, R. and Künsch, H. R. (1987). Edge effects and efficient parameter estimation on staitonary random fields, Biometrika, 74, Doukhan, P., Oppenheim, G. and Taqqu, M. (2002). Theory and Applications of Long-Range Dependence, Birkhäuser. Du, J., Zhang, H. and Mandrekar, V. (2009). Fixd-domain asymptotic properties of tapered maximum likelihood estimators, Ann. Statist., 37, Dunsmuir, W. (1979). A central limit theorem for parameter estimation in stationary vector time series and its application to model for a signal observed with noise, Ann. Statist., 7, Dunsmuir, W. and Robinson, P. M. (1981). Parametric estimators for stationary time series with missing observations, Adv. Appl. Probab., 13, Fan, J. and Yao, Q. (2003). Nonlinear Time Series: Nonparametric and Parametric Methods, Springer. Feller, W. (1971). An Introduction to Probability Theory and Its Applications, vol. II (2nd ed.), Wiley. Finkenstät, B., Held, L. and Isham, V. (2007). Statistical Methods for Spatio-Temporal Systems, Chapman& Hall/CRC. Fox, R. and Taqqu, M. S. (1985). Noncentral limit theorems for quadratic forms in random variables having long-range dependence, Ann. Probab., 13, Fox, R. and Taqqu, M. S. (1986). Large-sample proeprties of parameter estimation for strongly dependent stationary Gaussian time series, Ann. Statist., 14, Fox, R. and Taqqu, M. S. (1987). Central limit theorems for quadratic forms in random variables having long-range dependence, Probab. Th. Rel. Fields, 74, Fuentes, M., Chen, L. and Davis, J. M. (2008). A class of nonseparable and nonstationary spatial temporal covariance functions, Environmetrics, 19, Fuller, W. A. (1976). Introduction to Statistical Time Series (1st ed.), Wiley. Furrer, R., Genton, M. G. and Nychka, D. (2006). Covariance tapering for interpolation of large spatial datasets, J. Comp. Graph. Statist., 15, Gelfand, A. E., Diggle, P. J., Fuentes, M. and Guttorp, P. (2010). Handbook of Spatial Statistics, Chapman & Hall/CRC. Gikhman, I. I and Skorokhod, A. V. (1974). The Theory of Stochastic Processes I, Springer. Giraitis, L. and Surgailis, D. (1990). A central limit theorem for quadratic forms in strongly dependent linear variables and its application to asymptotic normality of Whittle s estimate, Prob. Th. Rel. Fields, 86, Gneiting, T, (2002). Nonseparable stationary covariance functions for space-time data, J. Amer. Statist. Assoc., 97, Granger, C. W. J. and Joyeux, R. (1980). An introduction to long-range time series models and fractional differencing, J. Time Ser. Anal., 1, Grenander, U. and Szegö, G. (1984). Toeplitz Froms and their Applications (2nd ed.), Chelsea. Guoriéroux, C. (1997). ARCH Models and Finance Applications, Springer. Guttorp, P. and Gneiting, T. (2006). Studies in the history of probability and statistics XLIX. On the Matérn correlation family, Biometrika, 93, Guyon, X. (1995). Random Fields on a Network, Modeling, Statistics, and Applications, Springer Handcock, M. S. and Stein, M. L. (1993). A Baysesian analysis kriging, Technometrics, 35, Hannan, E. J. (1970). Multiple Time Series, Wiley. Hannan, E. J. (1973). The asymptotic theory of linear time series models, J. Appl. Probab., 10, Hosking, J. R. M. (1981), Fractional differencing, Biometrika, 68, Hosoya, Y. (1997). A limit theory for long-range dependence and statistical inference on related models, Ann. Statist., 25,
25 243 Hosoya, Y. and Taniguchi, M. (1982). A central limit theorem for stationary processes and the parameter estimation of linear processes, Ann. Statist., 10, , Correction: (1993). 21, Istas, J. (2007). Identifying the anisotropical function of a d-dimensional Gaussian self-similar prcess with stationary increments, Statist. Inf. Stoch. Proc., 10, Johansen, S. (1996). Likelihood-Based Inference in Cointegrated Vector Autoregressive Models (2nd ed.), Oxford University Press. Jones, R. H. and Zhang, Y. (1997). Models for continuous stationary space-time prcosses, Modelling Longitudinal and Spatially Correlated Data (eds. T. G. Gregoire et al.), Lecture Notes in Statistics 122, Springer, Karatzas, I, and Shreve, S. E. (1991). Brownian Motion and Stochastic Clculus (2nd ed.), Springer. (2003)., 8,. Kaufman, C., Schervish, M. and Nychka, D. (2008). Covariance tapering for likelihood-base estimation in large sptial data sets, J. Amer. Statist. Assoc., 103, Kelbert, M., Leonenko, N. and Ruiz-Medina, M. D. (2005). Fractional random fields associated with stochastic fractional heat equations, Add. Appl. Probab., 37, Lavancier, F. and Philippe, A. (2011). Some convegence results on quadratic forms for random fields and application to empirical covariances, Prob. Th. Rel. Fields, 149, LeSage, J. and Pace, R. K. (2009). Introductionto Spatial Econometrics, Chapman& Hall/CRC. Ludeña, C. and Lavielle, M. (1999). The Whittle estimator for strongly dependent stationary Gaussian fields, Scand. J. Statist., 26, Ma, C. (2008). Recent developments on the construction of spatio-temporal covariance models, Envir. Res. and Risk Asses., 22, S39 S47. Manderbrot, B. B. and van Ness, J. W. (1968). Fractional Brownian motions, fractional noise and applications, SIAM Rev., 10, (2010). R GeoR,. Matérn, B. (1947). Metoder art Uppskatta Noggranhetten vid Linje- och Provytetaxering, Stockholm: Medd Staten Skogsforskningsinstitut, 36, no. 1 (in Swedish with substantial English summary). Matérn, B. (1960). Spatial Variation-Stochastic Models and Their Application to some Problems in Forest Surveys and other Sampling Investigations, Stockholm: Medd. Statens Skogsforskningsinstitut, 49, no. 5. Matérn, B. (1986). Spatial Variation (2nd ed.), Springer. Matsuda, Y. and Yajima, Y.(2009). Fourier analysis of irregularly spaced data on R d, J. Roy. Statist. Soc., B71, Priestley, M. B. (1965). Evolutionary spectral and non-stationary processes, J. Roy. Statist. Soc., B27, Priestley, M. B. (1981). Spetrum Analysis and Time Series, Vols. 1 and 2, Academic Press. Robinson, P. M. (2003), Time Series with Long Memory, Oxford University Press. Rosenblatt, M. (1985). Stationary Sequences and Random Fields, Birkhäuser Ruiz-Medina, M. D., Anguko, J. M. and Anh, V. V. (2004). Fractional random fields on domain with fractal boundary conditions, Inf. Dim. Anal. Quantum Probab. Rel. Top., 7, Samorodnitsky, G. and Taqqu, M. (1994). Stable Non-Gaussian Random Processes: Stochastic Models with Infinite Variance, Chapman & Hall/CRC. Schoenberg, I. J. (1938). Metric spaces and completely monotone functions, Ann. Math., 39, Shaman, P. (1976). Approximations for stationary covariance matrices and their inverses with application to ARMA models, Ann. Statist., 4, Sherman, M. (2011). Spatial Statistics and Spatio-Temporal Data: Covariance Functions and Directional Properties, Wiley. Sinai, Ya. G. (1976). Self-similar probability distribution, Th. Probab. Appl., 21, Stein, M. L. (1999). Interpolation of Spatial Data: Some Theory for Kriging, Springer. Stein, M. L. (2005). Space-time covariance functions, J. Amer. Statist. Assoc., 100,
26 Taylor, S. J. (1994). Modelling stochastic volatility;a review and comparative studies, Mathematical Finance, 4, Tong, H. (1990). Non-Linear Time Series: A Dynamic System Approach, Oxford University Press. von Kármán, T. (1948a). Progress in the statistical theory of turbulence, J. Marine Res., 7, von Kármán, T. (1948b). Progress in the statistical theory of turbulence, Proc. Nat. Acad. Sci., 34, Walker, A. M. (1964). Asymptotic properties of least-square estimates of parameters of the spectrum of a stationary nondeterministic time series, J. Austral. Math. Soc., 4, Wang, D. and Loh, W.-L. (2011). On fixed-domain asymptotics and covariance tapering in Gaussian random fields, Electronic J. Statistics, 5, Whittle, P. (1954). On stationary processes in the plane, Biometrika, 41, Whittle, P. (1961). Gaussian estimation in stationary time seris, Bull. Internat. Statist. Inst., 39, Yaglom, A. M. (1987). Correlation Theory of Stationary and Related Random Functions, vol. I, Springer. Yajima, Y, (1985). On estimation of long-memory time series models, Austral. J. Statist., 27, Yajima, Y. (1992). Asymptotic properties of estimates in incorrect ARMA models for long-memory time series, New Directions in Time Sereis Analysis, Vol. II (eds. D. Brillinger et al.),
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