Stationary Gaussian Markov Processes As Limits of Stationary Autoregressive Time Series

Size: px
Start display at page:

Download "Stationary Gaussian Markov Processes As Limits of Stationary Autoregressive Time Series"

Transcription

1 Stationary Gaussian Markov Processes As Limits of Stationary Autoregressive Time Series Lawrence D. Brown, Pilip A. Ernst, Larry Sepp, and Robert Wolpert August 27, 2015 Abstract We consider te class, C p, of all zero mean stationary Gaussian processes, Y t, t (, ) wit p derivatives, for wic te vector valued process ( Y (0) t, Y (1) t ),..., Y (p) t, t 0 ( ) is a p + 1-vector Markov process, were Y (0) t = Y (t). We provide a rigorous description and treatment of tese stationary Gaussian processes as limits of stationary AR(p) time series. MSC 2010 Primary: 60G10, Secondary: 60G15 Keywords: Continuous autoregressive processes, stationary Gaussian Markovian processes, stocastic differential. equations 1 Introduction In many data-driven applications in bot te natural sciences and in finance, time series data are often discretized prior to analysis and are ten formulated using autoregressive models. Te teoretical and applied properties 1

2 of te convergence of discrete autoregressive ( AR ) processes to teir continuous analogs (continuous autoregressive or CAR processes) as been well studied by many matematicians, statisticians, and economists. See, for example, te works of [3, [4, [2, and [5. A special class of autoregressive processes are te discrete-time zero-mean stationary Gaussian Markovian processes on te line (, ). Te continuous time analogs of tese processes are documented in [9 (c.10) and [10 (pp ). For processes in tis class, te sample pats possess p 1 derivatives at eac value of t, and te evolution of te process following t depends only on te values of tese derivatives at t. Notationally, we term suc a process as a member of te class C p. For convenience, we will use te notation CAR(p)=C p. Te standard Ornstein-Ulenbeck processes is of course a member of C 1, and ence CAR(p) processes can be described as a generalization of te Ornstein-Ulenbeck process. It is well understood tat te Ornstein-Ulenbeck process is related to te usual Gaussian AR(1) process on a discrete-time index, and tat an Ornstein- Ulenbeck process can be described as a limit of appropriately cosen AR(1) processes (see [7). In an analogous fasion we sow tat processes in C p are related to AR(p) processes and can be described as limits of an appropriately cosen sequence of AR(p) processes. Section 2 begins by reviewing te literature on CAR(p) processes, recalling tree equivalent definitions of te processes in C p. Section 3 discusses ow to correctly approximate C p by discrete AR(p) processes. Tis construction is, to te best of our knowledge, novel. 2 Equivalent Descriptions of te Class C p We give ere tree distinct descriptions of processes comprising te class C p, wic are documented in [10 (p. 212), but in different notation. [10 prove (p ) tat tese descriptions are equivalent ways of describing te same class of processes. Te first description matces te euristic description given in te introduction. Te remaining descriptions provide more explicit descriptions tat can be useful in construction and interpretation of tese processes. In all te descriptions Y = {Y (t)} symbolizes a zero-mean Gaussian process on t [0, ). 2

3 2.1 Tree Definitions (I) Y is stationary. Te sample pats are continuous and are p 1 times differentiable, a.e., at eac t [0, ) (Te derivatives at t = 0 are defined only from te rigt. At all oter values of t, te derivatives can be computed from eiter te left or te rigt, and bot rigt and left derivatives are equal). We denote te derivatives at t by Y (i) (t), i = 1,..., p 1. At any t 0 (0, ), te conditional evolution of te process given Y (t), t [0, t 0 depends only on te values of Y (i) (t 0 ), i = 0,..., p 1. Te above can be formalized as ( follows: let Y (0) t, Y (1) t,..., Y (p 1) t Itô vector diffusion process defined by te system of equations ), t 0 denote te values of a mean zero dy (i 1) t = Y (i) t dt, t > 0, i = 1, 2,..., p 1 p 1 (2.1) dy (p 1) t = a i+1 Y (i) t dt + σdw t i=0 for all t > 0, were σ > 0 and te coefficients {a j } satisfy conditions (2.3) and (2.4), below. Ten let Y (t) = Y (0) t. (II) Eac Y C p is given uniquely by a certain polynomial P (z) via te covariance of any suc Y as follows: E [Y s Y t = R(s, t) = r(t s) = e i(t s)z P (z) 2 dz. (2.2) P (z) is a complex polynomial of degree p + 1. It as positive leading coefficients and all complex roots ζ j = ρ j + iσ j, j = 0,..., p wit σ j > 0, and ρ j real. We impose te following constraint on te roots of P (z): wenever ρ j 0, ten tere is anoter ζ j = ζ j wic is te negative conjugate of ζ j. Tis definition of P (z) ensures tat P (z) 2 is an even function. Finally, it can easily be sown tat, for all t, r(t) automatically as 2p derivatives. Te conditions in equations (2.3) and (2.4) below link equations (2.2) and (2.1) and caracterize wic processes satisfying (2.1) are stationary. Te coefficients a i are te unique solution of te equations: 3

4 r (p+i+1) (0 + ) = a j r (i+j) (0), i = 0, 1,..., p 1. (2.3) j=0 Note tat te left and rigt derivatives of r (j) are equal except for j = 2p. Te diffusion coefficient, σ, is given by σ 2 = a j r (j+p) (0)( 1) j+1 + ( 1) p r (2p+1) (0 ). (2.4) j=0 Te stationarity of te process in (2.1) can also be determined via te caracterization in Section 2.2. (III) Equivalently, it is necessary and sufficient tat Y C p as te representation via Wiener integrals wit a standard Brownian motion, W, Y t = g(t u)dw (u), (2.5) were g as te L 2 Fourier transform ĝ(z) = 1 P (z). (2.6) By well-known results from bot Fourier analysis and stocastic integration, a full treatment of wic is given in [6, (2.5) and (2.6) jointly are equivalent to construction (II). Furter, by [6, an equivalent construction to tat given jointly by equations (2.5) and (2.6) is te following: given a pair of independent standard Brownian motions, W 1 and W 2, Y as te following spectral representation: Y t = cos tzĝ dw 1 (z) + sin tzĝ dw 2 (z). (2.7) Wit regard to initial conditions for (2.1), we note tat te process in (2.2) as a stationary distribution. If we use tat distribution as te initial distribution for (2.1), and ceck tat equations (2.3) and (2.4) old, we arrive at a stationary process. 4

5 2.2 Caracterization of Stationarity via (2.1) Te system in (2.1) is linear. Stationary of vector-valued processes described in suc a way as been studied elsewere. See in particular ([7, p. 357, Teorem 5.6.7). Te coefficients in (2.1) tat yield stationarity can be caracterized via te caracteristic polynomial of te matrix Λ, were Λ λi is: λ p a p λ p 1... a 2 λ a 1 = 0. (2.8) Te process is stationary if and only if all te roots of equation (2.8) ave strictly negative real parts. In order to discover weter te coefficients in (2.1) yield a stationary process it is tus necessary and sufficient to ceck weter all te roots of equation (2.8) ave strictly negative real parts. In te case of C 2 te condition for stationarity is quite simple, namely tat a 1, a 2 sould lie in te quadrant a i < 0, i = 1, 2. Te covariance functions for C 2 can be found in [9 (p. 326). For iger order order processes te conditions for stationarity are not so easily described. Indeed, for C 3 it is necessary tat a i < 0, i = 1, 2, 3, but te set of values for wic stationarity olds is not te entire octant. For larger p one needs to study te solutions of te iger order polynomial in equation (2.8). 3 Weak Convergence of te -AR(2) Process to CAR(2) Process 3.1 Discrete Time Analogs of te CAR Processes We now turn our focus to describing te discrete time analogs of te CAR processes and te expression of te CAR processes as limits of tese discrete time processes. In tis section, we discuss te situation for p = 2. Define te -AR(2) processes on te discrete time domain domain {0,, 2,...} via X t = b 1X t + b 2X t 2 + ς Z t, (3.1) Z t IID N(0, 1), t = 2, 3,... Te goal is to establis conditions on te coefficients b 1, b 2 and ς so tat tese AR(2) processes converge to te continuous time CAR(2) process as in 5

6 te system of equations given in (2.1). We ten discuss some furter features of tese processes. To see te similarity of te -AR(2) process in (3.1) wit te CAR(2) process of (2.1), we introduce te corresponding -VAR(2) processes { 0;t, 1;t} defined via 0;t 0;t = 1;t, From (3.2) we see tat 1;t 1;t = [ c 1 0;t + c 2 1;t + ξ Z t. Z t IID N(0, 1), t =, 2,... (3.2) 0;t = 0;t + 1;t = 0;t + 1;t + [ c 1 0;t + c 2 1;t 2 + ξ Z t = [ 2 + c c 2 0;t [ 1 + c 2 0;t 2 + ξ Z t. Tis sows tat te -AR(2) process of (3.1) is equivalent to te -VAR(2) in (3.2) wit b 1 c c 2 + 2, b 2 c 2 1, and ς ξ, (3.3) or, equivalently, c 1 2 [ b 1 + b 2 1, c 2 1 [ 1 b 2, and ξ 1 ς. (3.4) From above, te -AR(2) process of (3.1) wit coefficients given by (3.3) is equivalent to te -VAR(2) in equations (3.2). Teorem 3.1. Consider a sequence of -AR(2) processes of (3.1) wit coefficients given by (3.3), were c j a j, j = 1, 2, and ξ / σ as 0. Tis sequence converges in distribution to te CAR(2) process of (2.1). Proof. It suffices to sow tat te -VAR(2) process of (3.2) converges to te SDE system of dy t = Ẏtdt, t > 0 dẏt = [ a 1 Y t + a 2 Ẏ t dt + σdwt, t > 0. (3.5) 6

7 We employ te framework of Teorems 2.1 and 2.2 of [8. Let M t be te σ-algebra generated by and 0;0, 0;, 0;2,..., 0;t 1;0, 1;, 1;2,..., 1;t for t =, 2,.... Te -VAR(2) process of (3.2) is clearly Markovian of order 1, since to construct { 0;t, 1;t} from { 0;t, 1;t } one needs to use te second equation of (3.2) to construct 1;t and ten use te first equation to construct 0;t as well. Tis establises tat 0;t is M t adapted. Tus, te corresponding drifts per unit of time conditioned on information at time t are given by: [ 0;t [ 0;t E M 0;t + 1;t 0;t t = E M t = 1;t (3.6) and [ 1;t+ [( ) 1;t c E M 1 0;t + c 2 1;t + ξ Z t+ t = E M t = c 1 0;t + c 2 1;t. (3.7) Furtermore, te variances and covariances per unit of time are given by [( 0;t 2 [( ) 0;t ) 2 E M 1;t t = E M t = ( 1;t) 2 (3.8) and [ ( 1;t+ 1;t) 2 [ (c ) 2 E M 1 0;t + c 2 1;t + ξ Z t+ t = E M t = [ ( c 1 0;t + c 21;t 2 [ + 2 c 1 0;t + c 21;t ) ξ 2 ξ E [Z t+ + E [ Zt+ 2 = [ ( ) c 1 0;t + c 2 2 ξ 2 1;t +, (3.9) 7

8 were te last equality assumes tat ɛ t+ IID N(0, 1). By te same logic, [( )( 0;t 0;t 1;t+ 1;t) E M t [ (c ) = E 1;t 1 0;t + c 2 1;t + ξ Z t+ M t (3.10) [ = 1;t c 1 0;t + c 21;t. Te relationsips in (3.8) - (3.10) become [( 0;t 2 0;t ) E M t = o(1), (3.11) [( 1;t+ 2 1;t) E M t = ( ξ ) 2 + o(1), (3.12) and [( )( 0;t 0;t 1;t+ 1;t) E M t = o(1). (3.13) Te o(1) terms vanis uniformly on compact sets. We may additionally sow by brute force tat te limits of [( 0;t 4 0;t ) E M t and [( 1;t+ 4 1;t) E M t exist and converge to zero as 0. We proceed to define te continuous time version of te -VAR(2) process of (3.2) by 8

9 0;t 0;k and 1;t 1;k for k t < (k + 1). Ten, according to te Teorem 2.2 in [8, te relationsips (3.6), (3.7) and (3.11) - (3.13) provide te weak (in distribution) limit diffusion [ [ [ [ [ Yt 0 1 Yt d = dt + d, a 1 a 2 0 σ W t Ẏ t Ẏ t were W t, t 0, is a Brownian motion. Tis is te linear SDE system of (3.5) and it as a unique solution. Remark 3.1. [8 Teorems 2.1 and 2.2 are explicitly stated for real-valued processes but apply to vector valued processes as well. One only needs to explicitly allow te processes to be vector valued, and to write te regularity conditions to allow for te full cross-covariance of te vector valued observations, rater tan just ordinary covariance functions. Our processes are muc better beaved tan te most general type of process [8 considers since our error variance is constant (depending only on ) and our distributions are Gaussian, and ence very ligt tailed. Tus bot of Teorems 2.1 and 2.2 in [8 apply. 3.2 Stationarity of AR(2)-VAR(2) process In tis section we present necessary and sufficient conditions for stationarity of te AR(2) process and its equivalent VAR(2) process and connect tis to te stationary condition for CAR(2). First, we invoke te following proposition, wic is easily proved using well-known results from te time series literature (see [1). Proposition 3.1. Te AR(2) process X t = b 1 X t 1 + b 2 X t 2 + ς Z t, Z t IID N(0, 1). (3.14) is stationary if and only if 2 < b 1 < 2, b 2 b 1 < 1 and b 1 + b 2 < 1, (3.15) wic require ( ) b 1, b 2 to lie in te interior of te triangle wit vertices (-2,-1), (0,1) and (2,-1). Its stationary variance is given by γ 0 = ς 2 1 b2 1 1 b 2 b 2 ( b b 2 + b 2 ). (3.16) 9

10 Because of te relations in (3.3) and (3.4), it follows tat we ave te following corollary to Proposition 3.1. Corollary 3.1. Te VAR(2) process 0;t 0;t 1 = 1;t, 1;t 1;t 1 = c 1 0;t 1 + c 2 1;t 1 + ξz t, Z t IID N(0, 1), t = 1, 2,..., is equivalent to te AR(2) process of (3.14) for b 1 = c 1 + c b 2 = c 2 1 and ς = ξ. Furtermore, te VAR(2) process is stationary if and only if 4 < c 1 < 0 and 2 c 1 2 < c 2 < 0. (3.17) (3.17) is equivalent to te condition tat (c 1, c 2 ) lies in te interior of te triangle wit vertices (-4,0), (0,0) and (0,-2). 3.3 Stationary Variance of -VAR(2) Process In tis section we investigate te stationarity of a special version of te - VAR(2) process in Teorem 5.1.1, wic converges to te CAR(2) process of (3.5) as 0, troug te stationarity of its equivalent -AR(2) process. Proposition 3.2. Te -VAR(2) process of (3.2) for c 1 = a 1, c 2 = a 2 and ξ = σ is stationary as 0 if and only if a j < 0, j = 1, 2. Ten its stationary variance satisfies lim γ0 = 0 σ2 2a 1 a 2. (3.18) Proof. From (3.3), te -VAR(2) process of te ypotesis is equivalent to te -AR(2) process of equation (3.1) wit coefficients given by b 1 = a a 2 + 2, b 2 = a 2 1 and ς = σ ( ) 3. (3.19) From condition (3.15) of Proposition 3.1, tis -AR(2) process is stationary if and only if te following conditions old: b 1 + b 2 < 1 a a a 2 1 < 1 a 1 < 0, 10

11 b 1 < 2 a a < 2 a 2 < a 1 0 a 2 < 0, 2 < b 1 2 < a a a a > 0 0 < < a 2 a a 1 2a 1, b 2 b 1 < 1 a 2 1 a 1 2 a 2 2 < 1 a a > 0 0 < < a 2 a 2 2 4a 1 a 1, were te last two conditions old as 0. Finally, from equation (3.16) and (3.19) we can compute te stationary variance as follows: ( ) ς 2 γ0 = ( ) 2 [( ) 2, b 1 1 b b b 2 1 b 2 1 b 2 = σ 2 (2 + a 2 ) a 1 a 2 (4 + a a 2 ) 0 = σ2. 2a 1 a 2 Tis concludes te proof. 3.4 Stationarity of CAR(2) Process Tis section provides a new derivation of te necessary and sufficient conditions for te stationarity of a CAR(2) ( process. ) It also gives te stationary covariance function of te vector Y (0) t, Y (1) t. Teorem 3.2. Te CAR(2) process given by te SDEs system [ [ [ Yt Yt 0 d = Λ dt + Σ d, t > 0, (3.20) Ẏ t Ẏ t W t were [ 0 1 Λ = a 1 a 2 and Σ = [ σ, 11

12 is stationary if and only if a j < 0, j = 1, 2. Ten its solution [Y t, Ẏt, t 0, is a zero-mean 2-dimensional Gaussian process wit covariance V 0 e tλ ΣΣ e tλ dt (3.21) and covariance function ([ Ys [ Ẏt ) ρ(s, t) E Y t, Ẏs { e (s t)λ V, 0 t s < ; = V e (t s)λ, 0 s t <. Proof. According to Teorem 6.7 in Capter 5 of [7, te assertion of te teorem olds if all te eigenvalues of matrix Λ ave negative real parts. Hence, we compute te eigenvalues of matrix Λ. We calculate te caracteristic polynomial as λ 1 φ(λ) = Λ λi = a 2 λ = λ2 a 2 λ a 1, a 1 wic is of quadratic order wit a discriminant equal to D = a a 1. We ten consider te following cases: (i) If D = 0 a2 2 4 = a 1, te caracteristic polynomial as te double root λ 1,2 = a 2 2. (ii) If D > 0 a2 2 4 > a 1, te caracteristic polynomial as te two real roots λ 1,2 = a 2 ± a a 1. 2 (iii) If D < 0 a2 2 4 < a 1, te caracteristic polynomial as te two complex roots λ 1,2 = a 2 ± i 4a 1 + a In every case we need to impose conditions on te coefficients of te caracteristic polynomial so as te real part of all eigenvalues is negative. 12

13 Indeed, in case (i) te double real root of te caracteristic polynomial is negative if and only if a 2 < 0, wic troug te discriminant condition implies also tat a 1 < 0. In case (ii) we need to impose tat bot real eigenvalues are negative; i.e., λ 1 = a 2 a a 1 2 < 0, λ 2 = a 2 + a a 1 < 0 2 a a 1 < a 2 a 2 <0 a a 1 < a 2 2 a 1 < 0. Note tat te latter condition implies bot tat a j < 0 for j = 1, 2. Ten te former condition olds as well. In case (iii) te common real part of te two complex eigenvalues is negative if and only if a 2 < 0, wic troug te discriminant condition also implies tat a 1 < 0. Consequently, in all cases te real part of bot eigenvalues of matrix Λ is negative if and only if a j < 0, j = 1, 2. We now compute te stationary variance V of te CAR(2) process of (3.20), as given in (3.21), beginning wit te computation of te matrix e tλ, t 0. In particular, we are looking for f(λ), were f(λ) = e λt. From standard matrix teory, tis can be computed via a polynomial expression of order 1, and tus f(λ) = δ 0 I + δ 1 Λ. Hence, it suffices to set g(λ) = δ 0 + δ 1 λ and to demand tat f(λ) and g(λ) to be equal on te spectrum of Λ. Ten we will ave tat f(λ) = g(λ). Te roots (one double or two real/complex) λ 1, λ 2 of te caracteristic polynomial φ(λ) of Λ satisfy te relationsips: λ 1 + λ 2 = a 2 and λ 1 λ 2 = a 1. (3.22) Since te polynomials f(λ) = e λt and g(λ) = δ 0 + δ 1 λ must be equal on te spectrum of Λ, we ave tat f(λ 1 ) = g(λ 1 ) e λ 1 t = δ 0 + δ 1 λ 1, f(λ 2 ) = g(λ 2 ) e λ 2 t = δ 0 + δ 1 λ 2. 13

14 Ten, e Λt = f(λ) = g(λ) = δ 0 I + δ 1 Λ = δ 0 δ 1. a 1 δ 1 δ 0 + a 2 δ 1 From (3.21), we compute te stationary variance V = 0 e tλ ΣΣ e tλ dt = σ 2 0 e tλ [ (e tλ ) dt. For any a < 0 we ave tat e (a+bi)t dt = e(a+bi)t (a + bi) 0 0 = 1 a + bi. Using te equalities in (3.22), we can rewrite te covariance function as: = σ 2 λ 2e λ 1 (s t) λ 1 e λ 2 (s t) 2a 1 a 2 (λ 2 λ 1 ) σ 2 eλ 2 (s t) e λ 1 (s t) 2a 2 (λ 2 λ 1 ) σ 2 eλ 2 (s t) e λ 1 (s t) 2a 2 (λ 2 λ 1 ) σ 2 λ 2e λ 2 (s t) λ 1 e λ 1 (s t) 2a 2 (λ 2 λ 1 ), 0 t s <. 3.5 Weak Convergence of -AR(p) process to CAR(p) process We now consider te AR(p) process on te discrete time domain {0,, 2,...}, given as X t = b 1X t + b 2X t b i X t i + + b px t p + ς Z t, (3.23) Z t IID N(0, 1), t = p, (p + 1),..., and sow tat subject to suitable conditions on te coefficients b 1, b 2,... b p and ς, tis converges as 0 to its continuous time CAR(p) process of te form p 1 Y (p) t = a i+1 Y (i) t + σw t, t > 0, (3.24) i=0 14

15 for a j 0, j = 1, 2,..., p, and σ 2 > 0. Define te coefficients {c j : j = 1,..., p} and ζ troug te equations { (p ) ( ) } k 1 b i ( 1) i 1 + p k+1 c k, and (3.25) i i 1 ς p 1 ξ. k=i Te following teorem, wic is relegated to te Appendix, can be proven: Teorem 3.3. Te -AR(p) process of (3.23) wit coefficients given by (3.25), were c j a j, j = 1, 2,..., p, and ξ / σ as 0, converges in distribution to te CAR(p) process of (3.24). It is of interest to note te scaling for te Gaussian variable Z t in (3.23). In order to ave te desired convergence, one must ave ζ σ and via (3.25 tis entails ζ σ p 1/2. APPENDIX Te Appendix proves Teorem 5.3. To do so, we first study te similarity of te -AR(p) process in (3.23) wit te CAR(p) process (3.24). We begin by introducing te corresponding -VAR(p) process 0;t 0;t = 1;t, 1;t 1;t = 2;t, i 1;t i 1;t = i;t,. (A.1) p 2;t p 2;t = p 1;t,. p 1 p 1;t p 1;t = c i+1 i;t + ξ Z t, i=0 Te process of (A.1) immediately yields: i=1 = 1;t = 0;t 0;t 2 Z t IID N(0, 1), t =, 2,... 15

16 = ( ) 1 ( 1) 0 0;t + 0 i=2 = 2 2;t = [ 1;t 1;t 2 ( ) 1 ( 1) 1 1 0;t 2, = [ 0;t 0;t 2 [ 0;t 2 1;t 3 = 0;t 2 0;t 2 + 0;t 3 ( ) ( ) ( ) = ( 1) 0 0;t + ( 1) 1 0;t 2 + ( 1) ;t 3. Te process of (A.1) generalizes as follows: i+1 ( ) i i i;t = ( 1) k 1 k 1 0;t k, k=1 (A.2) for i = 1, 2,..., p 1. We prove (A.2) via matematical induction. (i) For i = 1 te relationsip (A.2) olds trivially. (ii) Let (A.2) old for i = m. (iii) We sall sow tat (A.2) also olds for i = m + 1. m+1 m+1;t (A.1) for i=m+1 =========== m m;t m m;t 2 m+1 (ii) === k=1 m+1 k=1 ( ) m ( 1) k 1 k 1 0;t k ( ) m ( 1) k 1 0;t (k+1) k 1 m+1 2nd sum: l=k+1 =========== = m+2 k=1 k=1 m+2 l=2 ( ) m ( 1) k 1 k 1 0;t k+ ( ) m ( 1) l 1 0;t l l 2 ( ) m + 1 ( 1) k 1 k 1 0;t k. 16

17 Furtermore, we ave tat 0;t (A.1) for i=1 ========= 0;t + 1;t (A.1) for i=2 ========= 0;t + [ 1;t + 2;t = 0;t + 1;t + 2 2;t p 2 = = i i;t + p 1 p 1;t i=0 p 2 by te last equation of (A.1) ================== p 1 (A.2) ==== i=0 i i;t + [ p 1 p 1;t + i=0 p 1 c i+1 i;t + ξ Z t i=0 [ i p i c i+1 by intercanging te sums =============== k=1 ( ) i ( 1) k 1 0;t k + p 1 ξ Z t k 1 { p 1 ( 1) k 1 k=1 i=k 1 0;t k + p 1 ξ Z t ( ) i [ } 1 + p i c i+1 k 1 telescopic sum ========== { (p ) ( 1) k 1 + k k=1 p 1 ξ Z t, i=k ( ) } i 1 p i+1 c i k 1 0;t k+ wic, wen compared wit te -AR(p) process of (3.23), yields te relationsips { (p ) ( ) } k 1 b i ( 1) i 1 + p k+1 c k, and (A.3) i i 1 ς p 1 ξ k=i 17

18 for all i = 1, 2..., p. From above, te -AR(p) process of (3.23) wit coefficients given by (3.25) is equivalent to te -VAR(p) of (A.1). We conclude wit a statement of Teorem 5.3, te proof and supporting details of wic are in te Appendix. We sall next find te coefficients c i, i = 1, 2,..., p, in terms of te coefficients b i, i = 1, 2,..., p. In particular, we ave tat, from (3.25), {( ) ( ) } i=p p p 1 = b p = ( 1) p 1 + c p p p 1 [ ( ) p 1 c p = 1 ( 1) p 1 b p 1 p 1 and { ( ) i=p 1 p = b p 1 = ( 1) p 2 + p 1 k=p 1 { [( ) p 2 c p 1 = 2 ( 1) p 2 b p 1 + p 2 ( ) } k 1 p k+1 c k p 2 ( ) } p 1 b p 1. p 2 Proposition A.1. Tis gives te general formula [ ( ) k 1 c i = p+i 1 ( 1) i 1 b k 1, i = 1, 2,..., p. (A.4) i 1 k=i Proof. We prove Proposition A.1 by backward induction. (i) For i = p te relationsip (A.4) olds trivially. (ii) Let (A.4) old for every i = p 1, p 2,..., m + 1. (iii) We sall sow tat (A.4) also olds for i = m. { ( ) i=m p = b m = ( 1) m 1 + m i=m+1 i=m ( ) (i), (ii) p = ( 1) m 1 b m = + p m+1 c m m+ ( ) i 1 ( 1) i 1 m 1 ( ) i 1 p i+1 c i m 1 k=i } ( ) k 1 b k i 1 i=m+1 ( ) i 1. m 1 Hence, intercanging te order of summation in te double sum, te former 18

19 index bounds i k p and m+1 i p ave now become m+1 i k and m + 1 k p. We furter ave: as well as i=m+1 ( ) i 1 ( ) k 1 ( 1) i 1 b k = m 1 i 1 i=m+1 k=i k ( )( ) i 1 k 1 = b k ( 1) i 1 m 1 i 1 k=m+1 j=i m ====== i=m+1 k=m+1 b k = ( 1) m 1 k=m+1 ( ) k m k 1 ( ) k m ( 1) j+m 1 m 1 j b k Newton ====== ( 1) m 1 = ( 1) m ( ) i 1 = m 1 k=m+1 i=m+1 Te last relationsip yields b k j=1 ( ) [ k m k 1 ( ) k m ( 1) j m 1 j k=m+1 b k ( ) k 1, m 1 [( ) i m j=0 1 ( ) k 1 [ ( 1 + 1) k m 1 m 1 ( ) i 1 m telescopic sum ========== ( ) p ( 1) m 1 b m = + p m+1 c m + ( 1) m m [( ) p 1 m ( ) k 1 p m+1 c m = ( 1) m 1 b k 1, m 1 k=m concluding part (iii) and tus te proof. 19 k=m+1 b k ( ) p 1. m ( ) k 1 m 1

20 Finally, for t > 0 we know tat: dy t = Y (1) t dt, dy (1) dy (i 1) t dy (p 2) t t = Y (2) t dt,.. = Y (i) t dt, (A.5) = Y (p 1) t dt, and from (3.24) we ave also tat [ dy (p 1) t = a 1 Y t + a 2 Y (1) t + + a i Y (i 1) t + + a p 1 Y (p 2) t + a p Y (p 1) t dt + σdw t. (A.6) Tus te CAR(p) process of (3.24) is equivalent from (A.5) and (A.6) to te system of stocastic differential equations in (2.1). Teorem 5.3 Te -AR(p) process of (3.23) wit coefficients given by (3.25), were c j a j, j = 1, 2,..., p, and ξ / σ as 0, converges in distribution to te CAR(p) process of (3.24). Proof. We generalize Teorem 3.3 by proving tat it suffices to sow tat te -VAR(p) process of (A.1) converges to te SDEs system of (2.1). As in Teorem 5.1.1, we employ te framework of Teorems 2.1 and 2.2 of [8. Let M t be te σ-algebra generated by i;0, i;, i;2,..., i;t, i = 0, 1,..., p 2, and p 1;0, p 1;, p 1;2,..., p 1;t for t =, 2,... Te -VAR(p) process of (A.1) is clearly Markovian of order 1, since we may construct 0;t, 1;t, 2;t,..., p 1;t from 0;t, 1;t, 2;t,..., p 1;t by constructing first p 1;t from te last equation of (A.1), p 2;t from (A.1) for i = p 1, and so fort, and ten finally 0;t from (A.1) for i = 1. Tis also establises tat i;t, i = 0, 1,..., p 2 is M t adapted. Tus te corresponding drifts per unit of time conditioned on information at time t are given by: [ i 1;t [ i 1;t E M (A.1) i 1;t + i;t i 1;t t ==== E M t 20

21 = i;t, i = 1, 2,..., p 1, (A.7) and [ p 1;t+ p 1;t E M t [ by te last equation of (A.1) p 1 i=0 ================== E c i+1 i;t + ξ Z t+ M t = c 1 0;t + c 2 1;t + + c p p 1;t. (A.8) Furtermore, te variances and covariances per unit of time are given by ( ) 2 ( ) i 1;t 2 i 1;t E M t ==== (A.1) i;t E M t ( 2, = i;t) i = 1, 2,..., p 1, (A.9) and ( p 1;t+ p 1;t E ) 2 M t [ by te last equation of (A.1) 2 p 1 i=0 c i+1 i;t) + ξ Z t+ ================== E M t = [ c 1 0;t + c 2 1;t + + c p p 1;t 2 + ( ξ ) 2, (A.10) were te last equality assumes tat Z t+ IID N(0, 1). By te same logic: ( )( ) i 1;t i 1;t j 1;t j 1;t E M t 21

22 and ( )( ) (A.1) i;t j;t ==== E M t = i;t j;t, i, j = 1, 2,..., p 1, i j, (A.11) ( )( ) i 1;t i 1;t p 1;t+ E p 1;t M t [ (c ) (A.1) ==== E i;t 1 0;t + c 2 1;t + + c p p 1;t + ξ Z t+ M t [ = i;t c 1 0;t + c 2 1;t + + c p p 1;t, i = 1, 2,..., p 1. (A.12) Terefore, te relationsips of (A.9) - (A.12) become ( i 1;t i 1;t E ) 2 M t = o(1), i = 1, 2,..., p 1, (A.13) ( p 1;t+ p 1;t E ) 2 M t = ( ξ ) 2 + o(1), (A.14) ( )( E i 1;t i 1;t j 1;t j 1;t ) M t = o(1) (A.15) and ( )( E i, j = 1, 2,..., p 1, i j i 1;t i 1;t p 1;t+ p 1;t ) M t = o(1), (A.16) 22

23 i = 1, 2,..., p 1, were te o(1) terms vanis uniformly on compact sets. We may also sow by brute force tat te limits of ( ) 4 i 1;t i 1;t E M t, i = 1, 2,..., p 1 and ( p 1;t+ p 1;t E ) 4 M t exist and converge to zero as 0. We can ten define te continuous time version of te -VAR(p) process of (A.1) by i;t i;k for k t < (k + 1) and i = 0, 1,..., p 1. Tus, according to Teorem 2.2 in [8, te relationsips (A.7), (A.8) and (A.13) - (A.16) provide te weak (in distribution) limit diffusion. Tis is precisely te linear SDE system of (2.1) and it as a unique solution. References [1 Anderson, T. Te Statistical Analysis of Time Series. Wiley- Interscience, [2 Brockwell, P. J., Ferrazzano, V., and Klüppelberg, C. Higfrequency sampling and kernel estimation for continuous-time moving average processes. J. Time Series Anal. 34, 3 (2013), [3 Brockwell, P. J., and Lindner, A. Existence and uniqueness of stationary Lévy-driven CARMA processes. Stocastic Process. Appl. 119, 8 (2009), [4 Brockwell, P. J., and Lindner, A. Strictly stationary solutions of autoregressive moving average equations. Biometrika 97, 3 (2010),

24 [5 Brockwell, P. Davis, R., and Yang, Y. Continuous-time Gaussian autoregression. Statistica Sinica 17, 1 (2007), 63. [6 Dym, H., and McKean, H. Gaussian Processes, Function Teory, an te Inverse Spectral Problem. Academic Press, [7 Karatzas, I., and Sreve, S. Brownian Motion and Stocastic Calculus. Springer, [8 Nelson, D. ARCH models as diffusion approximations. Journal of Econometrics 45, 1 (1990), [9 Papoulis, A. Probability, Random Variables, Stocastic Processes. Mc- Graw Hill, [10 Rasmussen, C., and Williams, C. Te Statistical Analysis of Time Series. MIT Press,

Stationary Gaussian Markov processes as limits of stationary autoregressive time series

Stationary Gaussian Markov processes as limits of stationary autoregressive time series Stationary Gaussian Markov processes as liits of stationary autoregressive tie series Pilip A. rnst 1,, Lawrence D. Brown 2,, Larry Sepp 3,, Robert L. Wolpert 4, Abstract We consider te class, C p, of

More information

Differentiation in higher dimensions

Differentiation in higher dimensions Capter 2 Differentiation in iger dimensions 2.1 Te Total Derivative Recall tat if f : R R is a 1-variable function, and a R, we say tat f is differentiable at x = a if and only if te ratio f(a+) f(a) tends

More information

HOMEWORK HELP 2 FOR MATH 151

HOMEWORK HELP 2 FOR MATH 151 HOMEWORK HELP 2 FOR MATH 151 Here we go; te second round of omework elp. If tere are oters you would like to see, let me know! 2.4, 43 and 44 At wat points are te functions f(x) and g(x) = xf(x)continuous,

More information

Polynomial Interpolation

Polynomial Interpolation Capter 4 Polynomial Interpolation In tis capter, we consider te important problem of approximatinga function fx, wose values at a set of distinct points x, x, x,, x n are known, by a polynomial P x suc

More information

Financial Econometrics Prof. Massimo Guidolin

Financial Econometrics Prof. Massimo Guidolin CLEFIN A.A. 2010/2011 Financial Econometrics Prof. Massimo Guidolin A Quick Review of Basic Estimation Metods 1. Were te OLS World Ends... Consider two time series 1: = { 1 2 } and 1: = { 1 2 }. At tis

More information

The derivative function

The derivative function Roberto s Notes on Differential Calculus Capter : Definition of derivative Section Te derivative function Wat you need to know already: f is at a point on its grap and ow to compute it. Wat te derivative

More information

Lecture XVII. Abstract We introduce the concept of directional derivative of a scalar function and discuss its relation with the gradient operator.

Lecture XVII. Abstract We introduce the concept of directional derivative of a scalar function and discuss its relation with the gradient operator. Lecture XVII Abstract We introduce te concept of directional derivative of a scalar function and discuss its relation wit te gradient operator. Directional derivative and gradient Te directional derivative

More information

1 The concept of limits (p.217 p.229, p.242 p.249, p.255 p.256) 1.1 Limits Consider the function determined by the formula 3. x since at this point

1 The concept of limits (p.217 p.229, p.242 p.249, p.255 p.256) 1.1 Limits Consider the function determined by the formula 3. x since at this point MA00 Capter 6 Calculus and Basic Linear Algebra I Limits, Continuity and Differentiability Te concept of its (p.7 p.9, p.4 p.49, p.55 p.56). Limits Consider te function determined by te formula f Note

More information

Mathematics 5 Worksheet 11 Geometry, Tangency, and the Derivative

Mathematics 5 Worksheet 11 Geometry, Tangency, and the Derivative Matematics 5 Workseet 11 Geometry, Tangency, and te Derivative Problem 1. Find te equation of a line wit slope m tat intersects te point (3, 9). Solution. Te equation for a line passing troug a point (x

More information

Polynomial Interpolation

Polynomial Interpolation Capter 4 Polynomial Interpolation In tis capter, we consider te important problem of approximating a function f(x, wose values at a set of distinct points x, x, x 2,,x n are known, by a polynomial P (x

More information

POLYNOMIAL AND SPLINE ESTIMATORS OF THE DISTRIBUTION FUNCTION WITH PRESCRIBED ACCURACY

POLYNOMIAL AND SPLINE ESTIMATORS OF THE DISTRIBUTION FUNCTION WITH PRESCRIBED ACCURACY APPLICATIONES MATHEMATICAE 36, (29), pp. 2 Zbigniew Ciesielski (Sopot) Ryszard Zieliński (Warszawa) POLYNOMIAL AND SPLINE ESTIMATORS OF THE DISTRIBUTION FUNCTION WITH PRESCRIBED ACCURACY Abstract. Dvoretzky

More information

Solutions to the Multivariable Calculus and Linear Algebra problems on the Comprehensive Examination of January 31, 2014

Solutions to the Multivariable Calculus and Linear Algebra problems on the Comprehensive Examination of January 31, 2014 Solutions to te Multivariable Calculus and Linear Algebra problems on te Compreensive Examination of January 3, 24 Tere are 9 problems ( points eac, totaling 9 points) on tis portion of te examination.

More information

Volume 29, Issue 3. Existence of competitive equilibrium in economies with multi-member households

Volume 29, Issue 3. Existence of competitive equilibrium in economies with multi-member households Volume 29, Issue 3 Existence of competitive equilibrium in economies wit multi-member ouseolds Noriisa Sato Graduate Scool of Economics, Waseda University Abstract Tis paper focuses on te existence of

More information

Analytic Functions. Differentiable Functions of a Complex Variable

Analytic Functions. Differentiable Functions of a Complex Variable Analytic Functions Differentiable Functions of a Complex Variable In tis capter, we sall generalize te ideas for polynomials power series of a complex variable we developed in te previous capter to general

More information

A SHORT INTRODUCTION TO BANACH LATTICES AND

A SHORT INTRODUCTION TO BANACH LATTICES AND CHAPTER A SHORT INTRODUCTION TO BANACH LATTICES AND POSITIVE OPERATORS In tis capter we give a brief introduction to Banac lattices and positive operators. Most results of tis capter can be found, e.g.,

More information

Symmetry Labeling of Molecular Energies

Symmetry Labeling of Molecular Energies Capter 7. Symmetry Labeling of Molecular Energies Notes: Most of te material presented in tis capter is taken from Bunker and Jensen 1998, Cap. 6, and Bunker and Jensen 2005, Cap. 7. 7.1 Hamiltonian Symmetry

More information

1. Introduction. Tis paper is concerned wit estimation of te parameters of a non-negative Levydriven Ornstein-Ulenbeck process and of te parameters of

1. Introduction. Tis paper is concerned wit estimation of te parameters of a non-negative Levydriven Ornstein-Ulenbeck process and of te parameters of Estimation for on-negative Levy-driven Ornstein-Ulenbeck Processes Peter J. Brockwell, Ricard A. Davis and Yu Yang, Department of Statistics, Colorado State University, Fort Collins, CO 8523-1877 Abstract

More information

Function Composition and Chain Rules

Function Composition and Chain Rules Function Composition and s James K. Peterson Department of Biological Sciences and Department of Matematical Sciences Clemson University Marc 8, 2017 Outline 1 Function Composition and Continuity 2 Function

More information

Exam 1 Review Solutions

Exam 1 Review Solutions Exam Review Solutions Please also review te old quizzes, and be sure tat you understand te omework problems. General notes: () Always give an algebraic reason for your answer (graps are not sufficient),

More information

NUMERICAL DIFFERENTIATION

NUMERICAL DIFFERENTIATION NUMERICAL IFFERENTIATION FIRST ERIVATIVES Te simplest difference formulas are based on using a straigt line to interpolate te given data; tey use two data pints to estimate te derivative. We assume tat

More information

WYSE Academic Challenge 2004 Sectional Mathematics Solution Set

WYSE Academic Challenge 2004 Sectional Mathematics Solution Set WYSE Academic Callenge 00 Sectional Matematics Solution Set. Answer: B. Since te equation can be written in te form x + y, we ave a major 5 semi-axis of lengt 5 and minor semi-axis of lengt. Tis means

More information

1 Calculus. 1.1 Gradients and the Derivative. Q f(x+h) f(x)

1 Calculus. 1.1 Gradients and the Derivative. Q f(x+h) f(x) Calculus. Gradients and te Derivative Q f(x+) δy P T δx R f(x) 0 x x+ Let P (x, f(x)) and Q(x+, f(x+)) denote two points on te curve of te function y = f(x) and let R denote te point of intersection of

More information

University Mathematics 2

University Mathematics 2 University Matematics 2 1 Differentiability In tis section, we discuss te differentiability of functions. Definition 1.1 Differentiable function). Let f) be a function. We say tat f is differentiable at

More information

GELFAND S PROOF OF WIENER S THEOREM

GELFAND S PROOF OF WIENER S THEOREM GELFAND S PROOF OF WIENER S THEOREM S. H. KULKARNI 1. Introduction Te following teorem was proved by te famous matematician Norbert Wiener. Wiener s proof can be found in is book [5]. Teorem 1.1. (Wiener

More information

On convexity of polynomial paths and generalized majorizations

On convexity of polynomial paths and generalized majorizations On convexity of polynomial pats and generalized majorizations Marija Dodig Centro de Estruturas Lineares e Combinatórias, CELC, Universidade de Lisboa, Av. Prof. Gama Pinto 2, 1649-003 Lisboa, Portugal

More information

Derivatives of Exponentials

Derivatives of Exponentials mat 0 more on derivatives: day 0 Derivatives of Eponentials Recall tat DEFINITION... An eponential function as te form f () =a, were te base is a real number a > 0. Te domain of an eponential function

More information

MVT and Rolle s Theorem

MVT and Rolle s Theorem AP Calculus CHAPTER 4 WORKSHEET APPLICATIONS OF DIFFERENTIATION MVT and Rolle s Teorem Name Seat # Date UNLESS INDICATED, DO NOT USE YOUR CALCULATOR FOR ANY OF THESE QUESTIONS In problems 1 and, state

More information

Preface. Here are a couple of warnings to my students who may be here to get a copy of what happened on a day that you missed.

Preface. Here are a couple of warnings to my students who may be here to get a copy of what happened on a day that you missed. Preface Here are my online notes for my course tat I teac ere at Lamar University. Despite te fact tat tese are my class notes, tey sould be accessible to anyone wanting to learn or needing a refreser

More information

Quantum Numbers and Rules

Quantum Numbers and Rules OpenStax-CNX module: m42614 1 Quantum Numbers and Rules OpenStax College Tis work is produced by OpenStax-CNX and licensed under te Creative Commons Attribution License 3.0 Abstract Dene quantum number.

More information

LIMITS AND DERIVATIVES CONDITIONS FOR THE EXISTENCE OF A LIMIT

LIMITS AND DERIVATIVES CONDITIONS FOR THE EXISTENCE OF A LIMIT LIMITS AND DERIVATIVES Te limit of a function is defined as te value of y tat te curve approaces, as x approaces a particular value. Te limit of f (x) as x approaces a is written as f (x) approaces, as

More information

Math 161 (33) - Final exam

Math 161 (33) - Final exam Name: Id #: Mat 161 (33) - Final exam Fall Quarter 2015 Wednesday December 9, 2015-10:30am to 12:30am Instructions: Prob. Points Score possible 1 25 2 25 3 25 4 25 TOTAL 75 (BEST 3) Read eac problem carefully.

More information

THE IDEA OF DIFFERENTIABILITY FOR FUNCTIONS OF SEVERAL VARIABLES Math 225

THE IDEA OF DIFFERENTIABILITY FOR FUNCTIONS OF SEVERAL VARIABLES Math 225 THE IDEA OF DIFFERENTIABILITY FOR FUNCTIONS OF SEVERAL VARIABLES Mat 225 As we ave seen, te definition of derivative for a Mat 111 function g : R R and for acurveγ : R E n are te same, except for interpretation:

More information

. If lim. x 2 x 1. f(x+h) f(x)

. If lim. x 2 x 1. f(x+h) f(x) Review of Differential Calculus Wen te value of one variable y is uniquely determined by te value of anoter variable x, ten te relationsip between x and y is described by a function f tat assigns a value

More information

1.5 Functions and Their Rates of Change

1.5 Functions and Their Rates of Change 66_cpp-75.qd /6/8 4:8 PM Page 56 56 CHAPTER Introduction to Functions and Graps.5 Functions and Teir Rates of Cange Identif were a function is increasing or decreasing Use interval notation Use and interpret

More information

3.4 Worksheet: Proof of the Chain Rule NAME

3.4 Worksheet: Proof of the Chain Rule NAME Mat 1170 3.4 Workseet: Proof of te Cain Rule NAME Te Cain Rule So far we are able to differentiate all types of functions. For example: polynomials, rational, root, and trigonometric functions. We are

More information

Combining functions: algebraic methods

Combining functions: algebraic methods Combining functions: algebraic metods Functions can be added, subtracted, multiplied, divided, and raised to a power, just like numbers or algebra expressions. If f(x) = x 2 and g(x) = x + 2, clearly f(x)

More information

Pre-Calculus Review Preemptive Strike

Pre-Calculus Review Preemptive Strike Pre-Calculus Review Preemptive Strike Attaced are some notes and one assignment wit tree parts. Tese are due on te day tat we start te pre-calculus review. I strongly suggest reading troug te notes torougly

More information

Math 31A Discussion Notes Week 4 October 20 and October 22, 2015

Math 31A Discussion Notes Week 4 October 20 and October 22, 2015 Mat 3A Discussion Notes Week 4 October 20 and October 22, 205 To prepare for te first midterm, we ll spend tis week working eamples resembling te various problems you ve seen so far tis term. In tese notes

More information

Continuity and Differentiability Worksheet

Continuity and Differentiability Worksheet Continuity and Differentiability Workseet (Be sure tat you can also do te grapical eercises from te tet- Tese were not included below! Typical problems are like problems -3, p. 6; -3, p. 7; 33-34, p. 7;

More information

5.1 We will begin this section with the definition of a rational expression. We

5.1 We will begin this section with the definition of a rational expression. We Basic Properties and Reducing to Lowest Terms 5.1 We will begin tis section wit te definition of a rational epression. We will ten state te two basic properties associated wit rational epressions and go

More information

158 Calculus and Structures

158 Calculus and Structures 58 Calculus and Structures CHAPTER PROPERTIES OF DERIVATIVES AND DIFFERENTIATION BY THE EASY WAY. Calculus and Structures 59 Copyrigt Capter PROPERTIES OF DERIVATIVES. INTRODUCTION In te last capter you

More information

Generic maximum nullity of a graph

Generic maximum nullity of a graph Generic maximum nullity of a grap Leslie Hogben Bryan Sader Marc 5, 2008 Abstract For a grap G of order n, te maximum nullity of G is defined to be te largest possible nullity over all real symmetric n

More information

Solution. Solution. f (x) = (cos x)2 cos(2x) 2 sin(2x) 2 cos x ( sin x) (cos x) 4. f (π/4) = ( 2/2) ( 2/2) ( 2/2) ( 2/2) 4.

Solution. Solution. f (x) = (cos x)2 cos(2x) 2 sin(2x) 2 cos x ( sin x) (cos x) 4. f (π/4) = ( 2/2) ( 2/2) ( 2/2) ( 2/2) 4. December 09, 20 Calculus PracticeTest s Name: (4 points) Find te absolute extrema of f(x) = x 3 0 on te interval [0, 4] Te derivative of f(x) is f (x) = 3x 2, wic is zero only at x = 0 Tus we only need

More information

Definition of the Derivative

Definition of the Derivative Te Limit Definition of te Derivative Tis Handout will: Define te limit grapically and algebraically Discuss, in detail, specific features of te definition of te derivative Provide a general strategy of

More information

More on generalized inverses of partitioned matrices with Banachiewicz-Schur forms

More on generalized inverses of partitioned matrices with Banachiewicz-Schur forms More on generalized inverses of partitioned matrices wit anaciewicz-scur forms Yongge Tian a,, Yosio Takane b a Cina Economics and Management cademy, Central University of Finance and Economics, eijing,

More information

4. The slope of the line 2x 7y = 8 is (a) 2/7 (b) 7/2 (c) 2 (d) 2/7 (e) None of these.

4. The slope of the line 2x 7y = 8 is (a) 2/7 (b) 7/2 (c) 2 (d) 2/7 (e) None of these. Mat 11. Test Form N Fall 016 Name. Instructions. Te first eleven problems are wort points eac. Te last six problems are wort 5 points eac. For te last six problems, you must use relevant metods of algebra

More information

Cointegration in functional autoregressive processes

Cointegration in functional autoregressive processes Dipartimento di Scienze Statistice Sezione di Statistica Economica ed Econometria Massimo Franci Paolo Paruolo Cointegration in functional autoregressive processes DSS Empirical Economics and Econometrics

More information

= 0 and states ''hence there is a stationary point'' All aspects of the proof dx must be correct (c)

= 0 and states ''hence there is a stationary point'' All aspects of the proof dx must be correct (c) Paper 1: Pure Matematics 1 Mark Sceme 1(a) (i) (ii) d d y 3 1x 4x x M1 A1 d y dx 1.1b 1.1b 36x 48x A1ft 1.1b Substitutes x = into teir dx (3) 3 1 4 Sows d y 0 and states ''ence tere is a stationary point''

More information

Poisson Equation in Sobolev Spaces

Poisson Equation in Sobolev Spaces Poisson Equation in Sobolev Spaces OcMountain Dayligt Time. 6, 011 Today we discuss te Poisson equation in Sobolev spaces. It s existence, uniqueness, and regularity. Weak Solution. u = f in, u = g on

More information

Smoothness of solutions with respect to multi-strip integral boundary conditions for nth order ordinary differential equations

Smoothness of solutions with respect to multi-strip integral boundary conditions for nth order ordinary differential equations 396 Nonlinear Analysis: Modelling and Control, 2014, Vol. 19, No. 3, 396 412 ttp://dx.doi.org/10.15388/na.2014.3.6 Smootness of solutions wit respect to multi-strip integral boundary conditions for nt

More information

Lecture 21. Numerical differentiation. f ( x+h) f ( x) h h

Lecture 21. Numerical differentiation. f ( x+h) f ( x) h h Lecture Numerical differentiation Introduction We can analytically calculate te derivative of any elementary function, so tere migt seem to be no motivation for calculating derivatives numerically. However

More information

How to Find the Derivative of a Function: Calculus 1

How to Find the Derivative of a Function: Calculus 1 Introduction How to Find te Derivative of a Function: Calculus 1 Calculus is not an easy matematics course Te fact tat you ave enrolled in suc a difficult subject indicates tat you are interested in te

More information

Test 2 Review. 1. Find the determinant of the matrix below using (a) cofactor expansion and (b) row reduction. A = 3 2 =

Test 2 Review. 1. Find the determinant of the matrix below using (a) cofactor expansion and (b) row reduction. A = 3 2 = Test Review Find te determinant of te matrix below using (a cofactor expansion and (b row reduction Answer: (a det + = (b Observe R R R R R R R R R Ten det B = (((det Hence det Use Cramer s rule to solve:

More information

Quaternion Dynamics, Part 1 Functions, Derivatives, and Integrals. Gary D. Simpson. rev 01 Aug 08, 2016.

Quaternion Dynamics, Part 1 Functions, Derivatives, and Integrals. Gary D. Simpson. rev 01 Aug 08, 2016. Quaternion Dynamics, Part 1 Functions, Derivatives, and Integrals Gary D. Simpson gsim1887@aol.com rev 1 Aug 8, 216 Summary Definitions are presented for "quaternion functions" of a quaternion. Polynomial

More information

Strongly continuous semigroups

Strongly continuous semigroups Capter 2 Strongly continuous semigroups Te main application of te teory developed in tis capter is related to PDE systems. Tese systems can provide te strong continuity properties only. 2.1 Closed operators

More information

Semigroups of Operators

Semigroups of Operators Lecture 11 Semigroups of Operators In tis Lecture we gater a few notions on one-parameter semigroups of linear operators, confining to te essential tools tat are needed in te sequel. As usual, X is a real

More information

arxiv: v1 [math.pr] 28 Dec 2018

arxiv: v1 [math.pr] 28 Dec 2018 Approximating Sepp s constants for te Slepian process Jack Noonan a, Anatoly Zigljavsky a, a Scool of Matematics, Cardiff University, Cardiff, CF4 4AG, UK arxiv:8.0v [mat.pr] 8 Dec 08 Abstract Slepian

More information

Functions of the Complex Variable z

Functions of the Complex Variable z Capter 2 Functions of te Complex Variable z Introduction We wis to examine te notion of a function of z were z is a complex variable. To be sure, a complex variable can be viewed as noting but a pair of

More information

lecture 26: Richardson extrapolation

lecture 26: Richardson extrapolation 43 lecture 26: Ricardson extrapolation 35 Ricardson extrapolation, Romberg integration Trougout numerical analysis, one encounters procedures tat apply some simple approximation (eg, linear interpolation)

More information

Chapter 5 FINITE DIFFERENCE METHOD (FDM)

Chapter 5 FINITE DIFFERENCE METHOD (FDM) MEE7 Computer Modeling Tecniques in Engineering Capter 5 FINITE DIFFERENCE METHOD (FDM) 5. Introduction to FDM Te finite difference tecniques are based upon approximations wic permit replacing differential

More information

Click here to see an animation of the derivative

Click here to see an animation of the derivative Differentiation Massoud Malek Derivative Te concept of derivative is at te core of Calculus; It is a very powerful tool for understanding te beavior of matematical functions. It allows us to optimize functions,

More information

The Verlet Algorithm for Molecular Dynamics Simulations

The Verlet Algorithm for Molecular Dynamics Simulations Cemistry 380.37 Fall 2015 Dr. Jean M. Standard November 9, 2015 Te Verlet Algoritm for Molecular Dynamics Simulations Equations of motion For a many-body system consisting of N particles, Newton's classical

More information

ACCESS TO SCIENCE, ENGINEERING AND AGRICULTURE: MATHEMATICS 1 MATH00030 SEMESTER /2019

ACCESS TO SCIENCE, ENGINEERING AND AGRICULTURE: MATHEMATICS 1 MATH00030 SEMESTER /2019 ACCESS TO SCIENCE, ENGINEERING AND AGRICULTURE: MATHEMATICS MATH00030 SEMESTER 208/209 DR. ANTHONY BROWN 6. Differential Calculus 6.. Differentiation from First Principles. In tis capter, we will introduce

More information

Differential Calculus (The basics) Prepared by Mr. C. Hull

Differential Calculus (The basics) Prepared by Mr. C. Hull Differential Calculus Te basics) A : Limits In tis work on limits, we will deal only wit functions i.e. tose relationsips in wic an input variable ) defines a unique output variable y). Wen we work wit

More information

NUMERICAL DIFFERENTIATION. James T. Smith San Francisco State University. In calculus classes, you compute derivatives algebraically: for example,

NUMERICAL DIFFERENTIATION. James T. Smith San Francisco State University. In calculus classes, you compute derivatives algebraically: for example, NUMERICAL DIFFERENTIATION James T Smit San Francisco State University In calculus classes, you compute derivatives algebraically: for example, f( x) = x + x f ( x) = x x Tis tecnique requires your knowing

More information

MATH1131/1141 Calculus Test S1 v8a

MATH1131/1141 Calculus Test S1 v8a MATH/ Calculus Test 8 S v8a October, 7 Tese solutions were written by Joann Blanco, typed by Brendan Trin and edited by Mattew Yan and Henderson Ko Please be etical wit tis resource It is for te use of

More information

7.1 Using Antiderivatives to find Area

7.1 Using Antiderivatives to find Area 7.1 Using Antiderivatives to find Area Introduction finding te area under te grap of a nonnegative, continuous function f In tis section a formula is obtained for finding te area of te region bounded between

More information

Consider a function f we ll specify which assumptions we need to make about it in a minute. Let us reformulate the integral. 1 f(x) dx.

Consider a function f we ll specify which assumptions we need to make about it in a minute. Let us reformulate the integral. 1 f(x) dx. Capter 2 Integrals as sums and derivatives as differences We now switc to te simplest metods for integrating or differentiating a function from its function samples. A careful study of Taylor expansions

More information

DELFT UNIVERSITY OF TECHNOLOGY Faculty of Electrical Engineering, Mathematics and Computer Science

DELFT UNIVERSITY OF TECHNOLOGY Faculty of Electrical Engineering, Mathematics and Computer Science DELFT UNIVERSITY OF TECHNOLOGY Faculty of Electrical Engineering, Matematics and Computer Science. ANSWERS OF THE TEST NUMERICAL METHODS FOR DIFFERENTIAL EQUATIONS (WI3097 TU) Tuesday January 9 008, 9:00-:00

More information

A = h w (1) Error Analysis Physics 141

A = h w (1) Error Analysis Physics 141 Introduction In all brances of pysical science and engineering one deals constantly wit numbers wic results more or less directly from experimental observations. Experimental observations always ave inaccuracies.

More information

SFU UBC UNBC Uvic Calculus Challenge Examination June 5, 2008, 12:00 15:00

SFU UBC UNBC Uvic Calculus Challenge Examination June 5, 2008, 12:00 15:00 SFU UBC UNBC Uvic Calculus Callenge Eamination June 5, 008, :00 5:00 Host: SIMON FRASER UNIVERSITY First Name: Last Name: Scool: Student signature INSTRUCTIONS Sow all your work Full marks are given only

More information

232 Calculus and Structures

232 Calculus and Structures 3 Calculus and Structures CHAPTER 17 JUSTIFICATION OF THE AREA AND SLOPE METHODS FOR EVALUATING BEAMS Calculus and Structures 33 Copyrigt Capter 17 JUSTIFICATION OF THE AREA AND SLOPE METHODS 17.1 THE

More information

Chapter 2 Limits and Continuity

Chapter 2 Limits and Continuity 4 Section. Capter Limits and Continuity Section. Rates of Cange and Limits (pp. 6) Quick Review.. f () ( ) () 4 0. f () 4( ) 4. f () sin sin 0 4. f (). 4 4 4 6. c c c 7. 8. c d d c d d c d c 9. 8 ( )(

More information

A Goodness-of-fit test for GARCH innovation density. Hira L. Koul 1 and Nao Mimoto Michigan State University. Abstract

A Goodness-of-fit test for GARCH innovation density. Hira L. Koul 1 and Nao Mimoto Michigan State University. Abstract A Goodness-of-fit test for GARCH innovation density Hira L. Koul and Nao Mimoto Micigan State University Abstract We prove asymptotic normality of a suitably standardized integrated square difference between

More information

New families of estimators and test statistics in log-linear models

New families of estimators and test statistics in log-linear models Journal of Multivariate Analysis 99 008 1590 1609 www.elsevier.com/locate/jmva ew families of estimators and test statistics in log-linear models irian Martín a,, Leandro Pardo b a Department of Statistics

More information

SECTION 3.2: DERIVATIVE FUNCTIONS and DIFFERENTIABILITY

SECTION 3.2: DERIVATIVE FUNCTIONS and DIFFERENTIABILITY (Section 3.2: Derivative Functions and Differentiability) 3.2.1 SECTION 3.2: DERIVATIVE FUNCTIONS and DIFFERENTIABILITY LEARNING OBJECTIVES Know, understand, and apply te Limit Definition of te Derivative

More information

f a h f a h h lim lim

f a h f a h h lim lim Te Derivative Te derivative of a function f at a (denoted f a) is f a if tis it exists. An alternative way of defining f a is f a x a fa fa fx fa x a Note tat te tangent line to te grap of f at te point

More information

5.74 Introductory Quantum Mechanics II

5.74 Introductory Quantum Mechanics II MIT OpenCourseWare ttp://ocw.mit.edu 5.74 Introductory Quantum Mecanics II Spring 9 For information about citing tese materials or our Terms of Use, visit: ttp://ocw.mit.edu/terms. Andrei Tokmakoff, MIT

More information

, meant to remind us of the definition of f (x) as the limit of difference quotients: = lim

, meant to remind us of the definition of f (x) as the limit of difference quotients: = lim Mat 132 Differentiation Formulas Stewart 2.3 So far, we ave seen ow various real-world problems rate of cange and geometric problems tangent lines lead to derivatives. In tis section, we will see ow to

More information

ERROR BOUNDS FOR THE METHODS OF GLIMM, GODUNOV AND LEVEQUE BRADLEY J. LUCIER*

ERROR BOUNDS FOR THE METHODS OF GLIMM, GODUNOV AND LEVEQUE BRADLEY J. LUCIER* EO BOUNDS FO THE METHODS OF GLIMM, GODUNOV AND LEVEQUE BADLEY J. LUCIE* Abstract. Te expected error in L ) attimet for Glimm s sceme wen applied to a scalar conservation law is bounded by + 2 ) ) /2 T

More information

Numerical Differentiation

Numerical Differentiation Numerical Differentiation Finite Difference Formulas for te first derivative (Using Taylor Expansion tecnique) (section 8.3.) Suppose tat f() = g() is a function of te variable, and tat as 0 te function

More information

An approximation method using approximate approximations

An approximation method using approximate approximations Applicable Analysis: An International Journal Vol. 00, No. 00, September 2005, 1 13 An approximation metod using approximate approximations FRANK MÜLLER and WERNER VARNHORN, University of Kassel, Germany,

More information

1watt=1W=1kg m 2 /s 3

1watt=1W=1kg m 2 /s 3 Appendix A Matematics Appendix A.1 Units To measure a pysical quantity, you need a standard. Eac pysical quantity as certain units. A unit is just a standard we use to compare, e.g. a ruler. In tis laboratory

More information

Continuity and Differentiability of the Trigonometric Functions

Continuity and Differentiability of the Trigonometric Functions [Te basis for te following work will be te definition of te trigonometric functions as ratios of te sides of a triangle inscribed in a circle; in particular, te sine of an angle will be defined to be te

More information

SECTION 1.10: DIFFERENCE QUOTIENTS LEARNING OBJECTIVES

SECTION 1.10: DIFFERENCE QUOTIENTS LEARNING OBJECTIVES (Section.0: Difference Quotients).0. SECTION.0: DIFFERENCE QUOTIENTS LEARNING OBJECTIVES Define average rate of cange (and average velocity) algebraically and grapically. Be able to identify, construct,

More information

Continuous Stochastic Processes

Continuous Stochastic Processes Continuous Stocastic Processes Te term stocastic is often applied to penomena tat vary in time, wile te word random is reserved for penomena tat vary in space. Apart from tis distinction, te modelling

More information

Homework 1 Due: Wednesday, September 28, 2016

Homework 1 Due: Wednesday, September 28, 2016 0-704 Information Processing and Learning Fall 06 Homework Due: Wednesday, September 8, 06 Notes: For positive integers k, [k] := {,..., k} denotes te set of te first k positive integers. Wen p and Y q

More information

5 Ordinary Differential Equations: Finite Difference Methods for Boundary Problems

5 Ordinary Differential Equations: Finite Difference Methods for Boundary Problems 5 Ordinary Differential Equations: Finite Difference Metods for Boundary Problems Read sections 10.1, 10.2, 10.4 Review questions 10.1 10.4, 10.8 10.9, 10.13 5.1 Introduction In te previous capters we

More information

Fractional Derivatives as Binomial Limits

Fractional Derivatives as Binomial Limits Fractional Derivatives as Binomial Limits Researc Question: Can te limit form of te iger-order derivative be extended to fractional orders? (atematics) Word Count: 669 words Contents - IRODUCIO... Error!

More information

1. Questions (a) through (e) refer to the graph of the function f given below. (A) 0 (B) 1 (C) 2 (D) 4 (E) does not exist

1. Questions (a) through (e) refer to the graph of the function f given below. (A) 0 (B) 1 (C) 2 (D) 4 (E) does not exist Mat 1120 Calculus Test 2. October 18, 2001 Your name Te multiple coice problems count 4 points eac. In te multiple coice section, circle te correct coice (or coices). You must sow your work on te oter

More information

THE IMPLICIT FUNCTION THEOREM

THE IMPLICIT FUNCTION THEOREM THE IMPLICIT FUNCTION THEOREM ALEXANDRU ALEMAN 1. Motivation and statement We want to understand a general situation wic occurs in almost any area wic uses matematics. Suppose we are given number of equations

More information

1 Lecture 13: The derivative as a function.

1 Lecture 13: The derivative as a function. 1 Lecture 13: Te erivative as a function. 1.1 Outline Definition of te erivative as a function. efinitions of ifferentiability. Power rule, erivative te exponential function Derivative of a sum an a multiple

More information

Practice Problem Solutions: Exam 1

Practice Problem Solutions: Exam 1 Practice Problem Solutions: Exam 1 1. (a) Algebraic Solution: Te largest term in te numerator is 3x 2, wile te largest term in te denominator is 5x 2 3x 2 + 5. Tus lim x 5x 2 2x 3x 2 x 5x 2 = 3 5 Numerical

More information

Math Spring 2013 Solutions to Assignment # 3 Completion Date: Wednesday May 15, (1/z) 2 (1/z 1) 2 = lim

Math Spring 2013 Solutions to Assignment # 3 Completion Date: Wednesday May 15, (1/z) 2 (1/z 1) 2 = lim Mat 311 - Spring 013 Solutions to Assignment # 3 Completion Date: Wednesday May 15, 013 Question 1. [p 56, #10 (a)] 4z Use te teorem of Sec. 17 to sow tat z (z 1) = 4. We ave z 4z (z 1) = z 0 4 (1/z) (1/z

More information

New Distribution Theory for the Estimation of Structural Break Point in Mean

New Distribution Theory for the Estimation of Structural Break Point in Mean New Distribution Teory for te Estimation of Structural Break Point in Mean Liang Jiang Singapore Management University Xiaou Wang Te Cinese University of Hong Kong Jun Yu Singapore Management University

More information

Chapter 2. Limits and Continuity 16( ) 16( 9) = = 001. Section 2.1 Rates of Change and Limits (pp ) Quick Review 2.1

Chapter 2. Limits and Continuity 16( ) 16( 9) = = 001. Section 2.1 Rates of Change and Limits (pp ) Quick Review 2.1 Capter Limits and Continuity Section. Rates of Cange and Limits (pp. 969) Quick Review..... f ( ) ( ) ( ) 0 ( ) f ( ) f ( ) sin π sin π 0 f ( ). < < < 6. < c c < < c 7. < < < < < 8. 9. 0. c < d d < c

More information

MATH1151 Calculus Test S1 v2a

MATH1151 Calculus Test S1 v2a MATH5 Calculus Test 8 S va January 8, 5 Tese solutions were written and typed up by Brendan Trin Please be etical wit tis resource It is for te use of MatSOC members, so do not repost it on oter forums

More information

Subdifferentials of convex functions

Subdifferentials of convex functions Subdifferentials of convex functions Jordan Bell jordan.bell@gmail.com Department of Matematics, University of Toronto April 21, 2014 Wenever we speak about a vector space in tis note we mean a vector

More information

Bootstrap prediction intervals for Markov processes

Bootstrap prediction intervals for Markov processes arxiv: arxiv:0000.0000 Bootstrap prediction intervals for Markov processes Li Pan and Dimitris N. Politis Li Pan Department of Matematics University of California San Diego La Jolla, CA 92093-0112, USA

More information

Copyright c 2008 Kevin Long

Copyright c 2008 Kevin Long Lecture 4 Numerical solution of initial value problems Te metods you ve learned so far ave obtained closed-form solutions to initial value problems. A closedform solution is an explicit algebriac formula

More information