lecture 8
play

Lecture 8 AR, MA, and ARMA Models 9/27/2018 1 AR models AR(p) - PowerPoint PPT Presentation

Lecture 8 AR, MA, and ARMA Models 9/27/2018 1 AR models AR(p) models We can generalize from an AR(1) to an AR(p) model by simply adding additional autoregressive terms to the model. () =1 What are the


  1. Lecture 8 AR, MA, and ARMA Models 9/27/2018 1

  2. AR models

  3. AR(p) models We can generalize from an AR(1) to an AR(p) model by simply adding additional autoregressive terms to the model. 𝐵𝑆(𝑞) ∶ 𝑞 ∑ 𝑗=1 What are the properities of 𝐵𝑆(𝑞) , 1. Expected value? 2. Autocovariance / autocorrelation? 3. Stationarity conditions? 2 𝑧 𝑢 = 𝜀 + 𝜚 1 𝑧 𝑢−1 + 𝜚 2 𝑧 𝑢−2 + ⋯ + 𝜚 𝑞 𝑧 𝑢−𝑞 + 𝑥 𝑢 = 𝜀 + 𝑥 𝑢 + 𝜚 𝑗 𝑧 𝑢−𝑗

  4. AR(p) models We can generalize from an AR(1) to an AR(p) model by simply adding additional autoregressive terms to the model. 𝐵𝑆(𝑞) ∶ 𝑞 ∑ 𝑗=1 What are the properities of 𝐵𝑆(𝑞) , 1. Expected value? 2. Autocovariance / autocorrelation? 3. Stationarity conditions? 2 𝑧 𝑢 = 𝜀 + 𝜚 1 𝑧 𝑢−1 + 𝜚 2 𝑧 𝑢−2 + ⋯ + 𝜚 𝑞 𝑧 𝑢−𝑞 + 𝑥 𝑢 = 𝜀 + 𝑥 𝑢 + 𝜚 𝑗 𝑧 𝑢−𝑗

  5. 𝑀 2 𝑧 𝑢 = 𝑀 (𝑀 𝑧 𝑢 ) 𝑀 𝑙 𝑧 𝑢 = 𝑧 𝑢−𝑙 Lag operator The lag operator is convenience notation for writing out AR (and other) time series models. We define the lag operator 𝑀 as follows, this can be generalized where, = 𝑀 𝑧 𝑢−1 = 𝑧 𝑢−2 therefore, 3 𝑀 𝑧 𝑢 = 𝑧 𝑢−1

  6. Lag operator The lag operator is convenience notation for writing out AR (and other) time series models. We define the lag operator 𝑀 as follows, this can be generalized where, = 𝑀 𝑧 𝑢−1 = 𝑧 𝑢−2 therefore, 3 𝑀 𝑧 𝑢 = 𝑧 𝑢−1 𝑀 2 𝑧 𝑢 = 𝑀 (𝑀 𝑧 𝑢 ) 𝑀 𝑙 𝑧 𝑢 = 𝑧 𝑢−𝑙

  7. 𝑧 𝑢 − 𝜚 1 𝑀 𝑧 𝑢 − 𝜚 2 𝑀 2 𝑧 𝑢 − … − 𝜚 𝑞 𝑀 𝑞 𝑧 𝑢 = 𝜀 + 𝑥 𝑢 (1 − 𝜚 1 𝑀 − 𝜚 2 𝑀 2 − … − 𝜚 𝑞 𝑀 𝑞 ) 𝑧 𝑢 = 𝜀 + 𝑥 𝑢 𝜚 𝑞 (𝑀) = (1 − 𝜚 1 𝑀 − 𝜚 2 𝑀 2 − ⋯ − 𝜚 𝑞 𝑀 𝑞 ) Lag polynomial Lets rewrite the 𝐵𝑆(𝑞) model using the lag operator, This polynomial of lags is called the characteristic polynomial of the AR process. 4 𝑧 𝑢 = 𝜀 + 𝜚 1 𝑧 𝑢−1 + 𝜚 2 𝑧 𝑢−2 + … + 𝜚 𝑞 𝑧 𝑢−𝑞 + 𝑥 𝑢 𝑧 𝑢 = 𝜀 + 𝜚 1 𝑀 𝑧 𝑢 + 𝜚 2 𝑀 2 𝑧 𝑢 + … + 𝜚 𝑞 𝑀 𝑞 𝑧 𝑢 + 𝑥 𝑢

  8. 𝜚 𝑞 (𝑀) = (1 − 𝜚 1 𝑀 − 𝜚 2 𝑀 2 − ⋯ − 𝜚 𝑞 𝑀 𝑞 ) Lag polynomial Lets rewrite the 𝐵𝑆(𝑞) model using the lag operator, This polynomial of lags is called the characteristic polynomial of the AR process. 4 𝑧 𝑢 = 𝜀 + 𝜚 1 𝑧 𝑢−1 + 𝜚 2 𝑧 𝑢−2 + … + 𝜚 𝑞 𝑧 𝑢−𝑞 + 𝑥 𝑢 𝑧 𝑢 = 𝜀 + 𝜚 1 𝑀 𝑧 𝑢 + 𝜚 2 𝑀 2 𝑧 𝑢 + … + 𝜚 𝑞 𝑀 𝑞 𝑧 𝑢 + 𝑥 𝑢 𝑧 𝑢 − 𝜚 1 𝑀 𝑧 𝑢 − 𝜚 2 𝑀 2 𝑧 𝑢 − … − 𝜚 𝑞 𝑀 𝑞 𝑧 𝑢 = 𝜀 + 𝑥 𝑢 (1 − 𝜚 1 𝑀 − 𝜚 2 𝑀 2 − … − 𝜚 𝑞 𝑀 𝑞 ) 𝑧 𝑢 = 𝜀 + 𝑥 𝑢

  9. Lag polynomial Lets rewrite the 𝐵𝑆(𝑞) model using the lag operator, This polynomial of lags is called the characteristic polynomial of the AR process. 4 𝑧 𝑢 = 𝜀 + 𝜚 1 𝑧 𝑢−1 + 𝜚 2 𝑧 𝑢−2 + … + 𝜚 𝑞 𝑧 𝑢−𝑞 + 𝑥 𝑢 𝑧 𝑢 = 𝜀 + 𝜚 1 𝑀 𝑧 𝑢 + 𝜚 2 𝑀 2 𝑧 𝑢 + … + 𝜚 𝑞 𝑀 𝑞 𝑧 𝑢 + 𝑥 𝑢 𝑧 𝑢 − 𝜚 1 𝑀 𝑧 𝑢 − 𝜚 2 𝑀 2 𝑧 𝑢 − … − 𝜚 𝑞 𝑀 𝑞 𝑧 𝑢 = 𝜀 + 𝑥 𝑢 (1 − 𝜚 1 𝑀 − 𝜚 2 𝑀 2 − … − 𝜚 𝑞 𝑀 𝑞 ) 𝑧 𝑢 = 𝜀 + 𝑥 𝑢 𝜚 𝑞 (𝑀) = (1 − 𝜚 1 𝑀 − 𝜚 2 𝑀 2 − ⋯ − 𝜚 𝑞 𝑀 𝑞 )

  10. (𝜇 𝑞 − 𝜚 1 𝜇 𝑞−1 − 𝜚 2 𝜇 𝑞−2 − ⋯ − 𝜚 𝑞−1 𝜇 − 𝜚 𝑞 ) Stationarity of 𝐵𝑆(𝑞) processes Claim : An 𝐵𝑆(𝑞) process is stationary if the roots of the characteristic polynomial lay outside the complex unit circle If we define 𝜇 = 1/𝑀 then we can rewrite the characteristic polynomial as then as a corollary of our claim the 𝐵𝑆(𝑞) process is stationary if the roots of this new polynomial are inside the complex unit circle (i.e. |𝜇| < 1 ). 5

  11. Stationarity of 𝐵𝑆(𝑞) processes Claim : An 𝐵𝑆(𝑞) process is stationary if the roots of the characteristic polynomial lay outside the complex unit circle If we define 𝜇 = 1/𝑀 then we can rewrite the characteristic polynomial as then as a corollary of our claim the 𝐵𝑆(𝑞) process is stationary if the roots of this new polynomial are inside the complex unit circle (i.e. |𝜇| < 1 ). 5 (𝜇 𝑞 − 𝜚 1 𝜇 𝑞−1 − 𝜚 2 𝜇 𝑞−2 − ⋯ − 𝜚 𝑞−1 𝜇 − 𝜚 𝑞 )

  12. Example AR(1) 6

  13. Example AR(2) 7

  14. AR(2) Stationarity Conditions From Shumway&Stofer4thed. 8

  15. Proof Sketch ⎢ ⎦ ⎥ ⎥ ⎥ ⎤ 𝑧 𝑢−𝑞 ⋮ 𝑧 𝑢−3 𝑧 𝑢−2 𝑧 𝑢−1 ⎣ ⎢ ⎢ ⎡ ⎡ ⎦ ⎥ ⎥ ⎥ ⎤ 0 1 ⋯ 0 0 0 ⋮ + ⎢ We can rewrite the 𝐵𝑆(𝑞) model into an 𝐵𝑆(1) form using matrix ⎢ ⎦ ⎥ ⎥ ⎥ ⎤ 𝑧 𝑢−𝑞+1 ⋮ 𝑧 𝑢−2 𝑧 𝑢−1 𝑞 ⎣ ⎢ ⎢ ⎡ ⎢ = ⎦ ⎥ ⎥ ⎥ ⎤ 0 ⋮ 0 0 𝑥 𝑢 ⎣ ⎢ ⋮ ⋯ ⋮ ⎥ ⋮ 0 0 𝜀 ⎣ ⎢ ⎢ ⎢ ⎡ = ⎦ ⎥ ⎥ ⎤ ⎤ 𝑧 𝑢−𝑞+1 ⋮ 𝑧 𝑢−2 𝑧 𝑢−1 𝑧 𝑢 ⎣ ⎢ ⎢ ⎢ ⎡ where notation ⋮ 0 ⎥ 1 ⋮ 0 0 ⋯ 0 1 0 0 0 ⋯ 0 ⎥ 0 𝜚 𝑞 𝜚 𝑞−1 ⎥ ⎦ + ⎡ ⎢ ⎢ ⎢ ⎣ 𝜚 1 𝜚 2 𝜚 3 ⋯ 9 𝑧 𝑢 = 𝜀 + 𝜚 1 𝑧 𝑢−1 + 𝜚 2 𝑧 𝑢−2 + ⋯ + 𝜚 𝑞 𝑧 𝑢−𝑞 + 𝑥 𝑢 𝝄 𝑢 = 𝜺 + 𝐆 𝝄 𝑢−1 + 𝐱 𝑢 𝜀 + 𝑥 𝑢 + ∑ 𝑗=1 𝜚 𝑗 𝑧 𝑢−𝑗

  16. Proof sketch (cont.) ∑ and therefore we need lim 𝑗=0 ∑ 𝑢 So just like the original 𝐵𝑆(1) we can expand out the autoregressive 𝑗=0 𝑢 = ( equation 10 𝝄 𝑢 = 𝜺 + 𝐱 𝑢 + 𝐆 𝝄 𝑢−1 = 𝜺 + 𝐱 𝑢 + 𝐆 (𝜺 + 𝐱 𝑢−1 ) + 𝐆 2 (𝜺 + 𝐱 𝑢−2 ) + ⋯ + 𝐆 𝑢−1 (𝜺 + 𝐱 1 ) + 𝐆 𝑢 (𝜺 + 𝐱 0 ) 𝐺 𝑗 )𝜺 + 𝐺 𝑗 𝑥 𝑢−𝑗 𝑢→∞ 𝐺 𝑢 → 0 .

  17. 𝐺 𝑗 )𝜺 + 𝐺 𝑗 𝑥 𝑢−𝑗 𝝄 𝑢 = ( 𝐑𝚳 𝑗 𝐑 −1 𝑥 𝑢−𝑗 Proof sketch (cont.) 𝑗=0 ∑ 𝑢 𝐑𝚳 𝑗 𝐑 −1 )𝜺 + 𝑗=0 ∑ 𝑢 = ( ∑ 𝑗=0 𝑢 𝑗=0 ∑ 𝑢 Using this property we can rewrite our equation from the previous slide as A useful property of the eigen decomposition is that corresponding eigenvalues. columns of 𝐑 are the eigenvectors of 𝐆 and 𝚳 is a diagonal matrix of the 11 We can find the eigen decomposition such that 𝐆 = 𝐑𝚳𝐑 −1 where the 𝐆 𝑗 = 𝐑𝚳 𝑗 𝐑 −1

  18. Proof sketch (cont.) 𝑢 𝑗=0 ∑ 𝑢 𝐑𝚳 𝑗 𝐑 −1 )𝜺 + 𝑗=0 ∑ 𝑢 = ( 𝑗=0 ∑ 𝑗=0 ∑ 𝑢 Using this property we can rewrite our equation from the previous slide as A useful property of the eigen decomposition is that corresponding eigenvalues. columns of 𝐑 are the eigenvectors of 𝐆 and 𝚳 is a diagonal matrix of the 11 We can find the eigen decomposition such that 𝐆 = 𝐑𝚳𝐑 −1 where the 𝐆 𝑗 = 𝐑𝚳 𝑗 𝐑 −1 𝐺 𝑗 )𝜺 + 𝐺 𝑗 𝑥 𝑢−𝑗 𝝄 𝑢 = ( 𝐑𝚳 𝑗 𝐑 −1 𝑥 𝑢−𝑗

  19. Proof sketch (cont.) ⎦ ⋯ 𝜇 𝑗 𝑞 ⎤ ⎥ ⎥ Therefore, 0 lim when lim which requires that |𝜇 𝑗 | < 1 for all 𝑗 0 ⋮ ⋱ 0 ⎡ ⎢ ⎢ ⎣ 𝜇 𝑗 1 ⋯ 0 0 𝜇 𝑗 2 ⋯ 0 ⋮ ⋮ 12 𝚳 𝑗 = 𝑢→∞ 𝐺 𝑢 → 0 𝑢→∞ Λ 𝑢 → 0

  20. which if we multiply by 1/𝜇 𝑞 where 𝑀 = 1/𝜇 gives 1 − 𝜚 1 𝑀 − 𝜚 2 𝑀 2 − ⋯ − 𝜚 𝑞 1 𝑀 𝑞−1 − 𝜚 𝑞 𝑀 𝑞 = 0 Proof sketch (cont.) Eigenvalues are defined such that for 𝝁 , det (𝐆 − 𝝁 𝐉) = 0 based on our definition of 𝐆 our eigenvalues will therefore be the roots of 13 𝜇 𝑞 − 𝜚 1 𝜇 𝑞−1 − 𝜚 2 𝜇 𝑞−2 − ⋯ − 𝜚 𝑞 1 𝜇 1 − 𝜚 𝑞 = 0

  21. Proof sketch (cont.) Eigenvalues are defined such that for 𝝁 , det (𝐆 − 𝝁 𝐉) = 0 based on our definition of 𝐆 our eigenvalues will therefore be the roots of 13 𝜇 𝑞 − 𝜚 1 𝜇 𝑞−1 − 𝜚 2 𝜇 𝑞−2 − ⋯ − 𝜚 𝑞 1 𝜇 1 − 𝜚 𝑞 = 0 which if we multiply by 1/𝜇 𝑞 where 𝑀 = 1/𝜇 gives 1 − 𝜚 1 𝑀 − 𝜚 2 𝑀 2 − ⋯ − 𝜚 𝑞 1 𝑀 𝑞−1 − 𝜚 𝑞 𝑀 𝑞 = 0

  22. Properties of 𝐵𝑆(2) 𝑊 𝑏𝑠(𝑥 𝑢 ) = 𝜏 2 𝑥 14 For a stationary 𝐵𝑆(2) process where 𝑥 𝑢 has 𝐹(𝑥 𝑢 ) = 0 and

  23. Properties of 𝐵𝑆(𝑞) 𝑊 𝑏𝑠(𝑥 𝑢 ) = 𝜏 2 𝑥 𝐹(𝑍 𝑢 ) = 𝜀 𝑊 𝑏𝑠(𝑧 𝑢 ) = 𝛿(0) = 𝜚 1 𝛿(1) + 𝜚 2 𝛿(2) + … + 𝜚 𝑞 𝛿(𝑞) + 𝜏 2 𝑥 𝛿(ℎ) = 𝜚 1 𝛿(ℎ − 1) + 𝜚 2 𝛿(ℎ − 2) + … + 𝜚 𝑞 𝛿(ℎ − 𝑞) 15 For a stationary 𝐵𝑆(𝑞) process where 𝑥 𝑢 has 𝐹(𝑥 𝑢 ) = 0 and 1 − 𝜚 1 − 𝜚 2 − ⋯ − 𝜚 𝑞 𝜍(ℎ) = 𝜚 1 𝜍(ℎ − 1) + 𝜚 2 𝜍(ℎ − 2) + … + 𝜚 𝑞 𝜍(ℎ − 𝑞)

  24. Moving Average (MA) Processes

Download Presentation
Download Policy: The content available on the website is offered to you 'AS IS' for your personal information and use only. It cannot be commercialized, licensed, or distributed on other websites without prior consent from the author. To download a presentation, simply click this link. If you encounter any difficulties during the download process, it's possible that the publisher has removed the file from their server.

Recommend


More recommend