close
Warning:
Can't synchronize with repository "(default)" (/var/svn/tolp does not appear to be a Subversion repository.). Look in the Trac log for more information.
- Timestamp:
-
Mar 25, 2009, 7:07:58 PM (16 years ago)
- Author:
-
Víctor de Buen Remiro
- Comment:
-
Legend:
- Unmodified
- Added
- Removed
- Modified
-
v10
|
v11
|
|
25 | 25 | 1. The corresponding ARIMA noise is simply [[BR]][[LatexEquation(z' = Y' - X' \beta' $$)]] |
26 | 26 | 1. By means of Almagro method it's posible to calculate residuals [[LatexEquation(e' $$)]] and initial values [[LatexEquation(u' $$)]] that solve difference equation [[BR]] [[LatexEquation(e'_t = \frac{\phi'\left(B\right)}{\theta'\left(B\right)} z'_t $$)]] |
27 | | 1. Then we can purpose residuals and initial values for current system as [[BR]][[LatexEquation(e = \frac{\sigma}{\sigma'}e' $$)]] [[BR]] [[LatexEquation(u = \frac{\sigma}{\sigma'}u' $$)]] |
28 | | 1. Let be the standarized multinormal residuals [[BR]] [[LatexEquation( \epsilon=\frac{1}{\sigma}e $$)]] [[BR]] |
29 | | 1. Since [[LatexEquation(\beta $$)]] are determined by [[LatexEquation(\epsilon $$)]] by means of a full range linear equation, their densities have constant ratio, and logarithm of density of candidate vector can be calculated directly as [[BR]] [[LatexEquation(cte -\frac{T}{2}\log\left(2\pi\right)-\frac{1}{2}\sum_{t=1}^{T}\epsilon_{t}^{2}$$)]] |
30 | | 1. ARIMA noise for current system becomes simply [[BR]][[LatexEquation(z_t = \frac{\theta\left(B\right)}{\phi\left(B\right)} e_t $$)]] |
31 | | 1. Then, we can solve sparse linear system [[BR]][[LatexEquation(X \beta = Y-z $$)]] |
| 27 | 1. Let be the standarized multinormal residuals [[BR]] [[LatexEquation( \epsilon' =\frac{1}{\sigma'}e' $$)]] [[BR]] |
| 28 | 1. Since [[LatexEquation(\beta' $$)]] are determined by [[LatexEquation(\epsilon' $$)]] by means of a full range linear equation, their densities have constant ratio, and logarithm of density of candidate vector can be calculated directly as [[BR]] [[LatexEquation(cte -\frac{T}{2}\log\left(2\pi\right)-\frac{1}{2}\sum_{t=1}^{T}\epsilon'_{t}^{2}$$)]] |
| 29 | 1. Then we can propose residuals and initial values for current system as [[BR]][[LatexEquation(e^{*} = \frac{\sigma}{\sigma'}e' $$)]] [[BR]] [[LatexEquation(u = \frac{\sigma}{\sigma'}u' $$)]] |
| 30 | 1. ARIMA noise for current system becomes simply [[BR]][[LatexEquation(z^{*}_t = \frac{\theta\left(B\right)}{\phi\left(B\right)} e^{*}_t $$)]] |
| 31 | 1. In order to get the refined candidate, we will take minimum residuals solution of sparse linear system [[BR]][[LatexEquation(X \beta = Y-z^{*} $$)]] |
| 32 | 1. In order to calculate its exact density, it will be obtained the ARIMA noise [[BR]][[LatexEquation(z = Y - X \beta $$)]] to get standarized residuals from ARIMA equations. |
32 | 33 | 1. If resulting vector doesn't match constraining inequations [[BR]] [[LatexEquation(A \beta <= a $$)]][[BR]] density will be toggled to [[LatexEquation(-\infty $$)]] in order to force rejection. |
33 | 34 | |