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Copy file name to clipboardExpand all lines: lectures/ar1_processes.md
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@@ -356,9 +356,7 @@ In this equation, we can use observed data to evaluate the left hand side of {eq
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And we can use a theoretical AR(1) model to calculate the right hand side.
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If $\frac{1}{m} \sum_{t = 1}^m X_t$ is not close to $\psi^*(x)$, even for many
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observations, then our theory seems to be incorrect and we will need to revise
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it.
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If $\frac{1}{m} \sum_{t = 1}^m h(X_t)$ is not close to $\int h(x)\psi^*(x) dx$, even for many observations, then our theory seems to be incorrect and we will need to revise it.
All four values satisfy the stability condition $|\rho| < 1$ for the default $\alpha = 5$.
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All four values satisfy the stability condition $|\rho| < 1$ for the default $\alpha = 5$ and have $\rho > 0$.
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The case $\lambda = 0.86$ is closest to the stability boundary and therefore displays the largest oscillatory response.
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The case $\lambda = 0.86$ has the largest initial overshoot among these four values and then converges the fastest.
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As $\lambda$ moves closer to one, expectations become more inertial and the post-stabilization response decays more slowly but starts from a smaller jump.
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As $\lambda$ moves closer to one, expectations become more inertial, so the post-stabilization response decays more slowly but starts from a smaller jump.
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For $\alpha = 5$, an oscillatory stable response would require $0.8 < \lambda < 5/6$.
Copy file name to clipboardExpand all lines: lectures/cagan_ree.md
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The next code generates a multi-panel graph that includes outcomes of both experiments 1 and 2.
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That allows us to assess how important it is to understand whether the sudden permanent drop in $\mu_t$ at $t=T_1$ is fully unanticipated, as in experiment 1, or completely
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That allows us to assess how important it is to understand whether the sudden permanent drop in $\mu_t$ at $t=T_1$ is fully anticipated, as in experiment 1, or completely
Copy file name to clipboardExpand all lines: lectures/eigen_II.md
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@@ -117,7 +117,7 @@ Left eigenvectors will play important roles in what follows, including that of s
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A vector $w$ is called a left eigenvector of $A$ if $w$ is a right eigenvector of $A^\top$.
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In other words, if $w$ is a left eigenvector of matrix $A$, then $A^\top w = \lambda w$, where $\lambda$ is the eigenvalue associated with the left eigenvector $v$.
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In other words, if $w$ is a left eigenvector of matrix $A$, then $A^\top w = \lambda w$, where $\lambda$ is the eigenvalue associated with the left eigenvector $w$.
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This hints at how to compute left eigenvectors
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Now let's step back to the primitive matrices part of the Perron-Frobenius theorem
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```{prf:Theorem}Continous of Perron-Frobenius Theorem
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```{prf:Theorem}Continuity of Perron-Frobenius Theorem
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