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@ -65,8 +65,6 @@ envelope conditions can also be found:
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\begin{align}
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\begin{align}
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\nabla_{\vec s_t, \vec x^{\sim i}_t, D_t} V^i(\vec s_t, \vec x^{\sim i}_t, D_t)
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\nabla_{\vec s_t, \vec x^{\sim i}_t, D_t} V^i(\vec s_t, \vec x^{\sim i}_t, D_t)
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=& \nabla_{\vec s_t, \vec x^{\sim i}_t, D_t} u^i(\vec s_t, D_t) \notag \\
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=& \nabla_{\vec s_t, \vec x^{\sim i}_t, D_t} u^i(\vec s_t, D_t) \notag \\
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&- \der{}{x}{}F(x^i(\vec s_t, \vec x^{\sim i}_t, D_t)) \cdot
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\nabla_{\vec s_t, \vec x^{\sim i}_t, D_t} x^i(\vec s_t, \vec x^{\sim i}_t, D_t) \notag\\
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&+ \beta \left[
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&+ \beta \left[
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\nabla_{\vec s_{t+1}, \vec x^{\sim i}_{t+1}, D_{t+1} }
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\nabla_{\vec s_{t+1}, \vec x^{\sim i}_{t+1}, D_{t+1} }
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V^i(\vec s_{t+1}, \vec x^{\sim i}_{t+1}, D_{t+1})
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V^i(\vec s_{t+1}, \vec x^{\sim i}_{t+1}, D_{t+1})
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@ -75,25 +73,26 @@ envelope conditions can also be found:
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[ \vec s_{t+1}, \vec x^{\sim i}_{t+1}, D_{t+1} ]
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[ \vec s_{t+1}, \vec x^{\sim i}_{t+1}, D_{t+1} ]
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\right] \label{EQ:EnvelopeConditions}
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\right] \label{EQ:EnvelopeConditions}
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\\
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\\
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\nabla \vec V^i_t =& \vec u^i - \vec f + \beta A \cdot \nabla \vec V^i_{t+1}
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\nabla \vec V^i_t =& \vec u^i
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+ \beta A \cdot \nabla \vec V^i_{t+1}
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\label{EQ:SimplifiedEnvelopeConditions}
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\label{EQ:SimplifiedEnvelopeConditions}
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\end{align}
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\end{align}
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When interpreting this, note that
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When interpreting this, note that
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$$
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$$
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\nabla \vec V^i_{t+1} = \nabla_{\vec s_{t+1}, \vec x^{\sim i}_{t+1}, D_{t+1} }
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\nabla \vec V^i_{t+1} = \nabla_{[\vec s_{t+1}~ \vec x^{\sim i}_{t+1}~ D_{t+1}] }
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V^i(\vec s_{t+1}, \vec x^{\sim i}_{t+1}, D_{t+1})
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V^i(\vec s_{t+1}, \vec x^{\sim i}_{t+1}, D_{t+1})
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$$
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$$
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is a $2N \times 1$ vector of first derivatives but
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is a $2N \times 1$ vector of first derivatives but
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$$
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$$
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A = \nabla_{\vec s_t, \vec x^{\sim i}_t, D_t}
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A = \nabla_{\vec s_t, \vec x^{\sim i}_t, D_t}
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[ \vec s_{t+1}, \vec x^{\sim i}_{t+1}, D_{t+1} ]
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[ \vec s_{t+1}~ \vec x^{\sim i}_{t+1}~ D_{t+1} ]
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$$
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$$
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is a $2N \times 2N$ matrix of first derivatives.
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is a $2N \times 2N$ matrix of first derivatives.
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By solving for $\vec V^i_{t+1}$ as a function of $\vec V^i_{t}$ we get the
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By solving for $\vec V^i_{t+1}$ as a function of $\vec V^i_{t}$ we get the
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intertemporal condition:
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intertemporal condition:
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\begin{align}
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\begin{align}
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\frac{1}{\beta} A^{-1} \left(\nabla \vec V^i_t - \vec u^i +\vec f \right)
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\frac{1}{\beta} A^{-1} \left(\nabla \vec V^i_t - \vec u^i \right)
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= \nabla \vec V^i_{t+1}
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= \nabla \vec V^i_{t+1}
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\end{align}
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\end{align}
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Thus one crucial condition for the existence of a solution is that $A^{-1}$ exists for
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Thus one crucial condition for the existence of a solution is that $A^{-1}$ exists for
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@ -116,6 +115,5 @@ By substituting this defined value of $\nabla V^i_t$ into
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\cref{EQ:SimplifiedOptimalityCondition}
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\cref{EQ:SimplifiedOptimalityCondition}
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one final time, we get a function that fully determines the policy function.
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one final time, we get a function that fully determines the policy function.
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\cref{EQ:SimplifiedOptimalityConditions,EQ:SimplifiedEnvelopeConditions}
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\end{document}
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\end{document}
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