Add in a new major section to the derivation document where we will derive a continuous X discrete states.
[x] First, put in a "notation" section.
Let the index of the discrete state be n = 1, ... N and the discrete operator for the stochastic process when in those states be L^n.
Let the intensity matrix of the stochastic process for the markov chain of the discrete state be Q.
We will assume that the discrete and continuous stochastic processes are independent, which will simplify the setup.
Add in an example, where N= 2 and there is a diffusion process with different drifts depending on the discrete state. That is, the continous processes would evolve as
d X_{1t} = mu_1 dt + sigma d W_t
d X_{1t} = mu_2 dt + sigma d W_t
subject to reflecting boundaries at x_min and x_max.
and the intensity matrix of the markov chain is
Q = [-q_1 q_1
q_2 -q_2]
With this, the payoffs were just the pi(x) then the stationary bellman equation discounted at rate r would be the system
[x] After you write down the example, write the more generic form of this given extension operators L_1, ... L_N for the continuous dimensions and the Q intensity matrix.
The discretization of the joint process with M points on the interior is then a matrix of size an (M N) by ((M+2) N)
What does this look like? Take the n'th row and it looks something like this (I think)
And this row is of size M by (M+2)*N
Where the banded_I is some sort of banded matrix with a band of ones at the diagonal or slightly off of it. (Resolved by 8d540dc)
Add in a new major section to the derivation document where we will derive a continuous X discrete states.
n = 1, ... N
and the discrete operator for the stochastic process when in those states beL^n
.Q
.N= 2
and there is a diffusion process with different drifts depending on the discrete state. That is, the continous processes would evolve assubject to reflecting boundaries at x_min and x_max.
and the intensity matrix of the markov chain is
With this, the payoffs were just the
pi(x)
then the stationary bellman equation discounted at rater
would be the systemPoint out that if we stack the
v
in the discrete grid x_0 to x_M asThen we can discretize this as an extension operator
with 4 total equations in the boundary conditions.
(Resolved by ba99afb)
L_1, ... L_N
for the continuous dimensions and theQ
intensity matrix. The discretization of the joint process with M points on the interior is then a matrix of size an(M N) by ((M+2) N)
What does this look like? Take the n'th row and it looks something like this (I think)
And this row is of size M by (M+2)*N Where the banded_I is some sort of banded matrix with a band of ones at the diagonal or slightly off of it. (Resolved by 8d540dc)