physicsoxford said:
The only thing that we did in class that could relate to this would be the binomial tree model. So after looking up Markov Chain and reading a bit it makes more since but I am still struggling. Here is an attempt:
So the underlining reasoning is that S0P = S1 Where P is the transition probability matrix and S0 is the initial state distribution matrix and S1 = a later state distribution matrix.
P = Matrix:
p4, 1-p4, 0, 0
0, 0, p3, 1-p3
p2, 1-p2, 0, 0
0, 0, p1, 1-p1
As you showed in your response.
And S1 = matrix [∏WW,∏WL,∏LW, ∏LL]
and S0 = matrix [.25, .25, .25, .25] ?
Plug this in and solve for ∏WW, ...
Is this even close?
The steady-state probabilities π
i depend on the transition matrix P = (p
ij). For an n-state chain with transition matrix P they are solutions of a set of linear equations:
\pi_j = \sum_{i} \pi_i p_{ij}, j=1,2, \ldots, n, \;\text{ and } \sum_{j} \pi_j = 1.
The first n equations above can be summarized as \pi = \pi P, where \pi = (\pi_1, \pi_2, \ldots, \pi_n) is a row vector. Because each row of P sums to 1, one of the equations \pi_j = \sum_{i} \pi_i p_{ij} is redundant (that is, if n-1 of them hold, the nth one also holds), so we proceed by omitting anyone of those equations and replacing it by the normalization condition sum = 1. For the type of chain you have here (having a single "recurrent class") the system has a provably unique solution. Never mind for now if you don't know exactly what I am referring to; for now, it is enough to solve the equations to see what happens.
Let's do a little example, with three states:
P = \left[ \matrix{1/2&0&1/2\\0&1/4&3/4\\1/4&1/2&1/4} \right].
The steady-state equations are:
<br />
\begin{array}{rcl}<br />
\pi_1&=& \frac{1}{2} \pi_1 + \frac{1}{4} \pi_3 \\<br />
\pi_2&=& \frac{1}{4} \pi_2 + \frac{1}{2} \pi_3 \\<br />
\pi_3&=& \frac{1}{2} \pi_1 + \frac{3}{4} \pi_2 + \frac{1}{4} \pi_3<br />
\end{array}<br />
and \pi_1 + \pi_2 + \pi_3 = 1.
We leave out one of the first three equations (say the third one---but anyone of them would do) and replace it by the sum condition. That gives the linear system
<br />
\begin{array}{ccl}<br />
\pi_1&=& \frac{1}{2} \pi_1 + \frac{1}{4} \pi_3 \\<br />
\pi_2&=& \frac{1}{4} \pi_2 + \frac{1}{2} \pi_3 \\<br />
1 &=& \pi_1 + \pi_2 + \pi_3<br />
\end{array}<br />
The solution is \pi_1 = 3/13, \pi_2 = 4/13, \pi_3 = 6/13.
The theory behind all this can be found in textbooks and web pages.
RGV