1. Define the problem and the Markov Chain:
- The particle performs a random walk on the integer points of the semi-axis x≥0.
- The transition probabilities are:
- Moves to the right (from x to x+1) with probability a.
- Moves to the left (from x to x−1) with probability b, but if x=0, it stands still.
- Stands still with the remaining probability 1−a−b.
2. Steady-state probability distribution:
- Let π(k) be the steady-state probability of being at position k.
- For k≥1, the balance equations are:
π(k)a=bπ(k+1)
- For k=0, the balance equation is:
π(0)=π(0)(1−a)+bπ(1)
- From the first balance equation, we can express π(k+1) in terms of π(k):
π(k+1)=baπ(k)
- By iterating this relationship, we get:
π(k)=(ba)kπ(0)
- To find π(0), we use the normalization condition:
k=0∑∞π(k)=1
π(0)k=0∑∞(ba)k=1
- The series ∑k=0∞(ba)k converges if ba<1, which implies a<b:
k=0∑∞(ba)k=1−ba1=b−ab
- Therefore:
π(0)⋅b−ab=1⟹π(0)=bb−a
- The steady-state distribution is:
π(k)=(ba)kbb−a
3. **Expectation of x:**
- The expectation E[x] is given by:
E[x]=k=0∑∞kπ(k)
E[x]=k=0∑∞k(ba)kbb−a
- Using the formula for the sum of an infinite series:
k=0∑∞krk=(1−r)2rfor∣r∣<1
- Here, r=ba:
E[x]=bb−a⋅(1−ba)2ba=bb−a⋅(bb−a)2ba=b−aa
4. **Expectation of x2:**
- The expectation E[x2] is given by:
E[x2]=k=0∑∞k2π(k)
E[x2]=k=0∑∞k2(ba)kbb−a
- Using the formula for the sum of an infinite series:
k=0∑∞k2rk=(1−r)3r(1+r)for∣r∣<1
- Here, r=ba:
E[x2]=bb−a⋅(1−ba)3ba(1+ba)=bb−a⋅(bb−a)3ba(bb+a)
E[x2]=(b−a)2a(b+a)
The final answer is: