A partition of a sample space is a finite or countable family of nonempty events such thatThus exactly one event in the family occurs in each outcome. To use ordinary event-conditioned conditional expectations, one usually assumes ; any zero-probability blocks can instead be omitted from the expectation formula.
For an integrable random variable and a partition of a sample space , the law of total expectation statesIt follows by writing and using . Integrability justifies the countable sum. The same equality is valid with nonnegative, possibly infinite expectations when .
Let be the absorption time. Its expectation is finite: from every interior state, a string of at most successive left moves reaches , and the probability of such a string is at least . Hence the Markov property gives , a geometric tail bound, and .
For , one step is always spent before absorption or the remaining walk. Apply first-step analysis and the law of total expectation to the three possible first moves. The conditional expectations of the remaining absorption time are , respectively; independence of future moves gives the same law as a fresh random walk from the new position. Thuswhich rearranges toThe term also appears when the walk stays at , because staying still consumes a step.
The absorbing states give . Multiplying the difference equation in (i) by givesThe second finite difference of is , so a particular solution is ; the homogeneous solutions are . Imposing the two boundary conditions gives . ThereforeUniqueness follows because the difference of any two solutions has zero second finite difference, hence is affine function, and vanishes at both endpoints. This is the mean absorption time of a lazy symmetric random walk with holding probability .
For each random variable, the probability mass function givesLet . By linearity of expectation and variance additivity for independent random variables,The independence is needed for the variance calculation, but not for the mean.
Each has the same probability distribution as . By independence, the entire vector and its negative have the same joint law, so has a symmetric distribution about zero. The two disjoint tail events consequently have equal probabilities:Apply Chebyshev's inequality with the mean and variance from (i):Using only containment in the two-sided event would give ; the symmetry supplies the necessary extra factor .
Articles by others on the same topic
There are currently no matching articles.