A partition of a sample space is a finite or countable family of nonempty events such that
Thus 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 states
It 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. Thus
which rearranges to
The 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 gives
The second finite difference of is , so a particular solution is ; the homogeneous solutions are . Imposing the two boundary conditions gives . Therefore
Uniqueness 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 gives
Let . 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 .

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