For a nonnegative random variable and , Markov inequality statesFor a random variable of finite mean and variance , Chebyshev inequality states that for every ,To prove it, apply Markov inequality to the nonnegative variable at threshold :
For an indicator , . Covariances vanish for independent pairs. For dependent distinct pairs,Expanding the variance, with ordered pairs as in the definition of , givesFor sufficiently large , . By Chebyshev inequality,This is the second moment method: a vanishing relative variance makes a zero count unlikely.
A threshold function has the following meaning: if , the probability of a tends to zero; if , that probability tends to one. Behavior at a fixed constant multiple is not specified by this definition.
Let count the five-vertex subsets spanning in the Erdős-Rényi model . ThenIf , then , so Markov inequality gives .
Now let with . Then . Distinct copies have dependent indicators only if their vertex sets share at least two vertices. If they share vertices, they share edges; there are ordered such pairs, and their joint probability is . ConsequentlyPart (b) gives . ThereforeThis is the five-vertex instance of the fixed-size clique appearance threshold.
Start the Galton-Watson process with one ancestor, , and let every individual independently have a number of offspring distributed as . With independent copies ,where an empty sum is zero. Extinction is the event that some generation is empty; zero is then absorbing. Write for its probability and for the survival probability.
Set , with . Conditional on the ancestor's number of children, extinction by generation requires independent extinction by generation in every child subtree. ThusThe events increase, so . The probability generating function is continuous on , by domination of by , giving . If is any fixed point, then and monotonicity of inductively gives . Taking limits proves the Galton-Watson extinction fixed point characterization:In particular it is the smallest nonnegative fixed point wherever the generating series is defined, since it already lies in .
Let , allowing . The probability generating function is increasing and convex, with . If , its tangent inequality gives for , so . If and , there is positive mass at both zero and some integer at least two; strict convexity gives for , again . The exceptional case almost surely has one individual forever, so despite .
If , the left derivative at gives for sufficiently close to . Since , continuity supplies a fixed point below , possibly . Thus survival has positive probability precisely when , apart from deterministic one-child reproduction.
For the random bipartite graph, early exploration of a component alternates between the two vertex classes. Before many vertices are exposed, each discovered vertex has approximately new neighbors in the other class, since tends to that distribution. The two-type mean offspring matrix iswith spectral radius ; equivalently, the mean growth over two generations is . The branching-process comparison therefore predicts a giant component exactly whenFor , the local process dies out almost surely, so no linear-sized component is expected; is the critical case, not a positive-survival exception. For , the symmetric survival probability is , where , predicting approximately vertices in the giant. This last passage from local survival to a unique giant is the usual random-graph exploration argument; the branching-process reasoning here supplies the requested threshold explanation rather than a proof of that global theorem.
First take . For , independence of the Bernoulli trials givesFor and , Markov inequality yieldsDifferentiate the logarithm of the right-hand side to minimize it. The stationary point satisfieswhich is at least when . Substitution givesWhen , use the limit , giving the trivial bound .
For , take . On we have , so the same Markov inequality gives the same expression. Its minimizing is now nonpositive, yielding the stated lower-tail bound. No rounding of is needed, because the exponential event inclusion holds for real thresholds. The cases and are deterministic and follow directly, or by the corresponding limits.
Write the bound in part (a) as , where the Bernoulli Kullback-Leibler divergence with natural logarithms isFor fixed , , its first derivative with respect to vanishes at , andIntegrating this lower bound twice, on either side of , gives the Bernoulli relative entropy lower bound . Apply the two tails from part (a) at and and use the union bound:A tail with threshold outside is empty; thresholds at the endpoints follow by continuity of the bound. For the right-hand side is , so the assertion is immediate. This is the binomial form of Hoeffding inequality.
The sum of the first variables has distribution . For any fixed half-circle interval , putThe terms defining are independent Bernoulli variables of parameter , so and . Part (b), with , givesThere are at most cyclic intervals of length ; this also covers the non-wrapping interpretation in the question. They need not be independent, since the union bound always applies. HenceWith and natural logarithms, this becomes , which tends to zero for every . In particular,The argument proves uniform half-circle balance for independent Bernoulli variables. It improves on separately bounding the two half sums by recognizing the difference as one centered binomial variable.
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