The cumulative distribution function isFor an absolutely continuous probability distribution, the probability density function is a nonnegative integrable function withThus interval probabilities are integrals of , and almost everywhere, in particular at continuity points of .
The word “continuous” in the source is understood in this density sense. A merely continuous cumulative distribution function need not possess a probability density function; it can instead describe a singular continuous distribution.
For an absolutely continuous probability distribution, its expectation isThis is finite when . More generally it is an extended real value if only one of the positive and negative parts diverges; it is undefined if both diverge. For nonnegative it always exists in .
Let for . Since on the negative half-line, almost surely. We have almost everywhere. On a finite interval, integration by parts givesThe lower endpoint contributes zero. The stated hypothesis gives as . Taking the increasing limits of the two nonnegative integrals proves the tail-integral identityThe equality allows the value ; the boundary hypothesis alone does not force a finite expectation. In fact the formula for nonnegative also follows directly from Tonelli theorem, without that additional boundary hypothesis, by integrating against the probability density function.
Translate the inequality inside the cumulative distribution function:Differentiating with the chain rule gives the probability density functionalmost everywhere. Translation shifts the probability distribution without changing its shape or its total probability.
Reversing sign reverses the inequality. Since has a probability density function, it has no point masses, soDifferentiating the cumulative distribution function givesalmost everywhere: the minus sign outside cancels the minus sign from the chain rule. If point masses were allowed, the cumulative distribution function would instead require the left limit .
Since a square is nonnegative, for . For , the event is . As has no point masses,Differentiating for gives the contributions of the two inverse branches:The value assigned to the probability density function at is arbitrary. It can be unbounded near , but there is no atom there because . Both positive and negative preimages must be included; keeping just one would generally lose probability.
For any real , put . Since is integer-valued,Continuity of the cumulative distribution function of therefore givesThe strict inequality matters before using the absence of point masses. The resulting probability distribution is discrete, with probability mass functionThus has no ordinary probability density function with respect to length on the real line. Its cumulative distribution function is a step function; its derivative is zero almost everywhere and does not recover its probabilities. The floor function has converted a density into masses on the integers.
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