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Slides Chapter 1. Measure Theory and Probability

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<strong>1.</strong>8. RANDOM VARIABLES<br />

We will also use the notation p(X = x) = p X (x).<br />

The probability function induced by a discrete r.v. X, P X , is<br />

completely determined by the distribution function F X or by the<br />

mass function p X . Thus, in the following, when we speak about<br />

the “distribution” of a discrete r.v. X, we could be referring either<br />

to the probability function induced by X, P X , the distribution<br />

function F X , or the mass function p X .<br />

Example <strong>1.</strong>21 The r.v. X 1 : “Weight of a r<strong>and</strong>omly selected<br />

Spanish woman aged within 20 <strong>and</strong> 40”, defined in Example <strong>1.</strong>17<br />

(c), is continuous.<br />

Definition <strong>1.</strong>46 The probability density function (p.d.f.) of X<br />

is a function f X : IR → IR defined as<br />

{ 0 if x ∈ S;<br />

f X (x) =<br />

F X ′ (x) if x /∈ S.<br />

It is named probability density function of x because it gives the<br />

density of probability of an infinitesimal interval centered in x.<br />

The same as in the discrete case, the probabilities of a continuous<br />

r.v. X are determined either by P X , F X or the p.d.f. f X .<br />

Again, the “distribution” of a r.v., could be referring to any of<br />

these functions.<br />

R<strong>and</strong>omvariables, asmeasurable functions, inheritallthepropertiesofmeasurablefunctions.<br />

Furthermore, wewillbeabletocalculate<br />

Lebesgue integrals of measurable functions of r.v.’s using as<br />

measure their induced probability functions. This will be possible<br />

due to the following theorem.<br />

Theorem <strong>1.</strong>16 (Theorem of change of integrationspace)<br />

Let X be a r.v. from (Ω,A,P) in (IR,B) an g another r.v. from<br />

ISABEL MOLINA 41

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