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We formalize as follows:

A pair { X , Y } of random variables considered jointly is treated as the pair of coordinate functions for a two-dimensional random vector W = ( X , Y ) . To each ω Ω , W assigns the pair of real numbers ( t , u ) , where X ( ω ) = t and Y ( ω ) = u . If we represent the pair of values { t , u } as the point ( t , u ) on the plane, then W ( ω ) = ( t , u ) , so that

W = ( X , Y ) : Ω R 2

is a mapping from the basic space Ω to the plane R 2 . Since W is a function, all mapping ideas extend. The inverse mapping W - 1 plays a role analogous to that of the inverse mapping X - 1 for a real random variable. A two-dimensional vector W is a random vector iff W - 1 ( Q ) is an event for each reasonable set (technically, each Borel set) on the plane.

A fundamental result from measure theory ensures

W = ( X , Y ) is a random vector iff each of the coordinate functions X and Y is a random variable.

In the selection example above, we model X (the number of juniors selected)   and Y (the number of seniors selected) as random variables. Hence the vector-valued function

Induced distribution and the joint distribution function

In a manner parallel to that for the single-variable case, we obtain a mapping of probability mass from the basic space to the plane. Since W - 1 ( Q ) is an event for each reasonable set Q on the plane, we may assign to Q the probability mass

P X Y ( Q ) = P [ W - 1 ( Q ) ] = P [ ( X , Y ) - 1 ( Q ) ]

Because of the preservation of set operations by inverse mappings as in the single-variable case, the mass assignment determines P X Y as a probability measure on the subsets of the plane R 2 . The argument parallels that for the single-variable case. The result is the probability distribution induced by W = ( X , Y ) . To determine the probability that the vector-valued function W = ( X , Y ) takes on a (vector) value in region Q , we simply determine how much induced probability mass is in that region.

Induced distribution and probability calculations

To determine P ( 1 X 3 , Y > 0 ) , we determine the region for which the first coordinate value (which we call t ) is between one and three and the second coordinate value (which we call u ) is greater than zero. This corresponds to the set Q of points on the plane with 1 t 3 and u > 0 . Gometrically, this is the strip on the plane bounded by (but not including) the horizontal axis and by thevertical lines t = 1 and t = 3 (included). The problem is to determine how much probability mass lies in that strip. How this is acheived depends upon the nature of thedistribution and how it is described.

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As in the single-variable case, we have a distribution function.

Definition

The joint distribution function F X Y for W = ( X , Y ) is given by

F X Y ( t , u ) = P ( X t , Y u ) ( t , u ) R 2

This means that F X Y ( t , u ) is equal to the probability mass in the region Q t u on the plane such that the first coordinate is less than or equal to t and the second coordinate is less than or equal to u . Formally, we may write

F X Y ( t , u ) = P [ ( X , Y ) Q t u ] , where Q t u = { ( r , s ) : r t , s u }

Now for a given point ( a , b ) , the region Q a b is the set of points ( t , u ) on the plane which are on or to the left of the vertical line through ( t , 0 ) and on or below the horizontal line through ( 0 , u ) (see Figure 1 for specific point t = a , u = b ). We refer to such regions as semiinfinite intervals on the plane.

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Source:  OpenStax, Applied probability. OpenStax CNX. Aug 31, 2009 Download for free at http://cnx.org/content/col10708/1.6
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