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Unformatted text preview: May 2, 2007 HW6 Problem Solutions #8.1.2. Fix t, and calculate the joint density of ( B, F ) from first principles at ( b, a ) with 0 < b < t, a > 0, by: f B,F ( b, a ) h 2 P ( B ( b, b + h ) , F ( a, a + h )) P ( N ( t b ) N ( t b h ) = 1 , N ( t + a ) = N ( t b ) , N ( a + h ) N ( a ) = 1) = e 2 h ( h ) 2 e ( a + b ) so that the joint density is given by f B,F ( b, a ) = 2 e ( a + b ) I [0 <b<t, a> 0] Note that the probability mass does not integrate to 1, because with probability e t = P ( N ( t ) = 0) the backward recurrence time has the value t . Thus ( B, F ) is a random variable of mixed discretecontinuous type, but B, F are independent and in the limit of large t are both Expon( ) distributed. Also: lim t E ( B ( t ) + F ( t )) = 2 / , while E ( T n T n 1 ) = E ( T 1 ) = 1 / . This is paradoxical because it says that the interevent interval surrounding each time t is not typical in the sense of average length. But that is not really so surprising since the fact of containing t makes it more likely to be a large interval than a small one. #8.2.4. In this flipflop chain, the rate q i of leaving each state i = 0 , 1 is the same value , so the transition times can be viewed as the jump times of a Poisson process. We showed in class that the intensity matrix for a Poisson process has on the main diagonal and on the abovediagonal and all other entries 0. Since the flipflop chain moves at each jump to the opposite0....
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This note was uploaded on 09/09/2009 for the course STAT 650 taught by Professor Slud during the Spring '09 term at Maryland.
 Spring '09
 SLUD

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