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Suppose \(X\) is a Poisson random variable with mean \(\lambda .\) The parameter \(\lambda\) is itself a random variable whose distribution is exponential with mean \(1 .\) Show that \(P[X=\) \(n\\}=\left(\frac{1}{2}\right)^{n+1}\)

Short Answer

Expert verified
In summary, given that \(X\) is a Poisson random variable with mean \(\lambda\), and \(\lambda\) is an exponential random variable with mean 1, the probability \(P[X=n]\) can be computed as: \[P[X=n] = \left(\frac{1}{2}\right)^{n+1}\]

Step by step solution

01

Write down the PMF of Poisson and PDF of exponential distribution

Recall the PMF of a Poisson distribution with mean \(\lambda\) is given by: \[P(X=n|\lambda) = \frac{e^{-\lambda}\lambda^n}{n!}\] And the PDF of an exponential distribution with mean 1 is given by: \[f(\lambda) = e^{-\lambda}\]
02

Use the law of total probability to express \(P[X=n]\)

We want to find the probability \(P[X=n]\). Since \(X\) depends on \(\lambda\), which is itself a random variable, we should use the law of total probability, integrating over all possible values of \(\lambda\): \[P[X=n] = \int_0^{\infty} P(X=n|\lambda) f(\lambda) d\lambda\] Now, substitute the PMF of Poisson and PDF of exponential distributions into the expression: \[P[X=n] = \int_0^{\infty} \frac{e^{-\lambda}\lambda^n}{n!} \cdot e^{-\lambda} d\lambda\]
03

Calculate the integral and simplify the expression

Next, we need to calculate the integral. To do this, first simplify the expression inside the integral: \[P[X=n] = \int_0^{\infty} \frac{e^{-2\lambda}\lambda^n}{n!} d\lambda\] Now, use integration by substitution. Let \(u = 2\lambda\), so \(du = 2d\lambda\) and \(d\lambda = \frac{1}{2} du\): \[P[X=n] = \int_0^{\infty} \frac{e^{-u} (u/2)^n}{n!} \cdot \frac{1}{2} du\] \[P[X=n] = \frac{1}{2^{n+1}n!} \int_0^{\infty} e^{-u} u^n du\] We recognize the integral as the Gamma function, which is defined as: \[\Gamma(n+1) = \int_0^{\infty} e^{-u} u^n du\] Since \(\Gamma(n+1) = n!\) for any integer \(n\), we can replace the integral by the factorial. Therefore, the final expression for \(P[X=n]\) is: \[P[X=n] = \frac{1}{2^{n+1}n!} \cdot n!\] Cancel out the factorials, and we are left with: \[P[X=n] = \left(\frac{1}{2}\right)^{n+1}\] This is the desired probability.

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Most popular questions from this chapter

Suppose \(p(x, y, z)\), the joint probability mass function of the random variables \(X\), \(Y\), and \(Z\), is given by $$ \begin{array}{ll} p(1,1,1)=\frac{1}{8}, & p(2,1,1)=\frac{1}{4} \\ p(1,1,2)=\frac{1}{8}, & p(2,1,2)=\frac{3}{16} \\ p(1,2,1)=\frac{1}{16}, & p(2,2,1)=0 \\ p(1,2,2)=0, & p(2,2,2)=\frac{1}{4} \end{array} $$ \text { What is } E[X \mid Y=2] ? \text { What is } E[X \mid Y=2, Z=1] ?

Data indicate that the number of traffic accidents in Berkeley on a rainy day is a Poisson random variable with mean 9 , whereas on a dry day it is a Poisson random variable with mean \(3 .\) Let \(X\) denote the number of traffic accidents tomorrow. If it will rain tomorrow with probability \(0.6\), find (a) \(E[X]\); (b) \(P[X=0\\}\) (c) \(\operatorname{Var}(X)\)

An individual traveling on the real line is trying to reach the origin. However, the larger the desired step, the greater is the variance in the result of that step. Specifically, whenever the person is at location \(x\), he next moves to a location having mean 0 and variance \(\beta x^{2}\). Let \(X_{n}\) denote the position of the individual after having taken \(n\) steps. Supposing that \(X_{0}=x_{0}\), find (a) \(E\left[X_{n}\right]\); (b) \(\operatorname{Var}\left(X_{n}\right)\)

A coin that comes up heads with probability \(p\) is flipped \(n\) consecutive times. What is the probability that starting with the first flip there are always more heads than tails that have appeared?

The joint probability mass function of \(X\) and \(Y, p(x, y)\), is given by $$ \begin{array}{ll} p(1,1)=\frac{1}{9}, & p(2,1)=\frac{1}{3}, & p(3,1)=\frac{1}{9} \\ p(1,2)=\frac{1}{9}, & p(2,2)=0, & p(3,2)=\frac{1}{18} \\ p(1,3)=0, & p(2,3)=\frac{1}{6}, & p(3,3)=\frac{1}{9} \end{array} $$ Compute \(E[X \mid Y=i]\) for \(i=1,2,3\).

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