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<math>\phi_{X}\left(s\right)=P_{N\left(t\right)}\left(z\right)\biggl|_{z=\phi_{Y}\left(s\right)}=e^{-\lambda t\left(1-z\right)}\biggl|_{z=e^{-\lambda_{Y}t\left(1-e^{s}\right)}}=e^{-\lambda t\left(1-e^{-\lambda_{Y}t\left(1-e^{s}\right)}\right)}.</math>  
 
<math>\phi_{X}\left(s\right)=P_{N\left(t\right)}\left(z\right)\biggl|_{z=\phi_{Y}\left(s\right)}=e^{-\lambda t\left(1-z\right)}\biggl|_{z=e^{-\lambda_{Y}t\left(1-e^{s}\right)}}=e^{-\lambda t\left(1-e^{-\lambda_{Y}t\left(1-e^{s}\right)}\right)}.</math>  
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Revision as of 06:10, 17 November 2010

1.5 Poisson Process

There are Bernoulli trials at every $ dt $ and the probability of success is $ \lambda dt $ . If $ \mathbf{N}\left(t\right) $ is the number of success in time $ t $ , the set $ \left\{ \mathbf{N}\left(t\right),\; t\geq0\right\} $ is the Poinsson process. The distribution of $ \mathbf{N}\left(t\right) $ is gained by insering $ p=\frac{\lambda t}{n} $ and applying $ n\rightarrow\infty $ . $ P\left(\left\{ \mathbf{N}\left(t\right)=y\right\} \right)=\lim_{n\rightarrow\infty}\left(\begin{array}{c} n\\ y \end{array}\right)\left(\frac{\lambda t}{n}\right)^{y}\left(1-\frac{\lambda t}{n}\right)^{n-y}=\frac{\left(\lambda t\right)^{y}e^{-\lambda t}}{y!},\qquad y=0,1,2,\cdots $.

Moment generating function

$ \phi_{\mathbf{N}\left(t\right)}\left(s\right)=E\left[e^{s\cdot\mathbf{N}\left(t\right)}\right]=\sum_{k=0}^{\infty}e^{s\cdot k}\cdot\frac{\left(\lambda t\right)^{k}e^{-\lambda t}}{k!}=e^{-\lambda t}\sum_{k=0}^{\infty}\frac{\left(e^{s}\cdot\lambda t\right)^{k}}{k!}=e^{-\lambda t}\cdot e^{\lambda t\cdot e^{s}}=e^{-\lambda t\left(1-e^{s}\right)}. $

Example

Two independent Poisson process $ \mathbf{N}_{1}\left(t\right) $ and $ \mathbf{N}_{2}\left(t\right) $ have the mean $ \lambda_{1}t $ and $ \lambda_{2}t $ respectively. Find the distribution of $ \mathbf{N}_{1}\left(t\right)+\mathbf{N}_{2}\left(t\right) $ .

Solution

$ \phi_{\mathbf{N}_{1}\left(t\right)}\left(s\right)=e^{-\lambda_{1}t\left(1-e^{s}\right)}\text{ and }\phi_{\mathbf{N}_{2}\left(t\right)}\left(s\right)=e^{-\lambda_{2}t\left(1-e^{s}\right)} $.

$ \phi_{\mathbf{N}_{1}\left(t\right)+\mathbf{N}_{2}\left(t\right)}\left(s\right) $

Thus, $ \mathbf{N}_{1}\left(t\right)+\mathbf{N}_{2}\left(t\right) $ is a Poisson process with the mean $ \left(\lambda_{1}+\lambda_{2}\right)t $ .

Superposition

$ \left\{ \mathbf{N}_{i}\left(t\right),\; t\geq0\right\} $ is $ PP\left(\lambda_{i}\right),\; i=1,2,\cdots,n $ and independent each other. If $ \mathbf{N}\left(t\right)=\sum_{i=1}^{n}\mathbf{N}_{i}\left(t\right) $ and $ \lambda=\sum_{i=1}^{n}\lambda_{i} $ , then $ \left\{ \mathbf{N}\left(t\right),\; t\geq0\right\} $ is $ PP\left(\lambda\right) $ .

Compound Poisson process

$ \mathbf{Y}_{1},\mathbf{Y}_{2},\cdots $ are i.i.d. random variables. $ \mathbf{N}\left(t\right) $ is Poisson process $ \left(\lambda\right) $ and is independent with $ \mathbf{Y} $ s. Then, the set $ \left\{ \mathbf{X}\left(t\right),\; t\geq0\right\} $ is the compound Poisson process where $ \mathbf{X}\left(t\right)=\mathbf{Y}_{1}+\mathbf{Y}_{2}+\cdots+\mathbf{Y}_{\mathbf{N}\left(t\right)} $ .

$ E\left[\mathbf{X}\left(t\right)\right]=\sum_{i=1}^{E\left[\mathbf{N}\left(t\right)\right]}E\left[\mathbf{Y}_{i}\right]=E\left[\mathbf{N}\left(t\right)\right]E\left[\mathbf{Y}\right]=\lambda t\cdot E\left[\mathbf{Y}\right] $.

$ Var\left[\mathbf{X}\left(t\right)\right]=\lambda t\cdot E\left[\mathbf{Y}^{2}\right] $.

The necessary condition for $ \mathbf{X}\left(t\right) $ to become Poisson process is $ E\left[\mathbf{Y}\right]=E\left[\mathbf{Y}^{2}\right] $ .

If $ \mathbf{Y} $ s are Poisson process $ \left(\lambda_{Y}\right) $

The probability generating function for $ \mathbf{N}\left(t\right) $ is $ P_{N\left(t\right)}\left(z\right)=E\left[z^{N\left(t\right)}\right]=\sum_{k=0}^{\infty}z^{k}\cdot\frac{e^{-\lambda t}\cdot\left(\lambda t\right)^{k}}{k!}=e^{-\lambda t}\cdot\sum_{k=0}^{\infty}\frac{\left(z\lambda t\right)^{k}}{k!}=e^{-\lambda t}\cdot e^{z\lambda t}=e^{-\lambda t\left(1-z\right)} $.

The moment generating function for Y s is$ \phi_{Y}\left(s\right)=E\left[e^{sY}\right]=\sum_{k=0}^{\infty}e^{sk}\cdot\frac{e^{-\lambda_{Y}t}\cdot\left(\lambda_{Y}t\right)^{k}}{k!}=e^{-\lambda_{Y}t\left(1-e^{s}\right)} $.

Now, the moment generating function for $ X\left(t\right) $ is

$ \phi_{X}\left(s\right)=P_{N\left(t\right)}\left(z\right)\biggl|_{z=\phi_{Y}\left(s\right)}=e^{-\lambda t\left(1-z\right)}\biggl|_{z=e^{-\lambda_{Y}t\left(1-e^{s}\right)}}=e^{-\lambda t\left(1-e^{-\lambda_{Y}t\left(1-e^{s}\right)}\right)}. $


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