Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

For a nonhomogeneous Poisson process with intensity function \(\lambda(t), t \geqslant 0\), where \(\int_{0}^{\infty} \lambda(t) d t=\infty\), let \(X_{1}, X_{2}, \ldots\) denote the sequence of times at which events occur. (a) Show that \(\int_{0}^{X_{1}} \lambda(t) d t\) is exponential with rate 1 . (b) Show that \(\int_{X_{i-1}}^{X_{i}} \lambda(t) d t, i \geqslant 1\), are independent exponentials with rate 1, where \(X_{0}=0\) In words, independent of the past, the additional amount of hazard that must be experienced until an event occurs is exponential with rate 1 .

Short Answer

Expert verified
In summary, we have shown that for a nonhomogeneous Poisson process with intensity function \(\lambda(t)\), the time intervals between events \(\int_{0}^{X_{1}} \lambda(t) dt\) and \(\int_{X_{i-1}}^{X_{i}} \lambda(t) dt\) are exponentially distributed with rate 1 and are independent of each other, which demonstrates that the additional amount of hazard experienced until an event occurs is exponential with rate 1 regardless of the past.

Step by step solution

01

Introduce the exponential distribution

The exponential distribution has density function given by \(f(x)=\lambda e^{-\lambda x}\), where \(\lambda\) is the rate of the distribution, and its mean is 1/\(\lambda\). We will use this density function to show that the given time intervals are exponentially distributed with rate 1.
02

Compute the probability that an event occurs before time \(X_{1}\)

We want to find the probability that an event occurs before time \(X_{1}\), which is given by the integral \(\int_{0}^{X_{1}} \lambda(t) dt\). To show that this integral is exponentially distributed with rate 1, let \(F(x)\) be the cumulative distribution function (CDF), so that \(F(x) = \int_{0}^{x} \lambda(t) dt\). Then the exponential density function with rate 1, denoted as \(f(x)\), is equal to the derivative of \(F(x)\) with respect to \(x\), or \[f(x) = \frac{dF(x)}{dx} = \lambda(x),\] since \(\int_{0}^{X_{1}} \lambda(t) dt = F(X_{1})\).
03

Independence of events

Now we want to show that the integrals between consecutive event times, \(\int_{X_{i-1}}^{X_{i}} \lambda(t) dt, i \geq 1\), are independent of each other. Recall that in a Poisson process, the number of events in non-overlapping intervals are independent. Let \(N(t)\) denote the number of events in the interval \([0,t)\), and let \(Y(t)=\int_{0}^{t} \lambda(s) ds\). By definition, the number of events in the interval \((X_{i-1}, X_{i})\) is \(N(X_{i})=N(X_{i-1})+1\). Given that we observed \(N(X_{i-1})=n\), we want to find the conditional distribution of \(Y(X_{i})\) given \(Y(X_{i-1})=y\). That is, \[P(Y(X_{i}) \le z | Y(X_{i-1}) = y) = P(Y(X_{i})-Y(X_{i-1}) \le z-y | Y(X_{i-1})=y).\] Now let \(W_i = Y(X_{i})-Y(X_{i-1})\). Note that the events we saw up to time \(X_{i-1}\) do not affect the future events, so we have \[P(W_i \le z-y | Y(X_{i-1})=y) = P(W_i \le z-y) = F(z-y).\] Finally, taking the derivative with respect to \(z\) yields the density function, \[\frac{d}{dz} F(z-y) = \lambda(z).\] Thus, the distribution of the \(\int_{X_{i-1}}^{X_{i}} \lambda(t) dt\) are independent exponentials with rate 1, which completes the proof.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

Suppose we are able to simulate independent random variables \(X\) and \(Y .\) If we simulate \(2 k\) independent random variables \(X_{1}, \ldots, X_{k}\) and \(Y_{1}, \ldots, Y_{k}\), where the \(X_{i}\) have the same distribution as does \(X\), and the \(Y_{j}\) have the same distribution as does \(Y\), how would you use them to estimate \(P(X

In Example \(11.4\) we simulated the absolute value of a standard normal by using the Von Neumann rejection procedure on exponential random variables with rate \(1 .\) This raises the question of whether we could obtain a more efficient algorithm by using a different exponential density-that is, we could use the density \(g(x)=\) \(\lambda e^{-\lambda x}\). Show that the mean number of iterations needed in the rejection scheme is minimized when \(\lambda=1\).

The Discrete Rejection Metbod: Suppose we want to simulate \(X\) having probability mass function \(P\\{X=i\\}=P_{i}, i=1, \ldots, n\) and suppose we can easily simulate from the probability mass function \(Q_{i}, \sum_{i} Q_{i}=1, Q_{i} \geqslant 0 .\) Let \(C\) be such that \(P_{i} \leqslant C Q_{i}, i=1, \ldots, n .\) Show that the following algorithm generates the desired random variable: Step 1: Generate \(Y\) having mass function \(Q\) and \(U\) an independent random number. Step \(2:\) If \(U \leqslant P_{Y} / C Q_{Y}\), set \(X=Y .\) Otherwise return to step \(1 .\)

Show that if \(X\) and \(Y\) have the same distribution then $$ \operatorname{Var}((X+Y) / 2) \leqslant \operatorname{Var}(X) $$ Hence, conclude that the use of antithetic variables can never increase variance (though it need not be as efficient as generating an independent set of random numbers).

The Hit-Miss Method: Suppose \(g\) is bounded in \([0,1]-\) for instance, suppose \(0 \leqslant g(x) \leqslant b\) for \(x \in[0,1]\). Let \(U_{1}, U_{2}\) be independent random numbers and set \(X=U_{1}, Y=b U_{2}\) -so the point \((X, Y)\) is uniformly distributed in a rectangle of length 1 and height \(b\). Now set $$ I=\left\\{\begin{array}{ll} 1, & \text { if } Y

See all solutions

Recommended explanations on Math Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free