<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">AM</journal-id><journal-title-group><journal-title>Applied Mathematics</journal-title></journal-title-group><issn pub-type="epub">2152-7385</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/am.2014.53047</article-id><article-id pub-id-type="publisher-id">AM-42796</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  The Distribution of Multiple Shot Noise Process and Its Integral
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>iwook</surname><given-names>Jang</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Department of Applied Finance &amp;amp; Actuarial Studies, Faculty of Business and Economics,
Macquarie University, Sydney, Australia</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>jiwook.jang@mq.edu.au</email></corresp></author-notes><pub-date pub-type="epub"><day>07</day><month>02</month><year>2014</year></pub-date><volume>05</volume><issue>03</issue><fpage>478</fpage><lpage>489</lpage><history><date date-type="received"><day>October</day>	<month>30,</month>	<year>2013</year></date><date date-type="rev-recd"><day>November</day>	<month>30,</month>	<year>2013</year>	</date><date date-type="accepted"><day>December</day>	<month>7,</month>	<year>2013</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
   In this paper, we study multiple shot noise process and its integral. We analyse these two processes systematically for their theoretical distributions, based on the piecewise deterministic Markov process theory developed by Davis [1] and the martingale methodology used by Dassios and Jang [2]. The analytic expressions of the Laplace transforms of these two processes are presented. We also obtain the multivariate probability generating function for the number of jumps, for which we use a multivariate Cox process. To derive these, we assume that the Cox processes jumps, intensity jumps and primary event jumps are independent of each other. Using the Laplace transform of the integral of multiple shot noise process, we obtain the tail of multivariate distributions of the first jump times of the Cox processes, i.e. the multivariate survival functions. Their numerical calculations and other relevant joint distributions’ numerical values are also presented. 
 
</p></abstract><kwd-group><kwd>Multiple Shot Noise Process and Its Integral; Multivariate Cox Process; Piecewise Deterministic Markov Process; Martingale Methodology; Multivariate Survival Functions</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Due to global warming and climate changes, there have been increases in the frequency and intensity of floods in one area and draught in the other. So administrating the level of water in dams and rivers becomes much more significant task than ever before. Single (Poisson) shot noise process can be used to model the level of water in dams and rivers, but it is quite inadequate as rains do not occur according to only a Poisson process [<xref ref-type="bibr" rid="scirp.42796-ref3">3</xref>].</p><p>Increases in the frequency and intensity of storms, hail, bushfires and earthquakes have revealed shortcomings in the ways Catastrophe Insurance is priced. Hence more complicated models are needed to accommodate increasing frequency and intensity of catastrophic events. A Cox process with shot noise intensity has been suggested to use to predict claims arising from catastrophic events by Dassios and Jang [<xref ref-type="bibr" rid="scirp.42796-ref2">2</xref>].</p><p>In financial industry, a shock which initially affects a couple of institutions or a particular region of the economy spreads to the rest of the financial industry and then infects the larger economy. This is called “financial contagion” [4,5]. The US federal takeover of Fannie Mae and Freddie Mac, the Bank of America takeover of Countrywide Financial Corporation and the bankruptcy of New Century Financial Corporation due to mismanagement of subprime mortgage in US are the examples of financial contagion. The prevalence of above financial contagion has led to further bankruptcies and default of mortgage lenders in US announcing their significant losses in 2008. This subprime mortgage meltdown has also led to new ownership for Bears Stern and Merrill Lynch and the bankruptcy of Lehman Brothers. These contagious events have caused the collapse of stock prices in worldwide and it has shaken global financial markets further due to new waves of default and bankruptcy. Due to the failing of financial institutions in 2008, systemic risk has become the main concern to the governments requiring their interventions to ameliorate these contagious effects to the larger economy [<xref ref-type="bibr" rid="scirp.42796-ref6">6</xref>].</p><p>To these effects, in this paper we introduce multiple shot noise process [<xref ref-type="bibr" rid="scirp.42796-ref7">7</xref>]. It consists of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x1.png" xlink:type="simple"/></inline-formula> component</p><p>processes<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x2.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x3.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x4.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x6.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x5.png" xlink:type="simple"/></inline-formula>where each process acts as a jump intensity for the next one. For</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x8.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x7.png" xlink:type="simple"/></inline-formula>decays with rate<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x9.png" xlink:type="simple"/></inline-formula>, and additive jumps occur with rate of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x10.png" xlink:type="simple"/></inline-formula>, i.e. each</p><p>process acts as a jump intensity for the next one. Jump sizes are independent but not identically distributed</p><p>random variables with distribution function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x11.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x12.png" xlink:type="simple"/></inline-formula> decays with rate <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x13.png" xlink:type="simple"/></inline-formula> but its jump arrival rate</p><p>is deterministic<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x14.png" xlink:type="simple"/></inline-formula>. Its jump sizes have distribution function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x15.png" xlink:type="simple"/></inline-formula> Hence multiple shot noise process we consider has the following structure:</p><disp-formula id="scirp.42796-formula159"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/15-7401950x16.png"  xlink:type="simple"/></disp-formula><p>where:</p><p>・ <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x17.png" xlink:type="simple"/></inline-formula>are sequences of independent but not identically distributed random</p><p>variables with distribution function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x18.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x19.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x20.png" xlink:type="simple"/></inline-formula></p><p>・ <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x21.png" xlink:type="simple"/></inline-formula>is the total number of events up to time <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x22.png" xlink:type="simple"/></inline-formula></p><p>・ <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x23.png" xlink:type="simple"/></inline-formula>is the rate of exponential decay for the firm <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x24.png" xlink:type="simple"/></inline-formula></p><p>We also make the additional assumption that the point process <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x25.png" xlink:type="simple"/></inline-formula> and the sequences <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x26.png" xlink:type="simple"/></inline-formula> are independent of each other.</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x27.png" xlink:type="simple"/></inline-formula>follows a homogeneous Poisson process with frequency rate <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x28.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x29.png" xlink:type="simple"/></inline-formula> for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x30.png" xlink:type="simple"/></inline-formula> follows a Cox process with intensity rate<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x31.png" xlink:type="simple"/></inline-formula>, respectively [8-10]. So in this model, dependence between the processes <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x32.png" xlink:type="simple"/></inline-formula> comes from the structure that each process acts as a jump intensity for the next one.</p><p>The process <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x33.png" xlink:type="simple"/></inline-formula> is triggered by jumps (or primary events, or shocks) that will result in a positive jump in the process. As time passes, the process decreases with rate <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x34.png" xlink:type="simple"/></inline-formula> until another jump (or event) occurs which again will result in a positive jump in the process. The process <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x35.png" xlink:type="simple"/></inline-formula> is the jump arrival rate for the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x36.png" xlink:type="simple"/></inline-formula> process<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x37.png" xlink:type="simple"/></inline-formula>, and the process <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x38.png" xlink:type="simple"/></inline-formula> is the jump arrival rate for the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x39.png" xlink:type="simple"/></inline-formula> process<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x40.png" xlink:type="simple"/></inline-formula>, and so on. Hence the process <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x41.png" xlink:type="simple"/></inline-formula> is the prime trigger in influencing all other relative processes. As time passes, the processes <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x42.png" xlink:type="simple"/></inline-formula> decrease with rate <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x43.png" xlink:type="simple"/></inline-formula> for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x44.png" xlink:type="simple"/></inline-formula>, and additive jumps occur.</p><p>We use another Cox process <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x45.png" xlink:type="simple"/></inline-formula> for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x46.png" xlink:type="simple"/></inline-formula> to model the multivariate jump time and derive the tail of multivariate distribution of the first jump times of the Cox processes, i.e. the multivariate survival function, where it is assumed that the jumps in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x47.png" xlink:type="simple"/></inline-formula> for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x48.png" xlink:type="simple"/></inline-formula>, the jumps in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x49.png" xlink:type="simple"/></inline-formula> for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x50.png" xlink:type="simple"/></inline-formula> and primary event jumps in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x51.png" xlink:type="simple"/></inline-formula> are independent of each other.</p><p>If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x52.png" xlink:type="simple"/></inline-formula> (i.e.<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x53.png" xlink:type="simple"/></inline-formula>), this process becomes a double shot noise process, and it can be considered to model the level of water in dams and rivers using this process. Applying a double shot noise process in insurance context can be noticed in Dassios and Jang [<xref ref-type="bibr" rid="scirp.42796-ref11">11</xref>].</p><p>In Section 2, we start with deriving the Laplace transform of the vector</p><disp-formula id="scirp.42796-formula160"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x54.png"  xlink:type="simple"/></disp-formula><p>using the martingale methodology in Dassios and Jang [<xref ref-type="bibr" rid="scirp.42796-ref2">2</xref>], with which we obtain the expression for</p><disp-formula id="scirp.42796-formula161"><label>(1.2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/15-7401950x55.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x56.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x57.png" xlink:type="simple"/></inline-formula> for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x58.png" xlink:type="simple"/></inline-formula> For simplicity, it is assumed that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x59.png" xlink:type="simple"/></inline-formula> but it</p><p>can be easily extended to the higher dimensions. Using (1.2) in Section 3, we derive the tail of the multivariate</p><p>distribution of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x60.png" xlink:type="simple"/></inline-formula>’s, where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x61.png" xlink:type="simple"/></inline-formula>, i.e.</p><disp-formula id="scirp.42796-formula162"><label>(1.3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/15-7401950x62.png"  xlink:type="simple"/></disp-formula><p>that is equivalent to the first jump time of the Cox process<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x63.png" xlink:type="simple"/></inline-formula>. The expressions for relevant multivariate distributions such as</p><disp-formula id="scirp.42796-formula163"><label>(1.4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/15-7401950x64.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.42796-formula164"><label>(1.5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/15-7401950x65.png"  xlink:type="simple"/></disp-formula><p>are omitted as they can easily be obtained using (1.2) and (1.3), but their numerical calculations are shown in Section 4. Section 5 contains some concluding remarks.</p></sec><sec id="s2"><title>2. The Laplace Transform of the Vector <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x66.png" xlink:type="simple"/></inline-formula></title><p>We firstly consider using the Laplace transform of the vector</p><disp-formula id="scirp.42796-formula165"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x67.png"  xlink:type="simple"/></disp-formula><p>to derive the tail of the multivariate distribution of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x68.png" xlink:type="simple"/></inline-formula>’s. Once its expression is obtained, we can easily derive the tail of the multivariate distribution of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x69.png" xlink:type="simple"/></inline-formula>’s by setting <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x70.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x71.png" xlink:type="simple"/></inline-formula> in the Equation (1.2).</p><p>With the aid of piecewise deterministic Markov process theory and using the results in [<xref ref-type="bibr" rid="scirp.42796-ref1">1</xref>], the infinitesimal</p><p>generator of the process <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x72.png" xlink:type="simple"/></inline-formula> acting on a function</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x73.png" xlink:type="simple"/></inline-formula>within its domain <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x74.png" xlink:type="simple"/></inline-formula> is given by</p><disp-formula id="scirp.42796-formula166"><label>(2.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/15-7401950x75.png"  xlink:type="simple"/></disp-formula><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x76.png" xlink:type="simple"/></inline-formula> to belong to the domain of the generator<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x77.png" xlink:type="simple"/></inline-formula>, it is sufficient</p><p>that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x78.png" xlink:type="simple"/></inline-formula> is differentiable w.r.t.<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x79.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x81.png" xlink:type="simple"/></inline-formula>for all <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x82.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x83.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x84.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x85.png" xlink:type="simple"/></inline-formula>and that</p><disp-formula id="scirp.42796-formula167"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x86.png"  xlink:type="simple"/></disp-formula><p>We assume that the Cox processes jumps, intensity jumps and primary event jumps do not occur at the same time.</p><p>Let us find a suitable martingale to derive the Laplace transform of the vector<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x87.png" xlink:type="simple"/></inline-formula>, the</p><p>Laplace transform of the vector <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x88.png" xlink:type="simple"/></inline-formula> and the p.g.f. (probability generating function) of the vector</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x89.png" xlink:type="simple"/></inline-formula>respectively.</p><p>Theorem 2.1 Considering constants<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x90.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x91.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x92.png" xlink:type="simple"/></inline-formula> such that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x93.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x94.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x95.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.42796-formula168"><label>(2.2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/15-7401950x96.png"  xlink:type="simple"/></disp-formula><p>is a martingale, where</p><disp-formula id="scirp.42796-formula169"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x97.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.42796-formula170"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x98.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.42796-formula171"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x99.png"  xlink:type="simple"/></disp-formula><p>Proof. From (2.1), <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x100.png" xlink:type="simple"/></inline-formula>has to satisfy <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x101.png" xlink:type="simple"/></inline-formula> for it to be a martin-</p><p>gale. Setting</p><disp-formula id="scirp.42796-formula172"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x102.png"  xlink:type="simple"/></disp-formula><p>we get the Equation</p><disp-formula id="scirp.42796-formula173"><label>(2.3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/15-7401950x103.png"  xlink:type="simple"/></disp-formula><p>from which we have</p><disp-formula id="scirp.42796-formula174"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x104.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.42796-formula175"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x105.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.42796-formula176"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x106.png"  xlink:type="simple"/></disp-formula><p>Solve these Equations, then the result follows.</p><p>For simplicity, we set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x107.png" xlink:type="simple"/></inline-formula> (i.e. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x108.png" xlink:type="simple"/></inline-formula>and 1), but it can be easily extended to the higher dimension cases.</p><p>Theorem 2.2 Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x109.png" xlink:type="simple"/></inline-formula> be as defined. Then</p><disp-formula id="scirp.42796-formula177"><label>(2.4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/15-7401950x110.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.42796-formula178"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x111.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.42796-formula179"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x112.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.42796-formula180"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x113.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.42796-formula181"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x114.png"  xlink:type="simple"/></disp-formula><p>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x115.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x116.png" xlink:type="simple"/></inline-formula> for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x117.png" xlink:type="simple"/></inline-formula>.</p><p>Proof. Using the martingale derived in Theorem 2.1, we have</p><disp-formula id="scirp.42796-formula182"><label>(2.5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/15-7401950x118.png"  xlink:type="simple"/></disp-formula><p>Hence the result follows immediately if we set</p><disp-formula id="scirp.42796-formula183"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x119.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.42796-formula184"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x120.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.42796-formula185"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x121.png"  xlink:type="simple"/></disp-formula><p>in (2.5).</p><p>Corollary 2.3 Let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x122.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x123.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x124.png" xlink:type="simple"/></inline-formula> be as defined for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x125.png" xlink:type="simple"/></inline-formula> and 1. Then</p><disp-formula id="scirp.42796-formula186"><label>(2.6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/15-7401950x126.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.42796-formula187"><label>(2.7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/15-7401950x127.png"  xlink:type="simple"/></disp-formula><p>Proof. If we set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x128.png" xlink:type="simple"/></inline-formula> in (2.4), (2.6) follows. If we also set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x129.png" xlink:type="simple"/></inline-formula> in (2.4), (2.7) follows.</p><p>Now we can easily derive the Laplace transform of the vector <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x130.png" xlink:type="simple"/></inline-formula> the Laplace transform of the</p><p>vector <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x131.png" xlink:type="simple"/></inline-formula> and the p.g.f. of the vector<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x132.png" xlink:type="simple"/></inline-formula>, respectively.</p><p>Corollary 2.4 The Laplace transform of the vector <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x133.png" xlink:type="simple"/></inline-formula> and the Laplace transform of the vector <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x134.png" xlink:type="simple"/></inline-formula> are given by</p><disp-formula id="scirp.42796-formula188"><label>(2.8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/15-7401950x135.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.42796-formula189"><label>(2.9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/15-7401950x136.png"  xlink:type="simple"/></disp-formula><p>and the p.g.f. of the vector <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x137.png" xlink:type="simple"/></inline-formula> is given by</p><disp-formula id="scirp.42796-formula190"><label>(2.10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/15-7401950x138.png"  xlink:type="simple"/></disp-formula><p>Proof. If we set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x139.png" xlink:type="simple"/></inline-formula> in (2.6) and (2.7) respectively, (2.8) and (2.10) follow. If we also set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x140.png" xlink:type="simple"/></inline-formula> in (2.6) or set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x139.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x141.png" xlink:type="simple"/></inline-formula> in (2.7), (2.9) follows.</p><p>Remark 1: It would be interesting to apply the p.g.f. of the vector <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x142.png" xlink:type="simple"/></inline-formula> to model insurance claim arrivals as well as the number of losses to the entire financial system/market. Also using (2.10), the marginal probability generating function for the number of jump can be easily derived. The derivation of the</p><p>marginal probability generating function for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x143.png" xlink:type="simple"/></inline-formula> and its usage in insurance context can be</p><p>found in Dassios and Jang [2,12]. To obtain the mean and variance of the level of water in dams and rivers, the</p><p>Laplace transform of the vector<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x144.png" xlink:type="simple"/></inline-formula>, i.e. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x145.png" xlink:type="simple"/></inline-formula>can be also used.</p><p>Corollary 2.5 The Laplace transform of the vector<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x146.png" xlink:type="simple"/></inline-formula>, where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x147.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x148.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x146.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x149.png" xlink:type="simple"/></inline-formula> are jointly stationary is given by</p><disp-formula id="scirp.42796-formula191"><label>(2.11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/15-7401950x150.png"  xlink:type="simple"/></disp-formula><p>Proof. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x151.png" xlink:type="simple"/></inline-formula> in (2.9) and the result follows.</p></sec><sec id="s3"><title>3. Multivariate Survival Function</title><p>Having derived the Laplace transform of the vector <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x152.png" xlink:type="simple"/></inline-formula> and the Laplace transform of the vector <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x153.png" xlink:type="simple"/></inline-formula> in the previous section, we can easily obtain the tail of multivariate distributions of the first jump times of the Cox processes (i.e. the multivariate survival function), other relevant joint distributions and the marginal survival functions. To do so, we start with a corollary assuming that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x154.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x155.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x155.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x156.png" xlink:type="simple"/></inline-formula> are jointly stationary.</p><p>Corollary 3.1 The Laplace transform of the vector <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x157.png" xlink:type="simple"/></inline-formula> where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x158.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x159.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x160.png" xlink:type="simple"/></inline-formula> are jointly stationary, is given by</p><disp-formula id="scirp.42796-formula192"><label>(3.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/15-7401950x161.png"  xlink:type="simple"/></disp-formula><p>Proof. Take the expectation to (2.8) and use (2.11), then (3.1) follows.</p><p>Now, we can obtain the multivariate survival function, other relevant joint distributions and the marginal survival functions.</p><p>Corollary 3.2 The multivariate survival function, where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x162.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x163.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x164.png" xlink:type="simple"/></inline-formula> are jointly stationary, is given by</p><disp-formula id="scirp.42796-formula193"><label>(3.2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/15-7401950x165.png"  xlink:type="simple"/></disp-formula><p>Proof. If we set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x166.png" xlink:type="simple"/></inline-formula> in (3.1), (3.2) follows immediately.</p><p>Using (3.2), we can obtain other relevant joint distributions, three bivariate survival functions, i.e.</p><disp-formula id="scirp.42796-formula194"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x167.png"  xlink:type="simple"/></disp-formula><p>and other relevant bivariate distributions. We can also obtain three marginal survival functions, i.e.</p><disp-formula id="scirp.42796-formula195"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x168.png"  xlink:type="simple"/></disp-formula><p>They are omitted as they can easily be obtained by using the values for the vector <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x169.png" xlink:type="simple"/></inline-formula> with 0 or 1 in (3.1). Instead, we present numerical calculations of eight joint distributions with these survival functions in Section 4.</p></sec><sec id="s4"><title>4. Numerical Examples</title><p>In this section, we show the calculations of multivariate survival function, other relevant joint distributions and the survival functions, i.e. eight joint distributions, three bivariate survival functions and three marginal survival functions. To do so, we use three exponential distributions for jump sizes for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x170.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x171.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x171.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x172.png" xlink:type="simple"/></inline-formula>, respectively, which are:</p><disp-formula id="scirp.42796-formula196"><label>(4.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/15-7401950x173.png"  xlink:type="simple"/></disp-formula><p>Other distributions such as normal, log-normal, gamma and Pareto, etc. can be also applied for jump size distributions for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x174.png" xlink:type="simple"/></inline-formula> (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x175.png" xlink:type="simple"/></inline-formula>and 1).</p><p>Using (3.2), one of corresponding bivariate survival functions is given by</p><disp-formula id="scirp.42796-formula197"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/15-7401950x176.png"  xlink:type="simple"/></disp-formula><p>We can easily obtain other corresponding bivariate survival functions, i.e.</p><disp-formula id="scirp.42796-formula198"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x177.png"  xlink:type="simple"/></disp-formula><p>which are omitted as they have similar nested expressions to (4.2).</p><p>Using (3.2), one of corresponding marginal survival functions is given by</p><disp-formula id="scirp.42796-formula199"><label>(4.3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/15-7401950x178.png"  xlink:type="simple"/></disp-formula><p>which can be found in Dassios and Jang [<xref ref-type="bibr" rid="scirp.42796-ref2">2</xref>]. We can also find another corresponding marginal survival function, i.e.</p><disp-formula id="scirp.42796-formula200"><label>(4.4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/15-7401950x179.png"  xlink:type="simple"/></disp-formula><p>We can easily obtain remaining marginal survival function, i.e. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x180.png" xlink:type="simple"/></inline-formula>which are omitted as it has also similar extended nested expressions to (4.4).</p><p>Now let us illustrate the calculations of three marginal survival functions, three bivariate survival functions and eight joint distributions. To do so, we use the parameter values as below:</p><disp-formula id="scirp.42796-formula201"><label>(4.5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/15-7401950x181.png"  xlink:type="simple"/></disp-formula><p>Example 4.1 (Marginal survival functions)</p><p>The calculations of three marginal survival functions, i.e.</p><disp-formula id="scirp.42796-formula202"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x182.png"  xlink:type="simple"/></disp-formula><p>are given by</p><disp-formula id="scirp.42796-formula203"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x183.png"  xlink:type="simple"/></disp-formula><p>Example 4.2 (Bivariate survival functions)</p><p>The calculations of three bivariate survival functions, i.e.</p><disp-formula id="scirp.42796-formula204"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x184.png"  xlink:type="simple"/></disp-formula><p>are given by</p><disp-formula id="scirp.42796-formula205"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x185.png"  xlink:type="simple"/></disp-formula><p>Example 4.3 (Eight joint distributions)</p><p>The calculations of eight joint distributions, i.e.</p><disp-formula id="scirp.42796-formula206"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x186.png"  xlink:type="simple"/></disp-formula><p>are given by</p><disp-formula id="scirp.42796-formula207"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x187.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.42796-formula208"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x188.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.42796-formula209"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x189.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.42796-formula210"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x190.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.42796-formula211"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x191.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.42796-formula212"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x192.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.42796-formula213"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x193.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.42796-formula214"><graphic  xlink:href="http://html.scirp.org/file/15-7401950x194.png"  xlink:type="simple"/></disp-formula><p>Remark 2: Example 4.1 shows that the survival probability of the firm 1 is the highest and the firm 2’s and the firm 3’s, which can be modified with different parameter values for (4.5). Example 4.2 and 4.3 show that all relevant joint probabilities are in line with each survival probability in Example 4.1. For example, the joint survival probability of firm 2 and 1, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x195.png" xlink:type="simple"/></inline-formula>is the highest as the combination of these two firms’ survival probabilities are the highest. Also it can be easily noticed that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x195.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x196.png" xlink:type="simple"/></inline-formula> is the highest in Example 4.3 as the joint survival probability of firm 2 and 1 is the highest.</p><p>An economic interpretation from the perspective of the multiple shot noise process is the following. After the firm 3 ceases to function (e.g. default of Lehman Brothers), its intensity is still around affecting the other firms in the way of the multiple shot noise process. Hence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x197.png" xlink:type="simple"/></inline-formula> can be interpreted as the probability that the firm 2 and 1 survive together after the firm 3 ceases to function, but its intensity is still in action. Also <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x197.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x198.png" xlink:type="simple"/></inline-formula> can be interpreted as the probability that the firm 1 survives after the firm 3 and 2 cease to function, but their intensities are still in action.</p><p>After the failing of the firm 3, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/15-7401950x199.png" xlink:type="simple"/></inline-formula>can be considered as a measure to decide whether the government’s intervention is required not to fail the firm 2 and 1 with a threshold probability (e.g. 0.5) assumng that its intensity is still in action. Also by simulating the multiple shot noise process, this probability can be easily obtained as a systemic risk management tool for the governments.</p></sec><sec id="s5"><title>5. Conclusions</title><p>We introduced multiple shot noise process, where each process acts as a jump intensity for the next one, and its integral. These two processes can be used in hydropower, dam and river engineering fields. Based on the piecewise deterministic Markov process theory developed by Davis [<xref ref-type="bibr" rid="scirp.42796-ref1">1</xref>] and the martingale methodology used by Dassios and Jang [<xref ref-type="bibr" rid="scirp.42796-ref2">2</xref>], we derived the Laplace transforms of these two processes. Using the multivariate Cox process, the multivariate probability generating function for the number of jumps was also presented. To do so, we have made an assumption that the Cox processes jumps, intensity jumps and primary event jumps are independent of each other. This probability generating function can be considered applying to modeling insurance claim arrivals as well as the number of losses to the entire financial system/market.</p><p>Using the Laplace transform of the integral of multiple shot noise process, we obtained the tail of multivariate distributions of the first jump times of the Cox processes, i.e. the multivariate survival functions. These survival functions can be used as the measures to decide whether the government intervention is required to ameliorate the contagious effects to the entire financial system or larger economy. With exponential distributions for jump sizes, we calculated multivariate survival function, other relevant joint distributions and the survival functions. We leave the applications of what we presented in this paper, i.e. a multivariate Cox process with multiple shot noise intensity, multiple shot noise process and its integral to the fields mentioned above for further research.</p></sec></body><back><ref-list><title>References</title><ref id="scirp.42796-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">M. H. A. Davis, “Piecewise Deterministic Markov Processes: A General Class of Non Diffusion Stochastic Models,” Journal of the Royal Statistical Society B, Vol. 46, No. 3, 1984, pp. 353-388.</mixed-citation></ref><ref id="scirp.42796-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">A. Dassios and J. 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