A Brief Introduction to Compound Distributions (Part One)

The provided text discusses the concept of compound distributions, which arise when combining two independent distributions. The probability generating function (pgf) of a compound distribution is shown to be the composition of the pgfs of the primary and secondary distributions. Some of the examples are excerpted from Loss Model (Sixth Edition).

Some author16 min read

A compound distribution SS of a primary distribution with pgf PN(z)P_N(z) and secondary distribution with pgf PM(z)P_M(z) has the following probability generating function:

PS(z)=PN(PM(z))P_S(z)=P_N(P_M(z))

Recall our relation between moment generating function that

MX(t)=PX(et)M_X(t) = P_X(e^t)

for any distribution XX so we will have

MS(z)=PS(ez)=PN(PM(ez))=PN(MM(z)).M_S(z) = P_S(e^z) = P_N(P_M(e^z)) = P_N(M_M(z)).

The motivation of the compound distribution is the following, assuming that we have a series of i.i.d random variables A1,A2,...,AnA_1, A_2, ..., A_n, where the number nn itself is also a random variable independent of A1,...,AnA_1, ... ,A_n so we will have

the pgf of A1+A2+...+AnA_1+A_2 +...+A_n as

∑i=0∞Pr⁡[A1+A2+...+AN=i]zi\sum_{i=0}^{\infty}\Pr[A_1 + A_2 +... +A_N = i ]z^i

by conditioning over NN, we will have

∑i=0∞∑n=0∞Pr⁡[N=n]Pr⁡[A1+A2+...+An=i∣N=n]zi=∑n=0∞Pr⁡[N=n]∑i=0∞A1+A2+...+An=i∣N=n]zi=∑n=0∞Pr⁡[N=n](PA(z))n=PN(PA(z))\sum_{i=0}^{\infty}\sum_{n=0}^{\infty}\Pr[N=n]\Pr[A_1 + A_2 +... +A_n = i | N= n]z^i = \sum_{n=0}^\infty \Pr[N=n]\sum_{i=0}^{\infty}A_1 + A_2 +... +A_n = i | N= n]z^i \\= \sum_{n=0}^\infty \Pr[N=n] \left(P_A(z)\right)^n =P_N(P_A(z))

Example \textbf{Example } Demonstrate that any zero-modified distribution is a compound distribution.

Recall that pkM=cpk0p_k^M = cp_k^0, where pkp_k is the probability for zero modified distribution and pk0p_k^0 is the probability of zero-truncated distribution for k≥1k \ge 1.

Then we will have the following relation for the pgf:

pM(z)=p0M+c∑k=1∞pk0zk=p0M+c(P(z)−p00)p^M(z) = p_0^M + c\sum_{k=1}^{\infty} p^0_kz^k=p_0^M + c(P(z) - p_0^0)

If we set zz to be 11, then we will have

1=p0M+c(1−p00)  ⟹  c=1−p0M1−p001 = p_0^M + c(1-p_0^0) \implies c =\frac{1-p_0^M}{1-p_0^0}

and so

−1−p0M1−p00⋅p00+p0M=p0M−p0Mp00−p00+p0Mp001−p00=1−1−p0M1−p00-\frac{1-p_0^M}{1-p_0^0} \cdot p_0^0 + p_0^M = \frac{p_0^M-p_0^Mp_0^0 -p_0^0+p_0^Mp_0^0}{1-p_0^0}=1-\frac{1-p_0^M}{1-p_0^0}

and so we will have Bernoulli distribution with parameter 1−p0M1−p00\frac{1-p_0^M}{1-p_0^0} as primary distribution and a zero modified distribution as a secondary distribution.

Example \textbf{Example }

Consider the case where both MM and NN have a Poisson distribution, λ1,λ2\lambda_1, \lambda_2. Determine the pgf of this distribution.

We know that Poisson distribution XX with parameter λ\lambda has the following probability generating function:

PX(z)=exp⁡(λ(z−1))P_{X}(z) = \exp(\lambda(z-1))

And so by the definition of compound distribution, we will have

PS(z)=PM(PN(z))=PM(exp⁡(λ2(z−1)))=exp⁡(λ1(eλ2(z−1)−1)).P_{S}(z) = P_M(P_N(z)) = P_M(\exp(\lambda_2(z-1))) = \exp(\lambda_1(e^{\lambda_2(z-1)}-1)).

Back to our previous discussion, the probability of A1+A2+...+An=kA_1 +A_2 +...+A_n =k can be written as

Pr⁡[A1+A2+...+AN=k]=∑n=0∞Pr⁡[A1+A2+...+An=k∣N=n]Pr⁡[N=n]\Pr[A_1+A_2 +...+A_N = k] = \sum_{n=0}^{\infty}\Pr[A_1+A_2+...+A_n= k | N=n]\Pr[N=n]

And so we can express the probability as a series of convolution where we define Pr⁡[N=n]=pn\Pr[N=n] = p_n and Pr⁡[A=k]=qk\Pr[A =k] = q_k

Then we have

Pr⁡[A1+A2+...+AN=k]=∑n=0∞pnqk∗n.\Pr[A_1+A_2 +...+A_N = k] = \sum_{n=0}^{\infty} p_n q_k^{*n}.

If the primary distribution NN is of (a,b,0)(a,b,0) class, then. we will have a recursive formula for the compound distribution. We know (a,b,0)(a,b,0) class has the following recursive formula:

kPr⁡[N=k]=(ak+b)Pr⁡[N=k−1].k \Pr[N=k] = \left(ak+b\right)\Pr[N=k-1].

We want to know about PS(z)=PN(PM(z))=∑i=0∞Pr⁡[N=k](PM(z))kP_S(z) = P_N(P_M(z)) = \sum_{i=0}^{\infty}\Pr[N=k](P_M(z))^k. And so if we multiply the recursive formula both sides with (PM(z))k(P_M(z))^k and do the summation we will have

k∑k=1∞Pr⁡[N=k](PM(z))k=(ak+b)∑k=1∞Pr⁡[N=k−1](PM(z))k  ⟹  k(PS(z)−p0)=(ak+b)PM(z)PS(z)k \sum_{k=1}^{\infty}\Pr[N=k](P_M(z))^k = (ak+b)\sum_{k=1}^{\infty}\Pr[N=k-1](P_M(z))^k\\ \implies k (P_S(z)-p_0) = (ak+b) P_M(z)P_S(z)

,

which we can't conclude anything.

However, if we differentiate PS′(z)P_S'(z) by taking into account the method of moment, we will have PS′(z)=PN′(PM(z))PM′(z)=∑i=0∞k⋅Pr⁡[N=k](PM(z))k−1PM′(z)P'_S(z) = P_N'(P_M(z)) P_M'(z) = \sum_{i=0}^{\infty}k \cdot \Pr[N=k] (P_M(z))^{k-1} P_M'(z) and so we will have

∑k=1∞kPr⁡[N=k](PM(z))k−1PM′(z)=∑k=1∞(ak+b)Pr⁡[N=k−1](PM(z))k−1PM′(z)  ⟹  PS′(z)=∑k=1∞(ak−a+a+b)Pr⁡[N=k−1](PM(z))k−1PM′(z)  ⟹  PS′(z)=(PM(z))∑k=1∞a(k−1)Pr⁡[N=k−1](PM(z))k−2PM′(z)+(a+b)∑k=1∞Pr⁡[N=k−1](PM(z))k−1PM′(z)  ⟹  PS′(z)=(PM(z))∑k=0∞akPr⁡[N=k](PM(z))k−1PM′(z)+(a+b)PM′(z)PN(PM(z))  ⟹  PS′(z)=aPM(z)PS′(z)+(a+b)PM′(z)PS(z)\sum_{k=1}^{\infty }k \Pr[N=k] (P_M(z))^{k-1} P_M'(z) =\sum_{k=1}^{\infty }(ak+b)\Pr[N=k-1](P_M(z))^{k-1} P_M'(z)\\ \implies P_S'(z) = \sum_{k=1}^{\infty} (ak-a+a+b)\Pr[N=k-1](P_M(z))^{k-1} P_M'(z) \\ \implies P_S'(z) = (P_M(z))\sum_{k=1}^{\infty}a(k-1) \Pr[N=k-1](P_M(z))^{k-2} P_M'(z) + (a+b) \sum_{k=1}^{\infty}\Pr[N=k-1](P_M(z))^{k-1} P_M'(z) \\ \implies P_S'(z) = (P_M(z))\sum_{k=0}^{\infty}ak \Pr[N=k](P_M(z))^{k-1} P_M'(z) + (a+b) P_M'(z) P_N(P_M(z))\\ \implies P'_S(z) = aP_M(z) P_S'(z) + (a+b) P_M'(z) P_S(z)

And so we will also have

PS(z)=∑i=0∞f(k)zk  ⟹  PS′(z)=∑i=0∞f(k)kzk−1P_S(z) = \sum_{i=0}^{\infty} f(k) z^k \\ \implies P_S'(z) = \sum_{i=0}^{\infty} f(k) kz^{k-1}

and we also have

PM(z)=∑k=0∞g(k)zk  ⟹  PM′(z)=∑k=0∞g(k)kzk−1P_M(z) = \sum_{k=0}^{\infty}g(k) z^k \implies P_M'(z)= \sum_{k=0}^{\infty}g(k) kz^{k-1}

and so

∑i=0∞f(k)kzk−1=a(∑i=0∞f(k)kzk−1)(∑k=0∞g(k)zk)+(a+b)(∑k=0∞g(k)kzk−1)(∑i=0∞f(k)zk)\sum_{i=0}^{\infty} f(k) kz^{k-1}= a\left(\sum_{i=0}^{\infty} f(k) kz^{k-1}\right)\left(\sum_{k=0}^{\infty}g(k) z^k \right) + (a+b) \left(\sum_{k=0}^{\infty}g(k) kz^{k-1}\right)\left(\sum_{i=0}^{\infty} f(k) z^k \right)

and so for coefficient zk−1z^{k-1}, we will have f(k)kf(k)k on the left hand size and a∑i=0kf(i)ig(k−i)+(a+b)∑i=0kg(i)if(k−i)a\sum_{i=0}^k f(i)ig(k-i) +(a+b)\sum_{i=0}^kg(i) if(k-i)

and so the right hand side is the following:

a∑i=0kif(i)g(k−i)+(a+b)∑i=0k(k−i)g(k−i)f(i)=f(k)k  ⟹  a(∑i=0k−1if(i)g(k−i)+kf(k)g(0))+(a+b)∑i=0k−1(k−i)g(k−i)f(i)=f(k)k  ⟹  (1−ag(0))kf(k)=a∑i=0k−1if(i)g(k−i)+(a+b)∑i=0k−1(k−i)g(k−i)f(i)  ⟹  kf(k)=11−ag(0)∑i=0k−1(ai+(a+b)(k−i))g(k−i)f(i)=11−ag(0)∑i=0k−1(ak+b(k−i))g(k−i)f(i)a\sum_{i=0}^{k} i f(i)g(k-i) + (a+b) \sum_{i=0}^k (k-i)g(k-i)f(i)=f(k)k \\ \implies a \left(\sum_{i=0}^{k-1} i f(i)g(k-i)+kf(k)g(0)\right)+(a+b)\sum_{i=0}^{k-1} (k-i)g(k-i)f(i) = f(k)k \\ \implies (1-ag(0))kf(k) = a \sum_{i=0}^{k-1} i f(i) g(k-i) + (a+b) \sum_{i=0}^{k-1}(k-i)g(k-i)f(i) \\ \implies kf(k) = \frac{1}{1-ag(0)}\sum_{i=0}^{k-1} (ai +(a+b) (k-i)) g(k-i)f(i) \\=\frac{1}{1-ag(0)}\sum_{i=0}^{k-1} (ak +b(k -i)) g(k-i)f(i)

and so we will have

f(k)=11−ag(0)∑i=0k−1(a+b(k−i)k)g(k−i)f(i).f(k) = \frac{1}{1-ag(0)}\sum_{i=0}^{k-1} \left(a +\frac{b(k -i)}{k}\right) g(k-i)f(i).

For (a,b,1)(a,b,1) class, we will have

kPr⁡[N=k]=(ak+b)Pr⁡[N=k−1]k \Pr[N=k] = \left(ak+b\right)\Pr[N=k-1]

for k≥2k \ge 2 and so we will have the following

∑k=2∞kPr⁡[N=k]PM(z)k−1PM′(z)=∑k=2∞(ak−a+a+b)(PM(z))k−1PM′(z)Pr⁡[N=k−1]  ⟹  PS′(z)−Pr⁡[N=1]PM′(z)=aPM(z)PS′(z)+(a+b)PM′(z)(PS(z)−Pr⁡[N=0])\sum_{k=2}^{\infty} k \Pr[N=k] P_M(z)^{k-1} P_M'(z) = \sum_{k=2}^{\infty} (ak-a+a+b)(P_M(z))^{k-1} P_M'(z)\Pr[N=k-1] \\ \implies P_S'(z) -\Pr[N=1] P_M'(z) = a P_M(z) P_S'(z) +(a+b) P_M'(z) (P_S(z)-\Pr[N=0])

If we let PS(z)=∑i=0∞f(k)zkP_S(z) = \sum_{i=0}^{\infty} f(k) z^k and PM(z)=PM(z)=∑k=0∞g(k)zkP_M(z) = P_M(z) = \sum_{k=0}^{\infty}g(k) z^k, then we will have

f(k)k−p1kg(k)=a(∑i=0kif(i)g(k−i))+(a+b)∑i=0k−1(k−i)f(i)g(k−i)−(a+b)p0kg(k)f(k) k - p_1 kg(k)= a \left(\sum_{i=0}^k i f(i)g(k-i)\right)+(a+b)\sum_{i=0}^{k-1}(k-i)f(i)g(k-i)- (a+b) p_0 kg(k) f(k)k=(p1k−p0(a+b)k)g(k)+∑i=0k−1(ai+(a+b)(k−i))f(i)g(k−i)+akf(k)g(0)  ⟹  f(k)=(p1−p0(a+b))g(k)+∑i=0k−1(a+bk−ik)f(i)g(k−i)1−ag(0)f(k)k = (p_1k -p_0(a+b)k)g(k) + \sum_{i=0}^{k-1} (ai + (a+b)(k-i))f(i)g(k-i)+akf(k)g(0) \\ \implies f(k) = \frac{(p_1 -p_0(a+b))g(k) + \sum_{i=0}^{k-1} ( a+ b\frac{k -i}{k} )f(i)g(k-i)}{1-ag(0)}

So

f(k)=(p1−p0(a+b))g(k)+∑i=1k(a+bik)f(k−i)g(i)1−ag(0)f(k) = \frac{(p_1 -p_0(a+b))g(k) + \sum_{i=1}^{k} ( a+ b\frac{i}{k} )f(k-i)g(i)}{1-ag(0)}

Example. Develop the recursive formula for the case where the primary distribution is Poisson.

Recall that

 Distribution  A Bp0 Poisson 0λexp⁡(−λ) Negative Binomial β1+ββ1+β(r−1)(1+β)−r Binomial −q1−q(n+1)q1−q(1−q)n Geometric β1+β0(1+β)−1\begin{equation} \begin{array}{|c|c|c|c|} \hline \text { Distribution } & \text { A } & \text {B} & p_0 \\ \hline \text { Poisson } & 0 & \lambda & \exp(-\lambda) \\ \hline \text { Negative Binomial } & \frac{\beta}{1+\beta} & \frac{\beta}{1+\beta}(r-1) & (1+\beta)^{-r} \\ \hline \text { Binomial } & -\frac{q}{1-q} & (n+1)\frac{q}{1-q} & (1-q)^n \\ \hline \text { Geometric } & \frac{\beta}{1+\beta} & 0 & (1+\beta)^{-1} \\ \hline \end{array} \end{equation}

So we will have

f(k)=∑i=1kλikf(k−i)g(i)f(k) = \sum_{i=1}^{k} \frac{ \lambda i}{k} f(k-i)g(i)

With starting value

f(0)=PN(PM(0))=exp⁡(λ(PM(0)−1))f(0) = P_N(P_M(0)) = \exp(\lambda (P_M(0) -1)).

Calculate the probabilities for the Poisson-ETNB distribution, where λ=1\lambda=1 for the Poisson distribution and the ETNB distribution has r=−0.5r=-0.5 and β=1\beta=1.

Previously,

 Distribution  A Bp0 Poisson 0λexp⁡(−λ) Negative Binomial β1+ββ1+β(r−1)(1+β)−r Binomial −q1−q(n+1)q1−q(1−q)n Geometric β1+β0(1+β)−1\begin{equation} \begin{array}{|c|c|c|c|} \hline \text { Distribution } & \text { A } & \text {B} & p_0 \\ \hline \text { Poisson } & 0 & \lambda & \exp(-\lambda) \\ \hline \text { Negative Binomial } & \frac{\beta}{1+\beta} & \frac{\beta}{1+\beta}(r-1) & (1+\beta)^{-r} \\ \hline \text { Binomial } & -\frac{q}{1-q} & (n+1)\frac{q}{1-q} & (1-q)^n \\ \hline \text { Geometric } & \frac{\beta}{1+\beta} & 0 & (1+\beta)^{-1} \\ \hline \end{array} \end{equation} f(k)=∑i=1kikf(k−i)g(i)f(k) = \sum_{i=1}^{k} \frac{ i}{k} f(k-i)g(i) g(k)=(12−34k)g(k−1)g(k) =\left(\frac{1}{2} - \frac{3}{4k}\right) g(k-1)

The original "distribution" has the following:

g0(0)=(1+1)0.5=2g_0(0) = (1+1)^{0.5} = \sqrt{2} g0(1)=(12−1.52)⋅(1+1)0.5=−122g_0(1) = \left(\frac{1}{2} - \frac{1.5}{2}\right) \cdot (1+1)^{0.5} = -\frac{1}{2 \sqrt 2} g0(2)=−(12−38)122=−232g_0(2) = -(\frac{1}{2} - \frac{3}{8})\frac{1}{2 \sqrt 2}=-\frac{\sqrt 2}{32}

So it's more or less

g0(k)=(k−1.5k)(12)k−0.5=Γ(k−1.5+1)Γ(k+1)Γ(−0.5)(12)k−0.5g_0(k) = {k -1.5 \choose k} \left(\frac{1}{2}\right)^{k-0.5} = \frac{\Gamma(k-1.5+1)}{\Gamma(k+1) \Gamma(-0.5)}\left(\frac{1}{2}\right)^{k-0.5}

Notice that g0(2)=Γ(1.5)Γ(2)Γ(−0.5)(12)2−0.5=−132(12)−0.5=−232g_0(2) = \frac{\Gamma(1.5)}{\Gamma(2) \Gamma(-0.5)} \left(\frac{1}{2}\right)^{2-0.5} = -\frac{1}{32 } \left(\frac{1}{2}\right)^{-0.5} = -\frac{\sqrt 2}{32}, which matches. And so back to the problem, we will have

g(k)=11−2Γ(k−0.5)Γ(k+1)Γ(−0.5)(12)k−0.5g(k) = \frac{1}{1-\sqrt{2}}\frac{\Gamma(k-0.5)}{\Gamma(k+1) \Gamma(-0.5)} \left(\frac{1}{2}\right)^{k-0.5}

So we will have recursive formula as

f(k)=∑i=1kikf(k−i)g(i)=∑i=1kik21−2Γ(i−0.5)Γ(i+1)Γ(−0.5)(12)if(k−i)f(k) = \sum_{i=1}^{k} \frac{ i}{k} f(k-i)g(i) \\ = \sum_{i=1}^{k} \frac{ i}{k} \frac{\sqrt{2}}{1-\sqrt{2}}\frac{\Gamma(i-0.5)}{\Gamma(i+1) \Gamma(-0.5)} \left(\frac{1}{2}\right)^{i}f(k-i)

which we can't find a closed form for now.

Example. Show that the Poisson-logarithmic distribution is a negative binomial distribution.

The logarithmic distribution has the following pgf:

ln⁡(1−pz)ln⁡(1−p)\frac{\ln (1-p z)}{\ln (1-p)}

Notice here pp is constant.

And Poisson distribution has the following pgf:

exp⁡(λ(z−1))\exp(\lambda (z-1))

and so if we have them composed, we will have the following compound pgf:

exp⁡(λ(ln⁡(1−pz)ln⁡(1−p)−1))=exp⁡(λln⁡((1−pz)/(1−p))ln⁡(1−p))=(1−p+p−pz1−p)λ/ln⁡(1−p)=(1−p1−p(z−1))λ/ln⁡(1−p)\exp\left(\lambda\left(\frac{\ln(1-pz)}{\ln(1-p)} - 1\right)\right) = \exp\left(\lambda \frac{\ln((1-pz)/(1-p))}{\ln(1-p)}\right) \\= \left(\frac{1-p+p-pz }{1-p}\right)^{\lambda/ \ln(1-p)} = \left(1-\frac{p}{1-p}(z-1)\right)^{\lambda/ \ln(1-p)}

which is a negative binomial distribution with r=−λ/ln⁡(1−p)r=-\lambda/ \ln(1-p) and β=p1−p\beta=\frac{p}{1-p}.

We can know from the previous discussion:

PM(z)=p0(M)+(1−p0(M))pT(z)P^M(z)=p_0^{(M)}+\left(1-p_0^{(M)}\right) p^T(z)

So we can always write a general pgf as

P(z)=f0+(1−f0)PT(z).P(z) = f_0 +(1-f_0)P^T(z).

Theorem Here's a relationship between probability generating functions (pgfs) in a specific scenario. Suppose we have a pgf denoted by PM(z;θ)P_M(z ; \theta) that satisfies the equation:

PN(z;θ)=B[θ(z−1)]P_N(z ; \theta) = B[\theta(z-1)]

Here, θ\theta represents a parameter, and B(z)B(z) is a function that doesn't depend on θ\theta. Notably, the pgf contains θ\theta and zz solely in the form of θ(z−1)\theta(z-1).

In such a situation, we can rewrite the pgf PS(z)P_S(z) as a composition of pgfs, which is given by:

PS(z)=PN[PM(z);θ]P_S(z) = P_N[P_M(z) ; \theta] \quad

The new pgf PS(z)P_S(z) can also be expressed differently by using a zero-truncated pgf PMT(z)P_M^T(z) and a modified parameter θ(1−f0)\theta\left(1-f_0\right), leading to the following alternative expression:

PS(z)=PN[PMT(z);θ(1−f0)]P_S(z) = P_N[P_M^T(z) ; \theta\left(1-f_0\right)] \quad

Proof.

We know that PN(PM(z);θ)=B[θ(PM(z)−1)]=B[θ(f0+(1−f0)PMT(z)−1)]=B[θ(1−f0)PMT(z)−(1−f0)θ]=B[θ(1−f0)(PMT(z)−1)]=PN[PMT(z);θ(1−f0)].P_N(P_M(z) ; \theta) = B[\theta(P_M(z) -1)] = B[\theta (f_0 + (1-f_0)P_M^T(z)-1)] = B[\theta (1-f_0)P_M^T(z) -(1-f_0)\theta] = B[\theta(1-f_0)(P_M^T(z)-1)] = P_N[P_M^T(z);\theta(1-f_0)].

Determine the probabilities for a Poisson-zero-modified ETNB distribution where the parameters are λ,p0M,r,β\lambda, p_0^M, r, \beta

f(k)=λk∑i=1k(i)f(k−i)g(i)1−P0M⋅0=λk∑i=1k(i)f(k−i)g(i)f(k) = \frac{\lambda}{k}\frac{ \sum_{i=1}^{k} ( i )f(k-i)g(i)}{1-P_0^M \cdot 0} = \frac{\lambda}{k} \sum_{i=1}^{k} ( i )f(k-i)g(i)

and

g(i)=1−p0M1−(1+β)−rΓ(i+r)Γ(i+1)Γ(r)(11+β)r(ββ+1)i=1−p0M(1+β)r−1Γ(i+r)Γ(i+1)Γ(r)(ββ+1)ig(i) = \frac{1-p_0^M}{1-(1+\beta)^{-r}} \frac{\Gamma(i +r)}{\Gamma(i+1) \Gamma(r)} \left( \frac{1}{1+\beta}\right)^r\left( \frac{\beta}{\beta+1}\right)^i \\=\frac{1-p_0^M}{(1+\beta)^{r}-1} \frac{\Gamma(i +r)}{\Gamma(i+1) \Gamma(r)} \left( \frac{\beta}{\beta+1}\right)^i

And so

f(k)=λk∑i=1kif(k−i)1−p0M1−(1+β)−rΓ(i+r)Γ(i+1)Γ(r)(11+β)r(ββ+1)i=λk∑i=1kif(k−i)1−p0M(1+β)r−1Γ(i+r)Γ(i+1)Γ(r)(ββ+1)if(k) = \frac{\lambda}{k} \sum_{i=1}^{k} if(k-i)\frac{1-p_0^M}{1-(1+\beta)^{-r}} \frac{\Gamma(i +r)}{\Gamma(i+1) \Gamma(r)} \left( \frac{1}{1+\beta}\right)^r\left( \frac{\beta}{\beta+1}\right)^i \\=\frac{\lambda}{k} \sum_{i=1}^{k} if(k-i)\frac{1-p_0^M}{(1+\beta)^{r}-1} \frac{\Gamma(i +r)}{\Gamma(i+1) \Gamma(r)} \left( \frac{\beta}{\beta+1}\right)^i

and f(0)=exp⁡(p0M−λ).f(0) = \exp(p_0^M-\lambda).

Compound Poisson Class

Compound Poisson distributions are type of distributions satisfying the following:

PS(z)=exp⁡(λ(PM(z)−1))P_S(z) = \exp(\lambda(P_M(z)-1))

where PM(z)P_M(z) is some other distribution.

Let's consider its moment generating function:

PS(exp⁡(z))=exp⁡(λ(PM(exp⁡(z))−1))P_S(\exp(z)) = \exp(\lambda(P_M(\exp(z))-1))

If we differentiate with respect to zz, we will have

PS′(exp⁡(z))exp⁡(z)=exp⁡(λPM(exp⁡(z))−λ)λPM′(exp⁡(z))exp⁡(z)P_S'(\exp(z)) \exp(z) = \exp(\lambda P_M(\exp(z))-\lambda) \lambda P_M'(\exp(z)) \exp(z)

So the first (central) moment will have

ES[S]=λEM[M]\mathbb{E}_S[S] = \lambda\mathbb{E}_M[M]

If we differentiate it twice, we will have

PS′′(exp⁡(z))exp⁡(z)2+PS′(exp⁡(z))exp⁡(z)=exp⁡(λPM(exp⁡(z))−λ)λ2PM′(exp⁡(z))2exp⁡(z)2+exp⁡(λPM(exp⁡(z))−λ)λPM′′(exp⁡(z))exp⁡(z)2+exp⁡(λPM(exp⁡(z))−λ)λPM′(exp⁡(z))exp⁡(z)P_S''(\exp(z)) \exp(z)^2 + P_S'(\exp(z)) \exp(z) = \exp(\lambda P_M(\exp(z))-\lambda) \lambda^2 P_M'(\exp(z))^2 \exp(z)^2 + \exp(\lambda P_M(\exp(z))-\lambda) \lambda P_M''(\exp(z)) \exp(z)^2+ \exp(\lambda P_M(\exp(z))-\lambda) \lambda P_M'(\exp(z)) \exp(z)

Then we will have

ES[S2]+ES[S]=λ2EM[M]2+λEM[M2]+λEM[M]\mathbb{E}_S[S^2] + \mathbb{E}_S[S] = \lambda^2 \mathbb{E}_M[M]^2 +\lambda \mathbb{E}_M[M^2] + \lambda \mathbb{E}_M[M]

It means that

ES[S2]=λ2EM[M]2+λEM[M2]\mathbb{E}_S[S^2] = \lambda^2 \mathbb{E}_M[M]^2 +\lambda \mathbb{E}_M[M^2]

So the central moment is

ES[S2]−(ES[S])2=λEM[M2].\mathbb{E}_S[S^2] - (\mathbb{E}_S[S])^2= \lambda \mathbb{E}_M[M^2].

The formula are growing exponentially complicated, let's see an alternative approach:

PS′(z)=exp⁡(λPM(z)−λ)λPM′(z)P_S'(z) = \exp(\lambda P_M(z)-\lambda) \lambda P_M'(z) PS′′(z)=exp⁡(λPM(z)−λ)λ2PM′(z)2+exp⁡(λPM(z)−λ)λPM′′(z)P_S''(z) = \exp(\lambda P_M(z)-\lambda) \lambda^2 P_M'(z)^2 + \exp(\lambda P_M(z)-\lambda) \lambda P_M''(z) PS′′′(z)=exp⁡(λPM(z)−λ)λ3PM′(z)3+2exp⁡(λPM(z)−λ)λ2PM′′(z)PM′(z)+exp⁡(λM(z)−λ)λ2PM′′(z)PM′(z)+exp⁡(λPM(z)−λ)λPM′′′(z).P_S'''(z) = \exp(\lambda P_M(z) - \lambda)\lambda^3 P_M'(z)^3 + 2\exp(\lambda P_M(z)-\lambda)\lambda^2 P''_M(z)P_M'(z) + \exp(\lambda_M(z)-\lambda)\lambda^2 P_M''(z)P_M'(z) + \exp(\lambda P_M(z)-\lambda)\lambda P_M'''(z).

If we set zz to be 1, we will have

EN[N(N−1)(N−2)]=λ3EM[M]3+2λ2EM[M(M−1)]+λ2EM[M(M−1)]EM[M]+λEM[M(M−1)(M−2)].\mathbb{E}_N[N(N-1)(N-2)] = \lambda^3 \mathbb{E}_M[M]^3 + 2 \lambda^2 \mathbb{E}_M[M(M-1)]+\lambda^2 \mathbb{E}_M[M(M-1)] \mathbb{E}_M[M] + \lambda \mathbb{E}_M[M(M-1)(M-2)].

Notice that

PX(z)=∑k=0∞pkzkP_X(z) = \sum_{k=0}^{\infty}p_k z^k

and if we differentiate nn-times, we will have

∂∂znPX(z)∣z=1=∑k=n∞pkk!(k−n)!zk−n∣z=1=E[P(K,n)]\frac{\partial}{\partial z^n}P_X(z)\bigg |_{z=1} = \sum_{k=n}^{\infty} p_k \frac{k!}{(k-n)!} z^{k-n}|_{z=1} = \mathbb{E}[P(K, n) ]

N(N−1)=N2−NN(N-1)= N^2 - N and N(N−1)(N−2)=(N2−N)(N−2)=N3−N2−2N2+2N=N3−3N2+2NN(N-1)(N-2) = (N^2 -N)(N-2) = N^3 -N^2 - 2N^2 +2N = N^3 - 3N^2 +2N

So

EN[N3]−3EN[N2]+2EN[N]=λ3EM[M]3+2λ2(EM[M2]−EM[M])+λ2(EM[M2]−EM[M])EM[M]+λ(EM[M3]−3EM[M2]+2EM[M]).\mathbb{E}_N[N^3] - 3\mathbb{E}_N[N^2] +2\mathbb{E}_N[N] = \lambda^3 \mathbb{E}_M[M]^3 + 2 \lambda^2 (\mathbb{E}_M[M^2] - \mathbb{E}_M[M])+\lambda^2 (\mathbb{E}_M[M^2] - \mathbb{E}_M[M]) \mathbb{E}_M[M] + \lambda (\mathbb{E}_M[M^3] - 3\mathbb{E}_M[M^2] +2\mathbb{E}_M[M]).

We also know that

EN[(N−E[N])3]=EN[N3−3E[N]N2+3EN[N]2N−EN[N]3]\mathbb{E}_N[(N-\mathbb{E}[N])^3] = \mathbb{E}_N[N^3 - 3\mathbb{E}[N]N^2+3 \mathbb{E}_N[N]^2 N -\mathbb{E}_N[N]^3] EN[N3]−3EN[N]E[N2]+3EN[N]2EN[N]+EN[N]3=λ3EM[M]3+2λ2(EM[M2]−EM[M])+λ2(EM[M2]−EM[M])EM[M]+λ(EM[M3]−3EM[M2]+2EM[M])+3EN[N2]−2EN[N]−3EN[N]E[N2]+3EN[N]2EN[N]+EN[N]3\mathbb{E}_N[N^3] -3 \mathbb{E}_N[N]\mathbb{E}[N^2] + 3 \mathbb{E}_N[N]^2 \mathbb{E}_N[N] + \mathbb{E}_N[N]^3 = \lambda^3 \mathbb{E}_M[M]^3 + 2 \lambda^2 (\mathbb{E}_M[M^2] - \mathbb{E}_M[M])+\lambda^2 (\mathbb{E}_M[M^2] - \mathbb{E}_M[M]) \mathbb{E}_M[M] + \lambda (\mathbb{E}_M[M^3] - 3\mathbb{E}_M[M^2] +2\mathbb{E}_M[M]) + 3\mathbb{E}_N[N^2] -2\mathbb{E}_N[N]-3 \mathbb{E}_N[N]\mathbb{E}[N^2] + 3 \mathbb{E}_N[N]^2 \mathbb{E}_N[N] + \mathbb{E}_N[N]^3 EN[N3]−3EN[N]E[N2]+3EN[N]2EN[N]−EN[N]3=2λ2(EM[M2]−EM[M])+λ2(EM[M2]−EM[M])EM[M]+λ(EM[M3]−3EM[M2])+3EN[N2]−3EN[N]E[N2]+3EN[N]2EN[N]\mathbb{E}_N[N^3] -3 \mathbb{E}_N[N]\mathbb{E}[N^2] + 3 \mathbb{E}_N[N]^2 \mathbb{E}_N[N] - \mathbb{E}_N[N]^3 = 2 \lambda^2 (\mathbb{E}_M[M^2] - \mathbb{E}_M[M])+\lambda^2 (\mathbb{E}_M[M^2] - \mathbb{E}_M[M]) \mathbb{E}_M[M] + \lambda (\mathbb{E}_M[M^3] - 3\mathbb{E}_M[M^2]) + 3\mathbb{E}_N[N^2] -3 \mathbb{E}_N[N]\mathbb{E}[N^2] + 3 \mathbb{E}_N[N]^2 \mathbb{E}_N[N] =2λ2EM[M2]−2λ2EM[M]+λ2EM[M2]EM[M]−λ2EM[M]2+λEM[M3]−3λEM[M2]+3EN[N2]−3EN[N]E[N2]+3λ3EM[M]3= 2\lambda^2\mathbb{E}_M[M^2]-2\lambda^2\mathbb{E}_M[M]+\lambda^2\mathbb{E}_M[M^2] \mathbb{E}_M[M]-\lambda^2\mathbb{E}_M[M]^2+\lambda\mathbb{E}_M[M^3]-3\lambda\mathbb{E}_M[M^2]+ 3\mathbb{E}_N[N^2] -3 \mathbb{E}_N[N]\mathbb{E}[N^2] + 3 \lambda^3 \mathbb{E}_M[M]^3

Since we already know that

EN[N2]=λ2EM[M]2+λEM[M2]\mathbb{E}_N[N^2] = \lambda^2 \mathbb{E}_M[M]^2 +\lambda \mathbb{E}_M[M^2]

We will have

3EN[N2]EN[N]=3λEM[M](λ2EM[M]2+λEM[M2])3\mathbb{E}_N[N^2]\mathbb{E}_N[N] = 3 \lambda \mathbb{E}_M[M](\lambda^2 \mathbb{E}_M[M]^2 +\lambda \mathbb{E}_M[M^2])

So the old equation equals to

2λ2EM[M2]−2λ2EM[M]−2λ2EM[M2]EM[M]+λEM[M3]+2λ2EM[M]22\lambda^2\mathbb{E}_M[M^2]-2\lambda^2\mathbb{E}_M[M]-2\lambda^2\mathbb{E}_M[M^2] \mathbb{E}_M[M]+\lambda\mathbb{E}_M[M^3]+ 2\lambda^2 \mathbb{E}_M[M]^2

Ah life is so much difficult and the above to get the third central moment isn't even correct.

Let's do something truly innovative.

Let's define Sk=E[Sk]S_k = \mathbb{E}[S^k] for k≥1k \ge 1 and the same definition for MM.

Then we will have S=λMS = \lambda M, here we omit 11 for the sake of simplicity and we know the numerical interpretation and probability interpretation are different.

PS′′(z)=eλ(PM(z)−1)λ2(PM′(z))2+λeλ(PM(z)−1)PM′′(z)P_S''(z) = e^{\lambda(P_M(z)-1)} \lambda^2 (P_M'(z))^2 + \lambda e^{\lambda(P_M(z)-1)}P_M''(z)

which means S2=λ2M2+λM2S_2 = \lambda^2 M^2 + \lambda M_2

And if we differentiate, we will get

PS′′′(z)=eλ(PM(z)−1)λ3(PM′(z))3+2(eλ(PM(z)−1)λ2(PM′(z))PM′′(z))+λ2eλ(PM(z)−1)PM′(z)PM′′(z)+λeλ(PM(z)−1)PM′′′(z)P_S'''(z) = e^{\lambda(P_M(z)-1)} \lambda^3 (P_M'(z))^3 +2(e^{\lambda(P_M(z)-1)} \lambda^2 (P_M'(z))P_M''(z)) + \lambda^2 e^{\lambda(P_M(z)-1)}P_M'(z)P_M''(z) + \lambda e^{\lambda(P_M(z)-1)}P_M'''(z)

And so we will have

S3−3S2+2S=λ3M3+2λ2M(M2−M)+λ2M(M2−M)+λ(M3−3M2+2M)=λ3M3+2λ2MM2−2λ2M2+λ2MM2−λ2M2+λM3−3λM2+2λM=λ3M3+3λ2MM2−3λ2M2+λM3−3λM2+2λMS_3-3S_2 +2 S = \lambda^3 M^3 + 2 \lambda^2 M(M_2 -M) + \lambda^2 M (M_2 -M)+\lambda (M_3 - 3M_2 + 2M)\\ = \lambda^3 M^3 +2\lambda^2 MM_2 -2\lambda^2 M^2 +\lambda^2 MM_2 -\lambda^2 M^2 +\lambda M_3 -3\lambda M_2 +2\lambda M\\ = \lambda^3 M^3 +3\lambda^2 MM_2 -3\lambda^2 M^2 +\lambda M_3 -3\lambda M_2 +2\lambda M S3=λ3M3+3λ2MM2+λM3S_3 = \lambda^3 M^3 +3\lambda^2 MM_2 +\lambda M_3 S3−3S2S+2S3=λ3M3+3λ2MM2+λM3−3λM(λ2M2+λM2)+2λ3M3=λM3S_3 -3 S_2 S +2S^3 = \lambda^3 M^3 +3\lambda^2 MM_2 +\lambda M_3 - 3 \lambda M(\lambda^2 M^2 +\lambda M_2) +2\lambda^3 M^3 = \lambda M_3

And so the third central moment of the compound distribution is lambda times the third raw moment of the secondary distribution.

The coefficient of skewness is

γ1=S3−3S3S+2S3(S2−S2)3/2=λM3λ3/2M23/2=M3λ1/2M23/2.\gamma_1 = \frac{S_3 -3S_3 S + 2 S^3}{(S_2 -S^2)^{3/2}} = \frac{\lambda M_3}{\lambda^{3/2}M_2^{3/2}} = \frac{M_3}{\lambda^{1/2} M_2^{3/2}}.

If the underlying secondary distribution is a binomial distribution, specifically, binomial distribution has the following MGF:

f(z)=(1+q(exp⁡(z)−1))n.f(z)=(1+q(\exp(z)−1))^n.

If we take derivative, we will get

∂∂zf(z)=n(1+q(exp⁡(z)−1))n−1qexp⁡(z)\frac{\partial}{\partial z} f(z) = n (1 + q(\exp(z)-1))^{n-1} q \exp(z)

and so S=λnqS=\lambda n q.

If we take derivative again, we will get

∂∂z2f(z)=n(n−1)(1+q(exp⁡(z)−1))n−2q2exp⁡(z)2+n(1+q(exp⁡(z)−1))n−1qexp⁡(z)\frac{\partial}{\partial z^2 } f(z) = n(n-1)(1+q(\exp(z)-1))^{n-2} q^2 \exp(z)^2 + n (1 + q(\exp(z)-1))^{n-1} q \exp(z)

and so S2=λ(n(n−1)q2+nq)=λnq(1+(n−1)q)=S(1+(n−1)q)S_2 = \lambda (n(n-1)q^2 +nq) = \lambda nq(1+(n-1)q) = S (1+(n-1)q)

And if we take another derivative, we will have

∂∂z3f(z)=n(n−1)(n−2)(1+q(exp⁡(z)−1))n−3q3exp⁡(3z)+2n(n−1)(1+q(exp⁡(z)−1))n−2q2exp⁡(2z)+n(n−1)(1+q(exp⁡(z)−1))n−2q2exp⁡(2z)+n(1+q(exp⁡(z)−1))n−1qexp⁡(z)\frac{\partial}{\partial z^3 } f(z) = n(n-1)(n-2)(1+q(\exp(z)-1))^{n-3} q^3 \exp(3z) + 2n(n-1)(1+q(\exp(z)-1))^{n-2} q^2 \exp(2z)+\\ n(n-1)(1+q(\exp(z)-1))^{n-2}q^2\exp(2z) +n (1 + q(\exp(z)-1))^{n-1} q \exp(z)

So we will have

M3=n(n−1)(n−2)q3+2n(n−1)q2+n(n−1)q2+nq=n(n−1)(n−2)q3+3n(n−1)q2+nqM_3 = n(n-1)(n-2) q^3 + 2n(n-1)q^2 +n(n-1)q^2 +nq \\= n(n-1)(n-2) q^3 + 3n(n-1)q^2 +nq

So notice M2−M=M((n−1)q)M_2 -M = M((n-1)q) so (M2−M)2=M2(n−1)2q2(M_2 - M)^2 = M^2 (n-1)^2 q^2

So M3=M(n−1)(n−2)q2+3n(n−1)q2+3nq−2nq=M⋅(M2−M)2M2⋅n−2n−1+3M2−2M=(M2−M)2M⋅n−2n−1+3M2−2M.M_3 =M (n-1)(n-2)q^2 + 3n(n-1)q^2 +3nq - 2nq = M \cdot \frac{(M_2-M)^2}{M^2} \cdot \frac{n-2}{n-1} +3M_2-2M = \frac{(M_2-M)^2}{M} \cdot \frac{n-2}{n-1}+3M_2 -2M.

Now we consider the following example:

Obtain the pgf for the Poisson-ETNB distribution and show that it looks like the pgf of a Poisson-negative binomial distribution.

Recall that ETNB has the following pgf:

f(z)=1(1+β)r−1((1+β1−β(z−1))r−1)=11−(1+β)−r((1−β(z−1))−r−(1+β)−r).f(z)=\frac{1}{(1+\beta)^r-1}\left(\left(\frac{1+\beta}{1-\beta(z-1)}\right)^r-1\right) = \frac{1}{1-(1+\beta)^{-r}} \left((1-\beta(z-1))^{-r}-(1+\beta)^{-r}\right).

So the Possion-ETNB distribution will have the following pgf:

eλ(f(z)−1)e^{\lambda (f(z)-1)}

If we take ln, we will have

λ(f(z)−1)=λ(11−(1+β)−r((1−β(z−1))−r−(1+β)−r−1+(1+β)−r))=λ(1−β(z−1))−r−11−(1+β)−r=C((1−β(z−1))−r−1)\lambda (f(z)-1)= \lambda \left(\frac{1}{1-(1+\beta)^{-r}} \left((1-\beta(z-1))^{-r}-(1+\beta)^{-r}-1+(1+\beta)^{-r}\right)\right)= \lambda \frac{(1-\beta(z-1))^{-r}-1}{1-(1+\beta)^{-r}}\\= C ( (1-\beta(z-1))^{-r}-1)

So we have proven our example.