A compound distribution S S S of a primary distribution with pgf P N ( z ) P_N(z) P N ( z ) and secondary distribution with pgf P M ( z ) P_M(z) P M ( z ) has the following probability generating function:
P S ( z ) = P N ( P M ( z ) ) P_S(z)=P_N(P_M(z)) P S ( z ) = P N ( P M ( z ))
Recall our relation between moment generating function that
M X ( t ) = P X ( e t ) M_X(t) = P_X(e^t) M X ( t ) = P X ( e t )
for any distribution X X X so we will have
M S ( z ) = P S ( e z ) = P N ( P M ( e z ) ) = P N ( M M ( z ) ) . M_S(z) = P_S(e^z) = P_N(P_M(e^z)) = P_N(M_M(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 A 1 , A 2 , . . . , A n A_1, A_2, ..., A_n A 1 , A 2 , ... , A n , where the number n n n itself is also a random variable independent of A 1 , . . . , A n A_1, ... ,A_n A 1 , ... , A n so we will have
the pgf of A 1 + A 2 + . . . + A n A_1+A_2 +...+A_n A 1 + A 2 + ... + A n as
∑ i = 0 ∞ Pr [ A 1 + A 2 + . . . + A N = i ] z i \sum_{i=0}^{\infty}\Pr[A_1 + A_2 +... +A_N = i ]z^i i = 0 ∑ ∞ Pr [ A 1 + A 2 + ... + A N = i ] z i
by conditioning over N N N , we will have
∑ i = 0 ∞ ∑ n = 0 ∞ Pr [ N = n ] Pr [ A 1 + A 2 + . . . + A n = i ∣ N = n ] z i = ∑ n = 0 ∞ Pr [ N = n ] ∑ i = 0 ∞ A 1 + A 2 + . . . + A n = i ∣ N = n ] z i = ∑ n = 0 ∞ Pr [ N = n ] ( P A ( z ) ) n = P N ( P A ( 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)) i = 0 ∑ ∞ n = 0 ∑ ∞ Pr [ N = n ] Pr [ A 1 + A 2 + ... + A n = i ∣ N = n ] z i = n = 0 ∑ ∞ Pr [ N = n ] i = 0 ∑ ∞ A 1 + A 2 + ... + A n = i ∣ N = n ] z i = n = 0 ∑ ∞ Pr [ N = n ] ( P A ( z ) ) n = P N ( P A ( z ))
Example \textbf{Example } Example Demonstrate that any zero-modified distribution is a compound distribution.
Recall that p k M = c p k 0 p_k^M = cp_k^0 p k M = c p k 0 , where p k p_k p k is the probability for zero modified distribution and p k 0 p_k^0 p k 0 is the probability of zero-truncated distribution for k ≥ 1 k \ge 1 k ≥ 1 .
Then we will have the following relation for the pgf:
p M ( z ) = p 0 M + c ∑ k = 1 ∞ p k 0 z k = p 0 M + c ( P ( z ) − p 0 0 ) p^M(z) = p_0^M + c\sum_{k=1}^{\infty} p^0_kz^k=p_0^M + c(P(z) - p_0^0) p M ( z ) = p 0 M + c k = 1 ∑ ∞ p k 0 z k = p 0 M + c ( P ( z ) − p 0 0 )
If we set z z z to be 1 1 1 , then we will have
1 = p 0 M + c ( 1 − p 0 0 ) ⟹ c = 1 − p 0 M 1 − p 0 0 1 = p_0^M + c(1-p_0^0) \implies c =\frac{1-p_0^M}{1-p_0^0} 1 = p 0 M + c ( 1 − p 0 0 ) ⟹ c = 1 − p 0 0 1 − p 0 M
and so
− 1 − p 0 M 1 − p 0 0 ⋅ p 0 0 + p 0 M = p 0 M − p 0 M p 0 0 − p 0 0 + p 0 M p 0 0 1 − p 0 0 = 1 − 1 − p 0 M 1 − p 0 0 -\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} − 1 − p 0 0 1 − p 0 M ⋅ p 0 0 + p 0 M = 1 − p 0 0 p 0 M − p 0 M p 0 0 − p 0 0 + p 0 M p 0 0 = 1 − 1 − p 0 0 1 − p 0 M
and so we will have Bernoulli distribution with parameter 1 − p 0 M 1 − p 0 0 \frac{1-p_0^M}{1-p_0^0} 1 − p 0 0 1 − p 0 M as primary distribution and a zero modified distribution as a secondary distribution.
Example \textbf{Example } Example
Consider the case where both M M M and N N N have a Poisson distribution, λ 1 , λ 2 \lambda_1, \lambda_2 λ 1 , λ 2 . Determine the pgf of this distribution.
We know that Poisson distribution X X X with parameter λ \lambda λ has the following probability generating function:
P X ( z ) = exp ( λ ( z − 1 ) ) P_{X}(z) = \exp(\lambda(z-1)) P X ( z ) = exp ( λ ( z − 1 ))
And so by the definition of compound distribution, we will have
P S ( z ) = P M ( P N ( z ) ) = P M ( exp ( λ 2 ( z − 1 ) ) ) = exp ( λ 1 ( e λ 2 ( 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)). P S ( z ) = P M ( P N ( z )) = P M ( exp ( λ 2 ( z − 1 ))) = exp ( λ 1 ( e λ 2 ( z − 1 ) − 1 )) .
Back to our previous discussion, the probability of A 1 + A 2 + . . . + A n = k A_1 +A_2 +...+A_n =k A 1 + A 2 + ... + A n = k can be written as
Pr [ A 1 + A 2 + . . . + A N = k ] = ∑ n = 0 ∞ Pr [ A 1 + A 2 + . . . + A n = 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] Pr [ A 1 + A 2 + ... + A N = k ] = n = 0 ∑ ∞ 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 ] = p n \Pr[N=n] = p_n Pr [ N = n ] = p n and Pr [ A = k ] = q k \Pr[A =k] = q_k Pr [ A = k ] = q k
Then we have
Pr [ A 1 + A 2 + . . . + A N = k ] = ∑ n = 0 ∞ p n q k ∗ n . \Pr[A_1+A_2 +...+A_N = k] = \sum_{n=0}^{\infty} p_n q_k^{*n}. Pr [ A 1 + A 2 + ... + A N = k ] = n = 0 ∑ ∞ p n q k ∗ n .
If the primary distribution N N N is of ( a , b , 0 ) (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) ( a , b , 0 ) class has the following recursive formula:
k Pr [ N = k ] = ( a k + b ) Pr [ N = k − 1 ] . k \Pr[N=k] = \left(ak+b\right)\Pr[N=k-1]. k Pr [ N = k ] = ( ak + b ) Pr [ N = k − 1 ] .
We want to know about P S ( z ) = P N ( P M ( z ) ) = ∑ i = 0 ∞ Pr [ N = k ] ( P M ( z ) ) k P_S(z) = P_N(P_M(z)) = \sum_{i=0}^{\infty}\Pr[N=k](P_M(z))^k P S ( z ) = P N ( P M ( z )) = ∑ i = 0 ∞ Pr [ N = k ] ( P M ( z ) ) k . And so if we multiply the recursive formula both sides with ( P M ( z ) ) k (P_M(z))^k ( P M ( z ) ) k and do the summation we will have
k ∑ k = 1 ∞ Pr [ N = k ] ( P M ( z ) ) k = ( a k + b ) ∑ k = 1 ∞ Pr [ N = k − 1 ] ( P M ( z ) ) k ⟹ k ( P S ( z ) − p 0 ) = ( a k + b ) P M ( z ) P S ( 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) k k = 1 ∑ ∞ Pr [ N = k ] ( P M ( z ) ) k = ( ak + b ) k = 1 ∑ ∞ Pr [ N = k − 1 ] ( P M ( z ) ) k ⟹ k ( P S ( z ) − p 0 ) = ( ak + b ) P M ( z ) P S ( z )
,
which we can't conclude anything.
However, if we differentiate P S ′ ( z ) P_S'(z) P S ′ ( z ) by taking into account the method of moment, we will have P S ′ ( z ) = P N ′ ( P M ( z ) ) P M ′ ( z ) = ∑ i = 0 ∞ k ⋅ Pr [ N = k ] ( P M ( z ) ) k − 1 P M ′ ( 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) P S ′ ( z ) = P N ′ ( P M ( z )) P M ′ ( z ) = ∑ i = 0 ∞ k ⋅ Pr [ N = k ] ( P M ( z ) ) k − 1 P M ′ ( z ) and so we will have
∑ k = 1 ∞ k Pr [ N = k ] ( P M ( z ) ) k − 1 P M ′ ( z ) = ∑ k = 1 ∞ ( a k + b ) Pr [ N = k − 1 ] ( P M ( z ) ) k − 1 P M ′ ( z ) ⟹ P S ′ ( z ) = ∑ k = 1 ∞ ( a k − a + a + b ) Pr [ N = k − 1 ] ( P M ( z ) ) k − 1 P M ′ ( z ) ⟹ P S ′ ( z ) = ( P M ( z ) ) ∑ k = 1 ∞ a ( k − 1 ) Pr [ N = k − 1 ] ( P M ( z ) ) k − 2 P M ′ ( z ) + ( a + b ) ∑ k = 1 ∞ Pr [ N = k − 1 ] ( P M ( z ) ) k − 1 P M ′ ( z ) ⟹ P S ′ ( z ) = ( P M ( z ) ) ∑ k = 0 ∞ a k Pr [ N = k ] ( P M ( z ) ) k − 1 P M ′ ( z ) + ( a + b ) P M ′ ( z ) P N ( P M ( z ) ) ⟹ P S ′ ( z ) = a P M ( z ) P S ′ ( z ) + ( a + b ) P M ′ ( z ) P S ( 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) k = 1 ∑ ∞ k Pr [ N = k ] ( P M ( z ) ) k − 1 P M ′ ( z ) = k = 1 ∑ ∞ ( ak + b ) Pr [ N = k − 1 ] ( P M ( z ) ) k − 1 P M ′ ( z ) ⟹ P S ′ ( z ) = k = 1 ∑ ∞ ( ak − a + a + b ) Pr [ N = k − 1 ] ( P M ( z ) ) k − 1 P M ′ ( z ) ⟹ P S ′ ( z ) = ( P M ( z )) k = 1 ∑ ∞ a ( k − 1 ) Pr [ N = k − 1 ] ( P M ( z ) ) k − 2 P M ′ ( z ) + ( a + b ) k = 1 ∑ ∞ Pr [ N = k − 1 ] ( P M ( z ) ) k − 1 P M ′ ( z ) ⟹ P S ′ ( z ) = ( P M ( z )) k = 0 ∑ ∞ ak Pr [ N = k ] ( P M ( z ) ) k − 1 P M ′ ( z ) + ( a + b ) P M ′ ( z ) P N ( P M ( z )) ⟹ P S ′ ( z ) = a P M ( z ) P S ′ ( z ) + ( a + b ) P M ′ ( z ) P S ( z )
And so we will also have
P S ( z ) = ∑ i = 0 ∞ f ( k ) z k ⟹ P S ′ ( z ) = ∑ i = 0 ∞ f ( k ) k z k − 1 P_S(z) = \sum_{i=0}^{\infty} f(k) z^k \\ \implies P_S'(z) = \sum_{i=0}^{\infty} f(k) kz^{k-1} P S ( z ) = i = 0 ∑ ∞ f ( k ) z k ⟹ P S ′ ( z ) = i = 0 ∑ ∞ f ( k ) k z k − 1
and we also have
P M ( z ) = ∑ k = 0 ∞ g ( k ) z k ⟹ P M ′ ( z ) = ∑ k = 0 ∞ g ( k ) k z k − 1 P_M(z) = \sum_{k=0}^{\infty}g(k) z^k \implies P_M'(z)= \sum_{k=0}^{\infty}g(k) kz^{k-1} P M ( z ) = k = 0 ∑ ∞ g ( k ) z k ⟹ P M ′ ( z ) = k = 0 ∑ ∞ g ( k ) k z k − 1
and so
∑ i = 0 ∞ f ( k ) k z k − 1 = a ( ∑ i = 0 ∞ f ( k ) k z k − 1 ) ( ∑ k = 0 ∞ g ( k ) z k ) + ( a + b ) ( ∑ k = 0 ∞ g ( k ) k z k − 1 ) ( ∑ i = 0 ∞ f ( k ) z k ) \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) i = 0 ∑ ∞ f ( k ) k z k − 1 = a ( i = 0 ∑ ∞ f ( k ) k z k − 1 ) ( k = 0 ∑ ∞ g ( k ) z k ) + ( a + b ) ( k = 0 ∑ ∞ g ( k ) k z k − 1 ) ( i = 0 ∑ ∞ f ( k ) z k )
and so for coefficient z k − 1 z^{k-1} z k − 1 , we will have f ( k ) k f(k)k f ( k ) k on the left hand size and a ∑ i = 0 k f ( i ) i g ( k − i ) + ( a + b ) ∑ i = 0 k g ( i ) i f ( k − i ) a\sum_{i=0}^k f(i)ig(k-i) +(a+b)\sum_{i=0}^kg(i) if(k-i) a ∑ i = 0 k f ( i ) i g ( k − i ) + ( a + b ) ∑ i = 0 k g ( i ) i f ( k − i )
and so the right hand side is the following:
a ∑ i = 0 k i f ( i ) g ( k − i ) + ( a + b ) ∑ i = 0 k ( k − i ) g ( k − i ) f ( i ) = f ( k ) k ⟹ a ( ∑ i = 0 k − 1 i f ( i ) g ( k − i ) + k f ( k ) g ( 0 ) ) + ( a + b ) ∑ i = 0 k − 1 ( k − i ) g ( k − i ) f ( i ) = f ( k ) k ⟹ ( 1 − a g ( 0 ) ) k f ( k ) = a ∑ i = 0 k − 1 i f ( i ) g ( k − i ) + ( a + b ) ∑ i = 0 k − 1 ( k − i ) g ( k − i ) f ( i ) ⟹ k f ( k ) = 1 1 − a g ( 0 ) ∑ i = 0 k − 1 ( a i + ( a + b ) ( k − i ) ) g ( k − i ) f ( i ) = 1 1 − a g ( 0 ) ∑ i = 0 k − 1 ( a k + 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) a i = 0 ∑ k i f ( i ) g ( k − i ) + ( a + b ) i = 0 ∑ k ( k − i ) g ( k − i ) f ( i ) = f ( k ) k ⟹ a ( i = 0 ∑ k − 1 i f ( i ) g ( k − i ) + k f ( k ) g ( 0 ) ) + ( a + b ) i = 0 ∑ k − 1 ( k − i ) g ( k − i ) f ( i ) = f ( k ) k ⟹ ( 1 − a g ( 0 )) k f ( k ) = a i = 0 ∑ k − 1 i f ( i ) g ( k − i ) + ( a + b ) i = 0 ∑ k − 1 ( k − i ) g ( k − i ) f ( i ) ⟹ k f ( k ) = 1 − a g ( 0 ) 1 i = 0 ∑ k − 1 ( ai + ( a + b ) ( k − i )) g ( k − i ) f ( i ) = 1 − a g ( 0 ) 1 i = 0 ∑ k − 1 ( ak + b ( k − i )) g ( k − i ) f ( i )
and so we will have
f ( k ) = 1 1 − a g ( 0 ) ∑ i = 0 k − 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). f ( k ) = 1 − a g ( 0 ) 1 i = 0 ∑ k − 1 ( a + k b ( k − i ) ) g ( k − i ) f ( i ) .
For ( a , b , 1 ) (a,b,1) ( a , b , 1 ) class, we will have
k Pr [ N = k ] = ( a k + b ) Pr [ N = k − 1 ] k \Pr[N=k] = \left(ak+b\right)\Pr[N=k-1] k Pr [ N = k ] = ( ak + b ) Pr [ N = k − 1 ]
for k ≥ 2 k \ge 2 k ≥ 2 and so we will have the following
∑ k = 2 ∞ k Pr [ N = k ] P M ( z ) k − 1 P M ′ ( z ) = ∑ k = 2 ∞ ( a k − a + a + b ) ( P M ( z ) ) k − 1 P M ′ ( z ) Pr [ N = k − 1 ] ⟹ 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 ] ) \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]) k = 2 ∑ ∞ k Pr [ N = k ] P M ( z ) k − 1 P M ′ ( z ) = k = 2 ∑ ∞ ( ak − a + a + b ) ( P M ( z ) ) k − 1 P M ′ ( z ) Pr [ N = k − 1 ] ⟹ 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 P S ( z ) = ∑ i = 0 ∞ f ( k ) z k P_S(z) = \sum_{i=0}^{\infty} f(k) z^k P S ( z ) = ∑ i = 0 ∞ f ( k ) z k and P M ( z ) = P M ( z ) = ∑ k = 0 ∞ g ( k ) z k P_M(z) = P_M(z) = \sum_{k=0}^{\infty}g(k) z^k P M ( z ) = P M ( z ) = ∑ k = 0 ∞ g ( k ) z k , then we will have
f ( k ) k − p 1 k g ( k ) = a ( ∑ i = 0 k i f ( i ) g ( k − i ) ) + ( a + b ) ∑ i = 0 k − 1 ( k − i ) f ( i ) g ( k − i ) − ( a + b ) p 0 k g ( 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 − p 1 k g ( k ) = a ( i = 0 ∑ k i f ( i ) g ( k − i ) ) + ( a + b ) i = 0 ∑ k − 1 ( k − i ) f ( i ) g ( k − i ) − ( a + b ) p 0 k g ( k )
f ( k ) k = ( p 1 k − p 0 ( a + b ) k ) g ( k ) + ∑ i = 0 k − 1 ( a i + ( a + b ) ( k − i ) ) f ( i ) g ( k − i ) + a k f ( k ) g ( 0 ) ⟹ f ( k ) = ( p 1 − p 0 ( a + b ) ) g ( k ) + ∑ i = 0 k − 1 ( a + b k − i k ) f ( i ) g ( k − i ) 1 − a g ( 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)} f ( k ) k = ( p 1 k − p 0 ( a + b ) k ) g ( k ) + i = 0 ∑ k − 1 ( ai + ( a + b ) ( k − i )) f ( i ) g ( k − i ) + ak f ( k ) g ( 0 ) ⟹ f ( k ) = 1 − a g ( 0 ) ( p 1 − p 0 ( a + b )) g ( k ) + ∑ i = 0 k − 1 ( a + b k k − i ) f ( i ) g ( k − i )
So
f ( k ) = ( p 1 − p 0 ( a + b ) ) g ( k ) + ∑ i = 1 k ( a + b i k ) f ( k − i ) g ( i ) 1 − a g ( 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)} f ( k ) = 1 − a g ( 0 ) ( p 1 − p 0 ( a + b )) g ( k ) + ∑ i = 1 k ( a + b k i ) f ( k − i ) g ( i )
Example. Develop the recursive formula for the case where the primary distribution is Poisson.
Recall that
Distribution A B p 0 Poisson 0 λ exp ( − λ ) Negative Binomial β 1 + β β 1 + β ( r − 1 ) ( 1 + β ) − r Binomial − q 1 − q ( n + 1 ) q 1 − q ( 1 − q ) n Geometric β 1 + β 0 ( 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} Distribution Poisson Negative Binomial Binomial Geometric A 0 1 + β β − 1 − q q 1 + β β B λ 1 + β β ( r − 1 ) ( n + 1 ) 1 − q q 0 p 0 exp ( − λ ) ( 1 + β ) − r ( 1 − q ) n ( 1 + β ) − 1
So we will have
f ( k ) = ∑ i = 1 k λ i k f ( k − i ) g ( i ) f(k) = \sum_{i=1}^{k} \frac{ \lambda i}{k} f(k-i)g(i) f ( k ) = i = 1 ∑ k k λi f ( k − i ) g ( i )
With starting value
f ( 0 ) = P N ( P M ( 0 ) ) = exp ( λ ( P M ( 0 ) − 1 ) ) f(0) = P_N(P_M(0)) = \exp(\lambda (P_M(0) -1)) f ( 0 ) = P N ( P M ( 0 )) = exp ( λ ( P M ( 0 ) − 1 )) .
Calculate the probabilities for the Poisson-ETNB distribution, where λ = 1 \lambda=1 λ = 1 for the Poisson distribution and the ETNB distribution has r = − 0.5 r=-0.5 r = − 0.5 and β = 1 \beta=1 β = 1 .
Previously,
Distribution A B p 0 Poisson 0 λ exp ( − λ ) Negative Binomial β 1 + β β 1 + β ( r − 1 ) ( 1 + β ) − r Binomial − q 1 − q ( n + 1 ) q 1 − q ( 1 − q ) n Geometric β 1 + β 0 ( 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} Distribution Poisson Negative Binomial Binomial Geometric A 0 1 + β β − 1 − q q 1 + β β B λ 1 + β β ( r − 1 ) ( n + 1 ) 1 − q q 0 p 0 exp ( − λ ) ( 1 + β ) − r ( 1 − q ) n ( 1 + β ) − 1
f ( k ) = ∑ i = 1 k i k f ( k − i ) g ( i ) f(k) = \sum_{i=1}^{k} \frac{ i}{k} f(k-i)g(i) f ( k ) = i = 1 ∑ k k i f ( k − i ) g ( i )
g ( k ) = ( 1 2 − 3 4 k ) g ( k − 1 ) g(k) =\left(\frac{1}{2} - \frac{3}{4k}\right) g(k-1) g ( k ) = ( 2 1 − 4 k 3 ) g ( k − 1 )
The original "distribution" has the following:
g 0 ( 0 ) = ( 1 + 1 ) 0.5 = 2 g_0(0) = (1+1)^{0.5} = \sqrt{2} g 0 ( 0 ) = ( 1 + 1 ) 0.5 = 2
g 0 ( 1 ) = ( 1 2 − 1.5 2 ) ⋅ ( 1 + 1 ) 0.5 = − 1 2 2 g_0(1) = \left(\frac{1}{2} - \frac{1.5}{2}\right) \cdot (1+1)^{0.5} = -\frac{1}{2 \sqrt 2} g 0 ( 1 ) = ( 2 1 − 2 1.5 ) ⋅ ( 1 + 1 ) 0.5 = − 2 2 1
g 0 ( 2 ) = − ( 1 2 − 3 8 ) 1 2 2 = − 2 32 g_0(2) = -(\frac{1}{2} - \frac{3}{8})\frac{1}{2 \sqrt 2}=-\frac{\sqrt 2}{32} g 0 ( 2 ) = − ( 2 1 − 8 3 ) 2 2 1 = − 32 2
So it's more or less
g 0 ( k ) = ( k − 1.5 k ) ( 1 2 ) k − 0.5 = Γ ( k − 1.5 + 1 ) Γ ( k + 1 ) Γ ( − 0.5 ) ( 1 2 ) k − 0.5 g_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} g 0 ( k ) = ( k k − 1.5 ) ( 2 1 ) k − 0.5 = Γ ( k + 1 ) Γ ( − 0.5 ) Γ ( k − 1.5 + 1 ) ( 2 1 ) k − 0.5
Notice that g 0 ( 2 ) = Γ ( 1.5 ) Γ ( 2 ) Γ ( − 0.5 ) ( 1 2 ) 2 − 0.5 = − 1 32 ( 1 2 ) − 0.5 = − 2 32 g_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} g 0 ( 2 ) = Γ ( 2 ) Γ ( − 0.5 ) Γ ( 1.5 ) ( 2 1 ) 2 − 0.5 = − 32 1 ( 2 1 ) − 0.5 = − 32 2 , which matches. And so back to the problem, we will have
g ( k ) = 1 1 − 2 Γ ( k − 0.5 ) Γ ( k + 1 ) Γ ( − 0.5 ) ( 1 2 ) k − 0.5 g(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} g ( k ) = 1 − 2 1 Γ ( k + 1 ) Γ ( − 0.5 ) Γ ( k − 0.5 ) ( 2 1 ) k − 0.5
So we will have recursive formula as
f ( k ) = ∑ i = 1 k i k f ( k − i ) g ( i ) = ∑ i = 1 k i k 2 1 − 2 Γ ( i − 0.5 ) Γ ( i + 1 ) Γ ( − 0.5 ) ( 1 2 ) i f ( 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) f ( k ) = i = 1 ∑ k k i f ( k − i ) g ( i ) = i = 1 ∑ k k i 1 − 2 2 Γ ( i + 1 ) Γ ( − 0.5 ) Γ ( i − 0.5 ) ( 2 1 ) 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 − p z ) ln ( 1 − p ) \frac{\ln (1-p z)}{\ln (1-p)} ln ( 1 − p ) ln ( 1 − p z )
Notice here p p p is constant.
And Poisson distribution has the following pgf:
exp ( λ ( z − 1 ) ) \exp(\lambda (z-1)) exp ( λ ( z − 1 ))
and so if we have them composed, we will have the following compound pgf:
exp ( λ ( ln ( 1 − p z ) ln ( 1 − p ) − 1 ) ) = exp ( λ ln ( ( 1 − p z ) / ( 1 − p ) ) ln ( 1 − p ) ) = ( 1 − p + p − p z 1 − p ) λ / ln ( 1 − p ) = ( 1 − p 1 − 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)} exp ( λ ( ln ( 1 − p ) ln ( 1 − p z ) − 1 ) ) = exp ( λ ln ( 1 − p ) ln (( 1 − p z ) / ( 1 − p )) ) = ( 1 − p 1 − p + p − p z ) λ / l n ( 1 − p ) = ( 1 − 1 − p p ( z − 1 ) ) λ / l n ( 1 − p )
which is a negative binomial distribution with r = − λ / ln ( 1 − p ) r=-\lambda/ \ln(1-p) r = − λ / ln ( 1 − p ) and β = p 1 − p \beta=\frac{p}{1-p} β = 1 − p p .
We can know from the previous discussion:
P M ( z ) = p 0 ( M ) + ( 1 − p 0 ( M ) ) p T ( z ) P^M(z)=p_0^{(M)}+\left(1-p_0^{(M)}\right) p^T(z) P M ( z ) = p 0 ( M ) + ( 1 − p 0 ( M ) ) p T ( z )
So we can always write a general pgf as
P ( z ) = f 0 + ( 1 − f 0 ) P T ( z ) . P(z) = f_0 +(1-f_0)P^T(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 P M ( z ; θ ) P_M(z ; \theta) P M ( z ; θ ) that satisfies the equation:
P N ( z ; θ ) = B [ θ ( z − 1 ) ] P_N(z ; \theta) = B[\theta(z-1)] P N ( z ; θ ) = B [ θ ( z − 1 )]
Here, θ \theta θ represents a parameter, and B ( z ) B(z) B ( z ) is a function that doesn't depend on θ \theta θ . Notably, the pgf contains θ \theta θ and z z z solely in the form of θ ( z − 1 ) \theta(z-1) θ ( z − 1 ) .
In such a situation, we can rewrite the pgf P S ( z ) P_S(z) P S ( z ) as a composition of pgfs, which is given by:
P S ( z ) = P N [ P M ( z ) ; θ ] P_S(z) = P_N[P_M(z) ; \theta] \quad P S ( z ) = P N [ P M ( z ) ; θ ]
The new pgf P S ( z ) P_S(z) P S ( z ) can also be expressed differently by using a zero-truncated pgf P M T ( z ) P_M^T(z) P M T ( z ) and a modified parameter θ ( 1 − f 0 ) \theta\left(1-f_0\right) θ ( 1 − f 0 ) , leading to the following alternative expression:
P S ( z ) = P N [ P M T ( z ) ; θ ( 1 − f 0 ) ] P_S(z) = P_N[P_M^T(z) ; \theta\left(1-f_0\right)] \quad P S ( z ) = P N [ P M T ( z ) ; θ ( 1 − f 0 ) ]
Proof.
We know that P N ( P M ( z ) ; θ ) = B [ θ ( P M ( z ) − 1 ) ] = B [ θ ( f 0 + ( 1 − f 0 ) P M T ( z ) − 1 ) ] = B [ θ ( 1 − f 0 ) P M T ( z ) − ( 1 − f 0 ) θ ] = B [ θ ( 1 − f 0 ) ( P M T ( z ) − 1 ) ] = P N [ P M T ( z ) ; θ ( 1 − f 0 ) ] . 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)]. P N ( P M ( z ) ; θ ) = B [ θ ( P M ( z ) − 1 )] = B [ θ ( f 0 + ( 1 − f 0 ) P M T ( z ) − 1 )] = B [ θ ( 1 − f 0 ) P M T ( z ) − ( 1 − f 0 ) θ ] = B [ θ ( 1 − f 0 ) ( P M T ( z ) − 1 )] = P N [ P M T ( z ) ; θ ( 1 − f 0 )] .
Determine the probabilities for a Poisson-zero-modified ETNB distribution where the parameters are λ , p 0 M , r , β \lambda, p_0^M, r, \beta λ , p 0 M , r , β
f ( k ) = λ k ∑ i = 1 k ( i ) f ( k − i ) g ( i ) 1 − P 0 M ⋅ 0 = λ k ∑ i = 1 k ( 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) f ( k ) = k λ 1 − P 0 M ⋅ 0 ∑ i = 1 k ( i ) f ( k − i ) g ( i ) = k λ i = 1 ∑ k ( i ) f ( k − i ) g ( i )
and
g ( i ) = 1 − p 0 M 1 − ( 1 + β ) − r Γ ( i + r ) Γ ( i + 1 ) Γ ( r ) ( 1 1 + β ) r ( β β + 1 ) i = 1 − p 0 M ( 1 + β ) r − 1 Γ ( i + r ) Γ ( i + 1 ) Γ ( r ) ( β β + 1 ) i g(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 g ( i ) = 1 − ( 1 + β ) − r 1 − p 0 M Γ ( i + 1 ) Γ ( r ) Γ ( i + r ) ( 1 + β 1 ) r ( β + 1 β ) i = ( 1 + β ) r − 1 1 − p 0 M Γ ( i + 1 ) Γ ( r ) Γ ( i + r ) ( β + 1 β ) i
And so
f ( k ) = λ k ∑ i = 1 k i f ( k − i ) 1 − p 0 M 1 − ( 1 + β ) − r Γ ( i + r ) Γ ( i + 1 ) Γ ( r ) ( 1 1 + β ) r ( β β + 1 ) i = λ k ∑ i = 1 k i f ( k − i ) 1 − p 0 M ( 1 + β ) r − 1 Γ ( i + r ) Γ ( i + 1 ) Γ ( r ) ( β β + 1 ) i f(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 f ( k ) = k λ i = 1 ∑ k i f ( k − i ) 1 − ( 1 + β ) − r 1 − p 0 M Γ ( i + 1 ) Γ ( r ) Γ ( i + r ) ( 1 + β 1 ) r ( β + 1 β ) i = k λ i = 1 ∑ k i f ( k − i ) ( 1 + β ) r − 1 1 − p 0 M Γ ( i + 1 ) Γ ( r ) Γ ( i + r ) ( β + 1 β ) i
and f ( 0 ) = exp ( p 0 M − λ ) . f(0) = \exp(p_0^M-\lambda). f ( 0 ) = exp ( p 0 M − λ ) .
Compound Poisson Class
Compound Poisson distributions are type of distributions satisfying the following:
P S ( z ) = exp ( λ ( P M ( z ) − 1 ) ) P_S(z) = \exp(\lambda(P_M(z)-1)) P S ( z ) = exp ( λ ( P M ( z ) − 1 ))
where P M ( z ) P_M(z) P M ( z ) is some other distribution.
Let's consider its moment generating function:
P S ( exp ( z ) ) = exp ( λ ( P M ( exp ( z ) ) − 1 ) ) P_S(\exp(z)) = \exp(\lambda(P_M(\exp(z))-1)) P S ( exp ( z )) = exp ( λ ( P M ( exp ( z )) − 1 ))
If we differentiate with respect to z z z , we will have
P S ′ ( exp ( z ) ) exp ( z ) = exp ( λ P M ( exp ( z ) ) − λ ) λ P M ′ ( exp ( z ) ) exp ( z ) P_S'(\exp(z)) \exp(z) = \exp(\lambda P_M(\exp(z))-\lambda) \lambda P_M'(\exp(z)) \exp(z) P S ′ ( exp ( z )) exp ( z ) = exp ( λ P M ( exp ( z )) − λ ) λ P M ′ ( exp ( z )) exp ( z )
So the first (central) moment will have
E S [ S ] = λ E M [ M ] \mathbb{E}_S[S] = \lambda\mathbb{E}_M[M] E S [ S ] = λ E M [ M ]
If we differentiate it twice, we will have
P S ′ ′ ( exp ( z ) ) exp ( z ) 2 + P S ′ ( exp ( z ) ) exp ( z ) = exp ( λ P M ( exp ( z ) ) − λ ) λ 2 P M ′ ( exp ( z ) ) 2 exp ( z ) 2 + exp ( λ P M ( exp ( z ) ) − λ ) λ P M ′ ′ ( exp ( z ) ) exp ( z ) 2 + exp ( λ P M ( exp ( z ) ) − λ ) λ P M ′ ( 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) P S ′′ ( exp ( z )) exp ( z ) 2 + P S ′ ( exp ( z )) exp ( z ) = exp ( λ P M ( exp ( z )) − λ ) λ 2 P M ′ ( exp ( z ) ) 2 exp ( z ) 2 + exp ( λ P M ( exp ( z )) − λ ) λ P M ′′ ( exp ( z )) exp ( z ) 2 + exp ( λ P M ( exp ( z )) − λ ) λ P M ′ ( exp ( z )) exp ( z )
Then we will have
E S [ S 2 ] + E S [ S ] = λ 2 E M [ M ] 2 + λ E M [ M 2 ] + λ E M [ 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] E S [ S 2 ] + E S [ S ] = λ 2 E M [ M ] 2 + λ E M [ M 2 ] + λ E M [ M ]
It means that
E S [ S 2 ] = λ 2 E M [ M ] 2 + λ E M [ M 2 ] \mathbb{E}_S[S^2] = \lambda^2 \mathbb{E}_M[M]^2 +\lambda \mathbb{E}_M[M^2] E S [ S 2 ] = λ 2 E M [ M ] 2 + λ E M [ M 2 ]
So the central moment is
E S [ S 2 ] − ( E S [ S ] ) 2 = λ E M [ M 2 ] . \mathbb{E}_S[S^2] - (\mathbb{E}_S[S])^2= \lambda \mathbb{E}_M[M^2]. E S [ S 2 ] − ( E S [ S ] ) 2 = λ E M [ M 2 ] .
The formula are growing exponentially complicated, let's see an alternative approach:
P S ′ ( z ) = exp ( λ P M ( z ) − λ ) λ P M ′ ( z ) P_S'(z) = \exp(\lambda P_M(z)-\lambda) \lambda P_M'(z) P S ′ ( z ) = exp ( λ P M ( z ) − λ ) λ P M ′ ( z )
P S ′ ′ ( z ) = exp ( λ P M ( z ) − λ ) λ 2 P M ′ ( z ) 2 + exp ( λ P M ( z ) − λ ) λ P M ′ ′ ( 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) P S ′′ ( z ) = exp ( λ P M ( z ) − λ ) λ 2 P M ′ ( z ) 2 + exp ( λ P M ( z ) − λ ) λ P M ′′ ( z )
P S ′ ′ ′ ( z ) = exp ( λ P M ( z ) − λ ) λ 3 P M ′ ( z ) 3 + 2 exp ( λ P M ( z ) − λ ) λ 2 P M ′ ′ ( z ) P M ′ ( z ) + exp ( λ M ( z ) − λ ) λ 2 P M ′ ′ ( z ) P M ′ ( z ) + exp ( λ P M ( z ) − λ ) λ P M ′ ′ ′ ( 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). P S ′′′ ( z ) = exp ( λ P M ( z ) − λ ) λ 3 P M ′ ( z ) 3 + 2 exp ( λ P M ( z ) − λ ) λ 2 P M ′′ ( z ) P M ′ ( z ) + exp ( λ M ( z ) − λ ) λ 2 P M ′′ ( z ) P M ′ ( z ) + exp ( λ P M ( z ) − λ ) λ P M ′′′ ( z ) .
If we set z z z to be 1, we will have
E N [ N ( N − 1 ) ( N − 2 ) ] = λ 3 E M [ M ] 3 + 2 λ 2 E M [ M ( M − 1 ) ] + λ 2 E M [ M ( M − 1 ) ] E M [ M ] + λ E M [ 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)]. E N [ N ( N − 1 ) ( N − 2 )] = λ 3 E M [ M ] 3 + 2 λ 2 E M [ M ( M − 1 )] + λ 2 E M [ M ( M − 1 )] E M [ M ] + λ E M [ M ( M − 1 ) ( M − 2 )] .
Notice that
P X ( z ) = ∑ k = 0 ∞ p k z k P_X(z) = \sum_{k=0}^{\infty}p_k z^k P X ( z ) = k = 0 ∑ ∞ p k z k
and if we differentiate n n n -times, we will have
∂ ∂ z n P X ( z ) ∣ z = 1 = ∑ k = n ∞ p k k ! ( k − n ) ! z k − 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) ] ∂ z n ∂ P X ( z ) z = 1 = k = n ∑ ∞ p k ( k − n )! k ! z k − n ∣ z = 1 = E [ P ( K , n )]
N ( N − 1 ) = N 2 − N N(N-1)= N^2 - N N ( N − 1 ) = N 2 − N and N ( N − 1 ) ( N − 2 ) = ( N 2 − N ) ( N − 2 ) = N 3 − N 2 − 2 N 2 + 2 N = N 3 − 3 N 2 + 2 N N(N-1)(N-2) = (N^2 -N)(N-2) = N^3 -N^2 - 2N^2 +2N = N^3 - 3N^2 +2N N ( N − 1 ) ( N − 2 ) = ( N 2 − N ) ( N − 2 ) = N 3 − N 2 − 2 N 2 + 2 N = N 3 − 3 N 2 + 2 N
So
E N [ N 3 ] − 3 E N [ N 2 ] + 2 E N [ N ] = λ 3 E M [ M ] 3 + 2 λ 2 ( E M [ M 2 ] − E M [ M ] ) + λ 2 ( E M [ M 2 ] − E M [ M ] ) E M [ M ] + λ ( E M [ M 3 ] − 3 E M [ M 2 ] + 2 E M [ 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]). E N [ N 3 ] − 3 E N [ N 2 ] + 2 E N [ N ] = λ 3 E M [ M ] 3 + 2 λ 2 ( E M [ M 2 ] − E M [ M ]) + λ 2 ( E M [ M 2 ] − E M [ M ]) E M [ M ] + λ ( E M [ M 3 ] − 3 E M [ M 2 ] + 2 E M [ M ]) .
We also know that
E N [ ( N − E [ N ] ) 3 ] = E N [ N 3 − 3 E [ N ] N 2 + 3 E N [ N ] 2 N − E N [ 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] E N [( N − E [ N ] ) 3 ] = E N [ N 3 − 3 E [ N ] N 2 + 3 E N [ N ] 2 N − E N [ N ] 3 ]
E N [ N 3 ] − 3 E N [ N ] E [ N 2 ] + 3 E N [ N ] 2 E N [ N ] + E N [ N ] 3 = λ 3 E M [ M ] 3 + 2 λ 2 ( E M [ M 2 ] − E M [ M ] ) + λ 2 ( E M [ M 2 ] − E M [ M ] ) E M [ M ] + λ ( E M [ M 3 ] − 3 E M [ M 2 ] + 2 E M [ M ] ) + 3 E N [ N 2 ] − 2 E N [ N ] − 3 E N [ N ] E [ N 2 ] + 3 E N [ N ] 2 E N [ N ] + E N [ 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 E N [ N 3 ] − 3 E N [ N ] E [ N 2 ] + 3 E N [ N ] 2 E N [ N ] + E N [ N ] 3 = λ 3 E M [ M ] 3 + 2 λ 2 ( E M [ M 2 ] − E M [ M ]) + λ 2 ( E M [ M 2 ] − E M [ M ]) E M [ M ] + λ ( E M [ M 3 ] − 3 E M [ M 2 ] + 2 E M [ M ]) + 3 E N [ N 2 ] − 2 E N [ N ] − 3 E N [ N ] E [ N 2 ] + 3 E N [ N ] 2 E N [ N ] + E N [ N ] 3
E N [ N 3 ] − 3 E N [ N ] E [ N 2 ] + 3 E N [ N ] 2 E N [ N ] − E N [ N ] 3 = 2 λ 2 ( E M [ M 2 ] − E M [ M ] ) + λ 2 ( E M [ M 2 ] − E M [ M ] ) E M [ M ] + λ ( E M [ M 3 ] − 3 E M [ M 2 ] ) + 3 E N [ N 2 ] − 3 E N [ N ] E [ N 2 ] + 3 E N [ N ] 2 E N [ 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] E N [ N 3 ] − 3 E N [ N ] E [ N 2 ] + 3 E N [ N ] 2 E N [ N ] − E N [ N ] 3 = 2 λ 2 ( E M [ M 2 ] − E M [ M ]) + λ 2 ( E M [ M 2 ] − E M [ M ]) E M [ M ] + λ ( E M [ M 3 ] − 3 E M [ M 2 ]) + 3 E N [ N 2 ] − 3 E N [ N ] E [ N 2 ] + 3 E N [ N ] 2 E N [ N ]
= 2 λ 2 E M [ M 2 ] − 2 λ 2 E M [ M ] + λ 2 E M [ M 2 ] E M [ M ] − λ 2 E M [ M ] 2 + λ E M [ M 3 ] − 3 λ E M [ M 2 ] + 3 E N [ N 2 ] − 3 E N [ N ] E [ N 2 ] + 3 λ 3 E M [ 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 = 2 λ 2 E M [ M 2 ] − 2 λ 2 E M [ M ] + λ 2 E M [ M 2 ] E M [ M ] − λ 2 E M [ M ] 2 + λ E M [ M 3 ] − 3 λ E M [ M 2 ] + 3 E N [ N 2 ] − 3 E N [ N ] E [ N 2 ] + 3 λ 3 E M [ M ] 3
Since we already know that
E N [ N 2 ] = λ 2 E M [ M ] 2 + λ E M [ M 2 ] \mathbb{E}_N[N^2] = \lambda^2 \mathbb{E}_M[M]^2 +\lambda \mathbb{E}_M[M^2] E N [ N 2 ] = λ 2 E M [ M ] 2 + λ E M [ M 2 ]
We will have
3 E N [ N 2 ] E N [ N ] = 3 λ E M [ M ] ( λ 2 E M [ M ] 2 + λ E M [ M 2 ] ) 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]) 3 E N [ N 2 ] E N [ N ] = 3 λ E M [ M ] ( λ 2 E M [ M ] 2 + λ E M [ M 2 ])
So the old equation equals to
2 λ 2 E M [ M 2 ] − 2 λ 2 E M [ M ] − 2 λ 2 E M [ M 2 ] E M [ M ] + λ E M [ M 3 ] + 2 λ 2 E M [ M ] 2 2\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 2 λ 2 E M [ M 2 ] − 2 λ 2 E M [ M ] − 2 λ 2 E M [ M 2 ] E M [ M ] + λ E M [ M 3 ] + 2 λ 2 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 S k = E [ S k ] S_k = \mathbb{E}[S^k] S k = E [ S k ] for k ≥ 1 k \ge 1 k ≥ 1 and the same definition for M M M .
Then we will have S = λ M S = \lambda M S = λ M , here we omit 1 1 1 for the sake of simplicity and we know the numerical interpretation and probability interpretation are different.
P S ′ ′ ( z ) = e λ ( P M ( z ) − 1 ) λ 2 ( P M ′ ( z ) ) 2 + λ e λ ( P M ( z ) − 1 ) P M ′ ′ ( 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) P S ′′ ( z ) = e λ ( P M ( z ) − 1 ) λ 2 ( P M ′ ( z ) ) 2 + λ e λ ( P M ( z ) − 1 ) P M ′′ ( z )
which means S 2 = λ 2 M 2 + λ M 2 S_2 = \lambda^2 M^2 + \lambda M_2 S 2 = λ 2 M 2 + λ M 2
And if we differentiate, we will get
P S ′ ′ ′ ( z ) = e λ ( P M ( z ) − 1 ) λ 3 ( P M ′ ( z ) ) 3 + 2 ( e λ ( P M ( z ) − 1 ) λ 2 ( P M ′ ( z ) ) P M ′ ′ ( z ) ) + λ 2 e λ ( P M ( z ) − 1 ) P M ′ ( z ) P M ′ ′ ( z ) + λ e λ ( P M ( z ) − 1 ) P M ′ ′ ′ ( 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) P S ′′′ ( z ) = e λ ( P M ( z ) − 1 ) λ 3 ( P M ′ ( z ) ) 3 + 2 ( e λ ( P M ( z ) − 1 ) λ 2 ( P M ′ ( z )) P M ′′ ( z )) + λ 2 e λ ( P M ( z ) − 1 ) P M ′ ( z ) P M ′′ ( z ) + λ e λ ( P M ( z ) − 1 ) P M ′′′ ( z )
And so we will have
S 3 − 3 S 2 + 2 S = λ 3 M 3 + 2 λ 2 M ( M 2 − M ) + λ 2 M ( M 2 − M ) + λ ( M 3 − 3 M 2 + 2 M ) = λ 3 M 3 + 2 λ 2 M M 2 − 2 λ 2 M 2 + λ 2 M M 2 − λ 2 M 2 + λ M 3 − 3 λ M 2 + 2 λ M = λ 3 M 3 + 3 λ 2 M M 2 − 3 λ 2 M 2 + λ M 3 − 3 λ M 2 + 2 λ M S_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 S 3 − 3 S 2 + 2 S = λ 3 M 3 + 2 λ 2 M ( M 2 − M ) + λ 2 M ( M 2 − M ) + λ ( M 3 − 3 M 2 + 2 M ) = λ 3 M 3 + 2 λ 2 M M 2 − 2 λ 2 M 2 + λ 2 M M 2 − λ 2 M 2 + λ M 3 − 3 λ M 2 + 2 λ M = λ 3 M 3 + 3 λ 2 M M 2 − 3 λ 2 M 2 + λ M 3 − 3 λ M 2 + 2 λ M
S 3 = λ 3 M 3 + 3 λ 2 M M 2 + λ M 3 S_3 = \lambda^3 M^3 +3\lambda^2 MM_2 +\lambda M_3 S 3 = λ 3 M 3 + 3 λ 2 M M 2 + λ M 3
S 3 − 3 S 2 S + 2 S 3 = λ 3 M 3 + 3 λ 2 M M 2 + λ M 3 − 3 λ M ( λ 2 M 2 + λ M 2 ) + 2 λ 3 M 3 = λ M 3 S_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 S 3 − 3 S 2 S + 2 S 3 = λ 3 M 3 + 3 λ 2 M M 2 + λ M 3 − 3 λ M ( λ 2 M 2 + λ M 2 ) + 2 λ 3 M 3 = λ 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
γ 1 = S 3 − 3 S 3 S + 2 S 3 ( S 2 − S 2 ) 3 / 2 = λ M 3 λ 3 / 2 M 2 3 / 2 = M 3 λ 1 / 2 M 2 3 / 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}}. γ 1 = ( S 2 − S 2 ) 3/2 S 3 − 3 S 3 S + 2 S 3 = λ 3/2 M 2 3/2 λ M 3 = λ 1/2 M 2 3/2 M 3 .
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. f ( z ) = ( 1 + q ( exp ( z ) − 1 ) ) n .
If we take derivative, we will get
∂ ∂ z f ( z ) = n ( 1 + q ( exp ( z ) − 1 ) ) n − 1 q exp ( z ) \frac{\partial}{\partial z} f(z) = n (1 + q(\exp(z)-1))^{n-1} q \exp(z) ∂ z ∂ f ( z ) = n ( 1 + q ( exp ( z ) − 1 ) ) n − 1 q exp ( z )
and so S = λ n q S=\lambda n q S = λn q .
If we take derivative again, we will get
∂ ∂ 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 ) \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) ∂ 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 S 2 = λ ( n ( n − 1 ) q 2 + n q ) = λ n q ( 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) S 2 = λ ( n ( n − 1 ) q 2 + n q ) = λn q ( 1 + ( n − 1 ) q ) = S ( 1 + ( n − 1 ) q )
And if we take another derivative, we will have
∂ ∂ z 3 f ( z ) = n ( n − 1 ) ( n − 2 ) ( 1 + q ( exp ( z ) − 1 ) ) n − 3 q 3 exp ( 3 z ) + 2 n ( n − 1 ) ( 1 + q ( exp ( z ) − 1 ) ) n − 2 q 2 exp ( 2 z ) + n ( n − 1 ) ( 1 + q ( exp ( z ) − 1 ) ) n − 2 q 2 exp ( 2 z ) + n ( 1 + q ( exp ( z ) − 1 ) ) n − 1 q exp ( 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) ∂ z 3 ∂ f ( z ) = n ( n − 1 ) ( n − 2 ) ( 1 + q ( exp ( z ) − 1 ) ) n − 3 q 3 exp ( 3 z ) + 2 n ( n − 1 ) ( 1 + q ( exp ( z ) − 1 ) ) n − 2 q 2 exp ( 2 z ) + n ( n − 1 ) ( 1 + q ( exp ( z ) − 1 ) ) n − 2 q 2 exp ( 2 z ) + n ( 1 + q ( exp ( z ) − 1 ) ) n − 1 q exp ( z )
So we will have
M 3 = n ( n − 1 ) ( n − 2 ) q 3 + 2 n ( n − 1 ) q 2 + n ( n − 1 ) q 2 + n q = n ( n − 1 ) ( n − 2 ) q 3 + 3 n ( n − 1 ) q 2 + n q M_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 M 3 = n ( n − 1 ) ( n − 2 ) q 3 + 2 n ( n − 1 ) q 2 + n ( n − 1 ) q 2 + n q = n ( n − 1 ) ( n − 2 ) q 3 + 3 n ( n − 1 ) q 2 + n q
So notice M 2 − M = M ( ( n − 1 ) q ) M_2 -M = M((n-1)q) M 2 − M = M (( n − 1 ) q ) so ( M 2 − M ) 2 = M 2 ( n − 1 ) 2 q 2 (M_2 - M)^2 = M^2 (n-1)^2 q^2 ( M 2 − M ) 2 = M 2 ( n − 1 ) 2 q 2
So M 3 = M ( n − 1 ) ( n − 2 ) q 2 + 3 n ( n − 1 ) q 2 + 3 n q − 2 n q = M ⋅ ( M 2 − M ) 2 M 2 ⋅ n − 2 n − 1 + 3 M 2 − 2 M = ( M 2 − M ) 2 M ⋅ n − 2 n − 1 + 3 M 2 − 2 M . 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. M 3 = M ( n − 1 ) ( n − 2 ) q 2 + 3 n ( n − 1 ) q 2 + 3 n q − 2 n q = M ⋅ M 2 ( M 2 − M ) 2 ⋅ n − 1 n − 2 + 3 M 2 − 2 M = M ( M 2 − M ) 2 ⋅ n − 1 n − 2 + 3 M 2 − 2 M .
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 + β 1 − β ( z − 1 ) ) r − 1 ) = 1 1 − ( 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). f ( z ) = ( 1 + β ) r − 1 1 ( ( 1 − β ( z − 1 ) 1 + β ) r − 1 ) = 1 − ( 1 + β ) − r 1 ( ( 1 − β ( z − 1 ) ) − r − ( 1 + β ) − r ) .
So the Possion-ETNB distribution will have the following pgf:
e λ ( f ( z ) − 1 ) e^{\lambda (f(z)-1)} e λ ( f ( z ) − 1 )
If we take ln, we will have
λ ( f ( z ) − 1 ) = λ ( 1 1 − ( 1 + β ) − r ( ( 1 − β ( z − 1 ) ) − r − ( 1 + β ) − r − 1 + ( 1 + β ) − r ) ) = λ ( 1 − β ( z − 1 ) ) − r − 1 1 − ( 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) λ ( f ( z ) − 1 ) = λ ( 1 − ( 1 + β ) − r 1 ( ( 1 − β ( z − 1 ) ) − r − ( 1 + β ) − r − 1 + ( 1 + β ) − r ) ) = λ 1 − ( 1 + β ) − r ( 1 − β ( z − 1 ) ) − r − 1 = C (( 1 − β ( z − 1 ) ) − r − 1 )
So we have proven our example.