Throughout, N denotes the natural numbers, N0=N∪{0} the nonnegative integers as in the statement, and R the real numbers; λ, Λ, and N are as in the statement, and we use the properties of Λ recorded in Stochastic Process, Independent Increments, and Inhomogeneous Poisson Process: Λ(0)=0, Λ is nondecreasing, and Λ(t)−Λ(s)=∫stλ(u)du. From Basic Properties of the Exponential Function we use that exp is positive, exp′=exp, exp(u+v)=exp(u)exp(v), and the defining series.
Step 1 (Claim 1 and initial values). For t>0, condition 3 of Stochastic Process, Independent Increments, and Inhomogeneous Poisson Process with s=0 together with condition 1 gives that Nt=Nt−N0 has the Poisson distribution with parameter Λ(t)−Λ(0)=Λ(t); hence, since {k} is a Borel set,
pk(t)=P(Nt∈{k})=PΛ(t)({k})=exp(−Λ(t))k!Λ(t)k.
For t=0: N0=0, so p0(0)=1 and pk(0)=0 for k≥1, which agrees with the displayed formula since Λ(0)=0, exp(0)=1, and the conventions 0!=1 and 00=1 of Poisson Distribution, while 0k=0 for k≥1. This proves Claim 1 and the stated initial values.
Step 2 (derivative of Λ). By Fundamental Theorem of Calculus, Part I in One Dimension applied on [0,T] for any T>t, Λ has derivative Λ′(t)=λ(t) at every t>0; in particular Λ is continuous and, since λ is continuous, Λ is a C1 map on the open set (0,∞). At t=0 we use a direct squeeze: for h>0, let mh and Mh be the minimum and maximum of λ on [0,h] (Extreme Value Theorem on a Compact Interval); every lower and upper sum of λ on [0,h] lies between mhh and Mhh, so mh≤Λ(h)/h≤Mh, and by continuity of λ at 0 both bounds tend to λ(0) as h↓0; hence Λ(h)/h→λ(0) and Λ(h)→0.
Step 3 (Claim 2 for t>0). Fix t>0. By the one-dimensional chain rule and exp′=exp, the function t↦exp(−Λ(t)) has derivative −λ(t)exp(−Λ(t)). By the product rule for real functions — (fg)′(x)=f′(x)g(x)+f(x)g′(x), from the factorization f(x+s)g(x+s)−f(x)g(x)=(f(x+s)−f(x))g(x+s)+f(x)(g(x+s)−g(x)) and limit arithmetic (Derivative at an Interior Point) — and induction on k, the function t↦Λ(t)k has derivative kΛ(t)k−1λ(t) for k≥1. Hence for k≥1, using k/k!=1/(k−1)! (Factorial of a Natural Number and the convention 0!=1),
pk′(t)=exp(−Λ(t))(−λ(t)k!Λ(t)k+λ(t)k!kΛ(t)k−1)=λ(t)(pk−1(t)−pk(t)),
and for k=0, p0′(t)=−λ(t)p0(t).
Step 4 (Claim 2 at t=0). From the defining series, ∣exp(−u)−1+u∣≤u2 for 0≤u≤1: the remainder is ∑j≥2(−u)j/j!, bounded in absolute value by u2∑j≥21/j!≤u2. By Step 2, u=Λ(h)→0 as h↓0, so for small h>0,
hp0(h)−p0(0)=hexp(−Λ(h))−1=−hΛ(h)+hR(h),∣R(h)∣≤Λ(h)2,
and Λ(h)2/h=(Λ(h)/h)⋅Λ(h)→λ(0)⋅0=0; hence the one-sided derivative is p0′(0)=−λ(0)=−λ(0)p0(0). For k≥1, pk(0)=0 and
hpk(h)−pk(0)=exp(−Λ(h))⋅k!1⋅hΛ(h)⋅Λ(h)k−1 ⟶ {λ(0),0,k=1,k≥2,
which equals λ(0)(pk−1(0)−pk(0)) in both cases. This proves Claim 2.
Step 5 (Claim 3). Let (qk)k∈N0 be as in Claim 3 and set rk=qk−pk; each rk is differentiable in the same sense with rk(0)=0, and by subtracting the two systems,
r0′=−λr0,rk′=λrk−1−λrk(k≥1).
We show rk≡0 by induction on k. In the base case k=0, and in the inductive step where rk−1≡0, the relevant equation is rk′=−λrk on all of [0,∞). Consider φ(t)=rk(t)exp(Λ(t)). By the product and chain rules exactly as in Step 3, for every t>0,
φ′(t)=(rk′(t)+λ(t)rk(t))exp(Λ(t))=0.
Fix t>0. The function φ is continuous on [0,t] (differentiable functions are continuous, one-sidedly at the endpoints, directly from the difference-quotient limit) and differentiable on (0,t) with zero derivative, so Mean Value Theorem in One Dimension gives ξ∈(0,t) with φ(t)−φ(0)=φ′(ξ)t=0. Hence φ(t)=φ(0)=rk(0)exp(0)=0 for all t≥0, and since exp(Λ(t))>0 we get rk≡0. By induction, qk=pk for every k∈N0. ■