Pulling the constant outside and completing the contour shift (which is valid because the Gaussian decays faster than any exponential), the remaining integral equals σ2π. Hence:
φX(t)=exp(iμt−21σ2t2).
Part 2 — Exponential
φX(t)=∫0∞λe−(λ−it)xdx=λ−itλfor all t∈R.
The integral converges because Re(λ−it)=λ>0 regardless of t. So φX(t)=λ/(λ−it).
This is the CF of a Poisson(λ1+λ2). By CF uniqueness, X1+X2∼Poisson(λ1+λ2) — the well-known Poisson-convolution rule, recovered as one line of CF algebra.
Takeaways
CFs convert density integrals into clean algebraic formulae. Memorise the Gaussian CF eiμt−σ2t2/2 — it appears everywhere.
CF multiplicativity encodes the convolution rule for sums of independents. Many "closed under addition" properties (normal, Poisson, gamma with same rate) are one-line CF arguments.
Complex-analysis contour shifts are the routine trick for Gaussian-type CFs. Beyond sketchable here, but good to be aware of when deriving CFs of more general distributions.