Y(s)=∫0∞e−sty(t)dt, with transforms sY−y(0) and s2Y−sy(0)−y˙(0); eλt transforms to (s−λ)−1 and δ to 1. Algebra gives Y=GH with H=F+(s+2γ)y(0)+y˙(0), so y=g∗h. Writing a=∣γ2−ω2∣ gives g=e−γtsinh(at)/a for γ>ω, e−γtsin(at)/a for γ<ω, and te−γt at equality. If y(0)=0, h=f+y˙(0)δ, so the initial velocity contributes y˙(0)g(t).