Recall a few known results involving the Laplace transform. Given a function

, if the transform exists, then denote it by

. We have



Let's put all this together by taking the transform of both sides of the ODE:


Here we use the third fact and immediately compute the transform of the right hand side (I'll leave that up to you).
Now we invoke the first listed fact:

Let

. From the second fact, we get

From the first fact, we get

so we're left with

To summarize, taking the Laplace transform of both sides of the ODE yields

Isolating

gives


All that's left is to take the inverse transform. I'll leave that to you as well. You should end up with something resembling
