Oh, dear, oh dear, oh, dear! I really dislike the Laplace Transform! It can be used in two diametrically opposite ways- to "look up" solutions to non-homogeneous equations or to assert a form of a solution in very abstract theorems. The first is more easily done in other ways and the second, undergraduates never see.
I would look at that equation and immediately write down it characteristic equation:

. It's easy to see, by inspection, that r= 1 is a root of that and that
(r^2- 1)= (r- 1)^(r+ 1))
so that r= 1 is a double root and r= -1 is a root. That tells us that the general solution to the associated homogeneous equation is

.
The "non-homogeneos" part is

. Since

is already a solution to the associated homogeneous equation, we try a solution of the form
e^{-t})
. Then
e^{-t}- (At^2+ Bt)e^{-t}= (-At^2+ (A- B)t+ B)e^{-t})
,
t+ A- 2B)e^{-t})
, and
e^{-t}- (At^2+ (B- 3A)t+ A- 2B)e^{-t}= (-At^2+ (5A- B)t+ 3B- 5A)e^{-t})
.
Putting those into the differential equation will give you equations for A and B.