Apply polynomial theory to \(G(x)=0\) find roots and \(y_p\). And then take derivatives on \(y_p\), substitute back to original differential equation to get fixed values for constant coefficients.
Use complementary function to make particular solution.
Notation,
\[Dy = g(x)\]
\[y=\frac{1}{D}g(x)=\int g(x)dx\]
If \(y_1\) is a particular solution of \(f(D)y = G_1(x)\) and \(y_2\) is a particular solution of \(f(D)y = G_2(x)\) then
\[y = y_1 + y_2\]
is a particular solution of \(f(D)y = G_1(x) + G_2(x)\).
\(a_n\) is the nth coefficient in operator.
Case 1. \(a_n \ne 0\). The solution is \(y_p = G_0/a_n\).
Case 2. nth coefficient is zero, lowest order derivative down to \(k\),
\[y_p = \frac{G_0x^k}{k!a_{n-k}}\]