Step 1: Identify the complementary solution.
The complementary solution is
\[
y_c=C_1e^{-x}+C_2e^{2x}
\]
Step 2: Find roots of auxiliary equation.
The roots are
\[
m=-1,\quad m=2
\]
Step 3: Form the auxiliary equation.
\[
(m+1)(m-2)=0
\]
\[
m^2-m-2=0
\]
Step 4: Compare with standard auxiliary equation.
For
\[
y''+\beta y'+\gamma y=0
\]
auxiliary equation is
\[
m^2+\beta m+\gamma=0
\]
So, comparing,
\[
\beta=-1,\qquad \gamma=-2
\]
Step 5: Find particular integral form.
Since \(e^{-x}\) is already part of complementary solution, particular solution is of the form
\[
y_p=\alpha xe^{-x}
\]
Step 6: Apply operator to \(xe^{-x}\).
For \(P(m)=m^2-m-2\), we use
\[
P'(m)=2m-1
\]
At \(m=-1\),
\[
P'(-1)=2(-1)-1=-3
\]
Thus,
\[
L(xe^{-x})=-3e^{-x}
\]
Step 7: Compare with right hand side.
\[
\alpha(-3e^{-x})=-e^{-x}
\]
\[
-3\alpha=-1
\]
\[
\alpha=\frac{1}{3}
\]
Now,
\[
\alpha(\beta+\gamma)=\frac{1}{3}(-1-2)
\]
\[
=\frac{1}{3}(-3)=-1
\]
\[
\boxed{-1.0}
\]