Let us take Laplace transform of both sides of differential equation, using property of Laplace transform "L[y'] = s L[y] - y(0)" and table Laplace transform "L[e^{a t}] = \\frac{1}{s-a}" :
"s Y(s) - 3 + 4Y(s) = \\frac{6}{s-2}". Simplifying and solving for "Y(s)", obtain:
"Y(s)[s+4] = \\frac{6}{s-2} + 3 = \\frac{3 s}{s-2} \\Rightarrow Y(s) = \\frac{3 s}{(s+4)(s-2)}".
In order to take inverse Laplace transform, decompose the last expression into partial fractions:"\\frac{3 s}{(s+4)(s-2)} = \\frac{2}{s+4} + \\frac{1}{s-2}". Hence, using table Laplace transform "L[e^{a t}] = \\frac{1}{s-a}", obtain "y(t) = L^{-1}[Y(s)] = L^{-1}[\\frac{2}{s+4} + \\frac{1}{s-2}] = 2 e^{-4 t} + e^{2 t}".
It is straightforward to check that this is indeed the solution to given differential equation.
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