As usual next we construct two equations and solve for
k1 and
k2.
k1+k2=0
−k1−k2=0
We can choose
k1=1 then
k2=−1, but for
F U N we will choose
k1=4 so that
k2=−4. This is a good demonstration of that it does not matter what we choose as long as the two equations are satisfied! (Except of course the choice
k1=k2=0 which leads to the trivial solution that we don't want!)
This gives us the first solution which is:
X1=K1eλ1t=[4−4]et
But now we have a problem to find the second solution as
λ1=λ2.

With a careful study it was found out that when we have repeated eigenvalues, a second solution can be found with the following form:
X2=Peλ1t+Kteλ1t
This means that we only have to find
P and we are done!
Finding
P is the same way as finding
K, but its equations are non-homogeneous by
K values.
That is:
(A−λI)P=K
Or
p1+p2=4
−p1−p2=−4
We can even choose
p1=4 then
p2=0 but for
F U N we will choose
p1=1 so that
p2=3.
Then our second solution is:
X2=[13]et+[4−4]tet
And the general solution is:
X=c1X1+c2X2=c1[4−4]et+c2([13]et+[4−4]tet)

