I feel the solution to this problem is simple - but I am not entirely clear on what the question actually wants.
Given the following:
$$A = \left[ \begin{array}{ccc} -0.1005 & -0.266\\ -0.1498 & 0.2005 \end{array} \right] $$
$$\frac{dx}{dt} = Ax; $$ $$x(0) = x0 = [1; −2]$$
Show, in general, that the following form solves $\frac{dx}{dt} = Ax$
i)
$$ x(t) = e^{At}x_0$$
ii)
$$x(t) = \sum_{i}a_i e_i e^{\lambda_it}$$
Usually when I come across a problem I don'tt even understand, I try to solve simpler analogous problems. I can't quite find one comparable to this. Can someone point out the first couple of steps for me? Maybe for i), for example?
Given $x(t) = e^{At} x_0$, we have
$$\begin{align} x'(t) &= A ~ e^{At} x_0 \\ &= A~x(t) ~\Large\color{\green}{\unicode{10004}}\end{align}$$
From eigenvalues / eigenvectors, we know $\lambda_1 v_1 = Av_1, \lambda_2 v_2 = A v_2$ (this is in your book).
Given $\displaystyle x(t) = \sum_{i}c_i e^{\lambda_it} v_i$, we have
$$\begin{align} x'(t) &= \left(\displaystyle \sum_{i}c_i e^{\lambda_it} v_i\right)' \\ & = (c_1 e^{\lambda_1 t}v_1 + c_2 e^{\lambda_2 t} v_2)' \\ & = c_1 e^{\lambda_1 t} \lambda_1 v_1 + c_2 e^{\lambda_2 t} \lambda_2 v_2 \\ & = c_1 e^{\lambda_1 t} A v_1 + c_2 e^{\lambda_2 t} A v_2 \\ & = A(c_1 e^{\lambda_1 t}v_1 + c_2 e^{\lambda_2 t} v_2)\\ & = A~x(t) ~\Large\color{\green}{\unicode{10004}} \end{align}$$
For this particular problem, we have
$$A = \begin{bmatrix} -0.1005 & -0.266\\ -0.1498 & 0.2005 \end{bmatrix}, x(0) = x_0 = \begin{bmatrix} 1\\ -2 \end{bmatrix} $$
The solution is given by
$$x(t) = e^{At} x_0 = \left( \begin{array}{c} 1.26302 e^{0.299994 t}-0.263018 e^{-0.199994 t} \\ -0.0983787 e^{-0.199994 t}-1.90162 e^{0.299994 t} \\ \end{array} \right)$$
Note $A = P D P^{-1}, e^{At} = Pe^{Dt} P^{-1}$, can you find the eigenvalues / eigenvectors, matrix exponential and that $x(t)$?