Because the plates are rigid, both bars have the same total elongation. Let $\delta$ be that common elongation.
For each bar,
$$
F_i = k_i(\delta - \delta_{th,i}), \quad k_i = \frac{AE_i}{L}
$$
Compute the stiffnesses:
$$
k_s = \frac{400(200\,000)}{800} = 100\,000\ \text{N/mm}
$$
$$
k_a = \frac{400(70\,000)}{800} = 35\,000\ \text{N/mm}
$$
Compute the free thermal expansions:
$$
\delta_{th,s} = (12 \times 10^{-6})(800)(10) = 0.12\ \text{mm}
$$
$$
\delta_{th,a} = (23 \times 10^{-6})(800)(10) = 0.23\ \text{mm}
$$
Force equilibrium gives
$$
F_s + F_a = 18\,000
$$
and
$$
100\,000(\delta - 0.12) + 35\,000(\delta - 0.23) = 18\,000
$$
So
$$
135\,000\delta = 38\,050
$$
$$
\delta \approx 0.282\ \text{mm}
$$
Now compute the forces:
$$
F_s = 100\,000(0.282 - 0.12) \approx 16.2\ \text{kN}
$$
$$
F_a = 35\,000(0.282 - 0.23) \approx 1.8\ \text{kN}
$$
So the steel bar carries about $16.2\ \text{kN}$ and the aluminum bar carries about $1.8\ \text{kN}$.