Solution
= Solution
Radiation has $w=1/3$, matter $w=0$, and a cosmological constant has constant density. With negligible curvature and present-day normalization,
$$
H^2=H_0^2\left(\frac{\Omega_{R0}}{a^4}+
\frac{\Omega_{M0}}{a^3}+\Omega_{\Lambda0}\right),
$$
where the present density fractions sum to one.