Step 1: Use photons:
Think of the radiation as photons. Each photon of energy $\epsilon$ has momentum $\epsilon/c$. For a total energy $E$ the total momentum is $E/c$.
Step 2: Reflection:
A perfectly reflecting surface sends every photon straight back. So each photon changes its momentum from $+p$ to $-p$.
Step 3: Impulse on the surface:
The surface receives the momentum change, $2p$ per photon. Summed over all photons, \[ \Delta p_{surface} = 2 \times \frac{E}{c} \]
Step 4: Compare:
For an absorbing surface the value would be $E/c$. The reflecting case doubles this, so it is $2E/c$, the first option.
Final Answer:
The transferred momentum is $2E/c$.
\[ \boxed{\frac{2E}{c}} \]