Specular (mirror) reflection by metals of electromagnetic (EM) waves, including light, is not a quantum process. There are not absorbed and reemitted photons.
An EM wave has an alternating electric field that oscillates at the frequency of the wave. The limit condition of electric fields and perfect conductors is that the electric field in the perfect conductor must be zero. If not, the current should be infinite.
When free electrons in a metal "feel" an alternating electric field, they began to oscillate at the same frequency as the field. An oscillating electron radiates an EM wave polarized in the direction of its movement. That is, with the electric field parallel to the movement. This EM wave is radiates in all directions, with a maximum in the plane perpendicular to movement and a zero in the direction of movement.
In a perfect conductor, the amplitude of the emitted EM wave is identical to the incident wave. In a real metal the emitted wave is slightly smaller than the incident one.
The phase of the emitted EM wave is such that at the metal surface and in the metal side, the addition of the two waves is zero. In the incident wave side the two waves travel in opposite directions. Seen from outside one has the impression that the wave coming from the metal is the reflection of the incoming wave. It has the same frequency and amplitude. But, in reality, it is a wave that has been emitted by the metal electrons.
When the electric field is parallel to the surface of the mirror, the reemitted wave has the same polarization. When it is not the case the polarization of the reemitted wave is a little trickier.
There is not need of metals to obtain a "metallic" reflection: free electrons suffice. There are a lot of them in the ionospheric plasma. The ionosphere reflects radio waves at low radio frequencies (under a few MHz). And some metals can be transparent to light. The potassium is transparent to near UV.
Real metals are not perfect and their conductivity is frequency dependent. But except copper and gold, they reflect fairly uniformly in the visible band.