For an electron to hop between bands, an energy exchange must have occurred. In which case, by definition, it's not a conduction electron anymore (or hole, as the case may be).
The exact mechanics of recombination, scattering, electron-phonon interaction, defects/impurities, etc., I suppose aren't too important on an overview level (it's also been long enough since I worked with them that I'm rather rusty on these topics(!)).
Note that valence band electrons are not mobile by themselves; they are a bound state. They can only move when a vacancy arises -- an emergent behavior, which itself acts like a particle, hence we call it a pseudoparticle: a hole.
The conduction band is unbound (well, in relevant respects), so such an electron can simply move until bumped with enough energy to stop, or recombination occurs. In fact, both are necessary: a completely filled valence band means recombination is prohibited, because electrons are fermions which cannot occupy identical states, and filled states means no vacancy. Thus recombination can only occur (electron-hole annihilation), and the energy is exchanged through whatever applicable means; which might be an electron-phonon interaction (i.e. directly into thermal heat energy; and vice-versa, which is where spontaneous ionization comes from at T > 0), or emission of a photon (direct bandgap semiconductors), etc.
Ionization and recombination is a somewhat rare event, for room-temperature silicon; the half-life is on the order of several microseconds, and at diffusion drift rates, carriers can travel several micrometers. This is also why the concentration is minuscule, of course (~1010 cm-3; compare to atom density on the order of 1023 cm-3).
I don't recall a mechanism for conduction electrons to gain "super speed". Note that any excess energy is subject to rapid loss, as there are numerous exchange methods (e.g. electron-phonon) to sap that energy back down to the minimum; high energy electrons are only a short-range phenomena.
Excess energy is possible, of course; it is a conduction band after all, where energy levels within the band are practically a continuous variable, until the upper band edge. But travel distance at energy, is limited by available energy loss mechanisms.