There are mechanisms by which a radioactive substance can produce light without surrounding gas. The particles (alpha, beta and gamma) are generally
emitted inside the radioactive material (e.g. radium chloride) and are capable of ionizing atoms on the way out. These will then fall back to their
ground states, emitting photons, some of which may be optical. Also, when a charged particle is emitted from a nucleus (alpha, beta) the charge of
the nucleus changes, and the electron cloud in the atom has to adjust itself to the new nuclear charge. In more detail, this means that the ground
state of the atom with the old nucleus is not the ground state of the atom with the new nucleus; it is a linear combination of the new ground state
plus various excited states; the latter then decay toward the ground state, emitting photons. Also, if the nucleus emits an alpha particle, then the
atom left behind has too many electrons, for example, neutral Ra emits an alpha and produces Rn--. Surely Rn, a noble gas, does not have a stable
ion Rn--; rather, the two extra electrons are freed, with some energy to spare. These are capable of producing a photon by several mechanisms.
Finally, when a charged particle is emitted, there is a certain probability for a photon to be emitted at the same time; this may well be a higher
energy photon, but it could be optical.
None of this is to say that the light emitted is in the visible range (some of it is, some not), or that the intensity is enough to be comparable to
the light produce by ionization of surrounding gas. |