The possibility of stimulated light emission was discussed by Einstein
in 1917, eight years before the quantum-mechanical description of energy
levels of many-electron systems. Though it is imperative to use samples
having optical properties greatly different from the stan- dard
continuous spectrum of opaque objects ("black body" radia- tion) it is
not always necessary to restrict the study to monatomic entities. Thus,
spectral lines can be obtained (in absorption and in emission) from
lanthanide compounds, containing from one to thir- teen 4f electrons
going from trivalent cerium to ytterbium, that are nearly as sharp as
the ones from gaseous atoms. However, the presence of adjacent atoms
modifies the simple picture of an isolated electron configuration, and
in particular, it is possible to pump excited levels efficiently by
energy transfer from species with intense absorption bands, such as the
inter-shell transitions of other lanthanides and of thallium(I),
lead(II) and bismuth(III) or the electron transfer bands of the uranyl
ion or other complexes. On the other hand, it is possible to diminuish
the mUlti-phonon relaxation (competing with sharp line luminescence) by
selecting vitreous or crystalline materials with low phonon energies.
Obviously, one cannot circumvent the conservation of energy by lasers,
but they may have unprecedented consequences for the future by allowing
nuclear fusion of light elements, effects of non-linear optics and
time-resolved spectroscopy, besides the more conventional applications
of coherent light beams with negligible angular extension.