In an important phenomenon that can occur when light and matter interact is the
phenomenon known as light amplification by stimulated emission of
radiation or laser (informally, ``laser'' is used as a noun,
so the verb would be ``lasing''). If a molecule (or atom) is excited
to a state of energy
it can decay back down to the ground state
and emit a photon of frequency
. The phase
of the emitted photon will generally be random so that if many molecules
or atoms in the state
emit photons, the phases will, on average,
have a random distribution leading to ordinary light. A second emission
process called stimulated emission can also operate between these
two energy states leading to photons that have the same phase and
travel in the same direction. This is laser light.
If a substance has energy states
and
, and we subject it to
radiation of frequency
, then each time a photon of this
radiation is absorbed, a molecule will be excited to the state
. If it is possible to have more molecules in the excited
state than in the ground state, we achieve a phenomenon known
as ``population inversion''. Moreover, if we can trap the beam
in the sample and simply pass it back and forth many times, then
the intensity of the beam will be amplified, giving the properties
of laser light. The population inversion is usually achieved by
``pumping'' in extral thermal energy or by a technique known as
``optical pumping''. The laser cavity is equipped with two
mirrors at either end of the cavity. When the first few photons
are emitted from the material, they stimulate the emission of more
photons, and the resulting wave is reflected back and forth
within the cavity, stimulating more photons as it passes through
the material. The mirrors ensure that the photons are all traveling
in the same direction (photons not traveling along the axis joining
the mirrors is simply not amplified) and eventually, their phases come into alignment.
If one of the mirrors is only partially reflecting, then some of the
coherent light can escape and be used for applications. The basic
principle of lasing is illustrated in the figure below: