Metastable states
A metastable state in an atom (i.e. excited electron) is not really stable in the sense that it has indefinite lifetime, but it simply means that the lifetime is longer than a normal transition to ground state. The life time can be on the order of microseconds or even milliseconds.
Much of the recent work regarding metastable states is in the area of noble gases (He, Ne, Ar, Kr, Xe) and has applications in lithography and etching of semiconductors. Noble gases do not necessarily form compounds. Other metastable states have been explored in alkali and alkali Earth metals, and these would form compounds. Certainly in compounds, the molecular orbitals would prevent atomic metastable states.
However, there are certainly solid state materials, like Ti-doped sapphire (Al
2O
3) in which meta-stable states are exploited for production of laser.
Here are some references. The Nobel Lecture by Willis Lamb is particularly noteworthy for its historical significance. Enjoy.
http://raptor.physics.wisc.edu/expts/fb.htm
Lithography with metastable rare gas atoms
http://physics.nist.gov/Divisions/Div841/Gp3/Projects/Atom/metasam_proj.html
Atoms join in the race for lithography in the next century
http://physicsweb.org/articles/world/11/8/3/1
http://www.iqo.uni-hannover.de/ertmer/nebec/
Towards Bose-Einstein Condensation of Neon
http://arxiv.org/abs/physics/0402108
A discrete time-dependent method for metastable atoms in intense fields
http://www.icpig.uni-greifswald.de/proceedings/data/Baguer_1 (pdf file)
Role of the fast atoms, ions and metastable Ar atoms in a HCD by ...
http://chemistry.anl.gov/ResearchHighlights-2001-2002/Young-Highlight-2001.pdf
Optical production of metastable rare gases (abstract)
"Metastable rare gas atoms have found wide use in fields spawned by the revolution
in laser manipulation of atoms, such as cold collision physics, optical lattices, atom
lithography, rare isotope detection, and, most recently, Bose-Einstein Condensation
(BEC). The high internal energy of the metastable atom enables both novel detection
schemes in BEC studies and localized surface damage of suitable resists, and thus
provides a niche beyond similar studies with ground state atoms."
http://nobelprize.org/physics/laureates/1955/lamb-lecture.pdf
Willis E. Lamb, Jr Nobel Lecture (1955) - impressive history
Fine structure of the hydrogen atom
http://ipstmail.umd.edu/Hill_Lab/pub/jphysb_19_359_86.pdf
Quenching of resonant laser-driven ionisation at high buffer gas pressures
http://vcs.abdn.ac.uk/ENGINEERING/lasers/amplification.html
For spontaneous emission of a photon, the probability of occurrence is inversely related to the average length of time that an atom can reside in the upper level of the transition before it relaxes
known as the SPONTANEOUS LIFETIME
- typically, the spontaneous lifetime is some tens of nanoseconds
- the shorter the spontaneous lifetime, the greater is the probability that spontaneous emission will occur
For some pairs of energy levels in certain materials
- the spontaneous lifetime can be of the order of microseconds to a few milliseconds,
which is a METASTABLE STATE
- the likelihood that a spontaneous transition will take place between these levels is relatively low
As the likelihood of spontaneous emission decreases the conditions which favour stimulated emission are enhanced
- if an atom is excited into a metastable state it can stay there long enough for a photon of the correct frequency to arrive
- this will stimulate the emission of a second photon
- input of one photon in yields two out