Multi-phonon Transitions | previous | next | feedback |
Definition: transitions between electronic levels of atoms or ions in solid media, caused by emission of multiple phonons
The upper-state lifetime in a solid-state gain medium, or more generally the lifetime of a metastable electronic state of a dopant ion in such a medium, can be strongly reduced by decay processes which involve the simultaneous emission of several phonons. Such a process is called a multi-phonon transition. Multiple phonons are typically required for such transitions because the energy of a single phonon is not sufficient to match the difference of level energies.
The rate of multi-phonon transition exponentially decreases with an increasing number of required phonons. As a consequence, a certain metastable state may exhibit a very strong reduction in its lifetime by multi-phonon emission if the host medium supports phonons with relatively high energy, whereas the same process may be negligible for a host medium with lower phonon energies. For that reason, many upconversion lasers work only with gain media which have small phonon energies, such as heavy metal glasses, so that sufficient lifetimes of certain energy levels are achieved. In other cases, however, high enough phonon energies are important if these are required for facilitating certain non-radiative transitions, which are needed e.g. to populate the upper laser level or to depopulate the lower laser level.
Some concrete examples for the importance of multi-phonon processes in laser gain media are:
- In neodymium-doped gain media, one typically pumps ions from their ground state to an excited state above the upper laser level. From there, multi-phonon transitions take them to the upper laser level (4F3/2). Also, the lower laser level of most four-level solid-state gain media is rapidly depopulated by multiphonon emission.
- Upconversion lasers based on erbium-doped or thulium-doped glass require heavy metal glasses (e.g. fluoride glasses) as host media, since high phonon energy glasses such as silica would lead to too low lifetimes of required metastable levels (→ multi-phonon quenching).
- The same holds for many mid-infrared lasers, e.g. 3-μm erbium-doped fiber lasers. Mid-infrared wavelengths require a small energy gap between upper and lower laser level, and sufficient upper-state lifetimes can be achieved only with low phonon energy materials, because otherwise the laser transition is bypassed by multi-phonon emission. Low phonon energies are also important for transparency in the mid-infrared wavelength region.
Bibliography
| [1] | L. A. Riseberg and H. W. Moos, "Multiphonon orbit-lattice relaxation of excited states of rare-earth ions in crystals", Phys. Rev. 174 (2), 429 (1968) |
| [2] | C. B. Layne et al., "Multiphonon relaxation of rare earth ions in oxide glasses", Phys. Rev. B 16 (1), 10 (1977) |
| [3] | Y. V. Orlovskii et al., "Multiple-phonon nonradiative relaxation: Experimental rates in fluoride crystals doped with Er", Phys. Rev. B 49 (6), 3821 (1994) |
See also: gain media, rare-earth-doped gain media, upconversion lasers, fluoride fibers, quenching
Category: physical foundations
