Publication | Closed Access
Relation between Absorption and Emission in the Region of the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>R</mml:mi></mml:math>Lines of Ruby
255
Citations
34
References
1965
Year
Optical MaterialsEngineeringLaser ApplicationsAbsorption SpectroscopyLuminescence PropertyMath XmlnsReciprocal LifetimesRadiative TransferOptical PropertiesAbsorption Cross SectionsPhotophysical PropertyBiophysicsPhotonicsPhysicsPhotonic MaterialsRadiative AbsorptionAtomic PhysicsRadiation TransportFluorescent LifetimeNatural SciencesSpectroscopyApplied PhysicsLight AbsorptionPhosphorescenceEmissivity
The study discusses how the measured absorption and emission properties of ruby R lines impact laser performance. The authors measured radiative efficiency, absorption cross sections, and fluorescent lifetimes of ruby R lines across 20–373 K, then compared reciprocal lifetimes in thin and thick crystals using Einstein relations to relate to integrated absorption. The measurements confirm detailed balance for ruby R lines to within 5 % at 20 and 77 K, set a 0.002 cm⁻¹ upper limit on Stokes shift, show the lines are mainly electric‑dipole, reveal strong polarization dependence of radiative efficiency, and find that absorption increases ~20 % from 20 to 373 K while 10–30 % of decay is nonradiative or outside the observed range.
We have measured the radiative efficiency (ratio of $R$-line photons to the total number of photons emitted) and absorption cross sections for the $R$ lines of dilute ruby, as a function of polarization and temperature between 20 and 373\ifmmode^\circ\else\textdegree\fi{}K. We have also measured the fluorescent lifetime from 20 to 373\ifmmode^\circ\else\textdegree\fi{}K in optically thin crystals, and from 20 to 273\ifmmode^\circ\else\textdegree\fi{}K in optically thick crystals. The difference between the reciprocal lifetimes in thin and thick crystals is directly comparable (via the Einstein relations) with the integrated absorption in the $R$ lines. This comparison shows that for the $R$ lines at 20 and 77\ifmmode^\circ\else\textdegree\fi{}K detailed balance holds to well within the experimental error of 5%, a precision never to our knowledge previously approached in solids. An upper limit of 0.002 ${\mathrm{cm}}^{\ensuremath{-}1}$ was placed on any Stokes shift of the ${R}_{1}$ line, confirming that it is a no-phonon line. Comparison of $\ensuremath{\sigma}$ and $\ensuremath{\alpha}$ spectra confirms that the $R$ lines and their vibronic satellites are predominately electric-dipole in character. The radiative efficiency of the $R$ lines is strongly polarization dependent, a result which differs from that of previous workers. Its temperature dependence agrees well with that calculated from the observed vibronic spectrum at 77\ifmmode^\circ\else\textdegree\fi{}K. The integrated absorption in the $R$ lines increases by about 20% between 20 and 373\ifmmode^\circ\else\textdegree\fi{}K. The absorption in the vibronic satellites on the high-frequency side of the $R$ lines appears to be weaker than the corresponding emission on the low-frequency side. The temperature variation of the lifetime agrees well with that calculated from the absorption and radiative efficiency, but about 10% of the decay at 77\ifmmode^\circ\else\textdegree\fi{}K and 30% at 373\ifmmode^\circ\else\textdegree\fi{}K is either nonradiative or by emission at wavelengths outside the range of observation. The implications of our results for laser work are discussed.
| Year | Citations | |
|---|---|---|
Page 1
Page 1