P.P. Sorokin, J.D. Axe, et al.
Journal of Applied Physics
A crystal of SrF2: Sm2+ was operated as a pulsed optical maser at temperatures close to 4.2°K. The 6969 output corresponds to the wavelength of an exceedingly sharp line (<0.6 cm-1) in which almost all of the low-temperature fluorescence is concentrated. In contrast to what prevails in CaF2: Sm+2 masers, the output is characterized by strong relaxation oscillations. This may be explained by the large difference in the fluorescent lifetimes in the two systems. While in CaF2: Sm2+ the value of is approximately 1.5×10-6 sec, in SrF2: Sm2+ it has a value of 15 msec. The reason for the large difference in values, in turn, depends upon the relative proximity of the long-wavelength edge of the red band to the position of the metastable D05 level from which fluorescence occurs. Absorption measurements taken at helium temperatures on SrF2: Sm2+ show that the lowest vibrational level of the lowest lying 4f-5d band lies 600 cm-1 above the position of the D05 level while in CaF2: Sm2+ there is near coincidence of the corresponding levels and consequently strong configurational mixing. Crystals of SrCl2: Sm2+ were also studied in this regard and display an expected close similarity in spectral characteristics to SrF2: Sm2+. The vibrational structure on the 4f-5d bands is much more pronounced, however, than in CaF2: Sm2+ and SrF2: Sm2+, indicating weaker coupling to the lattice in the excited 5d state. A tentative interpretation for the splitting of the red band seen in the absorption spectra of Sm2+ ions is given. © 1962 The American Physical Society.
P.P. Sorokin, J.D. Axe, et al.
Journal of Applied Physics
J.H. Glownia, J. Misewich, et al.
QELS 1989
S. Goldberg, D.S. Moore, et al.
Applied Physics B Photophysics and Laser Chemistry
J.H. Glownia, D.R. Gnass, et al.
SPIE OE/LASE 1993