Page 319 - Tunable Lasers Handbook
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6  Transition Metal Solid-State Lasers   279
                        Quantum  efficiency  data  for these  laser  materials  are  complicated  by  the
                     varying definitions found in the literature. However, quantum efficiency, defined
                     as the  fraction  of  the  active  atoms  in  the  upper  laser  manifold  that  decay  by
                     direct emission  of  a photon,  is expected to be  low. For example, for a  similar
                     laser material,  Co:KMgF3. the  quantum  efficiency  even  at cryogenic  tempera-
                     tures has been estimated as only 0.7 [59]. Low values of the quantum efficiency
                     tend to indicate the presence of strong nonradiative decay.
                        Upper laser level lifetime is strongly temperature dependent. For Ni:MgF,.
                     the  upper laser level  lifetime drops precipitously  as the  temperature increases.
                     Lifetimes are  12.8. 11.5, and 3.7 ms at 20, 77, and 295 KI respectively  [60]. At
                     very  low  temperatures,  the  upper  laser  level  lifetime  of  Co:MgF7 is relatively
                     long,  about  1.8 ms.  However, above  about  80 K, the lifetime begins  to fall as
                     shown in Fig. 29 [61]. At room temperature. the upper laser level lifetime is only
                     about 36 ps.
                        Polarized emission spectra of Ni:MgF, - (Fig. 30j extend between  1.5 and 1.9
                     pm. At cryogenic temperatures, a strong emission feature occurs for both polar-
                     izations at about  1.54 pm [62]. This emission feature is associated with a pure
                     electronic transition. On the long-wavelength side of the electronic transition are
                     vibronic transitions. At low temperatures the TC polarized spectra is stronger than
                     the 0 polarized spectra. Relatively broad peaks can be observed in the nominal
                     vibronic transitions. As the temperature increases, these peaks tend to disappear
                     and the emission spectra become smoother.
                        Polarized  emission  spectra  of  CoMgF,  (Fig.  31)  display  broad  peaks
                     around  1.9 pm and relatively  sharp line spectia only at cryogenic temperatures.
                     At cryogenic temperatures,  around  80 K, six peaks  in the fluorescence  can be
                     observed.  These  peaks  are  associated  with  the  six  components  of  the  ground




                                   100,000 =-
                                                               rn  Co: MgFr
                                 A
                                 n"  10,000~
                                 f
                                  0
                                 u
                                 3  ,,ooo,
                                 2
                                  0
                                 ._
                                 5. 100:
                                 E"
                                 ._
                                 c    '0:
                                 0
                                 !e
                                 -I
                                       1 --
                                               I     I      I     I
                                              100   200    300    400     0
                                                   Temperature (K)
                     FIGURE  29  Upper laser level lifetime of Co:hlgF,.  Co:KhlgF,, Ni:hfgF,.  and V:M~F~ versus
                     temperature. (Courtesy of P. E Moulton, Schwanz Elecro-Optics.)
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