Page 185 - Handbook of Lasers
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Unlike crystals, which have a unique composition and structure, many glasses may be
                         formed in broad compositional ranges with varying parentages of glass network  formers
                         (e.g., silicate, phosphate, borate) and network modifiers (e.g., alkali ions, alkaline earths
                         ions). Compositional changes affect the stimulated emission cross sections, rates of radiative
                         and nonradiative transitions, crystalline field splittings, and inhomogeneous  broadening.
                         Although trivially small compositional changes might technically constitute a new host
                         material, the lasers listed in the tables in Section 1.2.2 are generally characterized by either
                         significantly different host glass compositions or different  operating  properties,  thus  the
                         tables are representative rather than exhaustive with respect to all glass lasers reported.

                            Because of site-to-site variations in the local fields in glass, there is a distribution of
                         energy  levels  and  transition  frequencies  that  appear  as  inhomogeneous  broadening  and
                         provide a small degree of tunability. Examples of reported tuning ranges of lanthanide-ion
                         glass lasers are shown in Figure 1.2.3.


                            Upconversion excitation  techniques  involving  multi-step  absorption,  energy  transfer,
                         excited state absorption, and photon avalanche have also been exploited for glass lasers.
                         Examples of upconversion pumping schemes that have been used for fluorozirconate fiber
                         lasers are given in Table 1.2.2.


                            In addition to glass laser operation involving a single transition, several cascade lasing
                         schemes have been demonstrated, although not as many as for crystalline lasers (see Table
                         1.1.1). These schemes for glass lasers are summarized in Table 1.2.3. In all cases the lasers
                         have utilized fluorozirconate fibers and have operated at room temperature.

                                             0.5           1.0            1.5           2.0           2.5           3.0

                                         Pr 3+ : fluorozirconate:


                                         Nd 3+ :silica:

                                         Ho 3+ : fluorozirconate:


                                         Er 3+ : fluorozirconate:


                                         Tm 3+ : fluorozirconate:


                                         Yb 3+ :silica:

                                            0.5           1.0            1.5           2.0           2.5           3.0
                                                                Wavelength ( mm)
                         Figure  1.2.3   Reported tuning ranges of lanthanide-ion glass lasers (see Tables for specific
                         wavelengths and host glasses).







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