Page 287 - Tunable Lasers Handbook
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6  Transition Metal Solid-State Lasers   247

                         X primary disadvantage of Cr:A1,0,  is its three-lekel operating scheme. In a
                     three-level scheme, the levels are the ground level, the pump level, and the upper
                     laser level. Figure 9 depicts the situation. In this scheme, the loner laser level is
                     the ground level. For lasing to occur, the population density of the upper  laser
                     level has to be greater than the population density of the lower laser level. If the
                     population density of the upper laser level is higher than the population densit)
                     of the lower laser level. a populuiioii im,el-sion is said to exist. To achieve a pop-
                     ulation  inversion,  roughly  half  of  the  Cr atoms  must  be  pumped  to  the  upper
                     laser level, Pumping levels must be high in order for this to occur. If  a popuia-
                     tion inversion is achieved, laser action can only be sustained as locg as the popu-
                     lation inversion is maintained. Consequently,  when lasing terminates, all of the
                     remaining energy stored in the upper laser level is lost. A three-lecel laser is rel-
                     atively inefficient because of this. First, a great deal of pump energy is expended
                     to store enough energy in the upper laser level to achieve population inversion or
                     threshold. Second, of the energy stored in the upper laser level, only that portion
                     of it which is above threshold is available for laser output. Despite this limitation
                     on the efficiency of the Cr:AI,O,,  the use of these lasers continues to this da:y.
                        A120,, or sapphire. is a c&tal  composed of alternate hexagonal layers of A1
                     and 0 atoms, as shown in the Fig.  10. Oxygen atoms fill a layer in a close-packed
                     hexagonal arrangement. On top of  this layer is a layer of A1  atoms. which nestle
                     in the depressions between three adjacent 0 atoms of the loner layer. In a filled
                     layer, one-third of the potential AI  sites is left unfilled. 4 third layer is composed
                     of 0 atoms. again in a close-packed hexagonal arrangement. However, this layer
                     is displaced from the first layer. To  first-order approximation,  each A1 atom has
                     six  0 neighbors  in  an  octahedral  arrangement.  However,  since  the  distance
                     between the 0 layers is larger than the distance between 0 atoms within a layer.


                                    Pump
                                  Manifold
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